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<article xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:oasis="http://docs.oasis-open.org/ns/oasis-exchange/table" xml:lang="en" dtd-version="3.0"><?xmltex \makeatother\@nolinetrue\makeatletter?>
  <front>
    <journal-meta><journal-id journal-id-type="publisher">ACP</journal-id><journal-title-group>
    <journal-title>Atmospheric Chemistry and Physics</journal-title>
    <abbrev-journal-title abbrev-type="publisher">ACP</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Atmos. Chem. Phys.</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">1680-7324</issn><publisher>
    <publisher-name>Copernicus Publications</publisher-name>
    <publisher-loc>Göttingen, Germany</publisher-loc>
  </publisher></journal-meta>
    <article-meta>
      <article-id pub-id-type="doi">10.5194/acp-20-5679-2020</article-id><title-group><article-title>Thermodynamic properties of isoprene- and monoterpene-derived organosulfates estimated with COSMO<italic>therm</italic></article-title><alt-title>Thermodynamic properties of organosulfates</alt-title>
      </title-group><?xmltex \runningtitle{Thermodynamic properties of organosulfates}?><?xmltex \runningauthor{N. Hyttinen et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Hyttinen</surname><given-names>Noora</given-names></name>
          <email>noora.hyttinen@oulu.fi</email>
        <ext-link>https://orcid.org/0000-0002-6025-5959</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Elm</surname><given-names>Jonas</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-3736-4329</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Malila</surname><given-names>Jussi</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-7236-6528</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Calderón</surname><given-names>Silvia M.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Prisle</surname><given-names>Nønne L.</given-names></name>
          <email>nonne.prisle@oulu.fi</email>
        <ext-link>https://orcid.org/0000-0002-2041-6105</ext-link></contrib>
        <aff id="aff1"><label>1</label><institution>Nano and Molecular Systems Research Unit, University of Oulu, P.O. Box 3000, 90014 Oulu, Finland</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Department of Chemistry and iClimate, Aarhus University, Langelandsgade 140, 8000 Aarhus C, Denmark</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Noora Hyttinen (noora.hyttinen@oulu.fi), and Nønne L. Prisle (nonne.prisle@oulu.fi)</corresp></author-notes><pub-date><day>13</day><month>May</month><year>2020</year></pub-date>
      
      <volume>20</volume>
      <issue>9</issue>
      <fpage>5679</fpage><lpage>5696</lpage>
      <history>
        <date date-type="received"><day>25</day><month>November</month><year>2019</year></date>
           <date date-type="rev-request"><day>17</day><month>December</month><year>2019</year></date>
           <date date-type="rev-recd"><day>9</day><month>April</month><year>2020</year></date>
           <date date-type="accepted"><day>10</day><month>April</month><year>2020</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2020 </copyright-statement>
        <copyright-year>2020</copyright-year>
      <license license-type="open-access"><license-p>This work is licensed under the Creative Commons Attribution 4.0 International License. To view a copy of this licence, visit <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/4.0/">https://creativecommons.org/licenses/by/4.0/</ext-link></license-p></license></permissions><self-uri xlink:href="https://acp.copernicus.org/articles/.html">This article is available from https://acp.copernicus.org/articles/.html</self-uri><self-uri xlink:href="https://acp.copernicus.org/articles/.pdf">The full text article is available as a PDF file from https://acp.copernicus.org/articles/.pdf</self-uri>
      <abstract><title>Abstract</title>
    <p id="d1e127">Organosulfates make significant contributions to atmospheric secondary organic aerosol (SOA), but little is known about the thermodynamic properties of atmospherically relevant organosulfates. We have used the COSMO<italic>therm</italic> program to calculate both the gas- and condensed-phase properties of previously identified atmospherically relevant monoterpene- and isoprene-derived organosulfates. Properties include solubilities, activities and saturation vapor pressures, which are critical to the aerosol-phase stability and atmospheric impact of organosulfate SOA. Based on the estimated saturation vapor pressures, the organosulfates of this study can all be categorized as semi-volatile or low-volatile, with saturation vapor pressures 4 to 8 orders of magnitude lower than that of sulfuric acid. The estimated p<inline-formula><mml:math id="M1" display="inline"><mml:mrow><mml:msub><mml:mi>K</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> values of all the organosulfates indicate a high degree of dissociation in water, leading in turn to high dissociation-corrected solubilities. In aqueous mixtures with inorganic sulfate, COSMO<italic>therm</italic> predicts a salting-out of both the organosulfates and their sodium salts from inorganic co-solutes. The salting-out effect of ammonium sulfate (less acidic) is stronger than of ammonium bisulfate (more acidic). Finally, COSMO<italic>therm</italic> predicts liquid–liquid-phase separation in systems containing water and monoterpene-derived organosulfates. The COSMO<italic>therm</italic>-estimated properties support the observed stability of organosulfates as SOA constituents and their long-range transport in the atmosphere but also show significant variation between specific compounds and ambient conditions.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

      <?xmltex \hack{\newpage}?>
<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d1e164">Organosulfates (<inline-formula><mml:math id="M2" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">R</mml:mi><mml:mo>-</mml:mo><mml:msub><mml:mi mathvariant="normal">OSO</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub><mml:mi mathvariant="normal">H</mml:mi></mml:mrow></mml:math></inline-formula>, OS) have been identified as components of atmospheric secondary organic aerosol (SOA) from a variety of environments <xref ref-type="bibr" rid="bib1.bibx48 bib1.bibx16 bib1.bibx17" id="paren.1"/>. In the Amazon, the contribution of organic sulfate was found to be 3 %–42 % of the total aerosol sulfate for the compounds measured using aerosol mass spectrometry <xref ref-type="bibr" rid="bib1.bibx16" id="paren.2"/>. In Atlanta, Georgia, organosulfates accounted for 16.5 % of the total organic carbon of fine particulate matter (PM<inline-formula><mml:math id="M3" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula>) <xref ref-type="bibr" rid="bib1.bibx22" id="paren.3"/>.</p>
      <p id="d1e202">Multiple laboratory studies have shown that organosulfates are formed in the condensed phase from reactions between organic molecules and either a sulfate ion (<inline-formula><mml:math id="M4" display="inline"><mml:mrow class="chem"><mml:msubsup><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>-</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula>) <xref ref-type="bibr" rid="bib1.bibx25 bib1.bibx35" id="paren.4"/> or a sulfate radical (<inline-formula><mml:math id="M5" display="inline"><mml:mrow class="chem"><mml:msubsup><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn><mml:mrow><mml:mo>⋅</mml:mo><mml:mo>-</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula>) <xref ref-type="bibr" rid="bib1.bibx43 bib1.bibx55" id="paren.5"/>. Organosulfates have been seen to form, for instance, from oxidation products of monoterpenes <xref ref-type="bibr" rid="bib1.bibx49" id="paren.6"/> and pinonaldehyde <xref ref-type="bibr" rid="bib1.bibx34" id="paren.7"/> in the presence of acidified sulfate seed and from isoprene-derived organosulfates in the presence of sulfate <xref ref-type="bibr" rid="bib1.bibx12" id="paren.8"/>. Some studies have suggested that the formation of organosulfate correlates with the acidity of the aerosol particles <xref ref-type="bibr" rid="bib1.bibx5" id="paren.9"/> such that more dilute acidic sulfate aerosol leads to a lower reactive uptake of isoprene epoxydiol (<inline-formula><mml:math id="M6" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">C</mml:mi><mml:mn mathvariant="normal">5</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">10</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, IEPOX) <xref ref-type="bibr" rid="bib1.bibx62" id="paren.10"/>, while other studies suggest that the abundance of the formed organosulfates correlates only with the sulfate content in the aerosol <xref ref-type="bibr" rid="bib1.bibx61 bib1.bibx4" id="paren.11"/>.</p>
      <p id="d1e283">Recent measurements close to Beijing using a Filter Inlet for Gas and Aerosol (FIGAERO) chemical ionization mass<?pagebreak page5680?> spectrometer (CIMS) have shown that sulfur-containing organic compounds, such as organosulfates,
organosulfonates and nitrooxy organosulfates, can also be present in the gas phase <xref ref-type="bibr" rid="bib1.bibx32" id="paren.12"/>. Higher temperatures promote the presence of sulfur compounds in the gas phase, and furthermore the partitioning to the particle phase was found to be dependent on ambient relative humidity. In urban areas, such as Xi'an in northwestern China, organosulfates are primarily of anthropogenic origin <xref ref-type="bibr" rid="bib1.bibx23" id="paren.13"/>, but in semirural locations 40 km northwest of Beijing, up to 19 % of the sulfur-containing organics have been identified to be of biogenic origin <xref ref-type="bibr" rid="bib1.bibx32" id="paren.14"/>.</p>
      <p id="d1e295">Very little is known of the physicochemical properties of specific atmospherically relevant organosulfates and how they affect the properties of SOA. This is in part due to challenges related to sampling and isolating sufficient amounts of organosulfate material from atmospheric organic aerosol for the subsequent analysis of single component properties, as well as synthesizing adequate amounts of known organosulfate reference compounds. The hygroscopic properties of organosulfate-containing aerosol have been measured using sodium salts of alkane sulfates <xref ref-type="bibr" rid="bib1.bibx59 bib1.bibx15" id="paren.15"/> and limonene-derived organosulfates <xref ref-type="bibr" rid="bib1.bibx20" id="paren.16"/>. Limonene-derived organosulfate was demonstrated to lower the surface tension of aqueous solutions even more effectively than atmospherically relevant strong organic acids <xref ref-type="bibr" rid="bib1.bibx20" id="paren.17"/>. The effect of surface activity was evident in both subsaturated hygroscopic growth and measured cloud condensation nuclei (CCN) properties of limonene-derived organosulfate and its mixtures with ammonium sulfate <xref ref-type="bibr" rid="bib1.bibx20" id="paren.18"/>. The addition of organosulfates lowers the relative humidity of deliquescence and efflorescence transitions of sodium chloride aerosol <xref ref-type="bibr" rid="bib1.bibx15" id="paren.19"/>. In addition, <xref ref-type="bibr" rid="bib1.bibx36 bib1.bibx37" id="text.20"/> have seen indications of the long-range transport of organosulfates, suggesting that organosulfates must have sufficiently low volatilities to remain in the aerosol phase over a wide range of atmospheric conditions.</p>
      <p id="d1e318">In this study, we use the COSMO<italic>therm</italic> program to estimate different thermodynamic properties related to the gas- and condensed-phase equilibrium of organosulfates and IEPOX in both pure water and aqueous mixtures with ammonium sulfate (<inline-formula><mml:math id="M7" display="inline"><mml:mrow class="chem"><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:msub><mml:mo>)</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, AS) and bisulfate (<inline-formula><mml:math id="M8" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">HSO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, ABS). The accuracy of COSMO<italic>therm</italic> p<inline-formula><mml:math id="M9" display="inline"><mml:mrow><mml:msub><mml:mi>K</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> calculations (parameterization BP_TZVPD_FINE_C30_1601) is 0.65 log units (root mean square deviation – RMSD) <xref ref-type="bibr" rid="bib1.bibx28" id="paren.21"/>, and experimental saturation vapor pressures can be predicted within a factor of 2 with a tendency to overpredict experimental values of carboxylic acids <xref ref-type="bibr" rid="bib1.bibx44" id="paren.22"/>.</p>
      <p id="d1e384">Figures <xref ref-type="fig" rid="Ch1.F1"/> and <xref ref-type="fig" rid="Ch1.F2"/> show the monoterpene- and isoprene-derived organosulfates, respectively, studied here. These compounds have previously been identified as components of atmospheric aerosol <xref ref-type="bibr" rid="bib1.bibx48 bib1.bibx49 bib1.bibx50 bib1.bibx25 bib1.bibx20" id="paren.23"/>. <inline-formula><mml:math id="M10" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-Pinene-OS-1 and <inline-formula><mml:math id="M11" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene-OS-2, and all of the <inline-formula><mml:math id="M12" display="inline"><mml:mi mathvariant="italic">β</mml:mi></mml:math></inline-formula>-pinene- and limonene-derived organosulfates are products of the monoterpene <inline-formula><mml:math id="M13" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> OH reaction. <inline-formula><mml:math id="M14" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-Pinene-OS-3 is formed from pinonaldehyde, <inline-formula><mml:math id="M15" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene-OS-4 from an oxidation product of <inline-formula><mml:math id="M16" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene <inline-formula><mml:math id="M17" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> OH, and <inline-formula><mml:math id="M18" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene-OS-5 and <inline-formula><mml:math id="M19" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene-OS-6 are derived from pinonic acid. Isoprene-OS-1 and isoprene-OS-2 are proposed to be formed from the aldehyde–keto form of an isoprene OH oxidation product in low-<inline-formula><mml:math id="M20" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> conditions. Isoprene-OS-3 and isoprene-OS-4 are likely formed from a nucleophilic attack by sulfate on the epoxy group of IEPOX <xref ref-type="bibr" rid="bib1.bibx12" id="paren.24"/>. In field measurements in the US <xref ref-type="bibr" rid="bib1.bibx21 bib1.bibx22" id="paren.25"/>, an organosulfate corresponding to the chemical formula of isoprene-OS-3 and isoprene-OS-4 dominated the bisulfate mass of PM<inline-formula><mml:math id="M21" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula>. Since primary organosulfates are more stable against hydrolysis than tertiary organosulfates <xref ref-type="bibr" rid="bib1.bibx12" id="paren.26"/>, isoprene-OS-3 is likely the more abundant isomer, compared to isoprene-OS-4, in acidic aerosol.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1"><?xmltex \currentcnt{1}?><label>Figure 1</label><caption><p id="d1e498">Structures of the studied monoterpene-derived organosulfates, provided by <inline-formula><mml:math id="M22" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">a</mml:mi></mml:msup></mml:math></inline-formula><xref ref-type="bibr" rid="bib1.bibx49" id="text.27"/>, <inline-formula><mml:math id="M23" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">b</mml:mi></mml:msup></mml:math></inline-formula><xref ref-type="bibr" rid="bib1.bibx48" id="text.28"/>, <inline-formula><mml:math id="M24" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">c</mml:mi></mml:msup></mml:math></inline-formula><xref ref-type="bibr" rid="bib1.bibx25" id="text.29"/> and <inline-formula><mml:math id="M25" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">d</mml:mi></mml:msup></mml:math></inline-formula><xref ref-type="bibr" rid="bib1.bibx20" id="text.30"/>.</p></caption>
        <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://acp.copernicus.org/articles/20/5679/2020/acp-20-5679-2020-f01.png"/>

      </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2"><?xmltex \currentcnt{2}?><label>Figure 2</label><caption><p id="d1e554">Structures of the studied isoprene-derived organosulfates, provided by <inline-formula><mml:math id="M26" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">a</mml:mi></mml:msup></mml:math></inline-formula><xref ref-type="bibr" rid="bib1.bibx48" id="text.31"/> and <inline-formula><mml:math id="M27" display="inline"><mml:msup><mml:mi/><mml:mi mathvariant="normal">b</mml:mi></mml:msup></mml:math></inline-formula><xref ref-type="bibr" rid="bib1.bibx50" id="text.32"/>. Isoprene-OS-3 and isoprene-OS-4 are IEPOX-derived organosulfates. </p></caption>
        <?xmltex \igopts{width=170.716535pt}?><graphic xlink:href="https://acp.copernicus.org/articles/20/5679/2020/acp-20-5679-2020-f02.png"/>

      </fig>

      <p id="d1e585">For comparison to monoterpene- and isoprene-derived organosulfate, we also studied the atmospherically abundant IEPOX (<inline-formula><mml:math id="M28" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">C</mml:mi><mml:mn mathvariant="normal">5</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">10</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>; see the different isomers in Fig. S1 of the<?pagebreak page5681?> Supplement) and the smallest organosulfate, methyl bisulfate (<inline-formula><mml:math id="M29" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">OSO</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub><mml:mi mathvariant="normal">H</mml:mi></mml:mrow></mml:math></inline-formula>).</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Computational methods</title>
      <p id="d1e635">We used COSMO<italic>therm</italic> release 19 <xref ref-type="bibr" rid="bib1.bibx10" id="paren.33"/> to estimate several thermodynamic properties, such as acidity (p<inline-formula><mml:math id="M30" display="inline"><mml:mrow><mml:msub><mml:mi>K</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>), Henry's law solubility, activity and vapor pressure. The COSMO<italic>therm</italic> program is based on the conductor-like screening model for real solvents (COSMO-RS; <xref ref-type="bibr" rid="bib1.bibx26 bib1.bibx27 bib1.bibx13" id="altparen.34"/>). COSMO<italic>therm</italic> combines quantum chemistry and statistical thermodynamics to predict the condensed-phase properties of liquids as well as partitioning between condensed and gas phases. Quantum chemical calculations provide input files (cosmo-files) for COSMO<italic>therm</italic>, and the same files can be used to estimate properties in various solutions. In addition, multiple conformers can be included in COSMO<italic>therm</italic> calculations to improve the description of conformer distributions in different solutions. Below we explain in detail how the input files for the COSMO<italic>therm</italic> calculations were computed and give definitions used by COSMO<italic>therm</italic> to estimate each of the properties. More detailed explanations for all of the methods can be found in the COSMO<italic>therm</italic> reference manual <xref ref-type="bibr" rid="bib1.bibx14" id="paren.35"/>. Without experimental reference data, we are not able to estimate the error for individual compounds. The error estimates are the same for all studied compounds, and we therefore do not show error bars in the figures.</p>
<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>COSMO input file generation</title>
      <p id="d1e691">To generate the input files for the COSMO<italic>therm</italic> calculations, we used the COSMO<italic>conf</italic> program version 4.3 <xref ref-type="bibr" rid="bib1.bibx8" id="paren.36"/>. COSMO<italic>conf</italic> contains conformer generation algorithms, different levels of theory of quantum chemical calculations for both the condensed and the gas phase, and various methods for reducing the number of conformers in a way that does not compromise the accuracy of the COSMO<italic>therm</italic> calculations.</p>
      <p id="d1e709">Including multiple conformers in the COSMO<italic>therm</italic> calculations is important when the conformers have different polarities, as is the case for molecules that are able to form intramolecular hydrogen bonds <xref ref-type="bibr" rid="bib1.bibx14" id="paren.37"/>. For finding an initial set of conformers, COSMO<italic>conf</italic> uses various conformer-generating algorithms. However, none of these methods allow for the systematic conformer sampling of the molecules. The nonsystematic conformer generation in COSMO<italic>conf</italic> has been shown to lead to significantly different results in COSMO<italic>therm</italic> depending on the initial geometry with molecules containing hydroxy and hydroperoxy functional groups <xref ref-type="bibr" rid="bib1.bibx31" id="paren.38"/>. Based on the recommendation by <xref ref-type="bibr" rid="bib1.bibx31" id="text.39"/>, we therefore used the systematic conformer sampling with the Merck molecular force field (MMFF94) in the Spartan '14 program <xref ref-type="bibr" rid="bib1.bibx58" id="paren.40"/>. In addition to the most common carbon and oxygen atom types, the MMFF94 is parameterized for the atom types of a sulfate group sulfur and oxygens <xref ref-type="bibr" rid="bib1.bibx18" id="paren.41"/>. This ensures that all unique conformers are found using the systematic sampling.</p>
      <p id="d1e740">The conformers from Spartan '14 were used as input to COSMO<italic>conf</italic>, and the TURBOMOLE program package version 7.11 <xref ref-type="bibr" rid="bib1.bibx54" id="paren.42"/> was used for the quantum chemical calculations. Our calculation template in COSMO<italic>conf</italic> follows the BP-TZVPD-FINE-COSMO.xml template found in the program, omitting the conformational sampling step at the beginning and setting the cutoffs (based on energy and the number of conformers) of conformers high enough that no conformers were discarded. The gas-phase conformers were obtained by BP/def-TZVP gas-phase geometry optimizations and BP/def2-TZVPD single-point energy calculations of the condensed-phase geometries from COSMO<italic>conf</italic> using the <italic>calculate</italic> function in TURBOMOLE. The BP/def2-TZVPD-FINE//BP/def-TZVP level .cosmo and .energy files from COSMO<italic>conf</italic> and TURBOMOLE were used in COSMO<italic>therm</italic> calculations. In addition, .cosmo, .energy and .vap files for <inline-formula><mml:math id="M31" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></inline-formula> and the inorganic ions were taken from the COSMO<italic>base</italic>17 database <xref ref-type="bibr" rid="bib1.bibx7" id="paren.43"/>.</p>
</sec>
<sec id="Ch1.S2.SS2">
  <label>2.2</label><?xmltex \opttitle{COSMO\textit{therm} calculations}?><title>COSMO<italic>therm</italic> calculations</title>
      <p id="d1e796">In our COSMO<italic>therm</italic> calculations, we have used the most recent BP_TZVPD_FINE_19 parameterization. All calculations were done at 298.15 <inline-formula><mml:math id="M32" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">K</mml:mi></mml:mrow></mml:math></inline-formula>.
To the best of our knowledge, experimental information on the pure component phase state of most atmospherically relevant organics is not available. We therefore assume that all of the organosulfates (OS) and the isoprene epoxydiols (IEPOX) are liquid at 298.15 K. Without melting point and heat of fusion data, we are not able to accurately estimate the solubilities of solid-phase organosulfates. If the OS and IEPOX are solid at 298.15 K,<?pagebreak page5682?> the solubility results shown here are the mole fractions of the virtual liquid of the solute in the two liquid phases of a solid–liquid–liquid equilibrium. Sodium salts of the organosulfates (<inline-formula><mml:math id="M33" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">R</mml:mi><mml:mi mathvariant="normal">−</mml:mi><mml:msub><mml:mi mathvariant="normal">OSO</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub><mml:mi mathvariant="normal">Na</mml:mi></mml:mrow></mml:math></inline-formula>, NaOS) are similar to sodium dodecyl sulfate (SDS) with regard to molar mass and functionality. SDS is solid at 298.15 K, and we therefore assume that NaOS is solid at this temperature. The organic compounds are treated as solutes and the aqueous solutions (pure water or binary aqueous ammonium salt mixtures) as the solvent.</p>
      <p id="d1e827">To select the maximum number of conformers needed for COSMO<italic>therm</italic> calculations, convergence on the number of conformers was tested by calculating the activities of isoprene-OS-1. In these test calculations, the change in activity of isoprene-OS-1 and <inline-formula><mml:math id="M34" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></inline-formula> (in different mole fractions of isoprene-OS-1 in water) was at most 0.005 between 40 and 45 conformers of isoprene-OS-1. Based on this, the maximum number of conformers was set to 40 for larger monoterpene-derived organosulfates and 50 for the smaller isoprene-derived molecules.</p>
      <p id="d1e846">In COSMO<italic>therm</italic> calculations, conformers are weighted according to the Boltzmann distribution based on the sum of their solvated energy and chemical potential in the solution. However, normally only conformers with the lowest solvated energies are selected for COSMO<italic>therm</italic> calculations. If the total number of unique conformers is high, not all conformers can be included in the COSMO<italic>therm</italic> calculation. When only a fraction of all conformers is used in a COSMO<italic>therm</italic> calculation, only those containing intramolecular hydrogen bonds are used, as they have the lowest solvated energies. However, the interaction between a compound and water is more favorable for conformers containing no intramolecular hydrogen bonds. Therefore, in aqueous solutions, the chemical potential of conformers containing no intramolecular hydrogen bonds is much lower than that of conformers that contain multiple hydrogen bonds. If a compound contains more unique conformers than can be included in COSMO<italic>therm</italic> calculations, more attention should be paid to selecting the conformers to represent the conformer distribution in the studied solutions.</p>
      <p id="d1e865"><xref ref-type="bibr" rid="bib1.bibx31" id="text.44"/> found that COSMO<italic>therm</italic> (release 18; <xref ref-type="bibr" rid="bib1.bibx9" id="altparen.45"/>) overestimates the effect of intramolecular hydrogen bonds and recommended that only conformers containing no intramolecular hydrogen bonds should be used in saturation vapor pressure calculations. We tested the difference in saturation vapor pressures calculated using releases 18 and 19 (parameterizations BP_TZVPD_FINE_18 and BP_TZVPD_FINE_19, respectively) and found that differences between the two parameterizations are larger using all conformers than when only conformers containing no intramolecular hydrogen bonds are used. Variation between estimates using different conformer sets is also smaller in release 19 than in release 18. We therefore omitted all conformers containing intramolecular hydrogen bonds from the calculations of OS and IEPOX. Generally, the omission of conformers containing intramolecular hydrogen bonds leads to lower saturation vapor pressures <xref ref-type="bibr" rid="bib1.bibx31" id="paren.46"/>.</p>
      <p id="d1e879">The number of intramolecular hydrogen bonds in the condensed phase was determined using release 18 of COSMO<italic>therm</italic>. For isoprene-OS-3 and isoprene-OS-4, we only found two and zero conformers containing no hydrogen bonds, respectively. For these two species, we used all conformers containing no full and any number of partial intramolecular hydrogen bonds or one full and no partial intramolecular hydrogen bonds. Many of the deprotonated organosulfates (sodium salt anions) have only conformers that contain intramolecular hydrogen bonds. For this reason, we chose to use all of their lowest-energy conformers in the COSMO<italic>therm</italic> calculations involving the NaOS. In the calculation of p<inline-formula><mml:math id="M35" display="inline"><mml:mrow><mml:msub><mml:mi>K</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> we used all conformers, since the calculation uses both the neutral and the ionic species.</p>
<sec id="Ch1.S2.SS2.SSS1">
  <label>2.2.1</label><title>Chemical potential</title>
      <p id="d1e906">The chemical potential (<inline-formula><mml:math id="M36" display="inline"><mml:mi mathvariant="italic">μ</mml:mi></mml:math></inline-formula>) of a component <inline-formula><mml:math id="M37" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> in a mixture is defined with respect to the chemical potential in a given reference state <inline-formula><mml:math id="M38" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> with constant temperature <inline-formula><mml:math id="M39" display="inline"><mml:mi>T</mml:mi></mml:math></inline-formula> and pressure <inline-formula><mml:math id="M40" display="inline"><mml:mi>P</mml:mi></mml:math></inline-formula> as
              <disp-formula id="Ch1.E1" content-type="numbered"><label>1</label><mml:math id="M41" display="block"><mml:mrow><mml:msub><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:msub><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mo>(</mml:mo><mml:mi>T</mml:mi><mml:mo>,</mml:mo><mml:mi>P</mml:mi><mml:mo>)</mml:mo><mml:mo>+</mml:mo><mml:mi>R</mml:mi><mml:mi>T</mml:mi><mml:mi>ln⁡</mml:mi><mml:msub><mml:mi>a</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
            where <inline-formula><mml:math id="M42" display="inline"><mml:mi>R</mml:mi></mml:math></inline-formula> is the gas constant, and <inline-formula><mml:math id="M43" display="inline"><mml:mrow><mml:msub><mml:mi>a</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>a</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is the activity of component <inline-formula><mml:math id="M44" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> at a given actual mole fraction <inline-formula><mml:math id="M45" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> with respect to the chosen reference state. COSMO<italic>therm</italic> uses the pseudo-chemical potential <xref ref-type="bibr" rid="bib1.bibx2" id="paren.47"/> <inline-formula><mml:math id="M46" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi><mml:mo>*</mml:mo></mml:msubsup></mml:mrow></mml:math></inline-formula>, which is defined as
              <disp-formula id="Ch1.E2" content-type="numbered"><label>2</label><mml:math id="M47" display="block"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi><mml:mo>*</mml:mo></mml:msubsup><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:msub><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mo>(</mml:mo><mml:mi>T</mml:mi><mml:mo>,</mml:mo><mml:mi>P</mml:mi><mml:mo>)</mml:mo><mml:mo>+</mml:mo><mml:mi>R</mml:mi><mml:mi>T</mml:mi><mml:mi>ln⁡</mml:mi><mml:msub><mml:mi mathvariant="italic">γ</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
            where <inline-formula><mml:math id="M48" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">γ</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M49" display="inline"><mml:mrow><mml:mo>=</mml:mo><mml:msub><mml:mi>a</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) is the activity coefficient of component <inline-formula><mml:math id="M50" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> at mole fraction <inline-formula><mml:math id="M51" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>. By definition, the activity coefficient is 1 when component <inline-formula><mml:math id="M52" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> is in the reference state (<inline-formula><mml:math id="M53" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">γ</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>). This means that in the reference state, chemical potential and pseudo-chemical potential are equal:
              <disp-formula id="Ch1.E3" content-type="numbered"><label>3</label><mml:math id="M54" display="block"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi><mml:mo>*</mml:mo></mml:msubsup><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mo>(</mml:mo><mml:mi>T</mml:mi><mml:mo>,</mml:mo><mml:mi>P</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:msub><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mo>(</mml:mo><mml:mi>T</mml:mi><mml:mo>,</mml:mo><mml:mi>P</mml:mi><mml:mo>)</mml:mo><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula></p>
      <?pagebreak page5683?><p id="d1e1276">In COSMO<italic>therm</italic>, the pseudo-chemical potential of component <inline-formula><mml:math id="M55" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> in system <inline-formula><mml:math id="M56" display="inline"><mml:mi>S</mml:mi></mml:math></inline-formula> is calculated using the <inline-formula><mml:math id="M57" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> potential:
              <disp-formula id="Ch1.E4" content-type="numbered"><label>4</label><mml:math id="M58" display="block"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi><mml:mo>*</mml:mo></mml:msubsup><mml:mo>=</mml:mo><mml:msubsup><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mo>,</mml:mo><mml:mi>S</mml:mi></mml:mrow></mml:msubsup><mml:mo>+</mml:mo><mml:mo movablelimits="false">∫</mml:mo><mml:msub><mml:mi>p</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>)</mml:mo><mml:msub><mml:mi mathvariant="italic">μ</mml:mi><mml:mi mathvariant="normal">S</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>)</mml:mo><mml:mi>d</mml:mi><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
            where <inline-formula><mml:math id="M59" display="inline"><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is the un-normalized <inline-formula><mml:math id="M60" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> profile, and <inline-formula><mml:math id="M61" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">μ</mml:mi><mml:mi mathvariant="normal">S</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is the chemical potential of a surface segment with the screening charge density <inline-formula><mml:math id="M62" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> (the <inline-formula><mml:math id="M63" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> potential), which describes the affinity of the system <inline-formula><mml:math id="M64" display="inline"><mml:mi>S</mml:mi></mml:math></inline-formula> to a surface of screening charge density <inline-formula><mml:math id="M65" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula>. The combinatorial contribution to the chemical potential (<inline-formula><mml:math id="M66" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mo>,</mml:mo><mml:mi>S</mml:mi></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula>),
              <disp-formula id="Ch1.E5" content-type="numbered"><label>5</label><mml:math id="M67" display="block"><mml:mtable rowspacing="0.2ex" class="split" columnspacing="1em" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi><mml:mrow><mml:mi>C</mml:mi><mml:mo>,</mml:mo><mml:mi>S</mml:mi></mml:mrow></mml:msubsup></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mo>=</mml:mo><mml:mi>R</mml:mi><mml:mi>T</mml:mi><mml:mo>[</mml:mo><mml:mo>(</mml:mo><mml:msub><mml:mover accent="true"><mml:mi mathvariant="italic">λ</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:mn mathvariant="normal">0</mml:mn></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mover accent="true"><mml:mi mathvariant="italic">λ</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>)</mml:mo><mml:mi>ln⁡</mml:mi><mml:mo>(</mml:mo><mml:msub><mml:mi>r</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>+</mml:mo><mml:msub><mml:mover accent="true"><mml:mi mathvariant="italic">λ</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi>r</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow><mml:mover accent="true"><mml:mi>r</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:mfrac></mml:mstyle><mml:mo>+</mml:mo><mml:mi>ln⁡</mml:mi><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi>r</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow><mml:mover accent="true"><mml:mi>r</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:mfrac></mml:mstyle><mml:mo>)</mml:mo></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mo>+</mml:mo><mml:msub><mml:mover accent="true"><mml:mi mathvariant="italic">λ</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi>q</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow><mml:mover accent="true"><mml:mi>q</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:mfrac></mml:mstyle><mml:mo>+</mml:mo><mml:mi>ln⁡</mml:mi><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi>q</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow><mml:mover accent="true"><mml:mi>q</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:mfrac></mml:mstyle><mml:mo>)</mml:mo><mml:mo>-</mml:mo><mml:msub><mml:mover accent="true"><mml:mi mathvariant="italic">λ</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover><mml:mn mathvariant="normal">3</mml:mn></mml:msub><mml:mi>ln⁡</mml:mi><mml:mo>(</mml:mo><mml:msub><mml:mi>r</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>]</mml:mo><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
            is derived from the similar combinatorial free energy expression. The prefactors <inline-formula><mml:math id="M68" display="inline"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi mathvariant="italic">λ</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover><mml:mn mathvariant="normal">0</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M69" display="inline"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi mathvariant="italic">λ</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M70" display="inline"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi mathvariant="italic">λ</mml:mi><mml:mo stretchy="false" mathvariant="normal">^</mml:mo></mml:mover><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> have fixed values, while <inline-formula><mml:math id="M71" display="inline"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi mathvariant="italic">λ</mml:mi><mml:mo mathvariant="normal" stretchy="false">^</mml:mo></mml:mover><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is adjustable. The total volume (<inline-formula><mml:math id="M72" display="inline"><mml:mover accent="true"><mml:mi>r</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:math></inline-formula>) and area (<inline-formula><mml:math id="M73" display="inline"><mml:mover accent="true"><mml:mi>q</mml:mi><mml:mo mathvariant="normal">‾</mml:mo></mml:mover></mml:math></inline-formula>) of all components <inline-formula><mml:math id="M74" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> are calculated as the mole-fraction-weighted sums of the dimensionless molecular volume (<inline-formula><mml:math id="M75" display="inline"><mml:mrow><mml:msub><mml:mi>r</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) and area (<inline-formula><mml:math id="M76" display="inline"><mml:mrow><mml:msub><mml:mi>q</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) of component <inline-formula><mml:math id="M77" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula>, respectively.</p>
</sec>
<sec id="Ch1.S2.SS2.SSS2">
  <label>2.2.2</label><title>Activity coefficient</title>
      <p id="d1e1766">The activity coefficient of component <inline-formula><mml:math id="M78" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> at mole fraction <inline-formula><mml:math id="M79" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> in a mixture can be calculated using Eq. (<xref ref-type="disp-formula" rid="Ch1.E2"/>) as
              <disp-formula id="Ch1.E6" content-type="numbered"><label>6</label><mml:math id="M80" display="block"><mml:mrow><mml:mi>ln⁡</mml:mi><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="italic">γ</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi><mml:mo>*</mml:mo></mml:msubsup><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>-</mml:mo><mml:msub><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mo>(</mml:mo><mml:mi>T</mml:mi><mml:mo>,</mml:mo><mml:mi>P</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mi>R</mml:mi><mml:mi>T</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>
            The value of the activity coefficient in a given solution state <inline-formula><mml:math id="M81" display="inline"><mml:mrow><mml:mo mathvariant="italic">{</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo mathvariant="italic">}</mml:mo></mml:mrow></mml:math></inline-formula> depends on the choice of reference state. As the default reference state, COSMO<italic>therm</italic> uses the pure compound (<inline-formula><mml:math id="M82" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula>, labeled as convention I in the following; <xref ref-type="bibr" rid="bib1.bibx33" id="altparen.48"/>) at 10<inline-formula><mml:math id="M83" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">5</mml:mn></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M84" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">Pa</mml:mi></mml:mrow></mml:math></inline-formula> pressure and 298.15 <inline-formula><mml:math id="M85" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">K</mml:mi></mml:mrow></mml:math></inline-formula> temperature. According to Eq. (<xref ref-type="disp-formula" rid="Ch1.E3"/>), with respect to this reference state, the pseudo-chemical potential is equal to the chemical potential when the system is in the reference state, <inline-formula><mml:math id="M86" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi><mml:mrow><mml:mo>*</mml:mo><mml:mo>,</mml:mo><mml:mi mathvariant="normal">I</mml:mi></mml:mrow></mml:msubsup><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:msubsup><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">I</mml:mi></mml:msubsup><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>, giving
              <disp-formula id="Ch1.E7" content-type="numbered"><label>7</label><mml:math id="M87" display="block"><mml:mrow><mml:mi>ln⁡</mml:mi><mml:mo>(</mml:mo><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">I</mml:mi></mml:msubsup><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi><mml:mo>*</mml:mo></mml:msubsup><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>-</mml:mo><mml:msubsup><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi><mml:mrow><mml:mo>*</mml:mo><mml:mo>,</mml:mo><mml:mi mathvariant="normal">I</mml:mi></mml:mrow></mml:msubsup><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mo>(</mml:mo><mml:mi>T</mml:mi><mml:mo>,</mml:mo><mml:mi>P</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mi>R</mml:mi><mml:mi>T</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula></p>
      <p id="d1e2080">Activity coefficient values derived from experiments are often determined with respect to an ideal infinite dilution reference state (<inline-formula><mml:math id="M88" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mo>→</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula>, labeled as convention II; <xref ref-type="bibr" rid="bib1.bibx33" id="altparen.49"/>). For comparison with such experimentally derived values, activity coefficients for a given actual state <inline-formula><mml:math id="M89" display="inline"><mml:mrow><mml:mo mathvariant="italic">{</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo mathvariant="italic">}</mml:mo></mml:mrow></mml:math></inline-formula> determined with respect to the pure component reference state (<inline-formula><mml:math id="M90" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">γ</mml:mi><mml:mi mathvariant="normal">I</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula>) can be converted to the infinite dilution reference state (<inline-formula><mml:math id="M91" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">γ</mml:mi><mml:mi mathvariant="normal">II</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula>) as
              <disp-formula id="Ch1.Ex1"><mml:math id="M92" display="block"><mml:mrow><mml:mi>ln⁡</mml:mi><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">I</mml:mi></mml:msubsup><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">I</mml:mi></mml:msubsup><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>→</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>=</mml:mo><mml:mi>ln⁡</mml:mi><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">I</mml:mi></mml:msubsup><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>-</mml:mo><mml:mi>ln⁡</mml:mi><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">I</mml:mi></mml:msubsup><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>→</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></disp-formula>

              <disp-formula id="Ch1.Ex2"><mml:math id="M93" display="block"><mml:mrow><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi><mml:mo>*</mml:mo></mml:msubsup><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>-</mml:mo><mml:msubsup><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi><mml:mrow><mml:mo>*</mml:mo><mml:mo>,</mml:mo><mml:mi mathvariant="normal">I</mml:mi></mml:mrow></mml:msubsup><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mo>(</mml:mo><mml:mi>T</mml:mi><mml:mo>,</mml:mo><mml:mi>P</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mi>R</mml:mi><mml:mi>T</mml:mi></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>-</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi><mml:mo>*</mml:mo></mml:msubsup><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>)</mml:mo><mml:mo>-</mml:mo><mml:msubsup><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi><mml:mrow><mml:mo>*</mml:mo><mml:mo>,</mml:mo><mml:mi mathvariant="normal">I</mml:mi></mml:mrow></mml:msubsup><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mo>(</mml:mo><mml:mi>T</mml:mi><mml:mo>,</mml:mo><mml:mi>P</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mi>R</mml:mi><mml:mi>T</mml:mi></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:math></disp-formula>

              <disp-formula id="Ch1.Ex3"><mml:math id="M94" display="block"><mml:mrow><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi><mml:mo>*</mml:mo></mml:msubsup><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>-</mml:mo><mml:msubsup><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi><mml:mo>*</mml:mo></mml:msubsup><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mi>R</mml:mi><mml:mi>T</mml:mi></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:math></disp-formula>

              <disp-formula id="Ch1.Ex4"><mml:math id="M95" display="block"><mml:mrow><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi><mml:mo>*</mml:mo></mml:msubsup><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>-</mml:mo><mml:msubsup><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi><mml:mrow><mml:mo>*</mml:mo><mml:mo>,</mml:mo><mml:mi mathvariant="normal">II</mml:mi></mml:mrow></mml:msubsup><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mo>(</mml:mo><mml:mi>T</mml:mi><mml:mo>,</mml:mo><mml:mi>P</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mi>R</mml:mi><mml:mi>T</mml:mi></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:math></disp-formula>

              <disp-formula id="Ch1.E8" content-type="numbered"><label>8</label><mml:math id="M96" display="block"><mml:mrow><mml:mo>=</mml:mo><mml:mi>ln⁡</mml:mi><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">II</mml:mi></mml:msubsup><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
            where <inline-formula><mml:math id="M97" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi><mml:mo>*</mml:mo></mml:msubsup><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:msubsup><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi><mml:mrow><mml:mo>*</mml:mo><mml:mo>,</mml:mo><mml:mi mathvariant="normal">II</mml:mi></mml:mrow></mml:msubsup><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mo>(</mml:mo><mml:mi>T</mml:mi><mml:mo>,</mml:mo><mml:mi>P</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> follows from Eq. (<xref ref-type="disp-formula" rid="Ch1.E2"/>), since <inline-formula><mml:math id="M98" display="inline"><mml:mrow><mml:msup><mml:mi mathvariant="italic">γ</mml:mi><mml:mi mathvariant="normal">II</mml:mi></mml:msup><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> at the reference state (<inline-formula><mml:math id="M99" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mo>→</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula>).</p>
      <p id="d1e2591">To the best of our knowledge, no experimental data on the isoprene- and monoterpene-derived organosulfates are currently available. Here, we  therefore do not show activity coefficients for these compounds with respect to the infinite dilution reference state, but they can be calculated from our data using Eq. (<xref ref-type="disp-formula" rid="Ch1.E8"/>).</p>
</sec>
<sec id="Ch1.S2.SS2.SSS3">
  <label>2.2.3</label><title>Solubility</title>
      <p id="d1e2604">We calculate both the absolute and relative solubilities of organosulfate solutes. The absolute solubilities are estimated by finding the liquid–liquid equilibrium (LLE; for liquid solutes) or the solid–liquid equilibrium (SLE; for solid solutes) using the solid–liquid equilibrium solver (SLESOL) in COSMO<italic>therm</italic>. For liquid solutes, the SLESOL finds the LLE between two phases (<inline-formula><mml:math id="M100" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M101" display="inline"><mml:mi mathvariant="italic">β</mml:mi></mml:math></inline-formula>) using the liquid-phase equilibrium condition4:
              <disp-formula id="Ch1.E9" content-type="numbered"><label>9</label><mml:math id="M102" display="block"><mml:mrow><mml:msubsup><mml:mi>a</mml:mi><mml:mi>i</mml:mi><mml:mrow><mml:mi mathvariant="normal">I</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">α</mml:mi></mml:mrow></mml:msubsup><mml:mo>=</mml:mo><mml:msubsup><mml:mi>a</mml:mi><mml:mi>i</mml:mi><mml:mrow><mml:mi mathvariant="normal">I</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">β</mml:mi></mml:mrow></mml:msubsup><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>
            In the LLE, Eq. (<xref ref-type="disp-formula" rid="Ch1.E9"/>) is true for both the solute and the solvent. Equation (<xref ref-type="disp-formula" rid="Ch1.E9"/>) is equivalent to the chemical potential of the solute being equal at the solubility limit in both phases, as opposed to the definition of the solubility of a solid solute in which the chemical potential of the solute at the solubility limit is equal to its chemical potential in the pure solute.</p>
      <p id="d1e2663">Based on their molecular structures, we expect organosulfates to have Brønsted acid properties. The acidity, in terms of the acid constant p<inline-formula><mml:math id="M103" display="inline"><mml:mrow><mml:msub><mml:mi>K</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M104" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:msub><mml:mi>log⁡</mml:mi><mml:mn mathvariant="normal">10</mml:mn></mml:msub><mml:msub><mml:mi>K</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> for the equilibrium constant <inline-formula><mml:math id="M105" display="inline"><mml:mrow><mml:msub><mml:mi>K</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> corresponding to the equilibrium <inline-formula><mml:math id="M106" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">R</mml:mi><mml:mo>-</mml:mo><mml:msub><mml:mi mathvariant="normal">OSO</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mo>+</mml:mo><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M107" display="inline"><mml:mo>⇌</mml:mo></mml:math></inline-formula> <inline-formula><mml:math id="M108" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">R</mml:mi><mml:mo>-</mml:mo><mml:msubsup><mml:mi mathvariant="normal">OSO</mml:mi><mml:mn mathvariant="normal">3</mml:mn><mml:mo>-</mml:mo></mml:msubsup><mml:mo>+</mml:mo><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub><mml:msup><mml:mi mathvariant="normal">O</mml:mi><mml:mo>+</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula>), is estimated using the deprotonated organosulfate species. COSMO<italic>therm</italic> estimates the p<inline-formula><mml:math id="M109" display="inline"><mml:mrow><mml:msub><mml:mi>K</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> of compound <inline-formula><mml:math id="M110" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> from the molar free energy (<inline-formula><mml:math id="M111" display="inline"><mml:mi>G</mml:mi></mml:math></inline-formula>; <inline-formula><mml:math id="M112" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">kJ</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">mol</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>) of the neutral and ionic species at infinite dilution using the linear free energy relationship (LFER):
              <disp-formula id="Ch1.E10" content-type="numbered"><label>10</label><mml:math id="M113" display="block"><mml:mrow><mml:mi mathvariant="normal">p</mml:mi><mml:msubsup><mml:mi>K</mml:mi><mml:mi mathvariant="normal">a</mml:mi><mml:mi>i</mml:mi></mml:msubsup><mml:mo>=</mml:mo><mml:mi>c</mml:mi><mml:mo>+</mml:mo><mml:mi>d</mml:mi><mml:mo>(</mml:mo><mml:msubsup><mml:mi>G</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">anion</mml:mi></mml:msubsup><mml:mo>-</mml:mo><mml:msubsup><mml:mi>G</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">neutral</mml:mi></mml:msubsup><mml:mo>)</mml:mo><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>
            The LFER parameters for solvent water (<inline-formula><mml:math id="M114" display="inline"><mml:mrow><mml:mi>c</mml:mi><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">130.152</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M115" display="inline"><mml:mrow><mml:mi>d</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.116</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M116" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mol</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">kJ</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>) are taken from COSMO<italic>therm</italic>'s parameter file. The energy difference (<inline-formula><mml:math id="M117" display="inline"><mml:mrow><mml:msubsup><mml:mi>G</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">anion</mml:mi></mml:msubsup><mml:mo>-</mml:mo><mml:msubsup><mml:mi>G</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">neutral</mml:mi></mml:msubsup></mml:mrow></mml:math></inline-formula>) is always positive because in a neutral solvent, a neutral compound is more favorable than a charged compound. Relatively lower anion energy (more favorable deprotonation) leads to a smaller energy difference, leading to lower p<inline-formula><mml:math id="M118" display="inline"><mml:mrow><mml:msub><mml:mi>K</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>. The parameterization in COSMO<italic>therm</italic> currently enables the calculation of p<inline-formula><mml:math id="M119" display="inline"><mml:mrow><mml:msub><mml:mi>K</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> only in water, dimethylsulfoxide, acetonitrile or heptane. We are therefore not able to estimate p<inline-formula><mml:math id="M120" display="inline"><mml:mrow><mml:msub><mml:mi>K</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> values of the organosulfates in other solvents relevant to this work, specifically aqueous ammonium sulfate and bisulfate solutions.</p>
      <?pagebreak page5684?><p id="d1e2966">Dissociation in aqueous solution is expected to enhance solubility compared to the undissociated species. We use p<inline-formula><mml:math id="M121" display="inline"><mml:mrow><mml:msub><mml:mi>K</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> values to calculate a dissociation correction to solubilities. The molar concentration of acid anion (A<inline-formula><mml:math id="M122" display="inline"><mml:msup><mml:mi/><mml:mo>-</mml:mo></mml:msup></mml:math></inline-formula>) after dissociation is calculated using the pH of the solvent (<inline-formula><mml:math id="M123" display="inline"><mml:mrow><mml:mi mathvariant="normal">pH</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">7.0</mml:mn></mml:mrow></mml:math></inline-formula> for water) and p<inline-formula><mml:math id="M124" display="inline"><mml:mrow><mml:msub><mml:mi>K</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> for the solute:
              <disp-formula id="Ch1.E11" content-type="numbered"><label>11</label><mml:math id="M125" display="block"><mml:mrow><mml:msubsup><mml:mi>c</mml:mi><mml:mi>i</mml:mi><mml:mrow><mml:msup><mml:mi>A</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:msubsup><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mi mathvariant="normal">pH</mml:mi></mml:mrow></mml:msup><mml:mo>+</mml:mo><mml:msqrt><mml:mrow><mml:mn mathvariant="normal">0.25</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn><mml:mi mathvariant="normal">pH</mml:mi></mml:mrow></mml:msup><mml:mo>+</mml:mo><mml:msubsup><mml:mi>c</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">HA</mml:mi></mml:msubsup><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mi mathvariant="normal">p</mml:mi><mml:msub><mml:mi>K</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:msup></mml:mrow></mml:msqrt><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>
            Here, the molar concentration of dissolved undissociated molecular organosulfate (HA) is calculated from the solubility mole fraction estimated using the SLESOL method, the mole-fraction-weighted density (<inline-formula><mml:math id="M126" display="inline"><mml:mi mathvariant="italic">ρ</mml:mi></mml:math></inline-formula>) of the system and the average molar mass of the solution (<inline-formula><mml:math id="M127" display="inline"><mml:mrow><mml:msub><mml:mi>M</mml:mi><mml:mi mathvariant="normal">solution</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mo>∑</mml:mo><mml:mi>i</mml:mi></mml:msub><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:msub><mml:mi>M</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, where <inline-formula><mml:math id="M128" display="inline"><mml:mrow><mml:msub><mml:mi>M</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the molar mass of component <inline-formula><mml:math id="M129" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula>):
              <disp-formula id="Ch1.E12" content-type="numbered"><label>12</label><mml:math id="M130" display="block"><mml:mrow><mml:msubsup><mml:mi>c</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">HA</mml:mi></mml:msubsup><mml:mo>=</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mi mathvariant="italic">ρ</mml:mi><mml:mrow><mml:msub><mml:mi>M</mml:mi><mml:mi mathvariant="normal">solution</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>
            The calculation of composition-dependent solution densities is explained in Sect. S1 of the Supplement. The dissociation-corrected mole fraction solubility (<inline-formula><mml:math id="M131" display="inline"><mml:mrow><mml:msup><mml:mi>x</mml:mi><mml:mi mathvariant="normal">DC</mml:mi></mml:msup></mml:mrow></mml:math></inline-formula>) is then calculated from the sum of the anionic and molecular molar concentrations using Eq. (<xref ref-type="disp-formula" rid="Ch1.E12"/>):
              <disp-formula id="Ch1.E13" content-type="numbered"><label>13</label><mml:math id="M132" display="block"><mml:mrow><mml:msubsup><mml:mi>x</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">DC</mml:mi></mml:msubsup><mml:mo>=</mml:mo><mml:mo>(</mml:mo><mml:msubsup><mml:mi>c</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">HA</mml:mi></mml:msubsup><mml:mo>+</mml:mo><mml:msubsup><mml:mi>c</mml:mi><mml:mi>i</mml:mi><mml:mrow><mml:msup><mml:mi mathvariant="normal">A</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:msubsup><mml:mo>)</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi>M</mml:mi><mml:mi mathvariant="normal">solution</mml:mi></mml:msub></mml:mrow><mml:mi mathvariant="italic">ρ</mml:mi></mml:mfrac></mml:mstyle><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>
            The average molar mass and composition-weighted density of the solution can be expressed using the mole fraction of the organic compound (see Sect. S1 for the equations), which is calculated iteratively from the dissociation-corrected molar concentration <inline-formula><mml:math id="M133" display="inline"><mml:mrow><mml:msubsup><mml:mi>c</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">HA</mml:mi></mml:msubsup><mml:mo>+</mml:mo><mml:msubsup><mml:mi>c</mml:mi><mml:mi>i</mml:mi><mml:mrow><mml:msup><mml:mi mathvariant="normal">A</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula>.</p>
      <p id="d1e3264">For solid solutes, here the organosulfate sodium salts, the SLESOL finds the solid–liquid equilibrium (SLE) using the solid–liquid-phase equilibrium condition:
              <disp-formula id="Ch1.E14" content-type="numbered"><label>14</label><mml:math id="M134" display="block"><mml:mrow><mml:msub><mml:mi>log⁡</mml:mi><mml:mn mathvariant="normal">10</mml:mn></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mrow><mml:mi mathvariant="normal">SOL</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi><mml:mrow><mml:mo>*</mml:mo><mml:mo>,</mml:mo><mml:mi mathvariant="normal">I</mml:mi></mml:mrow></mml:msubsup><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mo>-</mml:mo><mml:msubsup><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi><mml:mo>*</mml:mo></mml:msubsup><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>-</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>G</mml:mi><mml:mi mathvariant="normal">fus</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>T</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mi>R</mml:mi><mml:mi>T</mml:mi><mml:mi>ln⁡</mml:mi><mml:mo>(</mml:mo><mml:mn mathvariant="normal">10</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>
            The temperature-dependent molar free energy of fusion (<inline-formula><mml:math id="M135" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>G</mml:mi><mml:mi mathvariant="normal">fus</mml:mi></mml:msub><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M136" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">kJ</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">mol</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> for solid solutes) is an experimentally determined parameter, which can also be calculated from the experimental molar heat of fusion (<inline-formula><mml:math id="M137" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>H</mml:mi><mml:mi mathvariant="normal">fus</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) and melting temperature (<inline-formula><mml:math id="M138" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">melt</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) using the Schröder–van Laar equation <xref ref-type="bibr" rid="bib1.bibx39" id="paren.50"/>:
              <disp-formula id="Ch1.E15" content-type="numbered"><label>15</label><mml:math id="M139" display="block"><mml:mtable columnspacing="1em" class="split" rowspacing="0.2ex" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>G</mml:mi><mml:mi mathvariant="normal">fus</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>T</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mo>=</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>H</mml:mi><mml:mi mathvariant="normal">fus</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>-</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mi>T</mml:mi><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">melt</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>)</mml:mo><mml:mo>-</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mi>p</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">fus</mml:mi></mml:mrow></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">melt</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:mi>T</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mo>+</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mi>p</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">fus</mml:mi></mml:mrow></mml:msub><mml:mi>T</mml:mi><mml:mi>ln⁡</mml:mi><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">melt</mml:mi></mml:msub></mml:mrow><mml:mi>T</mml:mi></mml:mfrac></mml:mstyle><mml:mo>.</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
            The heat capacity of fusion (<inline-formula><mml:math id="M140" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mi>p</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">fus</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula>) can be obtained from experiments, estimated as
              <disp-formula id="Ch1.E16" content-type="numbered"><label>16</label><mml:math id="M141" display="block"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mi>p</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">fus</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>H</mml:mi><mml:mi mathvariant="normal">fus</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">melt</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
            or assumed to be zero. Equation (<xref ref-type="disp-formula" rid="Ch1.E16"/>) is physically a better estimate than <inline-formula><mml:math id="M142" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mi>p</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">fus</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M143" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">kJ</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">mol</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">K</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> for nonspherical and neutral compounds at temperatures above 150 <inline-formula><mml:math id="M144" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">K</mml:mi></mml:mrow></mml:math></inline-formula> and within 200 <inline-formula><mml:math id="M145" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">K</mml:mi></mml:mrow></mml:math></inline-formula> of the melting point <xref ref-type="bibr" rid="bib1.bibx14" id="paren.51"/>. Since experimental data are not available for the organosulfate sodium salts, we use the COSMO<italic>therm</italic> estimate of <inline-formula><mml:math id="M146" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mi>p</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">fus</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math></inline-formula> in solubility calculations for solid solutes. As the melting point and heat of fusion, we use the experimental values of a related organosulfate compound, SDS, <inline-formula><mml:math id="M147" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">melt</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">478.15</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M148" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">K</mml:mi></mml:mrow></mml:math></inline-formula> <xref ref-type="bibr" rid="bib1.bibx42" id="paren.52"/> and <inline-formula><mml:math id="M149" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>H</mml:mi><mml:mi mathvariant="normal">fus</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">50</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M150" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">kJ</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">mol</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> (the heat of fusion of hydrated solid surfactant to micellar state; <xref ref-type="bibr" rid="bib1.bibx45" id="altparen.53"/>).</p>
      <p id="d1e3749">In COSMO<italic>therm</italic>, small atomic metal ions have extreme screening charge densities (<inline-formula><mml:math id="M151" display="inline"><mml:mrow><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>&lt;</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.025</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M152" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">e</mml:mi></mml:mrow></mml:math></inline-formula> Å<inline-formula><mml:math id="M153" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> or <inline-formula><mml:math id="M154" display="inline"><mml:mrow><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>&gt;</mml:mo><mml:mn mathvariant="normal">0.025</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M155" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">e</mml:mi></mml:mrow></mml:math></inline-formula> Å<inline-formula><mml:math id="M156" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>). In reality, extreme screening charge densities of ions would lead to the formation of a solvation shell, whereby polar solvent molecules form strong hydrogen bonds with the ion. This is not accounted for in COSMO<italic>therm</italic>, which leads to unrealistic behavior of the sodium ion in water. To improve the description of sodium cation solvation in the case of the organosulfate sodium salts, we use a hydrated sodium cation instead of the dry sodium cation. Hydration of ions has previously been used in a model combining COSMO<italic>therm</italic> to describe the short-range ion–molecule and molecule–molecule interactions in combination with the Pitzer–Debye–Hückel solvation model (PDHS) to describe long-range ion–ion interactions <xref ref-type="bibr" rid="bib1.bibx53" id="paren.54"/>. The choice of hydration number for sodium is explained in more detail in Sect. S2 and Fig. S2. The screening charge densities of larger ions, such as ammonium, sulfate and bisulfate, are less extreme (<inline-formula><mml:math id="M157" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.025</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M158" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">e</mml:mi></mml:mrow></mml:math></inline-formula> Å<inline-formula><mml:math id="M159" display="inline"><mml:mrow><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup><mml:mo>&lt;</mml:mo><mml:mi mathvariant="italic">σ</mml:mi><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.025</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M160" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">e</mml:mi></mml:mrow></mml:math></inline-formula> Å<inline-formula><mml:math id="M161" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>; see Fig. S4), and the non-hydrated ions can be used in COSMO<italic>therm</italic> calculations.</p>
      <p id="d1e3894">We also calculate solubilities in ternary systems containing water, organosulfate (OS or NaOS) and inorganic salt (<inline-formula><mml:math id="M162" display="inline"><mml:mrow class="chem"><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:msub><mml:mo>)</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> or <inline-formula><mml:math id="M163" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">HSO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>). In these cases, the inorganic salt is considered part of the solvent and treated here in the form of its individual dissociated ions, leading to differently scaled mole fractions. The conversion of results from COSMO<italic>therm</italic>'s framework to the ternary system framework is explained in Sect. S2 and Fig. S3.</p>
      <p id="d1e3939">Relative organic solubilities with respect to either the binary water–organic system or the ternary water–organic–inorganic salt system are calculated using the relative screening option in COSMO<italic>therm</italic>. The relative solubilities are estimated using a zeroth-order approximation of the solubility (<inline-formula><mml:math id="M164" display="inline"><mml:mrow><mml:msubsup><mml:mi>x</mml:mi><mml:mrow><mml:mi mathvariant="normal">SOL</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula>):
              <disp-formula id="Ch1.E17" content-type="numbered"><label>17</label><mml:math id="M165" display="block"><mml:mrow><?xmltex \hack{\hbox\bgroup\fontsize{9}{9}\selectfont$\displaystyle}?><mml:msub><mml:mi>log⁡</mml:mi><mml:mn mathvariant="normal">10</mml:mn></mml:msub><mml:mo>(</mml:mo><mml:msubsup><mml:mi>x</mml:mi><mml:mrow><mml:mi mathvariant="normal">SOL</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:msubsup><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi><mml:mrow><mml:mo>*</mml:mo><mml:mo>,</mml:mo><mml:mi mathvariant="normal">I</mml:mi></mml:mrow></mml:msubsup><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mo>-</mml:mo><mml:msubsup><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi><mml:mo>*</mml:mo></mml:msubsup><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>)</mml:mo><mml:mo>-</mml:mo><mml:mo>max⁡</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>,</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>G</mml:mi><mml:mi mathvariant="normal">fus</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>T</mml:mi><mml:mo>)</mml:mo><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mi>R</mml:mi><mml:mi>T</mml:mi><mml:mi>ln⁡</mml:mi><mml:mo>(</mml:mo><mml:mn mathvariant="normal">10</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo><?xmltex \hack{$\egroup}?></mml:mrow></mml:math></disp-formula>
            where the solubility of component <inline-formula><mml:math id="M166" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> (in our case OS or NaOS) is assumed to be small enough to consider the component in a state of infinite dilution (<inline-formula><mml:math id="M167" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn></mml:mrow></mml:math></inline-formula>) instead of the actual composition at the solubility limit (<inline-formula><mml:math id="M168" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi mathvariant="normal">SOL</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>). In this approximation, the concentration of solute in the solvent is therefore assumed to be very small. The advantage of this zeroth-order approximation in the solubility calculation of solid solutes is that the solubility is calculated using only the chemical potential of the solute in the infinite dilution of the solvent, while the reference-state (pure solute) chemical potential and the free energy of fusion cancel out. For a solute <inline-formula><mml:math id="M169" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> in two different systems with solvents <inline-formula><mml:math id="M170" display="inline"><mml:mrow><mml:mi>S</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M171" display="inline"><mml:mrow><mml:mi>S</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula>,
              <disp-formula id="Ch1.E18" content-type="numbered"><label>18</label><mml:math id="M172" display="block"><mml:mtable columnspacing="1em" class="split" rowspacing="0.2ex" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd><mml:mrow><mml:msub><mml:mi>log⁡</mml:mi><mml:mn mathvariant="normal">10</mml:mn></mml:msub><mml:mo>(</mml:mo><mml:msubsup><mml:mi>x</mml:mi><mml:mrow><mml:mi mathvariant="normal">SOL</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow><mml:mrow><mml:mi>S</mml:mi><mml:mn mathvariant="normal">1</mml:mn><mml:mo>,</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:msubsup><mml:mo>)</mml:mo></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mo>-</mml:mo><mml:msub><mml:mi>log⁡</mml:mi><mml:mn mathvariant="normal">10</mml:mn></mml:msub><mml:mo>(</mml:mo><mml:msubsup><mml:mi>x</mml:mi><mml:mrow><mml:mi mathvariant="normal">SOL</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow><mml:mrow><mml:mi>S</mml:mi><mml:mn mathvariant="normal">2</mml:mn><mml:mo>,</mml:mo><mml:mo>(</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:msubsup><mml:mo>)</mml:mo></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi><mml:mrow><mml:mo>*</mml:mo><mml:mo>,</mml:mo><mml:mi mathvariant="normal">I</mml:mi></mml:mrow></mml:msubsup><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mo>-</mml:mo><mml:msubsup><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi><mml:mrow><mml:mo>*</mml:mo><mml:mo>,</mml:mo><mml:mi>S</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msubsup><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>)</mml:mo><mml:mo>-</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>G</mml:mi><mml:mi mathvariant="normal">fus</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>T</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mi>R</mml:mi><mml:mi>T</mml:mi><mml:mi>ln⁡</mml:mi><mml:mo>(</mml:mo><mml:mn mathvariant="normal">10</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mo>-</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi><mml:mrow><mml:mo>*</mml:mo><mml:mo>,</mml:mo><mml:mi mathvariant="normal">I</mml:mi></mml:mrow></mml:msubsup><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mo>-</mml:mo><mml:msubsup><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi><mml:mrow><mml:mo>*</mml:mo><mml:mo>,</mml:mo><mml:mi>S</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msubsup><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>)</mml:mo><mml:mo>-</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>G</mml:mi><mml:mi mathvariant="normal">fus</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>T</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mi>R</mml:mi><mml:mi>T</mml:mi><mml:mi>ln⁡</mml:mi><mml:mo>(</mml:mo><mml:mn mathvariant="normal">10</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>-</mml:mo><mml:msubsup><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi><mml:mrow><mml:mo>*</mml:mo><mml:mo>,</mml:mo><mml:mi>S</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msubsup><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>)</mml:mo><mml:mo>+</mml:mo><mml:msubsup><mml:mi mathvariant="italic">μ</mml:mi><mml:mi>i</mml:mi><mml:mrow><mml:mo>*</mml:mo><mml:mo>,</mml:mo><mml:mi>S</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msubsup><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mi>R</mml:mi><mml:mi>T</mml:mi><mml:mi>ln⁡</mml:mi><mml:mo>(</mml:mo><mml:mn mathvariant="normal">10</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>.</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
           <?pagebreak page5685?> The relative screening is especially useful in cases in which the solute is solid and the experimental free energy of fusion is unknown.</p>
</sec>
<sec id="Ch1.S2.SS2.SSS4">
  <label>2.2.4</label><title>Vapor pressure and Henry's law</title>
      <p id="d1e4488">The saturation vapor pressure (<inline-formula><mml:math id="M173" display="inline"><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mi mathvariant="normal">sat</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) of a pure compound (<inline-formula><mml:math id="M174" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula>) is estimated from the molar free energy of the compound in the liquid phase (<inline-formula><mml:math id="M175" display="inline"><mml:mrow><mml:msubsup><mml:mi>G</mml:mi><mml:mi>i</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>l</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula>) and the gas phase (<inline-formula><mml:math id="M176" display="inline"><mml:mrow><mml:msubsup><mml:mi>G</mml:mi><mml:mi>i</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>g</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula>):
              <disp-formula id="Ch1.E19" content-type="numbered"><label>19</label><mml:math id="M177" display="block"><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mrow><mml:mi mathvariant="normal">sat</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:msup><mml:mi>e</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mstyle scriptlevel="+1"><mml:mfrac><mml:mrow><mml:msubsup><mml:mi>G</mml:mi><mml:mi>i</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>l</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msubsup><mml:mo>-</mml:mo><mml:msubsup><mml:mi>G</mml:mi><mml:mi>i</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>g</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msubsup></mml:mrow><mml:mrow><mml:mi>R</mml:mi><mml:mi>T</mml:mi></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:msup><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">5</mml:mn></mml:msup><mml:mi mathvariant="normal">Pa</mml:mi><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>
            COSMO<italic>therm</italic> calculates the infinite dilution Henry's law volatility (<inline-formula><mml:math id="M178" display="inline"><mml:mrow><mml:msubsup><mml:mi>H</mml:mi><mml:mi mathvariant="normal">vol</mml:mi><mml:mi mathvariant="normal">∞</mml:mi></mml:msubsup></mml:mrow></mml:math></inline-formula>, in pressure units) as a product of the pure solute saturation vapor pressure and the activity coefficient of the solute in the infinite dilution state (<inline-formula><mml:math id="M179" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">I</mml:mi></mml:msubsup><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>→</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>):
              <disp-formula id="Ch1.E20" content-type="numbered"><label>20</label><mml:math id="M180" display="block"><mml:mrow><mml:msubsup><mml:mi>H</mml:mi><mml:mrow><mml:mi mathvariant="normal">vol</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow><mml:mi mathvariant="normal">∞</mml:mi></mml:msubsup><mml:mo>=</mml:mo><mml:msub><mml:mi>P</mml:mi><mml:mrow><mml:mi mathvariant="normal">sat</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow></mml:msub><mml:mo>⋅</mml:mo><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">I</mml:mi></mml:msubsup><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>→</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>)</mml:mo><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>
            This formula is based on the assumption that the solubility of compound <inline-formula><mml:math id="M181" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> in the solvent is small, allowing for the use of the zeroth-order solubility approximation (<inline-formula><mml:math id="M182" display="inline"><mml:mrow><mml:msubsup><mml:mi>x</mml:mi><mml:mrow><mml:mi mathvariant="normal">SOL</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:msubsup><mml:mo>≅</mml:mo><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">I</mml:mi></mml:msubsup><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>→</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>). Note that <inline-formula><mml:math id="M183" display="inline"><mml:mrow><mml:msubsup><mml:mi mathvariant="italic">γ</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">I</mml:mi></mml:msubsup><mml:mo>(</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>→</mml:mo><mml:mn mathvariant="normal">0</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is evaluated at infinite dilution but with respect to the pure component reference state.</p>
      <p id="d1e4794">Using the density and molar mass of the pure solvent, Henry's law volatilities in units of pressure can be converted to Henry's law solubilities (<inline-formula><mml:math id="M184" display="inline"><mml:mrow><mml:msubsup><mml:mi>H</mml:mi><mml:mi mathvariant="normal">sol</mml:mi><mml:mi mathvariant="normal">∞</mml:mi></mml:msubsup></mml:mrow></mml:math></inline-formula>; <inline-formula><mml:math id="M185" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">mol</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">Pa</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>):
              <disp-formula id="Ch1.E21" content-type="numbered"><label>21</label><mml:math id="M186" display="block"><mml:mrow><mml:msubsup><mml:mi>H</mml:mi><mml:mrow><mml:mi mathvariant="normal">sol</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow><mml:mi mathvariant="normal">∞</mml:mi></mml:msubsup><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mi mathvariant="italic">ρ</mml:mi><mml:mrow><mml:msub><mml:mi>M</mml:mi><mml:mi mathvariant="normal">solvent</mml:mi></mml:msub><mml:mo>⋅</mml:mo><mml:msubsup><mml:mi>H</mml:mi><mml:mrow><mml:mi mathvariant="normal">vol</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow><mml:mi mathvariant="normal">∞</mml:mi></mml:msubsup></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>
            The solvent density and molar mass are equal to the corresponding values for the solution under the assumption of infinite dilution. Densities (<inline-formula><mml:math id="M187" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">cm</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>) of aqueous <inline-formula><mml:math id="M188" display="inline"><mml:mrow class="chem"><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:msub><mml:mo>)</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M189" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">HSO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> solvents in the conversion of Henry's law volatility into Henry's law solubility are calculated using the experimental polynomial fit by <xref ref-type="bibr" rid="bib1.bibx51" id="text.55"/>:
              <disp-formula id="Ch1.E22" content-type="numbered"><label>22</label><mml:math id="M190" display="block"><mml:mrow><mml:mi mathvariant="italic">ρ</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.9971</mml:mn><mml:mo>+</mml:mo><mml:munderover><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mn mathvariant="normal">3</mml:mn></mml:munderover><mml:msub><mml:mi>A</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>w</mml:mi><mml:mi>t</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mi mathvariant="italic">%</mml:mi><mml:msup><mml:mo>)</mml:mo><mml:mi>i</mml:mi></mml:msup><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>
            For ammonium sulfate, <inline-formula><mml:math id="M191" display="inline"><mml:mrow><mml:msub><mml:mi>A</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5.92</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M192" display="inline"><mml:mrow><mml:msub><mml:mi>A</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">5.036</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">6</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M193" display="inline"><mml:mrow><mml:msub><mml:mi>A</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1.024</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">8</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>, and for ammonium bisulfate, <inline-formula><mml:math id="M194" display="inline"><mml:mrow><mml:msub><mml:mi>A</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">5.87</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M195" display="inline"><mml:mrow><mml:msub><mml:mi>A</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mo>=</mml:mo><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1.89</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">6</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M196" display="inline"><mml:mrow><mml:msub><mml:mi>A</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1.763</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">7</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>.</p>
      <p id="d1e5145">In addition, we calculate an alternative LLE-based Henry's law solubility using the molar concentration of the solute (<inline-formula><mml:math id="M197" display="inline"><mml:mrow><mml:msubsup><mml:mi>c</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">HA</mml:mi></mml:msubsup></mml:mrow></mml:math></inline-formula>) obtained from the LLE solubility calculation. This gives an estimate of the Henry's law solubility in a non-dilute solution:
              <disp-formula id="Ch1.E23" content-type="numbered"><label>23</label><mml:math id="M198" display="block"><mml:mrow><mml:msubsup><mml:mi>H</mml:mi><mml:mrow><mml:mi mathvariant="normal">sol</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow><mml:mi mathvariant="normal">LLE</mml:mi></mml:msubsup><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msubsup><mml:mi>c</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">HA</mml:mi></mml:msubsup></mml:mrow><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mrow><mml:mi mathvariant="normal">sat</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>
            This definition also allows for the calculation of the effective Henry's law solubility, whereby the dissociation of the solute is included in the total molar concentration:
              <disp-formula id="Ch1.E24" content-type="numbered"><label>24</label><mml:math id="M199" display="block"><mml:mrow><mml:msubsup><mml:mi>H</mml:mi><mml:mrow><mml:mi mathvariant="normal">sol</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow><mml:mi mathvariant="normal">eff</mml:mi></mml:msubsup><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msubsup><mml:mi>c</mml:mi><mml:mi>i</mml:mi><mml:mi mathvariant="normal">HA</mml:mi></mml:msubsup><mml:mo>+</mml:mo><mml:msubsup><mml:mi>c</mml:mi><mml:mi>i</mml:mi><mml:mrow><mml:msup><mml:mi mathvariant="normal">A</mml:mi><mml:mo>-</mml:mo></mml:msup></mml:mrow></mml:msubsup></mml:mrow><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mrow><mml:mi mathvariant="normal">sat</mml:mi><mml:mo>,</mml:mo><mml:mi>i</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula></p>
</sec>
</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Results and discussion</title>
<sec id="Ch1.S3.SS1">
  <label>3.1</label><title>Solubility in pure water</title>
      <p id="d1e5276">Solubilities of organics in pure water and of water in the organic-rich phase were calculated using COSMO<italic>therm</italic> as the respective mole fractions at the liquid–liquid equilibrium of OS–water mixtures. Results are shown in Fig. <xref ref-type="fig" rid="Ch1.F3"/>.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3"><?xmltex \currentcnt{3}?><label>Figure 3</label><caption><p id="d1e5286"><bold>(a)</bold> The solubility of organosulfates and their sodium salts in pure water; <bold>(b)</bold> the solubility of water in the organosulfate phase (<inline-formula><mml:math id="M200" display="inline"><mml:mrow><mml:mi>T</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">298.15</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M201" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">K</mml:mi></mml:mrow></mml:math></inline-formula>). Solubilities were estimated using the SLESOL method to solve the liquid–liquid (LLE) or solid–liquid (SLE) equilibrium in COSMO<italic>therm</italic>. <inline-formula><mml:math id="M202" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">LLE</mml:mi><mml:mo>/</mml:mo><mml:mi mathvariant="normal">SLE</mml:mi></mml:mrow></mml:math></inline-formula> was not found for the systems with missing points, indicating that the solute is fully miscible with the solvent. Relative solubilities of organosulfates and IEPOX were calculated using the LLE solubility of each compound in 0.09 mole fraction of the inorganic salt (AS or ABS) as a reference for the pure water solubility.</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://acp.copernicus.org/articles/20/5679/2020/acp-20-5679-2020-f03.png"/>

        </fig>

      <p id="d1e5335">The LLE was not found for isoprene-derived organosulfates, IEPOX isomers or methyl bisulfate, indicating that these compounds are fully miscible with pure water at 298.15 <inline-formula><mml:math id="M203" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">K</mml:mi></mml:mrow></mml:math></inline-formula>. We therefore also calculated the pure water solubilities relative to the organosulfate solubility in a 0.09 mole fraction salt solution by solving the LLE of ternary systems in which the solvent contains 0.09 mole fraction of either ammonium sulfate (AS, <inline-formula><mml:math id="M204" display="inline"><mml:mrow class="chem"><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:msub><mml:mo>)</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) or ammonium bisulfate (ABS, <inline-formula><mml:math id="M205" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">HSO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>). Solubility calculations for ternary systems are described in more detail in Sect. <xref ref-type="sec" rid="Ch1.S3.SS2"/>. This is done to get a quantitative estimate of the relative solubilities of the compounds that are fully soluble in pure water. The 0.09 mole fraction is below the solubility limit of both <inline-formula><mml:math id="M206" display="inline"><mml:mrow class="chem"><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:msub><mml:mo>)</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M207" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mrow><mml:mi mathvariant="normal">SOL</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">AS</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.094</mml:mn></mml:mrow></mml:math></inline-formula>) and <inline-formula><mml:math id="M208" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">HSO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M209" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mrow><mml:mi mathvariant="normal">SOL</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">ABS</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.33</mml:mn></mml:mrow></mml:math></inline-formula>) in water at 298.15 <inline-formula><mml:math id="M210" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">K</mml:mi></mml:mrow></mml:math></inline-formula> <xref ref-type="bibr" rid="bib1.bibx51" id="paren.56"/>. The specific inorganic salt mole fraction was chosen to be as high as possible while within the aqueous solubility limit of the salt to ensure that the organic compounds are typically not fully miscible with the salt solution. Results are shown in Fig. <xref ref-type="fig" rid="Ch1.F3"/> together with corresponding binary organic solubilities. Compared to the binary LLE solubility, the aqueous solubility calculated as a relative solubility for monoterpene-derived organosulfates is on average 3.1 times higher (1.8–5.5) using <inline-formula><mml:math id="M211" display="inline"><mml:mrow class="chem"><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:msub><mml:mo>)</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> solutions as a reference and 2.2 times higher (1.7–2.9) using <inline-formula><mml:math id="M212" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">HSO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> solutions. The LLE was not found in the ternary systems containing IEPOX and 0.09 mole fraction of <inline-formula><mml:math id="M213" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">HSO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>.</p>
      <p id="d1e5537">Based on LLE calculations, the monoterpene-derived organosulfates are less soluble in the ammonium sulfate and<?pagebreak page5686?> bisulfate solutions than in pure water, which means that the ammonium salts have a salting-out effect on the OS. From the solubilities calculated as relative solubility compared to <inline-formula><mml:math id="M214" display="inline"><mml:mrow class="chem"><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:msub><mml:mo>)</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M215" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">HSO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> solutions, we can see that the relative solubility calculation in COSMO<italic>therm</italic> overestimates the salting-out effect of both ammonium salts compared to the more accurate LLE calculation. In addition, the salting-out effect of <inline-formula><mml:math id="M216" display="inline"><mml:mrow class="chem"><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:msub><mml:mo>)</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is overestimated more than that of <inline-formula><mml:math id="M217" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">HSO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>. The relative solubility calculation uses the zeroth-order solubility approximation, which means that the estimate is less accurate when the absolute solubility of the solute is high. The largest difference between the aqueous LLE and the solubility calculated relative to the ternary LLE is seen for the OS with the higher absolute solubilities.</p>
      <p id="d1e5621">We see in Fig. <xref ref-type="fig" rid="Ch1.F3"/> that <inline-formula><mml:math id="M218" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene-OS-1 has the lowest solubility of all the organosulfates. There are only minor structural differences between <inline-formula><mml:math id="M219" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene-OS-1 and <inline-formula><mml:math id="M220" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene-OS-2, but this still leads to a factor of 3.6 difference in the calculated solubility. All the <inline-formula><mml:math id="M221" display="inline"><mml:mi mathvariant="italic">β</mml:mi></mml:math></inline-formula>-pinene and limonene organosulfates, with the same functional groups as <inline-formula><mml:math id="M222" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene-OS-1 and <inline-formula><mml:math id="M223" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene-OS-2, have solubilities between those of <inline-formula><mml:math id="M224" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene-OS-1 and <inline-formula><mml:math id="M225" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene-OS-2. These results show that even minor differences in the molecular structure, such as the placement of functional groups, can have a large impact on the solubility of organosulfates.</p>
      <p id="d1e5683">The most soluble monoterpene-derived organosulfates are <inline-formula><mml:math id="M226" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene-OS-5 and <inline-formula><mml:math id="M227" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene-OS-6, which each have both a carboxylic acid group and a carbonyl group. <inline-formula><mml:math id="M228" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-Pinene-OS-4 has a flexible carbon backbone and three carbonyl functionalities; however, it still has a relatively low solubility compared to the other <inline-formula><mml:math id="M229" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene-OS. The effect of the different types of oxygen-containing functional groups on the solubilities is caused by their ability to form intermolecular hydrogen bonds with the solvent water. This explains the lower solubility of <inline-formula><mml:math id="M230" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene-OS-4, which has mainly hydrogen-bond-accepting carbonyl groups, compared to <inline-formula><mml:math id="M231" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene-OS-3, <inline-formula><mml:math id="M232" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene-OS-5 and <inline-formula><mml:math id="M233" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene-OS-6, which contain hydroxy groups that can act as both H-bond acceptors and donors.</p>
      <p id="d1e5743">We calculated acid constants (p<inline-formula><mml:math id="M234" display="inline"><mml:mrow><mml:msub><mml:mi>K</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) for all organosulfates to capture the effect of the dissociation of the neutral molecules in water. Estimated p<inline-formula><mml:math id="M235" display="inline"><mml:mrow><mml:msub><mml:mi>K</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> values of the organosulfates are between <inline-formula><mml:math id="M236" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">4.57</mml:mn></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M237" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2.37</mml:mn></mml:mrow></mml:math></inline-formula>, indicating that all of the organosulfates are strong acids that will likely be strongly dissociated in water. For comparison, we estimated the first p<inline-formula><mml:math id="M238" display="inline"><mml:mrow><mml:msub><mml:mi>K</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> of sulfuric acid with COSMO<italic>therm</italic> to be <inline-formula><mml:math id="M239" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3.51</mml:mn></mml:mrow></mml:math></inline-formula>. The organosulfates are therefore estimated to be of equivalent strength or even stronger acids than <inline-formula><mml:math id="M240" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, and thus for all practical purposes they fully dissociate in near-neutral solutions and even solutions at the most atmospherically relevant pH. The p<inline-formula><mml:math id="M241" display="inline"><mml:mrow><mml:msub><mml:mi>K</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> values for all organosulfates and sulfuric acid are shown in Table S1 of the Supplement.</p>
      <p id="d1e5840">Dissociation-corrected solubilities were calculated from Eq. (<xref ref-type="disp-formula" rid="Ch1.E11"/>) using the LLE solubilities in pure water and p<inline-formula><mml:math id="M242" display="inline"><mml:mrow><mml:msub><mml:mi>K</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> estimated with COSMO<italic>therm</italic>. Molar liquid volumes of the pure organic compounds used to calculate the densities of organic-water solutions for Eq. (<xref ref-type="disp-formula" rid="Ch1.E12"/>) are shown in Table S7. For all organic compounds, dissociation-corrected solubilities correspond to mole fractions higher than 1. This unphysical result is likely caused by the inability of Eq. (<xref ref-type="disp-formula" rid="Ch1.E11"/>) to accurately capture the solution behavior of very strongly acidic compounds. This equation is only used to calculate dissociation-corrected solubilities and has no effect on other property calculations. The dissociation of strong acids is expected to be high in solutions with higher pH than the p<inline-formula><mml:math id="M243" display="inline"><mml:mrow><mml:msub><mml:mi>K</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> of the solute <xref ref-type="bibr" rid="bib1.bibx6" id="paren.57"/>, as is the case here.</p>
      <p id="d1e5878">Since the organosulfates strongly dissociate in water, we also calculated the aqueous solubilities of their sodium salts (NaOS). For these sodium organosulfate salts, we used the heat capacity of fusion estimate (<inline-formula><mml:math id="M244" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>C</mml:mi><mml:mrow><mml:mi>p</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">fus</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>H</mml:mi><mml:mi mathvariant="normal">fus</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">melt</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) with a melting point of 478.15 <inline-formula><mml:math id="M245" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">K</mml:mi></mml:mrow></mml:math></inline-formula> <xref ref-type="bibr" rid="bib1.bibx42" id="paren.58"/> and a heat of fusion of 50 <inline-formula><mml:math id="M246" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">kJ</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msup><mml:mi mathvariant="normal">mol</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> <xref ref-type="bibr" rid="bib1.bibx45" id="paren.59"/>. Calculated solubilities of the NaOS salts are shown in Fig. <xref ref-type="fig" rid="Ch1.F3"/> and Table S1. For systems in which a solid–liquid equilibrium was found, the solubility of the organosulfate sodium salt is around 0.065 mole fraction.</p>
</sec>
<?pagebreak page5687?><sec id="Ch1.S3.SS2">
  <label>3.2</label><title>Solubility in aqueous ammonium sulfate and bisulfate solutions</title>
      <p id="d1e5957">Solubilities of both OS and NaOS were calculated by solving the LLE or the SLE, respectively, in aqueous solvents containing 0.09 mole fraction of either ammonium sulfate or ammonium bisulfate. Solubility values for the OS and NaOS in these solvents, and the aqueous ammonium sulfate and bisulfate salt solutions in the OS phase, are given in Table S2.</p>
      <p id="d1e5960">Organic solubilities in aqueous inorganic solutions ranging from pure water to 0.09 mole fraction of inorganic salt were calculated using relative screening. These relative solubilities were then scaled using the absolute solubility values of the 0.09 mole fraction binary solvents to obtain the final relative solubilities of the OS and NaOS with respect to each binary system at the different inorganic salt mole fractions. The procedure is described in detail in Sect. S2. Relative solubilities are shown in Fig. <xref ref-type="fig" rid="Ch1.F4"/> (OS in <inline-formula><mml:math id="M247" display="inline"><mml:mrow class="chem"><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:msub><mml:mo>)</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>), Fig. <xref ref-type="fig" rid="Ch1.F5"/> (NaOS in <inline-formula><mml:math id="M248" display="inline"><mml:mrow class="chem"><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:msub><mml:mo>)</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>), Fig. S7 (OS in <inline-formula><mml:math id="M249" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">HSO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) and Fig. S8 (NaOS in <inline-formula><mml:math id="M250" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">HSO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4" specific-use="star"><?xmltex \currentcnt{4}?><label>Figure 4</label><caption><p id="d1e6048">Relative solubilities of OS in <inline-formula><mml:math id="M251" display="inline"><mml:mrow class="chem"><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:msub><mml:mo>)</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> (aq) solutions (<inline-formula><mml:math id="M252" display="inline"><mml:mrow><mml:mi>T</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">298.15</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M253" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">K</mml:mi></mml:mrow></mml:math></inline-formula> relative to pure water) estimated in COSMO<italic>therm</italic> using relative screening. <bold>(a)</bold> Results for the lower binary salt mole fraction range from 0 to <inline-formula><mml:math id="M254" display="inline"><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> and <bold>(b)</bold> the whole range between 0 and 0.09 mole fraction of the salt. The black dotted line in <bold>(a)</bold> shows the relative solubility of 1, equivalent to the solubility of the OS in pure water.</p></caption>
          <?xmltex \igopts{width=369.885827pt}?><graphic xlink:href="https://acp.copernicus.org/articles/20/5679/2020/acp-20-5679-2020-f04.png"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5"><?xmltex \currentcnt{5}?><label>Figure 5</label><caption><p id="d1e6134">Relative solubilities of NaOS salts in <inline-formula><mml:math id="M255" display="inline"><mml:mrow class="chem"><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:msub><mml:mo>)</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> (aq) solutions (<inline-formula><mml:math id="M256" display="inline"><mml:mrow><mml:mi>T</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">298.15</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M257" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">K</mml:mi></mml:mrow></mml:math></inline-formula> relative to pure water) estimated using relative screening in COSMO<italic>therm</italic>.</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://acp.copernicus.org/articles/20/5679/2020/acp-20-5679-2020-f05.png"/>

        </fig>

      <p id="d1e6189">At low (<inline-formula><mml:math id="M258" display="inline"><mml:mrow><mml:mo>&lt;</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>) <inline-formula><mml:math id="M259" display="inline"><mml:mrow class="chem"><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:msub><mml:mo>)</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> mole fractions, the molecular organosulfates salt in, meaning
that the presence of the inorganic salt enhances the total amount of the organosulfate soluble in the aqueous phase. At higher inorganic salt mole fractions the organosulfates salt out. All IEPOX isomers and NaOS salts salt out in the presence of co-solvated <inline-formula><mml:math id="M260" display="inline"><mml:mrow class="chem"><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:msub><mml:mo>)</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> across the whole concentration range. At 0.09 mole fraction of <inline-formula><mml:math id="M261" display="inline"><mml:mrow class="chem"><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:msub><mml:mo>)</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, the organic compounds can be grouped into three categories based on their relative solubilities: methyl bisulfate with the highest relative solubility, isoprene-derived organosulfates and IEPOX in the middle, and all monoterpene-derived organosulfates with the lowest relative solubilities with respect to the pure aqueous solubility.</p>
      <p id="d1e6277">All of the organic compounds salt out in ternary aqueous solutions with <inline-formula><mml:math id="M262" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">HSO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> (see Figs. S7 and S8), but the salting-out effect of <inline-formula><mml:math id="M263" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">HSO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> on the organic compounds is weaker than that of <inline-formula><mml:math id="M264" display="inline"><mml:mrow class="chem"><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:msub><mml:mo>)</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>. This is due to the stronger salting interactions of the doubly charged sulfate ion compared to the singly charged bisulfate ion.</p>
      <p id="d1e6335">As was mentioned above, the salting-out of organosulfates from 0.09 mole fraction <inline-formula><mml:math id="M265" display="inline"><mml:mrow class="chem"><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:msub><mml:mo>)</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> solution is overestimated by a factor of 3.1 using the relative solubility calculation compared to the LLE calculation. <xref ref-type="bibr" rid="bib1.bibx56" id="text.60"/> found that COSMO<italic>therm</italic> overestimates the salting-out effect of <inline-formula><mml:math id="M266" display="inline"><mml:mrow class="chem"><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:msub><mml:mo>)</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> on average by a factor of 3 compared to experiments. They described the salting behavior using Setschenow constants calculated from COSMO<italic>therm</italic>-estimated (release 14) partition coefficients, which are comparable to relative solubilities. We used COSMO<italic>therm</italic>19-estimated relative solubilities to calculate corresponding Setschenow constants for the compounds used by <xref ref-type="bibr" rid="bib1.bibx56" id="text.61"/> that are
in COSMO<italic>base</italic>17 and the same 5 % <inline-formula><mml:math id="M267" display="inline"><mml:mrow class="chem"><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:msub><mml:mo>)</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> solution (<inline-formula><mml:math id="M268" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">w</mml:mi><mml:mo>/</mml:mo><mml:mi mathvariant="normal">v</mml:mi></mml:mrow></mml:math></inline-formula>, corresponding to <inline-formula><mml:math id="M269" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi mathvariant="normal">AS</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.007</mml:mn></mml:mrow></mml:math></inline-formula>) with solvent densities by <xref ref-type="bibr" rid="bib1.bibx51" id="text.62"/>. We found that COSMO<italic>therm</italic>19 overestimates the experimental Setschenow constant of these compounds in 5 % <inline-formula><mml:math id="M270" display="inline"><mml:mrow class="chem"><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:msub><mml:mo>)</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> solution on average by a factor of 1.5 (see Fig. S11), which is an improvement to the factor of 3 of COSMO<italic>therm</italic>14. The overestimation might be decreased by calculating LLE solubilities as opposed to relative solubilities that use the zeroth-order solubility approximation. However, finding the LLE of multiple systems is computationally infeasible and not certain to improve the results.</p>
      <p id="d1e6486">Liquid–liquid-phase separation (LLPS) has been detected in several aerosol experiments <xref ref-type="bibr" rid="bib1.bibx46 bib1.bibx47 bib1.bibx41 bib1.bibx19" id="paren.63"/>. For example, <xref ref-type="bibr" rid="bib1.bibx46" id="text.64"/> observed LLPS for ammonium sulfate aerosol that contained organic compounds with <inline-formula><mml:math id="M271" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">O</mml:mi><mml:mo>:</mml:mo><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula> below 0.8, whereas no LLPS was seen with <inline-formula><mml:math id="M272" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">O</mml:mi><mml:mo>:</mml:mo><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula> above 0.8, depending on the functional groups. In these experiments, organic compounds contained hydroxy, carbonyl and carboxylic acid groups <xref ref-type="bibr" rid="bib1.bibx46" id="paren.65"/>. In binary aerosol systems containing water and organic compounds (without inorganic salt), <xref ref-type="bibr" rid="bib1.bibx47" id="text.66"/> observed LLPS for <inline-formula><mml:math id="M273" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">O</mml:mi><mml:mo>:</mml:mo><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula> below 0.44 or 0.58 in systems with one or two different organic compounds, respectively. The compounds in this study contain ester, ether and hydroxy functional groups <xref ref-type="bibr" rid="bib1.bibx47" id="paren.67"/>. With <inline-formula><mml:math id="M274" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">O</mml:mi><mml:mo>:</mml:mo><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula> ratios of the monoterpene- and isoprene-derived organosulfates in the ranges 0.5–0.7 and 1.2–1.4, respectively, these results are consistent with the present work. On the other hand, in experiments with an OH-oxidized <inline-formula><mml:math id="M275" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene and water system <xref ref-type="bibr" rid="bib1.bibx19" id="paren.68"/> only a single organic-rich phase was observed, whereas LLPS was seen between water and ozone-oxidized <inline-formula><mml:math id="M276" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene products <xref ref-type="bibr" rid="bib1.bibx19" id="paren.69"/> or OH-oxidized isoprene products <xref ref-type="bibr" rid="bib1.bibx41" id="paren.70"/>. There are small differences in the partial charges of the oxygen atoms associated with a sulfate group compared to a carboxylic acid group (see Sect. S3 for a comparison of the <inline-formula><mml:math id="M277" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> potentials) that may influence the <inline-formula><mml:math id="M278" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">O</mml:mi><mml:mo>:</mml:mo><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula> ratio of organosulfates required for LLPS. From our results we can also see that other structural factors further affect the thermodynamic properties, in addition to the <inline-formula><mml:math id="M279" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">O</mml:mi><mml:mo>:</mml:mo><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula> ratio or the types of functional groups.</p>
</sec>
<sec id="Ch1.S3.SS3">
  <label>3.3</label><title>Activity</title>
      <p id="d1e6616">Activities were calculated for organosulfates, IEPOX isomers and water in binary aqueous mixtures with different organic-to-water molar ratios (see Table S3). Figure <xref ref-type="fig" rid="Ch1.F6"/> shows, as examples, binary mixing diagrams similar to that presented by <xref ref-type="bibr" rid="bib1.bibx40" id="text.71"/> for water and (a) <inline-formula><mml:math id="M280" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene-OS-5, (b) <inline-formula><mml:math id="M281" display="inline"><mml:mi mathvariant="italic">β</mml:mi></mml:math></inline-formula>-pinene-OS-1, (c) limonene-OS-1, (d) isoprene-OS-2, and (e) <inline-formula><mml:math id="M282" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">δ</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>-IEPOX. Diagonal dashed lines illustrate the ideal mole-fraction-based activities (<inline-formula><mml:math id="M283" display="inline"><mml:mrow><mml:msub><mml:mi>a</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) with respect to a pure compound (<inline-formula><mml:math id="M284" display="inline"><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mi mathvariant="normal">OS</mml:mi></mml:mrow></mml:math></inline-formula>, water) reference state. Since the solubility of the organics in water is much smaller than the solubility of water in the organics, the mixing diagrams for monoterpene-derived organosulfates (Fig. <xref ref-type="fig" rid="Ch1.F6"/>a–c) are divided into two sections (note the different scales of the two phase<?pagebreak page5688?> regions): the aqueous phase (left sides) and the organic phase (right sides). In between is a composition range corresponding to the miscibility gap. From Fig. <xref ref-type="fig" rid="Ch1.F6"/>a–c we see how the calculated water and organosulfate activities fulfill the liquid-phase equilibrium condition of Eq. (<xref ref-type="disp-formula" rid="Ch1.E9"/>) at the solubility limit.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6"><?xmltex \currentcnt{6}?><label>Figure 6</label><caption><p id="d1e6688">Activities of OS, IEPOX and water in binary mixtures; <bold>(a)</bold> <inline-formula><mml:math id="M285" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene-OS-5, <bold>(b)</bold> <inline-formula><mml:math id="M286" display="inline"><mml:mi mathvariant="italic">β</mml:mi></mml:math></inline-formula>-pinene-OS-1, <bold>(c)</bold> limonene-OS-1, <bold>(d)</bold> isoprene-OS-2, <bold>(e)</bold> <inline-formula><mml:math id="M287" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">δ</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>-IEPOX. The left-hand sides of panels <bold>(a–c)</bold> show the water-rich phase, and the right-hand sides show the corresponding organic-rich phase.</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://acp.copernicus.org/articles/20/5679/2020/acp-20-5679-2020-f06.png"/>

        </fig>

      <p id="d1e6741">Activities for the monoterpene-derived organosulfates display three different types of behavior. The most common is exemplified in Fig. <xref ref-type="fig" rid="Ch1.F6"/>a, where in the organic-rich phase, the organosulfate activity is lower than the mole fraction of the organics (<inline-formula><mml:math id="M288" display="inline"><mml:mrow><mml:msub><mml:mi>a</mml:mi><mml:mi mathvariant="normal">OS</mml:mi></mml:msub><mml:mo>≤</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi mathvariant="normal">OS</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>). A low activity indicates that the organosulfate is more stable in the organic-rich phase than in the ideal pure organosulfate. The water activity is below the ideal activity (<inline-formula><mml:math id="M289" display="inline"><mml:mrow><mml:msub><mml:mi>a</mml:mi><mml:mi mathvariant="normal">w</mml:mi></mml:msub><mml:mo>&lt;</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi mathvariant="normal">w</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) at low mole fractions of water and above the ideal activity (<inline-formula><mml:math id="M290" display="inline"><mml:mrow><mml:msub><mml:mi>a</mml:mi><mml:mi mathvariant="normal">w</mml:mi></mml:msub><mml:mo>&gt;</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi mathvariant="normal">w</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) at higher water mole fractions in the organic-rich phase. The organic activity at the solubility limit is low (<inline-formula><mml:math id="M291" display="inline"><mml:mrow><mml:msub><mml:mi>a</mml:mi><mml:mi mathvariant="normal">OS</mml:mi></mml:msub><mml:mo>&lt;</mml:mo><mml:mn mathvariant="normal">0.28</mml:mn></mml:mrow></mml:math></inline-formula> when <inline-formula><mml:math id="M292" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi mathvariant="normal">OS</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi mathvariant="normal">SOL</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) compared to the other monoterpene-derived organosulfates. Similar behavior is seen in <inline-formula><mml:math id="M293" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene-OS-3, <inline-formula><mml:math id="M294" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene-OS-4, <inline-formula><mml:math id="M295" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene-OS-6, <inline-formula><mml:math id="M296" display="inline"><mml:mi mathvariant="italic">β</mml:mi></mml:math></inline-formula>-pinene-2 and limonene-OS-4. A comparison between the activities of <inline-formula><mml:math id="M297" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene-OS-5 and <inline-formula><mml:math id="M298" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> calculated using COSMO<italic>therm</italic> and literature values of <inline-formula><mml:math id="M299" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> activities are shown in Fig. S9.</p>
      <p id="d1e6906">The opposite is seen in <inline-formula><mml:math id="M300" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene-OS-1, <inline-formula><mml:math id="M301" display="inline"><mml:mi mathvariant="italic">β</mml:mi></mml:math></inline-formula>-pinene-OS-1 (Fig. <xref ref-type="fig" rid="Ch1.F6"/>b) and limonene-OS-3, for which the activity of the organosulfate in the organic-rich phase is very close to or above the ideal activity. In addition, the activity at the solubility limit (both the solubility of the water and the organic) for these compounds is above 0.36. The third behavior type seen in Fig. <xref ref-type="fig" rid="Ch1.F6"/>c is between the first two cases, in which the water activity follows the ideal activity in small mole fractions of water. Here the organic activity at the solubility limit is around 0.3. The other compounds in this group are <inline-formula><mml:math id="M302" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene-OS-2 and limonene-OS-2.</p>
      <p id="d1e6934">Since the isoprene-derived organosulfates, IEPOX isomers and methyl bisulfate are fully miscible with pure water, liquid–liquid-phase separation was not observed for<?pagebreak page5689?> these systems. The mixing diagrams for all isoprene-derived organosulfates and methyl bisulfate are similar to the one shown in Fig. <xref ref-type="fig" rid="Ch1.F6"/>d. Calculated activities for all IEPOX isomers are close to the ideal activities at all mixing states (Fig. <xref ref-type="fig" rid="Ch1.F6"/>e).</p>
      <p id="d1e6941">Figure <xref ref-type="fig" rid="Ch1.F7"/>a–e show mixing diagrams for the same organic compounds as Fig. <xref ref-type="fig" rid="Ch1.F6"/>a–e but now with a solvent that is a 0.09 mole fraction binary aqueous solution of <inline-formula><mml:math id="M303" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">HSO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> instead of pure water. Here, COSMO<italic>therm</italic> also predicts LLPS for systems containing the isoprene-derived organosulfates (Fig. <xref ref-type="fig" rid="Ch1.F7"/>d). Again, activities for the organosulfates are higher than their mole fractions in the water-rich phase. Here we can also see that the predicted activity of water in the binary solvent is 0.78. The corresponding activity coefficients <inline-formula><mml:math id="M304" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">γ</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:msub><mml:mi>a</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>/</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> for the organic compounds and water in each system in Fig. <xref ref-type="fig" rid="Ch1.F7"/> are tabulated in Table S4.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7"><?xmltex \currentcnt{7}?><label>Figure 7</label><caption><p id="d1e6999">Activities for OS, IEPOX and water in ternary aqueous mixtures. The solvent is a 0.09 mole fraction ammonium bisulfate solution, and the ideal water activity is equal to the mole fraction of water; <bold>(a)</bold> <inline-formula><mml:math id="M305" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene-OS-5, <bold>(b)</bold> <inline-formula><mml:math id="M306" display="inline"><mml:mi mathvariant="italic">β</mml:mi></mml:math></inline-formula>-pinene-OS-1, <bold>(c)</bold> limonene-OS-1, <bold>(d)</bold> isoprene-OS-2, <bold>(e)</bold> <inline-formula><mml:math id="M307" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">δ</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>-IEPOX. The left-hand sides of panels <bold>(a–d)</bold> show the solvent-rich phase, and the right-hand sides show the organic-rich phase. The ABS-to-water ratio is kept constant in all calculated mixing states, which means that ammonium bisulfate and water are not individually at equilibrium at the solubility limits.</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://acp.copernicus.org/articles/20/5679/2020/acp-20-5679-2020-f07.png"/>

        </fig>

      <p id="d1e7052">The calculated activity of each organic compound in the aqueous phase is higher in the ternary <inline-formula><mml:math id="M308" display="inline"><mml:mrow><mml:mi mathvariant="normal">OS</mml:mi><mml:mo>+</mml:mo><mml:mi mathvariant="normal">aqueous</mml:mi></mml:mrow></mml:math></inline-formula> ammonium bisulfate systems compared to the binary <inline-formula><mml:math id="M309" display="inline"><mml:mrow><mml:mi mathvariant="normal">OS</mml:mi><mml:mo>+</mml:mo><mml:mi mathvariant="normal">water</mml:mi></mml:mrow></mml:math></inline-formula> systems. This means that the inorganic salt decreases the stability of the organosulfate in the aqueous phase. At the same time, the stability of the organosulfate in the organic-rich phase also decreases in the presence of the inorganic salt.</p>
      <p id="d1e7080">Similar mixing diagrams for 0.09 mole fraction aqueous ammonium sulfate solvent are shown in Fig. S10 and tabulated values in Table S5. In ammonium sulfate solutions, COSMO<italic>therm</italic> predicts a water activity of 1.14 in the aqueous solvent-rich phase, indicating that according to COSMO<italic>therm</italic>, the 0.09 mole fraction aqueous solution of ammonium sulfate is unstable. This discrepancy with the experimental solubility of <inline-formula><mml:math id="M310" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mrow><mml:mi mathvariant="normal">SOL</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">AS</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.094</mml:mn></mml:mrow></mml:math></inline-formula> <xref ref-type="bibr" rid="bib1.bibx51" id="paren.72"/> is possibly caused by an inadequate representation of the solvation of ionic liquids in COSMO-RS theory <xref ref-type="bibr" rid="bib1.bibx53" id="paren.73"/>.</p><?xmltex \hack{\newpage}?>
</sec>
<?pagebreak page5690?><sec id="Ch1.S3.SS4">
  <label>3.4</label><title>Saturation vapor pressure</title>
      <p id="d1e7124">We calculated saturation vapor pressures for the neutral organic compounds at 298.15 <inline-formula><mml:math id="M311" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">K</mml:mi></mml:mrow></mml:math></inline-formula> (Table <xref ref-type="table" rid="Ch1.T1"/>). Comparing the studied organosulfate compounds based on their functional groups, those containing carboxylic acid groups, i.e., <inline-formula><mml:math id="M312" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene-OS-5 and <inline-formula><mml:math id="M313" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene-OS-6, have the lowest saturation vapor pressures. <inline-formula><mml:math id="M314" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-Pinene-OS-4, also having an <inline-formula><mml:math id="M315" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">O</mml:mi><mml:mo>:</mml:mo><mml:mi mathvariant="normal">C</mml:mi></mml:mrow></mml:math></inline-formula> ratio of 0.7, has an order of magnitude higher saturation vapor pressure, indicating that two carbonyl groups are less effective at lowering the vapor pressure than a single carboxylic acid group. In addition, <inline-formula><mml:math id="M316" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene-OS-3 (one carbonyl and one hydroxy group) has a lower saturation vapor pressure than <inline-formula><mml:math id="M317" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene-OS-4 with one more oxygen atom.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1"><?xmltex \currentcnt{1}?><label>Table 1</label><caption><p id="d1e7188">Estimated saturation vapor pressures of the pure compounds and the ratio between the saturation vapor pressures of the organic compound and sulfuric acid.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="3">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Compound</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M318" display="inline"><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mi mathvariant="normal">sat</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M319" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">Pa</mml:mi></mml:mrow></mml:math></inline-formula>)</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M320" display="inline"><mml:mstyle displaystyle="false"><mml:mfrac style="text"><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mi mathvariant="normal">sat</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mrow><mml:mi mathvariant="normal">sat</mml:mi><mml:mo>,</mml:mo><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mstyle></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M321" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene-OS-1</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M322" display="inline"><mml:mrow><mml:mn mathvariant="normal">7.96</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">6</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M323" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.10</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">4</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M324" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene-OS-2</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M325" display="inline"><mml:mrow><mml:mn mathvariant="normal">2.00</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M326" display="inline"><mml:mrow><mml:mn mathvariant="normal">2.78</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">4</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M327" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene-OS-3</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M328" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.08</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">8</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M329" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.49</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">7</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M330" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene-OS-4</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M331" display="inline"><mml:mrow><mml:mn mathvariant="normal">4.31</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">8</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M332" display="inline"><mml:mrow><mml:mn mathvariant="normal">5.98</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">7</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M333" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene-OS-5</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M334" display="inline"><mml:mrow><mml:mn mathvariant="normal">5.19</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">9</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M335" display="inline"><mml:mrow><mml:mn mathvariant="normal">7.20</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">8</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"><inline-formula><mml:math id="M336" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene-OS-6</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M337" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.37</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">9</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M338" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.90</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">8</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M339" display="inline"><mml:mi mathvariant="italic">β</mml:mi></mml:math></inline-formula>-pinene-OS-1</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M340" display="inline"><mml:mrow><mml:mn mathvariant="normal">3.65</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">6</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M341" display="inline"><mml:mrow><mml:mn mathvariant="normal">5.07</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"><inline-formula><mml:math id="M342" display="inline"><mml:mi mathvariant="italic">β</mml:mi></mml:math></inline-formula>-pinene-OS-2</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M343" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.28</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M344" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.78</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">4</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">limonene-OS-1</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M345" display="inline"><mml:mrow><mml:mn mathvariant="normal">4.84</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">6</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M346" display="inline"><mml:mrow><mml:mn mathvariant="normal">6.72</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">limonene-OS-2</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M347" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.88</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">6</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M348" display="inline"><mml:mrow><mml:mn mathvariant="normal">2.61</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">limonene-OS-3</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M349" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.36</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">6</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M350" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.89</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">limonene-OS-4</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M351" display="inline"><mml:mrow><mml:mn mathvariant="normal">3.10</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">6</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M352" display="inline"><mml:mrow><mml:mn mathvariant="normal">4.31</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">isoprene-OS-1</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M353" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.68</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">6</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M354" display="inline"><mml:mrow><mml:mn mathvariant="normal">2.33</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">isoprene-OS-2</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M355" display="inline"><mml:mrow><mml:mn mathvariant="normal">2.15</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M356" display="inline"><mml:mrow><mml:mn mathvariant="normal">2.98</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">4</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">isoprene-OS-3</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M357" display="inline"><mml:mrow><mml:mn mathvariant="normal">2.42</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">8</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M358" display="inline"><mml:mrow><mml:mn mathvariant="normal">3.36</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">7</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">isoprene-OS-4</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M359" display="inline"><mml:mrow><mml:mn mathvariant="normal">2.07</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">8</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M360" display="inline"><mml:mrow><mml:mn mathvariant="normal">2.87</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">7</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><italic>cis</italic>-<inline-formula><mml:math id="M361" display="inline"><mml:mi mathvariant="italic">β</mml:mi></mml:math></inline-formula>-IEPOX</oasis:entry>
         <oasis:entry colname="col2">0.235</oasis:entry>
         <oasis:entry colname="col3">3.26</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><italic>trans</italic>-<inline-formula><mml:math id="M362" display="inline"><mml:mi mathvariant="italic">β</mml:mi></mml:math></inline-formula>-IEPOX</oasis:entry>
         <oasis:entry colname="col2">0.392</oasis:entry>
         <oasis:entry colname="col3">5.43</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M363" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">δ</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>-IEPOX</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M364" display="inline"><mml:mrow><mml:mn mathvariant="normal">2.35</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">1</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M365" display="inline"><mml:mrow><mml:mn mathvariant="normal">3.26</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"><inline-formula><mml:math id="M366" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">δ</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>-IEPOX</oasis:entry>
         <oasis:entry colname="col2">0.441</oasis:entry>
         <oasis:entry colname="col3">6.12</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">methyl bisulfate</oasis:entry>
         <oasis:entry colname="col2">1.04</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M367" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.44</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mn mathvariant="normal">1</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">sulfuric acid</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M368" display="inline"><mml:mrow><mml:mn mathvariant="normal">7.21</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3">1</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p id="d1e8188">The saturation vapor pressure of sulfuric acid (extrapolated from experimental data using ab initio data) is <inline-formula><mml:math id="M369" display="inline"><mml:mrow><mml:mn mathvariant="normal">2.10</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M370" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">Pa</mml:mi></mml:mrow></mml:math></inline-formula> at 298.15 <inline-formula><mml:math id="M371" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">K</mml:mi></mml:mrow></mml:math></inline-formula> <xref ref-type="bibr" rid="bib1.bibx1 bib1.bibx29 bib1.bibx38" id="paren.74"/>, while COSMO<italic>therm</italic> estimates the vapor pressure of the pure sulfuric acid to be <inline-formula><mml:math id="M372" display="inline"><mml:mrow><mml:mn mathvariant="normal">7.21</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M373" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">Pa</mml:mi></mml:mrow></mml:math></inline-formula> (about 34 times higher). Due to the previously demonstrated systematic overestimation of absolute saturation vapor pressures by COSMO<italic>therm</italic> <xref ref-type="bibr" rid="bib1.bibx30" id="paren.75"/>, we show both absolute vapor pressures and the vapor pressures relative to the estimated sulfuric acid saturation vapor pressure in Table <xref ref-type="table" rid="Ch1.T1"/>. The saturation vapor pressures of monoterpene- and isoprene-derived organosulfates are all 4 to 8 orders of magnitude lower than that of sulfuric acid. On the other hand, the saturation vapor pressures of IEPOX isomers and methyl bisulfate are higher than for sulfuric acid.</p>
      <p id="d1e8267">Compared to previously calculated saturation vapor pressures for <inline-formula><mml:math id="M374" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene autoxidation products using COSMO<italic>therm</italic>, the organosulfates studied here are significantly less volatile <xref ref-type="bibr" rid="bib1.bibx30" id="paren.76"/>. It should be noted, however, that in the study of <xref ref-type="bibr" rid="bib1.bibx30" id="text.77"/>, the number of intramolecular hydrogen bonds was not limited in the COSMO<italic>therm</italic> calculations, which likely led to higher saturation vapor pressure estimates <xref ref-type="bibr" rid="bib1.bibx31" id="paren.78"/>. Furthermore, as we have seen here, the acidic organosulfates readily dissociate in the particle phase, forming ionic species, which will effectively suppress their partitioning to the gas phase.</p>
      <p id="d1e8293"><inline-formula><mml:math id="M375" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">δ</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>-IEPOX has a higher saturation vapor pressure than the other IEPOX isomers. This can be understood from a structural point of view, as the lowest-energy conformer (highest weight in the COSMO<italic>therm</italic> calculations) of <inline-formula><mml:math id="M376" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">δ</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>-IEPOX seems to have two intramolecular hydrogen bonds. COSMO<italic>therm</italic> does not count either of these as full or partial intramolecular hydrogen bonds in the condensed phase. However, the gas-phase free energy (<inline-formula><mml:math id="M377" display="inline"><mml:mrow><mml:msup><mml:mi>G</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mi>g</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>) of the conformer is lower than for the other IEPOX conformers, leading to about 5 <inline-formula><mml:math id="M378" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">kJ</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">mol</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> of difference in the energy between the condensed and gas phase of <inline-formula><mml:math id="M379" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">δ</mml:mi><mml:mn mathvariant="normal">1</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>-IEPOX and <inline-formula><mml:math id="M380" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">δ</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>-IEPOX. This in turn leads to a relatively higher saturation vapor pressure (Eq. <xref ref-type="disp-formula" rid="Ch1.E19"/>) compared to the other IEPOX isomers.</p>
</sec>
<sec id="Ch1.S3.SS5">
  <label>3.5</label><title>Henry's law solubility</title>
      <p id="d1e8390">The activity coefficients at infinite dilution in water, the free energies of solvation and Henry's law solubilities in pure water calculated using the different methods (explained in Sect. <xref ref-type="sec" rid="Ch1.S2.SS2.SSS4"/>) at 298.15 <inline-formula><mml:math id="M381" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">K</mml:mi></mml:mrow></mml:math></inline-formula> are given in Table S6. Among the studied organics, Henry's law solubility is the highest for monoterpene- and isoprene-derived organosulfates containing the highest number of oxygen atoms and the lowest for methyl bisulfate and the IEPOX isomers.
The infinite dilution Henry's law solubilities (<inline-formula><mml:math id="M382" display="inline"><mml:mrow><mml:msubsup><mml:mi>H</mml:mi><mml:mi mathvariant="normal">sol</mml:mi><mml:mi mathvariant="normal">∞</mml:mi></mml:msubsup></mml:mrow></mml:math></inline-formula>) were calculated by COSMO<italic>therm</italic> using Eq. (<xref ref-type="disp-formula" rid="Ch1.E21"/>). We also calculated LLE-based Henry's law solubilities (<inline-formula><mml:math id="M383" display="inline"><mml:mrow><mml:msubsup><mml:mi>H</mml:mi><mml:mi mathvariant="normal">sol</mml:mi><mml:mi mathvariant="normal">LLE</mml:mi></mml:msubsup></mml:mrow></mml:math></inline-formula>) using Eq. (<xref ref-type="disp-formula" rid="Ch1.E23"/>) with the pure water solubilities of the organic compounds. A comparison between the infinite dilution and the LLE-based Henry solubilities is shown in Fig. <xref ref-type="fig" rid="Ch1.F8"/>. The LLE-based Henry's law solubility for monoterpene-derived <inline-formula><mml:math id="M384" display="inline"><mml:mrow><mml:mi mathvariant="normal">OS</mml:mi><mml:mo>+</mml:mo><mml:mi mathvariant="normal">water</mml:mi></mml:mrow></mml:math></inline-formula> is on average 4.4 times lower than the corresponding infinite dilution Henry's law solubility. Henry's law solubility is the equilibrium ratio between the abundance in the gas phase and in the aqueous phase for a dilute solution. For the fully miscible compounds, including the dissociation correction, the solution is<?pagebreak page5691?> no longer dilute. We therefore did not calculate the LLE-based Henry's law solubility of the isoprene-derived compounds and methyl bisulfate, which are fully miscible with pure water at 298.15 <inline-formula><mml:math id="M385" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">K</mml:mi></mml:mrow></mml:math></inline-formula>.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F8"><?xmltex \currentcnt{8}?><label>Figure 8</label><caption><p id="d1e8461">Comparison between infinite dilution Henry's law solubility (<inline-formula><mml:math id="M386" display="inline"><mml:mrow><mml:msubsup><mml:mi>H</mml:mi><mml:mi mathvariant="normal">sol</mml:mi><mml:mi mathvariant="normal">∞</mml:mi></mml:msubsup></mml:mrow></mml:math></inline-formula>) in water, hexanoic acid and <italic>cis</italic>-pinonic acid, and LLE based Henry's law solubility (<inline-formula><mml:math id="M387" display="inline"><mml:mrow><mml:msubsup><mml:mi>H</mml:mi><mml:mi mathvariant="normal">sol</mml:mi><mml:mi mathvariant="normal">LLE</mml:mi></mml:msubsup></mml:mrow></mml:math></inline-formula>) in water. The dashed line shows the <inline-formula><mml:math id="M388" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>:</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> ratio between <inline-formula><mml:math id="M389" display="inline"><mml:mrow><mml:msubsup><mml:mi>H</mml:mi><mml:mi mathvariant="normal">sol</mml:mi><mml:mi mathvariant="normal">∞</mml:mi></mml:msubsup></mml:mrow></mml:math></inline-formula> in water and the other Henry's law solubilities.</p></caption>
          <?xmltex \igopts{width=213.395669pt}?><graphic xlink:href="https://acp.copernicus.org/articles/20/5679/2020/acp-20-5679-2020-f08.png"/>

        </fig>

      <p id="d1e8524">Additionally, we calculated the infinite dilution Henry's law solubilities of all compounds in two organic solvents, hexanoic and <italic>cis</italic>-pinonic acids (see Fig. <xref ref-type="fig" rid="Ch1.F8"/> and Table S6). The densities of these organic acids (<inline-formula><mml:math id="M390" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mi mathvariant="normal">hexanoic</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.9400</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M391" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">cm</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M392" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ρ</mml:mi><mml:mrow><mml:mi mathvariant="normal">cis</mml:mi><mml:mo>-</mml:mo><mml:mi mathvariant="normal">pinonic</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1.0739</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M393" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">g</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">cm</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>) were estimated using COSMO<italic>therm</italic>. The Henry's law solubilities of the monoterpene-derived organosulfates are the lowest in water and the highest in <italic>cis</italic>-pinonic acid. The isoprene-derived compounds (OS and IEPOX) are all less soluble in hexanoic acid than in water. The more oxygenated isoprene-OS-3 and isoprene-OS-4 are also less soluble in <italic>cis</italic>-pinonic acid than in water, opposite to the less oxygenated isoprene-OS-1 and isoprene-OS-2, which are the most soluble in <italic>cis</italic>-pinonic acid. The epoxydiols are least soluble in hexanoic acid and the most soluble in water. This means that the phase separation behavior of OS from different precursors will be different in multiphase atmospheric aerosol, leading to different OS aerosol-phase states depending on the predominant precursor.</p>
      <p id="d1e8615">Figure <xref ref-type="fig" rid="Ch1.F9"/> shows the infinite dilution Henry's law solubilities for the organic compounds in the aqueous mixtures with different mole fractions of ammonium sulfate (panel a) and ammonium bisulfate (panel b). The decrease in Henry's law solubility is steeper with the increase in ammonium sulfate than in ammonium bisulfate. This is due to the stronger salting-out effect on the organics of ammonium sulfate than of ammonium bisulfate, also seen in the relative solubility calculations. In the case of both inorganic salts, all of the hydroxy sulfates, i.e., <inline-formula><mml:math id="M394" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene-OS-1 and <inline-formula><mml:math id="M395" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene-OS-2, and all <inline-formula><mml:math id="M396" display="inline"><mml:mi mathvariant="italic">β</mml:mi></mml:math></inline-formula>-pinene and limonene isomers have similar Henry's law solubilities and trends as a function of salt mole fractions. In ammonium sulfate solutions, the Henry's law solubility of isoprene-derived organosulfates decreases more slowly with the increase in ammonium salt concentration than the solubility of monoterpene-derived organosulfates.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F9" specific-use="star"><?xmltex \currentcnt{9}?><label>Figure 9</label><caption><p id="d1e8643">Infinite dilution Henry's law solubilities in aqueous solutions of <bold>(a)</bold> <inline-formula><mml:math id="M397" display="inline"><mml:mrow class="chem"><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:msub><mml:mo>)</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <bold>(b)</bold> <inline-formula><mml:math id="M398" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">HSO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> at 298.15 <inline-formula><mml:math id="M399" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">K</mml:mi></mml:mrow></mml:math></inline-formula>.</p></caption>
          <?xmltex \igopts{width=455.244094pt}?><graphic xlink:href="https://acp.copernicus.org/articles/20/5679/2020/acp-20-5679-2020-f09.png"/>

        </fig>

      <p id="d1e8705">COSMO<italic>therm</italic>-estimated Henry's law solubility has previously been reported for isoprene-derived 2-methyltetrol <xref ref-type="bibr" rid="bib1.bibx11" id="paren.79"/>, which is similar to isoprene-OS-3 and isoprene-OS-4 with the difference that the sulfate group is replaced by a hydroxy group. We calculated the Henry’s law solubility of 2-methyltetrol in water using COSMO<italic>therm</italic>19 and found that the compounds containing a sulfate group (isoprene-OS-3 and isoprene-OS-4) have Henry's law solubilities that are 4 orders of magnitude higher than the compound containing only hydroxy groups (2-methyltetrol). The higher Henry's law solubility of the organosulfate compared to 2-methyltetrol is caused by 5 orders of magnitude lower saturation vapor pressure and an order of magnitude higher activity coefficient at the infinite dilution of the solute. Similar differences are seen between the IEPOX isomers, isoprene-OS-1 and isoprene-OS-2, although the functional groups in isoprene-OS-1 and isoprene-OS-2 (hydroxy and carbonyl) are different than those in IEPOX (hydroxy and epoxy). This means that the presence of sulfate in SOA and the formation of organosulfate compounds enhance SOA formation, since organosulfates are less likely to evaporate than non-sulfate organics.</p>
</sec>
</sec>
<sec id="Ch1.S4" sec-type="conclusions">
  <label>4</label><title>Conclusions</title>
      <p id="d1e8727">We have used COSMO<italic>therm</italic> to evaluate the thermochemical properties (p<inline-formula><mml:math id="M400" display="inline"><mml:mrow><mml:msub><mml:mi>K</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, solubility, activity, Henry's law solubility and saturation vapor pressure) of organosulfates derived from isoprene, <inline-formula><mml:math id="M401" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene, <inline-formula><mml:math id="M402" display="inline"><mml:mi mathvariant="italic">β</mml:mi></mml:math></inline-formula>-pinene and limonene. These properties are key to governing the phase state behavior and stability of organosulfates as components of atmospheric SOA.</p>
      <p id="d1e8758">Interactions with atmospheric water are critical processes determining the growth of SOA and in turn any size-dependent effects, such as heterogeneous chemistry mediated by available surface area and both the direct and indirect climate effects of aerosols. The studied organosulfates have several polar functional groups and in many cases amphiphilic structures. Overall, the organosulfates display both favorable (<inline-formula><mml:math id="M403" display="inline"><mml:mrow><mml:msub><mml:mi>a</mml:mi><mml:mi mathvariant="normal">OS</mml:mi></mml:msub><mml:mo>&lt;</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi mathvariant="normal">OS</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) and unfavorable (<inline-formula><mml:math id="M404" display="inline"><mml:mrow><mml:msub><mml:mi>a</mml:mi><mml:mi mathvariant="normal">OS</mml:mi></mml:msub><mml:mo>&gt;</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi mathvariant="normal">OS</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) interactions with water in the condensed phase. Both behaviors are seen for the same compound in different regions of the mixing diagram. In <inline-formula><mml:math id="M405" display="inline"><mml:mrow><mml:mi mathvariant="normal">water</mml:mi><mml:mo>+</mml:mo><mml:mi mathvariant="normal">monoterpene</mml:mi></mml:mrow></mml:math></inline-formula>-derived organosulfate mixtures, COSMO<italic>therm</italic> predicts phase separation into organic-rich and water-rich phases. Particles with LLPS have<?pagebreak page5692?> already been detected in field samples and generated in numerous laboratory experiments when mixing inorganic sulfate salts and organic compounds (e.g., carboxylic acids and electrolytes, organosulfates from the oxidation of volatile organic compounds – VOCs) <xref ref-type="bibr" rid="bib1.bibx60 bib1.bibx3" id="paren.80"/>. When a miscibility gap exists, water uptake to the organic-rich aerosol phase, as well as organosulfate formation in the aqueous aerosol, is not a continuous function of relative humidity or organosulfate precursor availability.</p>
      <p id="d1e8815">In the particular case of cloud condensation nuclei (CCN) activation, elevated water activities in a water-rich phase due to the presence of organosulfate solute will suppress water uptake from a decreased Raoult effect (<inline-formula><mml:math id="M406" display="inline"><mml:mrow><mml:msub><mml:mi>a</mml:mi><mml:mi>w</mml:mi></mml:msub><mml:mo>&gt;</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>w</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) and decrease SOA CCN activity. However, interactions may not be constant across the phase diagram. Variations between organic-rich and water-rich phases, as well as between the organosulfates, can contribute to explaining the variation in the limonene-derived OS hygroscopicity parameter between subsaturated and supersaturated conditions observed by <xref ref-type="bibr" rid="bib1.bibx20" id="text.81"/>. They also found a nonlinear composition dependence of the CCN activity of mixed OS–AS aerosols and connected the inability of their Köhler model to capture this trend with the nonideal behavior of the droplet solutions <xref ref-type="bibr" rid="bib1.bibx20" id="paren.82"/>. The COSMO<italic>therm</italic>-estimated activities can be used in Köhler calculations to model the nonideality of aqueous droplet solutions. For instance, the hygroscopic growth factor (calculated as a ratio between wet and dry particle diameter) is higher for particles with lower water activity than for particles with higher water activity. From our calculation we can see that for some of the organosulfates, water activity in the organic phase is above ideality (<inline-formula><mml:math id="M407" display="inline"><mml:mrow><mml:msub><mml:mi>a</mml:mi><mml:mi>w</mml:mi></mml:msub><mml:mo>&gt;</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>w</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>), meaning a lower water uptake compared to the organosulfates with water activities below ideality (<inline-formula><mml:math id="M408" display="inline"><mml:mrow><mml:msub><mml:mi>a</mml:mi><mml:mi>w</mml:mi></mml:msub><mml:mo>&lt;</mml:mo><mml:msub><mml:mi>x</mml:mi><mml:mi>w</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>). Additionally, a miscibility gap means that the aerosol system has inaccessible mixing states. Therefore, not all conditions, including the CCN activation threshold, may be reached in a continuous fashion during cloud processing but could instead be short-circuited by aerosol LLPS.</p>
      <p id="d1e8882">Our calculations predict limited organosulfate solubility in pure water and even lower solubility in the aqueous solutions of ammonium sulfate and ammonium bisulfate. Solubility, however, is strongly enhanced by the formation of the corresponding organosulfate anionic species in aqueous environments that are not very strongly acidic. Previous experimental, modeling and computational studies <xref ref-type="bibr" rid="bib1.bibx56 bib1.bibx57" id="paren.83"/> have shown that ammonium sulfate has a salting-out effect on organic compounds. This is seen in our calculations for the IEPOX isomers, whereas a weak (at most 3.5 %) salting-in effect on the organosulfates is predicted at low concentrations of ammonium sulfate. COSMO<italic>therm</italic> has previously been shown to overestimate the salting-out effect of ammonium sulfate on diverse organic compounds <xref ref-type="bibr" rid="bib1.bibx56 bib1.bibx52" id="paren.84"/>. Based on this, it is possible that the salting-in of organosulfates may be underestimated in our present calculations. The presence of additional inorganic salt in the aerosol where organosulfate is formed may therefore enhance or decrease the SOA phase stability of the organosulfate, depending on the <inline-formula><mml:math id="M409" display="inline"><mml:mrow class="chem"><mml:mi mathvariant="normal">organic</mml:mi><mml:mo>:</mml:mo><mml:mi mathvariant="normal">inorganic</mml:mi></mml:mrow></mml:math></inline-formula> sulfate mixing ratio and relative humidity.</p>
      <?pagebreak page5693?><p id="d1e8907">Calculated saturation vapor pressures are lower for organosulfates than isoprene-derived dihydroxy dihydroperoxides, dihydroperoxy hydroxy aldehydes <xref ref-type="bibr" rid="bib1.bibx31" id="paren.85"/> and <inline-formula><mml:math id="M410" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>-pinene-derived oxidized compounds <xref ref-type="bibr" rid="bib1.bibx30" id="paren.86"/>. Based on this, organosulfates are more stable in the condensed phase than non-sulfate organic compounds. In addition, the saturation vapor pressure of <inline-formula><mml:math id="M411" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is higher than all of the organosulfates. Due to the low p<inline-formula><mml:math id="M412" display="inline"><mml:mrow><mml:msub><mml:mi>K</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> of all organosulfates (and <inline-formula><mml:math id="M413" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">H</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">SO</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>), if the aerosol contains molecules or ions capable of acting as bases, the effective vapor pressure (equilibrium vapor pressure) of OS SOA will be many orders of magnitude lower than the saturation vapor pressures. Overall, organosulfates are thus unlikely to evaporate from an aerosol in which they are formed. This means that the formation of organosulfates, in particular the formation of their salts, can significantly contribute to increasing the SOA mass in regions with high sulfate aerosol content. Not only will OS add to SOA, but this SOA will also be stable over a wide range of conditions, including salinity and acidity.</p>
      <p id="d1e8967">The results of this work show that COSMO<italic>therm</italic> is a viable path to obtaining compound-specific thermochemical properties of atmospheric organic aerosol, which may not be available through experimental methods anytime soon. We have calculated values for selected properties that are overall consistent with observations from a variety of aerosol measurements from both fieldwork and laboratory work. However, we also see that oxidized atmospheric organics from similar precursors and with similar chemical functionalities may exhibit surprisingly different compound-specific phase state properties. In combination with the variation of these properties across a range of conditions, this thermochemical heterogeneity of atmospheric organosulfates – and of other compound classes that may display similar variation – poses a real challenge for large-scale atmospheric simulations. In particular, we note that great caution must be taken when using single compounds to represent the properties of an entire group.</p>
</sec>

      
      </body>
    <back><notes notes-type="dataavailability"><title>Data availability</title>

      <p id="d1e8977">The research data have been deposited in a reliable public data repository (the CERN Zenodo service) and can be accessed at <ext-link xlink:href="https://doi.org/10.5281/zenodo.3552309" ext-link-type="DOI">10.5281/zenodo.3552309</ext-link> <xref ref-type="bibr" rid="bib1.bibx24" id="paren.87"/>.</p>
  </notes><app-group>
        <supplementary-material position="anchor"><p id="d1e8986">The supplement related to this article is available online at: <inline-supplementary-material xlink:href="https://doi.org/10.5194/acp-20-5679-2020-supplement" xlink:title="pdf">https://doi.org/10.5194/acp-20-5679-2020-supplement</inline-supplementary-material>.</p></supplementary-material>
        </app-group><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d1e8995">NLP conceived, planned, supervised and secured funding for the project. NH performed the calculations. NH and NLP analyzed the results and wrote the paper, with contributions from the other authors. NH revised the paper with input from the other authors.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d1e9001">The authors declare that they have no conflict of interest.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e9007">We thank Theo Kurtén for helpful discussions and  Frank Eckert and Jens Reinisch for advice on the use of COSMO<italic>therm</italic>. We thank the CSC IT Center for Science, Finland, for computational resources.</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d1e9015">This project has received funding from the European Research Council (ERC) under the European
Union's Horizon 2020 research and innovation program, Project SURFACE (grant agreement
no. 717022). Nønne L. Prisle, Noora Hyttinen, Jussi Malila, and Silvia M. Calderón also gratefully acknowledge the financial contribution from the Academy
of Finland (grant nos. 308238 and 314175). Jonas Elm is grateful for financial support
from the Swedish Research Council Formas (project number 2018-01745-COBACCA).</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d1e9021">This paper was edited by Manabu Shiraiwa and reviewed by two anonymous referees.</p>
  </notes><ref-list>
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    <!--<article-title-html>Thermodynamic properties of isoprene- and monoterpene-derived organosulfates estimated with COSMO<i>therm</i></article-title-html>
<abstract-html><p>Organosulfates make significant contributions to atmospheric secondary organic aerosol (SOA), but little is known about the thermodynamic properties of atmospherically relevant organosulfates. We have used the COSMO<i>therm</i> program to calculate both the gas- and condensed-phase properties of previously identified atmospherically relevant monoterpene- and isoprene-derived organosulfates. Properties include solubilities, activities and saturation vapor pressures, which are critical to the aerosol-phase stability and atmospheric impact of organosulfate SOA. Based on the estimated saturation vapor pressures, the organosulfates of this study can all be categorized as semi-volatile or low-volatile, with saturation vapor pressures 4 to 8 orders of magnitude lower than that of sulfuric acid. The estimated p<i>K</i><sub>a</sub> values of all the organosulfates indicate a high degree of dissociation in water, leading in turn to high dissociation-corrected solubilities. In aqueous mixtures with inorganic sulfate, COSMO<i>therm</i> predicts a salting-out of both the organosulfates and their sodium salts from inorganic co-solutes. The salting-out effect of ammonium sulfate (less acidic) is stronger than of ammonium bisulfate (more acidic). Finally, COSMO<i>therm</i> predicts liquid–liquid-phase separation in systems containing water and monoterpene-derived organosulfates. The COSMO<i>therm</i>-estimated properties support the observed stability of organosulfates as SOA constituents and their long-range transport in the atmosphere but also show significant variation between specific compounds and ambient conditions.</p></abstract-html>
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