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  <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-19-3043-2019</article-id><title-group><article-title>Country-scale greenhouse gas budgets using shipborne measurements: a case
study for the UK and Ireland</article-title><alt-title>Country-scale greenhouse gas budgets</alt-title>
      </title-group><?xmltex \runningtitle{Country-scale greenhouse gas budgets}?><?xmltex \runningauthor{C. Helfter et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Helfter</surname><given-names>Carole</given-names></name>
          <email>caro2@ceh.ac.uk</email>
        <ext-link>https://orcid.org/0000-0001-5773-4652</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Mullinger</surname><given-names>Neil</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-3148-6950</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Vieno</surname><given-names>Massimo</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>O'Doherty</surname><given-names>Simon</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-4051-6760</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Ramonet</surname><given-names>Michel</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-1157-1186</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4">
          <name><surname>Palmer</surname><given-names>Paul I.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-1487-0969</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Nemitz</surname><given-names>Eiko</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-1765-6298</ext-link></contrib>
        <aff id="aff1"><label>1</label><institution>Atmospheric Chemistry and Effects, Centre for Ecology and Hydrology, Penicuik, UK</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>School of Chemistry, University of Bristol, Bristol, UK</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>Laboratoire des Sciences du Climat et de l'Environnement,
CEA-CNRS-UVSQ, Gif-sur-Yvette, France</institution>
        </aff>
        <aff id="aff4"><label>4</label><institution>School of GeoSciences, University of Edinburgh, Edinburgh, UK</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Carole Helfter (caro2@ceh.ac.uk)</corresp></author-notes><pub-date><day>11</day><month>March</month><year>2019</year></pub-date>
      
      <volume>19</volume>
      <issue>5</issue>
      <fpage>3043</fpage><lpage>3063</lpage>
      <history>
        <date date-type="received"><day>7</day><month>September</month><year>2018</year></date>
           <date date-type="rev-request"><day>1</day><month>October</month><year>2018</year></date>
           <date date-type="rev-recd"><day>22</day><month>February</month><year>2019</year></date>
           <date date-type="accepted"><day>25</day><month>February</month><year>2019</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2019 </copyright-statement>
        <copyright-year>2019</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="d1e155">We present a mass balance approach to estimate the seasonal and annual
budgets of carbon dioxide (<inline-formula><mml:math id="M1" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) and methane (<inline-formula><mml:math id="M2" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) of the United
Kingdom (excluding Scotland) and the Republic of Ireland from concentration
measurements taken on a ferry along the east coast of the United Kingdom over
a 3-year period (2015–2017). We estimate the annual emissions of <inline-formula><mml:math id="M3" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> to
be <inline-formula><mml:math id="M4" display="inline"><mml:mrow><mml:mn mathvariant="normal">2.55</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.48</mml:mn></mml:mrow></mml:math></inline-formula> Tg, which is consistent with the combined 2.29 Tg
reported to the United Nations Framework Convention on Climate Change by the
individual countries. The net <inline-formula><mml:math id="M5" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> budget (i.e. including all
anthropogenic and biogenic sources and sinks of <inline-formula><mml:math id="M6" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) is estimated at
<inline-formula><mml:math id="M7" display="inline"><mml:mrow><mml:mn mathvariant="normal">881.0</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">125.8</mml:mn></mml:mrow></mml:math></inline-formula> Tg, with a net biogenic contribution of 458.7 Tg (taken
as the difference between the estimated net emissions and the inventory
value,
which accounts for anthropogenic emissions only). The largest emissions for
both gases were observed in a broad latitudinal band (52.5–54<inline-formula><mml:math id="M8" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N), which coincides with densely populated areas. The
emissions of both gases were seasonal (maxima in winter and minima in
summer), strongly correlated with natural gas usage and, to a lesser extent,
also anti-correlated with mean air temperature. Methane emissions exhibited a
statistically significant anti-correlation with air temperature at the
seasonal timescale in the central region spanning 52.8–54.2<inline-formula><mml:math id="M9" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, which hosts a relatively high density of waste treatment
facilities. Methane emissions from landfills have been shown to sometimes
increase with decreasing air temperature due to changes in the
<inline-formula><mml:math id="M10" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>-oxidising potential of the topsoil, and we speculate that the waste
sector contributes significantly to the <inline-formula><mml:math id="M11" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> budget of this central
region. This study brings independent verification of the emission budgets
estimated using alternative products (e.g. mass balance budgets by aircraft
measurements, inverse modelling, inventorying) and offers an opportunity to
investigate the seasonality of these emissions, which is usually not possible.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

      <?xmltex \hack{\allowdisplaybreaks}?><?xmltex \floatpos{t}?><fig id="Ch1.F1" specific-use="star"><label>Figure 1</label><caption><p id="d1e283">Google Earth map centred on the United Kingdom and Ireland. The
route of the ferry is indicated by a dark blue line joining the ports of
Rosyth (Scotland, UK) and Zeebrugge (Belgium). The location of the Mace Head
measurement station on the west coast of Ireland, which provided the carbon
dioxide and methane concentration baselines, is indicated by a red star. The
cities indicated by yellow stars are locations of interest cited in the
Discussion (Sect. 4).</p></caption>
      <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://acp.copernicus.org/articles/19/3043/2019/acp-19-3043-2019-f01.jpg"/>

    </fig>

<sec id="Ch1.S1" sec-type="intro">
  <title>Introduction</title>
      <p id="d1e297">The United Nations Framework Convention on Climate Change (UNFCCC)
kick-started an international political drive to reduce emissions of
greenhouse gases (GHGs) and stabilise their midterm to long-term impact on the
global climate. The focus of the international community over the past 2–3
decades has been on curbing emissions of carbon dioxide (<inline-formula><mml:math id="M12" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>), the most
abundant and well-understood GHG, but it is now recognised that emissions of
other GHGs such as methane (<inline-formula><mml:math id="M13" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) and nitrous oxide (<inline-formula><mml:math id="M14" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">N</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mi mathvariant="normal">O</mml:mi></mml:mrow></mml:math></inline-formula>) must also
be addressed in order to fulfil the goal of limiting irreversible climate
change set out under the 21st Convention of Parties (COP21). Reductions
in <inline-formula><mml:math id="M15" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> emissions in particular would be effective in reducing GHGs more
quickly, given its shorter lifetime. Annex 1 parties are required to report
their GHG inventories annually to the UNFCCC following the guidelines set
out by the Intergovernmental Panel on Climate Change (IPCC, 2006; UNFCCC,
2014). Emissions inventories are powerful tools but they intrinsically rely
on detailed knowledge of source abundance and strength, and they can
therefore carry significant uncertainties. For example,<?pagebreak page3044?> uncertainties on the
fossil fuel emissions from Europe and North America have been estimated to
be of the order of 2 % to 5 % (Marland, 2012); in contrast, a 1.4 Gt gap
in <inline-formula><mml:math id="M16" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> emissions was reported in China in 2010, which was equivalent to
<inline-formula><mml:math id="M17" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">5</mml:mn></mml:mrow></mml:math></inline-formula> % of the global budget (Guan et al., 2012). Because much
of its emission is directly linked to the amount of fossil fuel used,
<inline-formula><mml:math id="M18" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is the best-understood GHG but, despite this, regional and
consequently global emissions budgets are thought to be underestimated and
the uncertainties are increasing due to growing emissions from emerging
economies (Gregg, 2008; Gregg et al., 2008;  Peters et al., 2011). By
contrast, relatively more <inline-formula><mml:math id="M19" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> emission is mediated by biological
processes. After a period of stagnation in the first few years of the
21st century, atmospheric <inline-formula><mml:math id="M20" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> has been rising steadily since ca.
2007. This prompted renewed efforts by the international scientific
community to identify the drivers of <inline-formula><mml:math id="M21" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> at local, regional, and global
scales and reconcile bottom-up and top-down estimates (Kirschke et al.,
2013; Saunois et al., 2016). At the global scale, total methane emissions
from fossil fuels (from the fossil fuel industry and from geological
seepage) have been relatively steady over the past 3 decades, but
research indicates that the estimates must be revised upwards by as much as
60 %–110 % (Schwietzke et al., 2016). Several mechanisms have been
proposed to explain the recent rise in atmospheric methane; these include
increases in emissions from microbial sources, which are meteorologically
driven and can therefore exhibit substantial inter-annual variability
(Dlugokencky et al., 2011; Nisbet et al., 2016; Schwietzke et al., 2016), a
weakening of the hydroxyl (OH) chemical sink strength (Rigby et al., 2017;
Turner et al., 2017), and an increase in fossil fuel contributions in the
context of a stable OH sink and a downward revision of the biomass burning
budget term (Worden et al., 2017). Inventories are thought to overestimate
global emissions, and a difference of 130 Tg <inline-formula><mml:math id="M22" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> yr<inline-formula><mml:math id="M23" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> was found
between bottom-up and top-down estimates (Kirschke et al., 2013). In this
light, it is becoming increasingly clear that there is an urgent need to
seek independent validation of the emissions inventories using an integrated
range of measurements and modelling activities (Allen, 2016; Nisbet and
Weiss, 2010).</p>
      <p id="d1e436">The development in recent years of rugged, high-precision spectroscopic
instruments (e.g. Peltola et al., 2014) has opened up new opportunities for
continuous in situ measurements of methane at fine temporal resolution and
at relatively large spatial scales. For example, such sensors have been used
in airborne applications to study methane emissions from cities (Cambaliza
et al., 2014, 2015;  Mays et al., 2009; O'Shea et al.,
2014) as well as anthropogenic and biogenic area sources (Hiller et al.,
2014; Karion et al., 2013, 2015). Applications of
eddy covariance to measure emission–deposition directly at the field scale
are on the rise in a broad variety of environments ranging from agricultural
and wetlands (Dengel et al., 2011; Erkkila et al., 2018; Felber et al.,
2015; Meijide et al., 2011; Peltola et al., 2015; Podgrajsek et al., 2014;
Nicolini et al., 2013) to urban (Gioli et al., 2012; Helfter et al., 2011, 2016; Pawlak and Fortuniak, 2016; Pawlak et al., 2016).
Finally, networks of tall towers and networks thereof exist around the world
to monitor and model methane emissions at spatial scales ranging from
country to global (Bakwin et al., 1995; Bohnenstengel et al., 2015; Feng et
al., 2009, 2011; Miller et al., 2013; Oney et al., 2015; Rigby
et al., 2008; Stanley et al., 2018; Stavert et al., 2018).</p>
      <?pagebreak page3045?><p id="d1e439">The geography of the British Isles at the NE edge of Europe, with dominantly
SW winds advecting clean Atlantic air masses, particularly lends itself to a
further approach, namely boundary layer budget measurements of
concentrations in the inflow and outflow. This has previously been utilised for
airborne boundary layer budget measurements (Fowler et al., 1996; Gallagher
et al., 1994; Polson et al., 2011), but these can only provide snapshots of
the country emissions for a few individual days.</p>
      <p id="d1e442">Extending the concept of these earlier studies, we present 3 years of
continuous observations (2015–2017) of <inline-formula><mml:math id="M24" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M25" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentrations
measured on board a commercial freight ferry, which connects the ports of
Rosyth (Scotland, UK) to Zeebrugge (Belgium) and tracks the east coast of
most of Great Britain (Fig. 1). The route of the ferry transects the UK
outflow with a time-dependent footprint (Fig. 2), which, combined with
a typical west-to-east air mass travel time of 11 to 19 h across the
domain (median values for winter and summer, respectively), allows for
sub-daily emissions estimations. Furthermore, the three continuous years of
measurements also provide an opportunity to study seasonal and inter-annual
changes in emissions. This is to our knowledge the first example of
country-scale emission budgets using a mobile platform measuring
continuously over several years.</p>
      <p id="d1e468">These shipborne measurements formed part of a larger observation and
modelling programme – the Greenhouse gAs Uk and Global Emissions (GAUGE)
project (Palmer et al., 2018) – aimed at determining the magnitude, spatial
distribution, and uncertainties of the UK's GHG budgets of <inline-formula><mml:math id="M26" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>,
<inline-formula><mml:math id="M27" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>,
and <inline-formula><mml:math id="M28" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">N</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 this paper we utilise shipborne observations at the outflow
of the United Kingdom coupled with background measurements at the Mace Head
site (Ireland) to estimate seasonal and annual budgets of <inline-formula><mml:math id="M29" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and
<inline-formula><mml:math id="M30" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> using a mass balance approach.</p>
</sec>
<sec id="Ch1.S2">
  <title>Materials and methods</title>
      <p id="d1e534">This section describes the measurement systems used at the two experimental
sites (Mace Head and ferry) and provides details of the greenhouse gas
budget calculations and mass balance approach.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2" specific-use="star"><label>Figure 2</label><caption><p id="d1e539">Backward trajectory frequencies for a south-bound sailing with
westerly wind conditions (sailing start 17 May 2015 12:00, end 18 May 2015
10:00). The coloured contours represent the normalised frequency counts
(number of end points in a <inline-formula><mml:math id="M31" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.5</mml:mn><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mo>×</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> grid cell divided
by the maximum number of end points in any grid cell, expressed as a
percentage) and the source corresponds to the location of the ferry
(indicated by an arrow). The trajectories were run backward for 24 h at
3 h intervals using GDAS 1<inline-formula><mml:math id="M32" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> global meteorology (NOAA, 2018).</p></caption>
        <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://acp.copernicus.org/articles/19/3043/2019/acp-19-3043-2019-f02.png"/>

      </fig>

<sec id="Ch1.S2.SS1">
  <title>Experimental set-up</title>
<sec id="Ch1.S2.SS1.SSS1">
  <title>Shipborne measurements</title>
      <p id="d1e587">Measurements of concentrations of carbon dioxide (<inline-formula><mml:math id="M33" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) and methane
(<inline-formula><mml:math id="M34" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) began in February 2014 on board a commercial freight ferry
(operated by DFDS Seaways) which served the route between Rosyth (Scotland,
UK; 56<inline-formula><mml:math id="M35" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>1<inline-formula><mml:math id="M36" display="inline"><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:math></inline-formula>21.611<inline-formula><mml:math id="M37" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>′</mml:mo><mml:mo>′</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> N, 3<inline-formula><mml:math id="M38" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>26<inline-formula><mml:math id="M39" display="inline"><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:math></inline-formula>21.558<inline-formula><mml:math id="M40" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>′</mml:mo><mml:mo>′</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> W) and Zeebrugge
(Belgium; 51<inline-formula><mml:math id="M41" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>21<inline-formula><mml:math id="M42" display="inline"><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:math></inline-formula>16.96<inline-formula><mml:math id="M43" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>′</mml:mo><mml:mo>′</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> N, 3<inline-formula><mml:math id="M44" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>10<inline-formula><mml:math id="M45" display="inline"><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:math></inline-formula>34.645<inline-formula><mml:math id="M46" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>′</mml:mo><mml:mo>′</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> E). The
route of the ship followed the outline of the English coast on the east side
of the UK, which placed it downwind of Atlantic air masses blowing in from
the west over Ireland, Wales, and England (Figs. 2 and 3). The ship completed
three return journeys per week and typically operated for 48 weeks per
calendar year. The schedule of the weekly cruises allowed for the latitude
range to be sampled at different times of day and night as illustrated in
Fig. 4.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3" specific-use="star"><label>Figure 3</label><caption><p id="d1e736">Half-hourly averages of <bold>(a)</bold> <inline-formula><mml:math id="M47" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</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="M48" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> mole
fractions measured on board the freight ferry during the south-bound journey
on 29–30 July 2014. The arrows represent wind direction.</p></caption>
            <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://acp.copernicus.org/articles/19/3043/2019/acp-19-3043-2019-f03.png"/>

          </fig>

      <p id="d1e773">The roll-on–roll-off (Ro–Ro) cargo–container carrier vessel
<italic>Finnmerchant</italic>
(former name <italic>Longstone</italic>; IMO: 9234082; overall length and breadth: 193 m <inline-formula><mml:math id="M49" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 26 m) served the Rosyth–Zeebrugge route during the measurement period
25 February–15 April 2014. It was replaced by the Ro-Ro cargo ship <italic>Finlandia Seaways</italic> (IMO: 9198721; overall length and breadth: 163 m <inline-formula><mml:math id="M50" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 21 m) on
15 June 2014 and measurement restarted aboard the new vessel.</p>
      <p id="d1e799">Air was sampled on the topmost platform of the bow (port side on
<italic>Finnmerchant</italic> and starboard side on <italic>Finlandia Seaways</italic>) and analysed by a
cavity ring-down spectrometer (CRDS; Picarro 1301) housed in an
air-conditioned measurement container located on the weather deck. Air was
pumped at ca. 50 L min<inline-formula><mml:math id="M51" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> through 20 and 50 m of <inline-formula><mml:math id="M52" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:msup><mml:mn mathvariant="normal">2</mml:mn><mml:mrow><mml:mo>′</mml:mo><mml:mo>′</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> Synflex tubing
at approximate measurement heights of 20 m and 30 m a.s.l. (on <italic>Finnmerchant</italic> and
<italic>Finlandia Seaways</italic>, respectively) and subsampled at ca. 10 L min<inline-formula><mml:math id="M53" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> through 2 m
of <inline-formula><mml:math id="M54" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>/</mml:mo><mml:msup><mml:mn mathvariant="normal">2</mml:mn><mml:mrow><mml:mo>′</mml:mo><mml:mo>′</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> Synflex tube by a secondary pump. The subsampling
T piece was set up as a virtual impactor to prevent moisture and sea salt
from entering the CRDS sampling line, and the main sampling line was
protected from moisture ingress by three water traps arranged in series (at
the ambient air inlet point as well as immediately upstream and downstream
of the virtual impactor).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4" specific-use="star"><label>Figure 4</label><caption><p id="d1e878">Temporal coverage of the latitudinal range (0.2<inline-formula><mml:math id="M55" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> bins)
spanned by the ferry route expressed as a count density (frequency of
occurrence normalised by the total number of observations in each latitude
bin) for all data points which satisfied the data screening criteria
(Sect. 2.2.1) during the measurement period 1 January 2015–31 December 2017.</p></caption>
            <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://acp.copernicus.org/articles/19/3043/2019/acp-19-3043-2019-f04.png"/>

          </fig>

      <p id="d1e896">The gas measurement system was equipped with a bespoke auto-calibration
system controlled by an in-house LabView<sup>™</sup> programme, which also handled
the acquisition of data (0.5 Hz) from the Picarro gas analyser, a weather
station (WXT520, Vaisala) co-located with the air inlet on the ship's top
deck, and a GPS (<inline-formula><mml:math id="M56" display="inline"><mml:mrow><mml:mn mathvariant="normal">18</mml:mn><mml:mo>×</mml:mo></mml:mrow></mml:math></inline-formula> series, Garmin) receiver affixed to the roof of the sea
container. Calibrations using three gases spanning a realistic range of
<inline-formula><mml:math id="M57" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M58" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> concentrations ran every 169 h and lasted 65 min in total. The references gases were calibrated by the Swiss Federal
Laboratories for Materials Testing and Research (EMPA; Dübendorf,
Switzerland) using a Picarro 1301 CRDS. The calibration scales (NOAA/ESRL)
were WMO-<inline-formula><mml:math id="M59" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>-X2004 for methane and WMO-<inline-formula><mml:math id="M60" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>-X2007 for carbon
dioxide. Each gas standard was measured at 1 Hz for 15 min, and the average
and standard deviation were derived for the 15 min period. A 5 min
purge period using the gas standard to be measured was observed before each
active averaging period to flush out residual gas and eliminate sample
contamination. Each calibration event ended with a 5 min purge period
using ambient air before resuming normal operations. The gas concentration
time series were corrected using linear temporal interpolations between
calibration events. Table 1 provides a list of observables; Table 2
summarises the weekly auto-calibration procedure and provides information on
the three calibration gases used.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1"><label>Table 1</label><caption><p id="d1e960">List of instruments and observables recorded on board the Rosyth
(Scotland, UK; 56<inline-formula><mml:math id="M61" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>1<inline-formula><mml:math id="M62" display="inline"><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:math></inline-formula>21.611<inline-formula><mml:math id="M63" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>′</mml:mo><mml:mo>′</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> N, 3<inline-formula><mml:math id="M64" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>26<inline-formula><mml:math id="M65" display="inline"><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:math></inline-formula>21.558<inline-formula><mml:math id="M66" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>′</mml:mo><mml:mo>′</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> W) to
Zeebrugge (Belgium; 51<inline-formula><mml:math id="M67" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>21<inline-formula><mml:math id="M68" display="inline"><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:math></inline-formula>16.96<inline-formula><mml:math id="M69" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>′</mml:mo><mml:mo>′</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> N, 3<inline-formula><mml:math id="M70" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>10<inline-formula><mml:math id="M71" display="inline"><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:math></inline-formula>34.645<inline-formula><mml:math id="M72" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>′</mml:mo><mml:mo>′</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> E) freight ferry.</p></caption><oasis:table frame="topbot"><?xmltex \begin{scaleboxenv}{.88}[.88]?><oasis:tgroup cols="3">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="left"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Observable</oasis:entry>
         <oasis:entry colname="col2">Unit</oasis:entry>
         <oasis:entry colname="col3">Instrument</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M73" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> dry mole fraction</oasis:entry>
         <oasis:entry colname="col2">ppm</oasis:entry>
         <oasis:entry colname="col3">Picarro 1301 CRDS</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"><inline-formula><mml:math id="M74" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> dry mole fraction</oasis:entry>
         <oasis:entry colname="col2">ppb</oasis:entry>
         <oasis:entry colname="col3">Picarro 1301 CRDS</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Apparent wind speed</oasis:entry>
         <oasis:entry colname="col2">m s<inline-formula><mml:math id="M75" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3">Vaisala WXT520</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">(with respect to moving ship)</oasis:entry>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3"/>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Apparent wind direction</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M76" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3">Vaisala WXT520</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">(wind blowing from with respect</oasis:entry>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3"/>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">to prow of moving ship)</oasis:entry>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3"/>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Air temperature</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M77" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C</oasis:entry>
         <oasis:entry colname="col3">Vaisala WXT520</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Ambient pressure</oasis:entry>
         <oasis:entry colname="col2">hPa</oasis:entry>
         <oasis:entry colname="col3">Vaisala WXT520</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Relative humidity</oasis:entry>
         <oasis:entry colname="col2">%</oasis:entry>
         <oasis:entry colname="col3">Vaisala WXT520</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Ship speed</oasis:entry>
         <oasis:entry colname="col2">kt</oasis:entry>
         <oasis:entry colname="col3">Garmin <inline-formula><mml:math id="M78" display="inline"><mml:mrow><mml:mn mathvariant="normal">18</mml:mn><mml:mo>×</mml:mo></mml:mrow></mml:math></inline-formula> series GPS</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Ship bearing</oasis:entry>
         <oasis:entry colname="col2">degrees</oasis:entry>
         <oasis:entry colname="col3">Garmin <inline-formula><mml:math id="M79" display="inline"><mml:mrow><mml:mn mathvariant="normal">18</mml:mn><mml:mo>×</mml:mo></mml:mrow></mml:math></inline-formula> series GPS</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Ship position, latitude</oasis:entry>
         <oasis:entry colname="col2">decimal</oasis:entry>
         <oasis:entry colname="col3">Garmin <inline-formula><mml:math id="M80" display="inline"><mml:mrow><mml:mn mathvariant="normal">18</mml:mn><mml:mo>×</mml:mo></mml:mrow></mml:math></inline-formula> series GPS</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Ship position, longitude</oasis:entry>
         <oasis:entry colname="col2">decimal</oasis:entry>
         <oasis:entry colname="col3">Garmin <inline-formula><mml:math id="M81" display="inline"><mml:mrow><mml:mn mathvariant="normal">18</mml:mn><mml:mo>×</mml:mo></mml:mrow></mml:math></inline-formula> series GPS</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup><?xmltex \end{scaleboxenv}?></oasis:table></table-wrap>

</sec>
<?pagebreak page3046?><sec id="Ch1.S2.SS1.SSS2">
  <title>Mace Head site</title>
      <p id="d1e1370">The Mace Head station is located on the west coast of Ireland at
53<inline-formula><mml:math id="M82" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>20<inline-formula><mml:math id="M83" display="inline"><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:math></inline-formula> N, 9<inline-formula><mml:math id="M84" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>54<inline-formula><mml:math id="M85" display="inline"><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:math></inline-formula> W, 5 m a.s.l., and
a 23 m high tower is used to sample the air. Atmospheric concentrations of
<inline-formula><mml:math id="M86" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> have been continuously monitored at Mace Head since 1992 (Biraud et
al., 2000; Derwent et al., 2002; Ramonet et al., 2010). Since 2010 a cavity
ring-down spectrometer similar to the one used on board the ship (Picarro,
G1301) has been used for <inline-formula><mml:math id="M87" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M88" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> measurements (instrument
owned by the Environment Protection Agency (EPA), Ireland). A second CRDS
analyser (Picarro, G2301) was installed in 2013 (instrument owned by
Laboratoire des Sciences du Climat et de l'Environnement (LSCE), France) to
ensure the redundancy of measurements, thus reducing data gaps. Both analysers
are calibrated simultaneously every month using a suite of four calibration
cylinders whose concentrations span the atmospheric range. Those cylinders
have themselves been calibrated at LSCE with WMO/NOAA reference scales
(WMO2007 scale for <inline-formula><mml:math id="M89" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, WMO2004A scale for <inline-formula><mml:math id="M90" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>). In addition to
the calibration cylinders, two target cylinders are regularly analysed
(short-term target twice a day and long-term target once a month) in order
to assess measurement repeatability. Over the period 2014–2018 the
difference between the assigned values and the values measured<?pagebreak page3047?> every month
at Mace Head for the long-term target gas were <inline-formula><mml:math id="M91" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.01</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.02</mml:mn></mml:mrow></mml:math></inline-formula> ppm for
<inline-formula><mml:math id="M92" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> (both analysers) and <inline-formula><mml:math id="M93" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.08</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.19</mml:mn></mml:mrow></mml:math></inline-formula>  and <inline-formula><mml:math id="M94" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.01</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.17</mml:mn></mml:mrow></mml:math></inline-formula> ppb for <inline-formula><mml:math id="M95" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> with analyser G1301 and G2301, respectively. The
measurements are processed every day at LSCE (Hazan et al., 2016), ensuring
a high level of quality control of the dataset. The maintenance of the
analysers is coordinated through close collaboration between LSCE, EPA, and
the National University of Ireland, Galway (NUIG).</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T2" specific-use="star"><label>Table 2</label><caption><p id="d1e1527">Details of the weekly auto-calibration sequence (interval 169 h) and reference gases. The reference gases were calibrated by the Swiss
Federal Laboratories for Materials Testing and Research (World Calibration
Centre WCC-EMPA, Dübendorf, Switzerland) using a Picarro 1301 CRDS.
Calibration scales (NOAA/ ESRL): WMO-<inline-formula><mml:math id="M96" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>-X2004 for methane and
WMO-<inline-formula><mml:math id="M97" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>-X2007 for carbon dioxide. The measurement uncertainties
correspond to the standard deviation multiplied by a coverage factor  <inline-formula><mml:math id="M98" display="inline"><mml:mrow><mml:mi>k</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:math></inline-formula>, which provides a level of confidence of approximately 95 %.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="6">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="left"/>
     <oasis:colspec colnum="5" colname="col5" align="left"/>
     <oasis:colspec colnum="6" colname="col6" align="left"/>
     <oasis:thead>
       <oasis:row>
         <oasis:entry colname="col1">Step</oasis:entry>
         <oasis:entry colname="col2">Type</oasis:entry>
         <oasis:entry colname="col3">Time</oasis:entry>
         <oasis:entry colname="col4">Calibration</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M99" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M100" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> uncertainty</oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M101" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M102" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> uncertainty</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3">interval (s)</oasis:entry>
         <oasis:entry colname="col4">standard number</oasis:entry>
         <oasis:entry colname="col5">(ppm)</oasis:entry>
         <oasis:entry colname="col6">(ppb)</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">1</oasis:entry>
         <oasis:entry colname="col2">Purge</oasis:entry>
         <oasis:entry colname="col3">300</oasis:entry>
         <oasis:entry colname="col4">1</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M103" display="inline"><mml:mrow><mml:mn mathvariant="normal">384.23</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.15</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M104" display="inline"><mml:mrow><mml:mn mathvariant="normal">1815.36</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">1.45</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">2</oasis:entry>
         <oasis:entry colname="col2">Measurement</oasis:entry>
         <oasis:entry colname="col3">900</oasis:entry>
         <oasis:entry colname="col4">1</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M105" display="inline"><mml:mrow><mml:mn mathvariant="normal">384.23</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.15</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M106" display="inline"><mml:mrow><mml:mn mathvariant="normal">1815.36</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">1.45</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">3</oasis:entry>
         <oasis:entry colname="col2">Purge</oasis:entry>
         <oasis:entry colname="col3">300</oasis:entry>
         <oasis:entry colname="col4">2</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M107" display="inline"><mml:mrow><mml:mn mathvariant="normal">418.29</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.16</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M108" display="inline"><mml:mrow><mml:mn mathvariant="normal">2018.06</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">1.58</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">4</oasis:entry>
         <oasis:entry colname="col2">Measurement</oasis:entry>
         <oasis:entry colname="col3">900</oasis:entry>
         <oasis:entry colname="col4">2</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M109" display="inline"><mml:mrow><mml:mn mathvariant="normal">418.29</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.16</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M110" display="inline"><mml:mrow><mml:mn mathvariant="normal">2018.06</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">1.58</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">5</oasis:entry>
         <oasis:entry colname="col2">Purge</oasis:entry>
         <oasis:entry colname="col3">300</oasis:entry>
         <oasis:entry colname="col4">3</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M111" display="inline"><mml:mrow><mml:mn mathvariant="normal">474.86</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.18</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M112" display="inline"><mml:mrow><mml:mn mathvariant="normal">2426.77</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">1.86</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">6</oasis:entry>
         <oasis:entry colname="col2">Measurement</oasis:entry>
         <oasis:entry colname="col3">900</oasis:entry>
         <oasis:entry colname="col4">3</oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M113" display="inline"><mml:mrow><mml:mn mathvariant="normal">474.86</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.18</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col6"><inline-formula><mml:math id="M114" display="inline"><mml:mrow><mml:mn mathvariant="normal">2426.77</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">1.86</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">7</oasis:entry>
         <oasis:entry colname="col2">Purge</oasis:entry>
         <oasis:entry colname="col3">300</oasis:entry>
         <oasis:entry colname="col4">Ambient air</oasis:entry>
         <oasis:entry colname="col5">Ambient air</oasis:entry>
         <oasis:entry colname="col6">Ambient air</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

</sec>
</sec>
<sec id="Ch1.S2.SS2">
  <title>Mass balance budgets</title>
      <p id="d1e1946">The main underlying assumptions of the mass balance approach used to
calculate the spatially integrated emissions budgets of <inline-formula><mml:math id="M115" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and
<inline-formula><mml:math id="M116" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> from the Republic of Ireland, Northern Ireland, Wales, and England
are five-fold.
<list list-type="bullet"><list-item>
      <p id="d1e1973">Under westerly wind conditions, the Mace Head station on the
west coast of Ireland (53<inline-formula><mml:math id="M117" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>20<inline-formula><mml:math id="M118" display="inline"><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:math></inline-formula> N, 9<inline-formula><mml:math id="M119" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>54<inline-formula><mml:math id="M120" display="inline"><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:math></inline-formula> W; 5 m a.s.l.,
tower height 23 m) receives relatively clean Atlantic air, whilst the
concentrations measured along the ferry route result from enhancement in
<inline-formula><mml:math id="M121" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M122" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> due to land sources over the travel path of the air
mass. The concentrations at Mace Head are representative of the inflow into
the British Isles in both space and time.</p></list-item></list>
For each nominal temporal averaging period we assume the following.
<list list-type="bullet"><list-item>
      <p id="d1e2038">The planetary boundary layer (PBL) height is constant over the
entire spatial domain bounded to the east and west by the ferry route and
the meridian at the Mace Head station location. The north and
south boundaries of the domain are taken as the extrema of the latitudinal
range covered by the ferry route.</p></list-item><list-item>
      <p id="d1e2042">The air columns between the land surface and the top of the PBL
are well-mixed.</p></list-item><list-item>
      <p id="d1e2046">The horizontal wind direction is uniform.</p></list-item><list-item>
      <p id="d1e2050">There is no mass leakage out of or ingress into the 3-D domain.</p></list-item></list>
In the analysis, conditions are selected to fulfil these assumptions as best
as possible. Data screening and quality control are discussed in Sect. 2.2.1, the procedure for estimating background concentrations (baselines)
and PBL heights are presented in Sect. 2.2.2 and 2.2.3, and, finally, the
mass balance budget and uncertainty calculations are discussed in Sect. 2.2.4  and 2.2.5.</p>
<?pagebreak page3048?><sec id="Ch1.S2.SS2.SSS1">
  <title>Data screening</title>
      <p id="d1e2059">Prior to time averaging and flux calculation, raw data points were excluded
from further processing if any of the following criteria were realised.
<list list-type="bullet"><list-item>
      <p id="d1e2064">The ship was in port.</p></list-item><list-item>
      <p id="d1e2068">A calibration took place.</p></list-item><list-item>
      <p id="d1e2072">72 h back trajectories (500 m a.g.l.) for the Mace Head site and one point
along the route of the ferry (54.548<inline-formula><mml:math id="M123" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, 0.233<inline-formula><mml:math id="M124" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> W) as
calculated with HYSPLIT (NOAA Air Resources Laboratory, 2018) exhibited airflow patterns inconsistent with the mass balance assumptions (i.e.
non-westerly flow, evidence of recirculation).</p></list-item><list-item>
      <p id="d1e2094">The relative wind direction measured on the ship (the fixed reference point
being the prow of the vessel) was outside the range 150–210<inline-formula><mml:math id="M125" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>. This criterion was used to exclude data points potentially
contaminated by on-board activities (e.g. emissions from chimney stacks).</p></list-item><list-item>
      <p id="d1e2107">The wind direction measured on the ship (absolute direction from the north,
corrected for the movement of the ship) was outside the westerly range
(240–300<inline-formula><mml:math id="M126" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>).</p></list-item><list-item>
      <p id="d1e2120">The wind direction measured at the Mace Head station (data source: Met
Éireann, 2018) was outside the westerly range (240–300<inline-formula><mml:math id="M127" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>).</p></list-item></list>
The temporal coverage of the data points which satisfied the criteria listed
above is presented in histogram form in Fig. 4. The full details of the data
availability for the study period 2015–2017 are summarised in Table S1 of the
Supplement.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5" specific-use="star"><label>Figure 5</label><caption><p id="d1e2135">Hourly time series filtered for westerly wind directions (range
150–210<inline-formula><mml:math id="M128" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>) measured at the Mace Head station (open
circles) of <bold>(a)</bold> <inline-formula><mml:math id="M129" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</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="M130" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> mole fractions. Smoothing and gap
filling of the original time series was achieved by applying linear (Lin.)
and non-linear (Gauss.) regressions by parts for the data period 1 January 2014–31 December 2017 (solid lines).</p></caption>
            <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://acp.copernicus.org/articles/19/3043/2019/acp-19-3043-2019-f05.png"/>

          </fig>

</sec>
<sec id="Ch1.S2.SS2.SSS2">
  <title>Concentration baselines</title>
      <p id="d1e2187">The time series of hourly concentrations of <inline-formula><mml:math id="M131" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M132" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> measured
at Mace Head and filtered for westerly flow (wind direction range
240–300<inline-formula><mml:math id="M133" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>) were used to construct continuous
baselines for the measurement period February 2014–December 2017 (Fig. 5). The time series of both gases exhibited well-defined seasonal cycles
characterised by high concentrations towards the end of the winter and lower
concentrations in summer. The baselines were constructed for the data period
1 January 2014–31 December 2017 by applying regressions by parts consisting of
linear and non-linear (Gaussian) fitting functions over the temporal domain.
The composite fitting functions provided smoothing and gap filling of the
measured mole fraction time series and were subsequently used to construct
continuous time series of background concentrations of <inline-formula><mml:math id="M134" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M135" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>
with a 5 min time step, which corresponded to the averaging interval used
for the data measured on the ferry.</p>
</sec>
<sec id="Ch1.S2.SS2.SSS3">
  <title>Estimation of the planetary boundary layer height</title>
      <p id="d1e2249">The Weather Research and Forecast model version 3.7.1 (<uri>https://www.mmm.ucar.edu/weather-research-and-forecasting-model</uri>, last access:
5 March 2019)
(Skamarock et al., 2008) was used for this work. The WRF model initial and
boundary conditions were derived from the US National Center for
Environmental Prediction (NCEP)/National Center for Atmospheric Research
(NCAR) Global Forecast System (GFS) at <inline-formula><mml:math id="M136" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.0</mml:mn><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mo>×</mml:mo><mml:mn mathvariant="normal">1.0</mml:mn><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> resolution (National Centers for Environmental Prediction,
2000), including Newtonian nudging every 6 h. The Yonsei University
(YSU) scheme for planetary boundary layer physics was used here (Hong et
al., 2006).</p>
      <?pagebreak page3049?><p id="d1e2275">The WRF model set-up used in this study had three nested domains with
a horizontal resolution of <inline-formula><mml:math id="M137" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.5</mml:mn><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mo>×</mml:mo><mml:mn mathvariant="normal">0.5</mml:mn><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> for the
European domain, <inline-formula><mml:math id="M138" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.16</mml:mn><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mo>×</mml:mo><mml:mn mathvariant="normal">0.16</mml:mn><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> for the British
Isles domain, and <inline-formula><mml:math id="M139" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.055</mml:mn><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup><mml:mo>×</mml:mo><mml:mn mathvariant="normal">0.055</mml:mn><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> for the UK
model domain. The vertical column was divided into 21 layers from the
surface (bottom layer <inline-formula><mml:math id="M140" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">50</mml:mn></mml:mrow></mml:math></inline-formula> m) up to 100 hPa (<inline-formula><mml:math id="M141" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">16</mml:mn></mml:mrow></mml:math></inline-formula> km) in sigma coordinates.</p>
      <p id="d1e2358">The WRF model hourly output from the UK domain was used to calculate spatial
means and standard deviations of wind speed, wind direction, and
planetary boundary layer height. We estimate the spatial averages at a
height of <inline-formula><mml:math id="M142" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">450</mml:mn></mml:mrow></mml:math></inline-formula> m (fourth model layer) for an area defined
as follows: lower left corner coordinates of 52.0 latitude and <inline-formula><mml:math id="M143" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">10.0</mml:mn></mml:mrow></mml:math></inline-formula>
longitude and upper right corner of 57.0 latitude and 3.0 longitude.
Time series of hourly averages of wind speed, wind direction, and PBL height
were constructed for the data period 1 January 2014 to 31 December 2017. These hourly
values were extrapolated to the 5 min concentrations and ancillary (e.g.
meteorological, ship speed, coordinates) time series by assigning PBL height
and wind speed to the corresponding hour in the 5 min dataset (e.g. the
mean PBL height value estimated for the time period 03:00–04:00 UTC on
13 June 2015 was assigned to all 5 min averaging intervals from 03:00 to
03:55 UTC).</p>
      <p id="d1e2381">Daily means and standard deviations obtained by averaging the hourly values
of the PBL heights derived from WRF for the study period 2015–2017 are
presented in Fig. S1 of the Supplement.</p>
</sec>
<sec id="Ch1.S2.SS2.SSS4">
  <title>Mass balance calculations</title>
      <p id="d1e2391">The flux <inline-formula><mml:math id="M144" display="inline"><mml:mrow><mml:msub><mml:mi>F</mml:mi><mml:mi>C</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> of species <inline-formula><mml:math id="M145" display="inline"><mml:mi>C</mml:mi></mml:math></inline-formula> through a two-dimensional, vertical plane
perpendicular to the mean wind direction can be expressed as (Cambaliza et
al., 2014; White et al., 1976)

                  <disp-formula id="Ch1.E1" content-type="numbered"><mml:math id="M146" display="block"><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:msub><mml:mi>F</mml:mi><mml:mi>C</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:munderover><mml:mo movablelimits="false">∫</mml:mo><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mi mathvariant="normal">min</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mi mathvariant="normal">max</mml:mi></mml:msub></mml:mrow></mml:munderover><mml:munderover><mml:mo movablelimits="false">∫</mml:mo><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi mathvariant="normal">min</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi mathvariant="normal">max</mml:mi></mml:msub></mml:mrow></mml:munderover><mml:mfenced close=")" open="("><mml:mrow><mml:mi>C</mml:mi><mml:mo>-</mml:mo><mml:msub><mml:mi>C</mml:mi><mml:mi>b</mml:mi></mml:msub></mml:mrow></mml:mfenced><mml:mo>⋅</mml:mo><mml:mi>U</mml:mi><mml:msup><mml:mo>⊥</mml:mo><mml:mi>U</mml:mi></mml:msup><mml:mi mathvariant="normal">d</mml:mi><mml:mi>x</mml:mi><mml:mi mathvariant="normal">d</mml:mi><mml:mi>z</mml:mi><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>

            <inline-formula><mml:math id="M147" display="inline"><mml:mi>C</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M148" display="inline"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi>b</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> are the number of moles of species <inline-formula><mml:math id="M149" display="inline"><mml:mi>c</mml:mi></mml:math></inline-formula> downwind and
upwind of the vertical plane, and <inline-formula><mml:math id="M150" display="inline"><mml:mrow><mml:msub><mml:mi>U</mml:mi><mml:mo>⊥</mml:mo></mml:msub></mml:mrow></mml:math></inline-formula> is the mean wind speed
perpendicular to the plane bounded horizontally by <inline-formula><mml:math id="M151" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi mathvariant="normal">min</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M152" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi mathvariant="normal">max</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>
and vertically by <inline-formula><mml:math id="M153" display="inline"><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mi mathvariant="normal">min</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M154" display="inline"><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mi mathvariant="normal">max</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>.</p>
      <p id="d1e2568"><inline-formula><mml:math id="M155" display="inline"><mml:mrow><mml:msub><mml:mi>F</mml:mi><mml:mi>c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> can be expressed explicitly in units of mol s<inline-formula><mml:math id="M156" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> as
              <disp-formula id="Ch1.E2" content-type="numbered"><mml:math id="M157" display="block"><mml:mrow><mml:msub><mml:mi>F</mml:mi><mml:mi>C</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:munderover><mml:mo movablelimits="false">∫</mml:mo><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mi mathvariant="normal">ground</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mi mathvariant="normal">PBL</mml:mi></mml:msub></mml:mrow></mml:munderover><mml:munderover><mml:mo movablelimits="false">∫</mml:mo><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi mathvariant="normal">min</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi mathvariant="normal">max</mml:mi></mml:msub></mml:mrow></mml:munderover><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi mathvariant="italic">χ</mml:mi><mml:mi>C</mml:mi></mml:msub><mml:mo>⋅</mml:mo><mml:mi>U</mml:mi><mml:mo>⋅</mml:mo><mml:msub><mml:mi>n</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub><mml:mfenced close=")" open="("><mml:mi>z</mml:mi></mml:mfenced><mml:mi>cos⁡</mml:mi><mml:mi mathvariant="italic">θ</mml:mi><mml:mi mathvariant="normal">d</mml:mi><mml:mi>x</mml:mi><mml:mi mathvariant="normal">d</mml:mi><mml:mi>z</mml:mi><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>
            Here, <inline-formula><mml:math id="M158" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi mathvariant="italic">χ</mml:mi><mml:mi>c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is the enhancement of compound <inline-formula><mml:math id="M159" display="inline"><mml:mi>c</mml:mi></mml:math></inline-formula> in
mol mol<inline-formula><mml:math id="M160" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> above background, <inline-formula><mml:math id="M161" display="inline"><mml:mrow><mml:msub><mml:mi>n</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>z</mml:mi></mml:mrow></mml:math></inline-formula>) is the air density at height <inline-formula><mml:math id="M162" display="inline"><mml:mi>z</mml:mi></mml:math></inline-formula>,
cos<inline-formula><mml:math id="M163" display="inline"><mml:mrow><mml:mi mathvariant="italic">θ</mml:mi><mml:mi mathvariant="normal">d</mml:mi><mml:mi>x</mml:mi></mml:mrow></mml:math></inline-formula> (Fig. 6) is the ship track increment projected onto the crosswind
plane, and <inline-formula><mml:math id="M164" display="inline"><mml:mi>U</mml:mi></mml:math></inline-formula> is the mean wind speed within the PBL obtained by the WRF model
described in Sect. 2.2.3. Figure 6 illustrates the mass balance
calculation procedure.</p>
      <?pagebreak page3050?><p id="d1e2746">In practice, despite the 3 years of data, no single journey satisfied all the
quality control criteria detailed in Sect. 2.2.1 perfectly for all of the
individual 5 min averaging intervals, and we opted to aggregate the good
5 min data points into 0.2<inline-formula><mml:math id="M165" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> wide latitude bins using seasonal
grouping for each data year. The baseline mole fractions used to calculate
the upwind enhancement of compound <inline-formula><mml:math id="M166" display="inline"><mml:mi>c</mml:mi></mml:math></inline-formula> were time-shifted in order to account
for the mean air mass travel time across the domain (time taken to travel
west–east from the longitude of the Mace Head station to the location of the
ferry at hourly mean wind speed derived from the WRF model; see Table S2  for seasonal mean values and standard deviations).</p>
      <p id="d1e2765">Seasonal budgets were then calculated from the aggregated data as

                  <disp-formula specific-use="align" content-type="numbered"><mml:math id="M167" display="block"><mml:mtable displaystyle="true"><mml:mtr><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:msub><mml:mi>F</mml:mi><mml:mi>C</mml:mi></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:mo>=</mml:mo><mml:msubsup><mml:mo>∑</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mrow><mml:mi mathvariant="normal">lat</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="normal">bins</mml:mi></mml:mrow></mml:msubsup><mml:munder><mml:munder class="underbrace"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi mathvariant="italic">χ</mml:mi><mml:mo>(</mml:mo><mml:mi>i</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mo mathvariant="normal">︸</mml:mo></mml:munder><mml:mrow><mml:mo>≡</mml:mo><mml:mi mathvariant="normal">I</mml:mi></mml:mrow></mml:munder></mml:mrow></mml:mtd></mml:mtr><mml:mlabeledtr id="Ch1.E3"><mml:mtd/><mml:mtd><mml:mstyle displaystyle="true" class="stylechange"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mo>⋅</mml:mo><?xmltex \hack{\hbox\bgroup\fontsize{9}{9}\selectfont$\displaystyle}?><mml:mover accent="true"><mml:mrow><mml:munder><mml:munder class="underbrace"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi mathvariant="italic">χ</mml:mi><mml:mi>C</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>t</mml:mi><mml:mo>)</mml:mo><mml:mo>⋅</mml:mo><mml:mi>U</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>t</mml:mi><mml:mo>)</mml:mo><mml:mo>⋅</mml:mo><mml:mi>cos⁡</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="italic">θ</mml:mi><mml:mo>(</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>t</mml:mi><mml:mo>)</mml:mo><mml:mo>)</mml:mo><mml:mo>⋅</mml:mo><mml:msubsup><mml:mo>∫</mml:mo><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mi mathvariant="normal">ground</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mi mathvariant="normal">PBL</mml:mi></mml:msub></mml:mrow></mml:msubsup><mml:msub><mml:mi>n</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>t</mml:mi><mml:mo>,</mml:mo><mml:mi>z</mml:mi><mml:mo>)</mml:mo><mml:mi mathvariant="normal">d</mml:mi><mml:mi>z</mml:mi></mml:mrow><mml:mo mathvariant="normal">︸</mml:mo></mml:munder><mml:mrow><mml:mo>≡</mml:mo><mml:mi mathvariant="normal">II</mml:mi></mml:mrow></mml:munder></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><?xmltex \hack{$\egroup}?><mml:mo>.</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

              In Eq. (3), term I is the distance travelled per nominal latitude bin <inline-formula><mml:math id="M168" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> along a meridian (the
crosswind projection is done by multiplication with cos(<inline-formula><mml:math id="M169" display="inline"><mml:mi mathvariant="italic">θ</mml:mi></mml:math></inline-formula>) in term
II) and term II is the mean (the horizontal bar denotes averaging), for latitude
bin <inline-formula><mml:math id="M170" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula>, of the product over all the 5 min averaging periods (<inline-formula><mml:math id="M171" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:math></inline-formula>)
that passed the quality control tests.</p>
      <p id="d1e2968">The total variability in seasonal fluxes was approximated as

                  <disp-formula specific-use="align" content-type="numbered"><mml:math id="M172" display="block"><mml:mtable displaystyle="true"><mml:mtr><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>F</mml:mi><mml:mi>c</mml:mi></mml:msub></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><?xmltex \hack{\hbox\bgroup\fontsize{9.5}{9.5}\selectfont$\displaystyle}?><mml:mo>=</mml:mo><mml:msqrt><mml:mrow><mml:msubsup><mml:mo>∑</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mrow><mml:mi mathvariant="normal">lat</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="normal">bins</mml:mi></mml:mrow></mml:msubsup><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi><mml:mfenced close=")" open="("><mml:mi>i</mml:mi></mml:mfenced><mml:mo>⋅</mml:mo><mml:msup><mml:mi mathvariant="italic">σ</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mfenced close="" open="("><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi mathvariant="italic">χ</mml:mi><mml:mi>C</mml:mi></mml:msub><mml:mfenced close=")" open="("><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:mfenced><mml:mo>⋅</mml:mo><mml:mi>U</mml:mi><mml:mfenced close=")" open="("><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:mfenced><mml:mo>⋅</mml:mo><mml:mi>cos⁡</mml:mi><mml:mi mathvariant="italic">θ</mml:mi><mml:mfenced close=")" open="("><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:mfenced></mml:mrow></mml:mfenced></mml:mrow></mml:msqrt><?xmltex \hack{$\egroup}?></mml:mrow></mml:mtd></mml:mtr><mml:mlabeledtr id="Ch1.E4"><mml:mtd/><mml:mtd><mml:mstyle class="stylechange" displaystyle="true"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mover accent="true"><mml:mrow><mml:mfenced open="" close=")"><mml:mrow><mml:mo>⋅</mml:mo><mml:munderover><mml:mo movablelimits="false">∫</mml:mo><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mi mathvariant="normal">ground</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mi mathvariant="normal">PBL</mml:mi></mml:msub></mml:mrow></mml:munderover><mml:msub><mml:mi>n</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub><mml:mfenced close=")" open="("><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>t</mml:mi><mml:mo>,</mml:mo><mml:mi>z</mml:mi></mml:mrow></mml:mfenced><mml:mi mathvariant="normal">d</mml:mi><mml:mi>z</mml:mi></mml:mrow></mml:mfenced></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

              where <inline-formula><mml:math id="M173" display="inline"><mml:mi mathvariant="italic">σ</mml:mi></mml:math></inline-formula> denotes the standard deviation of the mean. Finally, the
annual budgets were obtained by summing the seasonal budgets.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6"><label>Figure 6</label><caption><p id="d1e3125">Schematic of the mass balance flux calculation procedure expressed
in Eq. (2). The total flux is the sum of flux elements through a vertical
surface with the height of the planetary boundary layer (PBL) and
the width the ship track increment (<inline-formula><mml:math id="M174" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi><mml:mo>=</mml:mo><mml:msub><mml:mi>v</mml:mi><mml:mi mathvariant="normal">ship</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>(t) <inline-formula><mml:math id="M175" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:math></inline-formula>)
during a nominal averaging time interval <inline-formula><mml:math id="M176" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:math></inline-formula> projected onto the
crosswind direction (cos(<inline-formula><mml:math id="M177" display="inline"><mml:mrow><mml:mi mathvariant="italic">θ</mml:mi><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>) <inline-formula><mml:math id="M178" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mi>x</mml:mi></mml:mrow></mml:math></inline-formula>).</p></caption>
            <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://acp.copernicus.org/articles/19/3043/2019/acp-19-3043-2019-f06.png"/>

          </fig>

</sec>
<sec id="Ch1.S2.SS2.SSS5">
  <title>Uncertainty and error propagation</title>
      <p id="d1e3201">In addition to the temporal variability <inline-formula><mml:math id="M179" display="inline"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi>F</mml:mi><mml:mi>c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, (Eq. 4) we
calculated the uncertainty on the total fluxes arising from the
uncertainties on the individual terms of the mass balance equation. Noting
that d<inline-formula><mml:math id="M180" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> represents the distance travelled by the ship with speed <inline-formula><mml:math id="M181" display="inline"><mml:mrow><mml:msub><mml:mi>v</mml:mi><mml:mi mathvariant="normal">ship</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>
during the infinitesimal time interval d<inline-formula><mml:math id="M182" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula>, Eq. (2) can be reformulated to express
the partial flux <inline-formula><mml:math id="M183" display="inline"><mml:mrow><mml:msub><mml:mi>f</mml:mi><mml:mi>c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> through a 2-D plane spanning the
horizontal distance d<inline-formula><mml:math id="M184" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> as a function of <inline-formula><mml:math id="M185" display="inline"><mml:mrow><mml:msub><mml:mi>v</mml:mi><mml:mi mathvariant="normal">ship</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and d<inline-formula><mml:math id="M186" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> (Eq. 5).
              <disp-formula id="Ch1.E5" content-type="numbered"><mml:math id="M187" display="block"><mml:mrow><mml:msub><mml:mi>f</mml:mi><mml:mi>C</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:munderover><mml:mo movablelimits="false">∫</mml:mo><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mi mathvariant="normal">ground</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mi mathvariant="normal">PBL</mml:mi></mml:msub></mml:mrow></mml:munderover><mml:mi mathvariant="normal">Δ</mml:mi><mml:msub><mml:mi mathvariant="italic">χ</mml:mi><mml:mi>C</mml:mi></mml:msub><mml:mo>⋅</mml:mo><mml:mi>U</mml:mi><mml:mo>⋅</mml:mo><mml:msub><mml:mi>n</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub><mml:mfenced open="(" close=")"><mml:mi>z</mml:mi></mml:mfenced><mml:mo>⋅</mml:mo><mml:mi>cos⁡</mml:mi><mml:mi mathvariant="italic">θ</mml:mi><mml:mo>⋅</mml:mo><mml:msub><mml:mi>v</mml:mi><mml:mi mathvariant="normal">ship</mml:mi></mml:msub><mml:mi mathvariant="normal">d</mml:mi><mml:mi>t</mml:mi><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="normal">d</mml:mi><mml:mi>z</mml:mi></mml:mrow></mml:math></disp-formula>
            Applying the rules of error propagation, the error on the flux term
<inline-formula><mml:math id="M188" display="inline"><mml:mrow><mml:msub><mml:mi>f</mml:mi><mml:mi>c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M189" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:msub><mml:mi>f</mml:mi><mml:mi>c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) is given by (with <inline-formula><mml:math id="M190" display="inline"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, the value of the
integral of <inline-formula><mml:math id="M191" display="inline"><mml:mrow><mml:msub><mml:mi>n</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>z</mml:mi></mml:mrow></mml:math></inline-formula>) evaluated over time step d<inline-formula><mml:math id="M192" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula>)

                  <disp-formula specific-use="align" content-type="numbered"><mml:math id="M193" display="block"><mml:mtable displaystyle="true"><mml:mtr><mml:mtd><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:msub><mml:mi>f</mml:mi><mml:mi>c</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:mfenced close="|" open="|"><mml:mrow><mml:msub><mml:mi>f</mml:mi><mml:mi>c</mml:mi></mml:msub></mml:mrow></mml:mfenced></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:mo>=</mml:mo><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msqrt><mml:mrow><mml:msup><mml:mfenced close=")" open="("><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:msub><mml:mi mathvariant="italic">χ</mml:mi><mml:mi>c</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi mathvariant="italic">χ</mml:mi><mml:mi>c</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>+</mml:mo><mml:msup><mml:mfenced open="(" close=")"><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mi>U</mml:mi></mml:mrow><mml:mi>U</mml:mi></mml:mfrac></mml:mstyle></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>+</mml:mo><mml:msup><mml:mfenced close=")" open="("><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mi>cos⁡</mml:mi><mml:mi mathvariant="italic">θ</mml:mi></mml:mrow><mml:mrow><mml:mi>cos⁡</mml:mi><mml:mi mathvariant="italic">θ</mml:mi></mml:mrow></mml:mfrac></mml:mstyle></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>+</mml:mo><mml:msup><mml:mfenced close=")" open="("><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:msub><mml:mi>v</mml:mi><mml:mi mathvariant="normal">ship</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>v</mml:mi><mml:mi mathvariant="normal">ship</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:msqrt></mml:mrow></mml:mtd></mml:mtr><mml:mlabeledtr id="Ch1.E6"><mml:mtd/><mml:mtd><mml:mstyle class="stylechange" displaystyle="true"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mover accent="true"><mml:mrow><mml:mo>+</mml:mo><mml:msup><mml:mfenced close=")" open="("><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mi mathvariant="normal">d</mml:mi><mml:mi>t</mml:mi></mml:mrow><mml:mrow><mml:mi mathvariant="normal">d</mml:mi><mml:mi>t</mml:mi></mml:mrow></mml:mfrac></mml:mstyle></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>+</mml:mo><mml:msup><mml:mfenced open="(" close=")"><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:msubsup><mml:mo>∫</mml:mo><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mi mathvariant="normal">ground</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mi mathvariant="normal">PBL</mml:mi></mml:msub></mml:mrow></mml:msubsup><mml:msub><mml:mi>n</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub><mml:mfenced close=")" open="("><mml:mi>z</mml:mi></mml:mfenced><mml:mi mathvariant="normal">d</mml:mi><mml:mi>z</mml:mi></mml:mrow><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mo>.</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

              Assuming that (a) the uncertainty on d<inline-formula><mml:math id="M194" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> is negligible and (b) the
uncertainty on the PBL height (<inline-formula><mml:math id="M195" display="inline"><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mi mathvariant="normal">PBL</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) is the dominant error term in the
integral of <inline-formula><mml:math id="M196" display="inline"><mml:mrow><mml:msub><mml:mi>n</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>z</mml:mi></mml:mrow></mml:math></inline-formula>) between height <inline-formula><mml:math id="M197" display="inline"><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mi mathvariant="normal">ground</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M198" display="inline"><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mi mathvariant="normal">PBL</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, Eq. (6) can be
approximated as

                  <disp-formula specific-use="align" content-type="numbered"><mml:math id="M199" display="block"><mml:mtable displaystyle="true"><mml:mtr><mml:mtd><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:msub><mml:mi>f</mml:mi><mml:mi>c</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:mfenced open="|" close="|"><mml:mrow><mml:msub><mml:mi>f</mml:mi><mml:mi>c</mml:mi></mml:msub></mml:mrow></mml:mfenced></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:mo>≈</mml:mo><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msqrt><mml:mrow><mml:msup><mml:mfenced open="(" close=")"><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:msub><mml:mi mathvariant="italic">χ</mml:mi><mml:mi>c</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi mathvariant="italic">χ</mml:mi><mml:mi>c</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>+</mml:mo><mml:msup><mml:mfenced open="(" close=")"><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mi>U</mml:mi></mml:mrow><mml:mi>U</mml:mi></mml:mfrac></mml:mstyle></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>+</mml:mo><mml:msup><mml:mfenced open="(" close=")"><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mi>cos⁡</mml:mi><mml:mi mathvariant="italic">θ</mml:mi></mml:mrow><mml:mrow><mml:mi>cos⁡</mml:mi><mml:mi mathvariant="italic">θ</mml:mi></mml:mrow></mml:mfrac></mml:mstyle></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup><mml:mo>+</mml:mo><mml:msup><mml:mfenced close=")" open="("><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:msub><mml:mi>v</mml:mi><mml:mi mathvariant="normal">ship</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>v</mml:mi><mml:mi mathvariant="normal">ship</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:msqrt></mml:mrow></mml:mtd></mml:mtr><mml:mlabeledtr id="Ch1.E7"><mml:mtd/><mml:mtd><mml:mstyle displaystyle="true" class="stylechange"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:mover accent="true"><mml:mrow><mml:mo>+</mml:mo><mml:msup><mml:mfenced close="]" open="["><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mfenced close=")" open="("><mml:mrow><mml:msub><mml:mi>n</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub><mml:mfenced open="(" close=")"><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mi mathvariant="normal">PBL</mml:mi></mml:msub></mml:mrow></mml:mfenced><mml:mo>-</mml:mo><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msub><mml:mi>n</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub><mml:mfenced open="(" close=")"><mml:mrow><mml:msub><mml:mi>z</mml:mi><mml:mi mathvariant="normal">ground</mml:mi></mml:msub></mml:mrow></mml:mfenced></mml:mrow></mml:mfenced><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mo>⋅</mml:mo><mml:mi mathvariant="italic">δ</mml:mi><mml:msub><mml:mi>z</mml:mi><mml:mi mathvariant="normal">PBL</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant="normal">air</mml:mi></mml:msub></mml:mrow></mml:mfrac></mml:mstyle></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow><mml:mo mathvariant="normal">‾</mml:mo></mml:mover><mml:mo>.</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

              Finally, similarly to Eq. (4), the total error on the flux <inline-formula><mml:math id="M200" display="inline"><mml:mrow><mml:msub><mml:mi>F</mml:mi><mml:mi>c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M201" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:msub><mml:mi>F</mml:mi><mml:mi>c</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) calculated for a complete transect of the ship between <inline-formula><mml:math id="M202" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi mathvariant="normal">min</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and
<inline-formula><mml:math id="M203" display="inline"><mml:mrow><mml:msub><mml:mi>x</mml:mi><mml:mi mathvariant="normal">max</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is given by
              <disp-formula id="Ch1.E8" content-type="numbered"><mml:math id="M204" display="block"><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:msub><mml:mi>F</mml:mi><mml:mi>c</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:mfenced close="|" open="|"><mml:mrow><mml:msub><mml:mi>F</mml:mi><mml:mi>c</mml:mi></mml:msub></mml:mrow></mml:mfenced></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>=</mml:mo><mml:msqrt><mml:mrow><mml:msubsup><mml:mo>∑</mml:mo><mml:mi>i</mml:mi><mml:mi>N</mml:mi></mml:msubsup><mml:msup><mml:mfenced open="{" close="}"><mml:mrow><mml:msub><mml:mfenced open="(" close=")"><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:msub><mml:mi>f</mml:mi><mml:mi>c</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:mfenced close="|" open="|"><mml:mrow><mml:msub><mml:mi>f</mml:mi><mml:mi>c</mml:mi></mml:msub></mml:mrow></mml:mfenced></mml:mrow></mml:mfrac></mml:mstyle></mml:mfenced><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:msqrt><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>
            The standard deviations of the individual terms in Eq. (7), calculated for
each 5 min averaging period and averaged over each nominal latitude bin,
were used as proxies for uncertainties. Table S2  summarises the total uncertainty on the calculated emissions
budgets and the relative contributions of the individual terms in Eq. (7).</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T3" specific-use="star"><label>Table 3</label><caption><p id="d1e3947">Seasonal and annual budgets for <inline-formula><mml:math id="M205" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M206" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> for the
United Kingdom (excluding Scotland) and Ireland estimated by a mass balance
approach using concentrations measured at the Mace Head station (Republic of
Ireland; 53<inline-formula><mml:math id="M207" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>19<inline-formula><mml:math id="M208" display="inline"><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:math></inline-formula>19.2<inline-formula><mml:math id="M209" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>′</mml:mo><mml:mo>′</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> N, 9<inline-formula><mml:math id="M210" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>54<inline-formula><mml:math id="M211" display="inline"><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:math></inline-formula>3.599<inline-formula><mml:math id="M212" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>′</mml:mo><mml:mo>′</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> W) and on
board the freight ferry which served the Rosyth (Scotland, UK; 56<inline-formula><mml:math id="M213" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>1<inline-formula><mml:math id="M214" display="inline"><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:math></inline-formula>21.611<inline-formula><mml:math id="M215" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>′</mml:mo><mml:mo>′</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> N, 3<inline-formula><mml:math id="M216" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>26<inline-formula><mml:math id="M217" display="inline"><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:math></inline-formula>21.558<inline-formula><mml:math id="M218" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>′</mml:mo><mml:mo>′</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> W) to Zeebrugge (Belgium;
51<inline-formula><mml:math id="M219" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>21<inline-formula><mml:math id="M220" display="inline"><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:math></inline-formula>16.96<inline-formula><mml:math id="M221" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>′</mml:mo><mml:mo>′</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> N, 3<inline-formula><mml:math id="M222" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>10<inline-formula><mml:math id="M223" display="inline"><mml:msup><mml:mi/><mml:mo>′</mml:mo></mml:msup></mml:math></inline-formula>34.645<inline-formula><mml:math id="M224" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>′</mml:mo><mml:mo>′</mml:mo></mml:mrow></mml:msup></mml:math></inline-formula> E) route. Seasonal
budgets were calculated by year when sufficient data were available;
seasonal budgets were also derived using the entire dataset with and without
segregation of the raw fluxes into day and night components. Annual budgets
were calculated with and without seasonality and with and without day–night
segregation. The variability and uncertainty terms were calculated using Eq. (4) and Eqs. (7)–(8), respectively.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="4">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="left"/>
     <oasis:colspec colnum="3" colname="col3" align="right"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:thead>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry rowsep="1" namest="col3" nameend="col4" align="center">Flux <inline-formula><mml:math id="M225" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula> uncertainty (variability) [Tg] </oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Season</oasis:entry>
         <oasis:entry colname="col2">Year</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M226" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M227" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1">Winter</oasis:entry>
         <oasis:entry colname="col2">2015</oasis:entry>
         <oasis:entry colname="col3">–</oasis:entry>
         <oasis:entry colname="col4">–</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Spring</oasis:entry>
         <oasis:entry colname="col2">2015</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M228" display="inline"><mml:mrow><mml:mn mathvariant="normal">92.6</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">21.1</mml:mn></mml:mrow></mml:math></inline-formula> (34.7)</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M229" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.43</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.13</mml:mn></mml:mrow></mml:math></inline-formula> (0.11)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Summer</oasis:entry>
         <oasis:entry colname="col2">2015</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M230" display="inline"><mml:mrow><mml:mn mathvariant="normal">27.6</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">79.5</mml:mn></mml:mrow></mml:math></inline-formula> (46.8)</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M231" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.45</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.72</mml:mn></mml:mrow></mml:math></inline-formula> (0.09)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Autumn</oasis:entry>
         <oasis:entry colname="col2">2015</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M232" display="inline"><mml:mrow><mml:mn mathvariant="normal">286.4</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">35.4</mml:mn></mml:mrow></mml:math></inline-formula> (47.6)</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M233" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.61</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.07</mml:mn></mml:mrow></mml:math></inline-formula> (0.14)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Winter</oasis:entry>
         <oasis:entry colname="col2">2016</oasis:entry>
         <oasis:entry colname="col3">–</oasis:entry>
         <oasis:entry colname="col4">–</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Spring</oasis:entry>
         <oasis:entry colname="col2">2016</oasis:entry>
         <oasis:entry colname="col3">–</oasis:entry>
         <oasis:entry colname="col4">–</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Summer</oasis:entry>
         <oasis:entry colname="col2">2016</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M234" display="inline"><mml:mrow><mml:mn mathvariant="normal">131.6</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">82.6</mml:mn></mml:mrow></mml:math></inline-formula> (36.5)</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M235" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.39</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.25</mml:mn></mml:mrow></mml:math></inline-formula> (0.09)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Autumn</oasis:entry>
         <oasis:entry colname="col2">2016</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M236" display="inline"><mml:mrow><mml:mn mathvariant="normal">261.3</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">164.3</mml:mn></mml:mrow></mml:math></inline-formula> (56.4)</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M237" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.75</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.40</mml:mn></mml:mrow></mml:math></inline-formula> (0.16)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Winter</oasis:entry>
         <oasis:entry colname="col2">2017</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M238" display="inline"><mml:mrow><mml:mn mathvariant="normal">341</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">17.2</mml:mn></mml:mrow></mml:math></inline-formula> (62.1)</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M239" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.78</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.05</mml:mn></mml:mrow></mml:math></inline-formula> (0.38)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Spring</oasis:entry>
         <oasis:entry colname="col2">2017</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M240" display="inline"><mml:mrow><mml:mn mathvariant="normal">197.5</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">40.4</mml:mn></mml:mrow></mml:math></inline-formula> (27.9)</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M241" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.49</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.14</mml:mn></mml:mrow></mml:math></inline-formula> (0.07)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Summer</oasis:entry>
         <oasis:entry colname="col2">2017</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M242" display="inline"><mml:mrow><mml:mn mathvariant="normal">155</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">81.8</mml:mn></mml:mrow></mml:math></inline-formula> (77.6)</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M243" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.32</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.14</mml:mn></mml:mrow></mml:math></inline-formula> (0.06)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Autumn</oasis:entry>
         <oasis:entry colname="col2">2017</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M244" display="inline"><mml:mrow><mml:mn mathvariant="normal">363.4</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">12.1</mml:mn></mml:mrow></mml:math></inline-formula> (65.7)</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M245" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.03</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.04</mml:mn></mml:mrow></mml:math></inline-formula> (0.15)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Winter</oasis:entry>
         <oasis:entry colname="col2">2016 &amp; 2017</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M246" display="inline"><mml:mrow><mml:mn mathvariant="normal">379.1</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">26.6</mml:mn></mml:mrow></mml:math></inline-formula> (68.8)</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M247" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.89</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.08</mml:mn></mml:mrow></mml:math></inline-formula> (0.35)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Spring</oasis:entry>
         <oasis:entry colname="col2">2015–2017</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M248" display="inline"><mml:mrow><mml:mn mathvariant="normal">161.5</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">30.9</mml:mn></mml:mrow></mml:math></inline-formula> (41.2)</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M249" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.55</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.08</mml:mn></mml:mrow></mml:math></inline-formula> (0.17)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Summer</oasis:entry>
         <oasis:entry colname="col2">2015–2017</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M250" display="inline"><mml:mrow><mml:mn mathvariant="normal">123.6</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">76.9</mml:mn></mml:mrow></mml:math></inline-formula> (64.6)</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M251" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.38</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.25</mml:mn></mml:mrow></mml:math></inline-formula> (0.09)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Autumn</oasis:entry>
         <oasis:entry colname="col2">2015–2017</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M252" display="inline"><mml:mrow><mml:mn mathvariant="normal">250.2</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">200.1</mml:mn></mml:mrow></mml:math></inline-formula> (57.8)</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M253" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.72</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.40</mml:mn></mml:mrow></mml:math></inline-formula> (0.16)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Winter (day–night weighting)</oasis:entry>
         <oasis:entry colname="col2">2016 &amp; 2017</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M254" display="inline"><mml:mrow><mml:mn mathvariant="normal">357.8</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">26.2</mml:mn></mml:mrow></mml:math></inline-formula> (66.8)</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M255" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.82</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.08</mml:mn></mml:mrow></mml:math></inline-formula> (0.34)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Spring (day–night weighting)</oasis:entry>
         <oasis:entry colname="col2">2015–2017</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M256" display="inline"><mml:mrow><mml:mn mathvariant="normal">162.5</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">30.9</mml:mn></mml:mrow></mml:math></inline-formula> (55.0)</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M257" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.57</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.08</mml:mn></mml:mrow></mml:math></inline-formula> (0.22)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Summer (day–night weighting)</oasis:entry>
         <oasis:entry colname="col2">2015–2017</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M258" display="inline"><mml:mrow><mml:mn mathvariant="normal">127.7</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">76.9</mml:mn></mml:mrow></mml:math></inline-formula> (78.7)</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M259" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.39</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.25</mml:mn></mml:mrow></mml:math></inline-formula> (0.12)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Autumn (day–night weighting)</oasis:entry>
         <oasis:entry colname="col2">2015–2017</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M260" display="inline"><mml:mrow><mml:mn mathvariant="normal">232.9</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">57.8</mml:mn></mml:mrow></mml:math></inline-formula> (72.2)</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M261" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.67</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.16</mml:mn></mml:mrow></mml:math></inline-formula> (0.19)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Annual (from seasonal budgets)</oasis:entry>
         <oasis:entry colname="col2">2015–2017</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M262" display="inline"><mml:mrow><mml:mn mathvariant="normal">914.4</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">218.1</mml:mn></mml:mrow></mml:math></inline-formula> (118.1)</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M263" display="inline"><mml:mrow><mml:mn mathvariant="normal">2.55</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.48</mml:mn></mml:mrow></mml:math></inline-formula> (0.43)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Annual (from seasonal, day–night weighted budgets)</oasis:entry>
         <oasis:entry colname="col2">2015–2017</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M264" display="inline"><mml:mrow><mml:mn mathvariant="normal">881.0</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">125.8</mml:mn></mml:mrow></mml:math></inline-formula> (137.5)</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M265" display="inline"><mml:mrow><mml:mn mathvariant="normal">2.44</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.30</mml:mn></mml:mrow></mml:math></inline-formula> (0.47)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Annual (no seasons)</oasis:entry>
         <oasis:entry colname="col2">2015–2017</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M266" display="inline"><mml:mrow><mml:mn mathvariant="normal">708.3</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">270.4</mml:mn></mml:mrow></mml:math></inline-formula> (241.9)</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M267" display="inline"><mml:mrow><mml:mn mathvariant="normal">2.1</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.67</mml:mn></mml:mrow></mml:math></inline-formula> (0.63)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Annual (no seasons, day–night weighted)</oasis:entry>
         <oasis:entry colname="col2">2015–2017</oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M268" display="inline"><mml:mrow><mml:mn mathvariant="normal">598.3</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">250.1</mml:mn></mml:mrow></mml:math></inline-formula> (274.9)</oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M269" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.66</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.60</mml:mn></mml:mrow></mml:math></inline-formula> (0.94)</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">UK (BEIS, 2017)</oasis:entry>
         <oasis:entry colname="col2">2015</oasis:entry>
         <oasis:entry colname="col3">415.1</oasis:entry>
         <oasis:entry colname="col4">2.1</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">RoI (EPA, 2017)</oasis:entry>
         <oasis:entry colname="col2">2015</oasis:entry>
         <oasis:entry colname="col3">38.4</oasis:entry>
         <oasis:entry colname="col4">0.53</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Scotland (Inventory, 2018)</oasis:entry>
         <oasis:entry colname="col2">2015</oasis:entry>
         <oasis:entry colname="col3">30.8</oasis:entry>
         <oasis:entry colname="col4">0.34</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Total inventory (UK–Scotland <inline-formula><mml:math id="M270" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula> RoI)</oasis:entry>
         <oasis:entry colname="col2">2015</oasis:entry>
         <oasis:entry colname="col3">422.7</oasis:entry>
         <oasis:entry colname="col4">2.29</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Ganesan  (Ganesan et al., 2015)</oasis:entry>
         <oasis:entry colname="col2">2012–2014</oasis:entry>
         <oasis:entry colname="col3">–</oasis:entry>
         <oasis:entry colname="col4">1.65–2.67</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Bergamaschi (Bergamaschi et al., 2015)</oasis:entry>
         <oasis:entry colname="col2">2006–2007</oasis:entry>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4">3.1–3.5</oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7" specific-use="star"><label>Figure 7</label><caption><p id="d1e5150">Box and whisker plots of 5 min binned averages of <inline-formula><mml:math id="M271" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>
fluxes along the route of the ferry (latitude bin width: 0.2<inline-formula><mml:math id="M272" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>).
The horizontal bar within each box corresponds to the median for a given
latitude bin, the upper and lower hinges represent the 75th and
25th quantiles, respectively, and the upper and lower whiskers indicate
the largest–smallest observation less–greater than or equal to upper–lower
hinge <inline-formula><mml:math id="M273" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:msup><mml:mn mathvariant="normal">1.5</mml:mn><mml:mo>*</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> IQR (inter-quantile range), respectively. The outliers are
represented by solid circles and arithmetic means by red diamonds. The flux
is integrated over the height of the planetary boundary layer and expressed
in units of mass flux per metre travelled crosswind within each latitude bin
per unit time.</p></caption>
            <?xmltex \igopts{width=355.659449pt}?><graphic xlink:href="https://acp.copernicus.org/articles/19/3043/2019/acp-19-3043-2019-f07.png"/>

          </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F8" specific-use="star"><label>Figure 8</label><caption><p id="d1e5195">Box and whisker plots of 5 min binned averages of <inline-formula><mml:math id="M274" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>
fluxes along the route of the ferry (latitude bin width: 0.2<inline-formula><mml:math id="M275" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>).
The horizontal bar within each box corresponds to the median for a given
latitude bin, the upper and lower hinges represent the 75th and
25th quantiles, respectively, and the upper and lower whiskers indicate
the largest–smallest observation less–greater than or equal to upper–lower
hinge <inline-formula><mml:math id="M276" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:msup><mml:mn mathvariant="normal">1.5</mml:mn><mml:mo>*</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> IQR (inter-quantile range), respectively. The outliers are
represented by solid circles and arithmetic means by red diamonds. The flux
is integrated over the height of the planetary boundary layer and expressed
in units of mass flux per metre travelled crosswind within each latitude bin
per unit time.</p></caption>
            <?xmltex \igopts{width=355.659449pt}?><graphic xlink:href="https://acp.copernicus.org/articles/19/3043/2019/acp-19-3043-2019-f08.png"/>

          </fig>

</sec>
</sec>
</sec>
<?pagebreak page3051?><sec id="Ch1.S3">
  <title>Results</title>
<sec id="Ch1.S3.SS1">
  <title>Seasonal and annual fluxes</title>
      <p id="d1e5251">The fluxes of <inline-formula><mml:math id="M277" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> (Fig. 7) and <inline-formula><mml:math id="M278" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> (Fig. 8) calculated from
measurements on board the North Sea ferry were variable in space (over the
latitude range 51.35–56.15<inline-formula><mml:math id="M279" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N) and time. The
calculated emissions of <inline-formula><mml:math id="M280" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M281" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> had maxima in winter (DJF;
<inline-formula><mml:math id="M282" display="inline"><mml:mrow><mml:mn mathvariant="normal">379.1</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">26.2</mml:mn></mml:mrow></mml:math></inline-formula> Tg <inline-formula><mml:math id="M283" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M284" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.89</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.08</mml:mn></mml:mrow></mml:math></inline-formula> Tg <inline-formula><mml:math id="M285" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>; 2016
and
2017 winter data only). Emission minima were observed in summer (JJA; <inline-formula><mml:math id="M286" display="inline"><mml:mrow><mml:mn mathvariant="normal">123.6</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">76.9</mml:mn></mml:mrow></mml:math></inline-formula> Tg <inline-formula><mml:math id="M287" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>; <inline-formula><mml:math id="M288" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.38</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.25</mml:mn></mml:mrow></mml:math></inline-formula> Tg <inline-formula><mml:math id="M289" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>; Table 3).
Springtime (MAM) emissions were <inline-formula><mml:math id="M290" display="inline"><mml:mrow><mml:mn mathvariant="normal">161.5</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">30.9</mml:mn></mml:mrow></mml:math></inline-formula> Tg for <inline-formula><mml:math id="M291" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and
<inline-formula><mml:math id="M292" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.55</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.08</mml:mn></mml:mrow></mml:math></inline-formula> Tg for <inline-formula><mml:math id="M293" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, and in autumn (SON) the measured
emissions were <inline-formula><mml:math id="M294" display="inline"><mml:mrow><mml:mn mathvariant="normal">250.2</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">200.1</mml:mn></mml:mrow></mml:math></inline-formula> Tg for <inline-formula><mml:math id="M295" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M296" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.72</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.40</mml:mn></mml:mrow></mml:math></inline-formula> Tg
for <inline-formula><mml:math id="M297" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>. For <inline-formula><mml:math id="M298" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M299" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, a statistically significant
difference in seasonal budgets was found between winter and spring as well
as between winter and summer. For both gases, the differences in emissions
between spring and summer were not statistically significant, whilst for
autumn the total uncertainty was large (80 % uncertainty for <inline-formula><mml:math id="M300" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and
56 % for <inline-formula><mml:math id="M301" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>). Annual budgets, estimated from seasonal values, were
<inline-formula><mml:math id="M302" display="inline"><mml:mrow><mml:mn mathvariant="normal">914.4</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">218.1</mml:mn></mml:mrow></mml:math></inline-formula> Tg for <inline-formula><mml:math id="M303" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M304" display="inline"><mml:mrow><mml:mn mathvariant="normal">2.55</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.48</mml:mn></mml:mrow></mml:math></inline-formula> for <inline-formula><mml:math id="M305" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>.
Without accounting for seasonality (i.e. using all data without seasonal
segregation, which could weight towards the periods of the year for which
the most data were available), the emissions budgets were <inline-formula><mml:math id="M306" display="inline"><mml:mrow><mml:mn mathvariant="normal">708.3</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">270.4</mml:mn></mml:mrow></mml:math></inline-formula> Tg for <inline-formula><mml:math id="M307" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M308" display="inline"><mml:mrow><mml:mn mathvariant="normal">2.1</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.67</mml:mn></mml:mrow></mml:math></inline-formula> for <inline-formula><mml:math id="M309" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F9" specific-use="star"><label>Figure 9</label><caption><p id="d1e5634">Box and whisker plots of 5 min binned averages of <inline-formula><mml:math id="M310" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>
fluxes along the route of the ferry (latitude bin width: 0.2<inline-formula><mml:math id="M311" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>)
segregated into day and night contributions. The horizontal bar within each
box corresponds to the median for a given latitude bin, the upper and lower
hinges represent the 75th and 25th quantiles, respectively, and
the upper and lower whiskers indicate the largest–smallest observation
less–greater than or equal to upper–lower hinge <inline-formula><mml:math id="M312" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:msup><mml:mn mathvariant="normal">1.5</mml:mn><mml:mo>*</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> IQR
(inter-quantile range), respectively. The outliers are represented by solid
circles and arithmetic means by red diamonds. The flux is integrated over
the height of the planetary boundary layer and expressed in units of mass
flux per metre travelled crosswind within each latitude bin per unit time.</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://acp.copernicus.org/articles/19/3043/2019/acp-19-3043-2019-f09.png"/>

        </fig>

      <?pagebreak page3053?><p id="d1e5676">In winter, spring, and autumn, the largest fluxes of both gases were found in
a broad central latitudinal band (52–54<inline-formula><mml:math id="M313" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N; Figs. 7 and 8). The lowest emissions were observed in summer across the
entire spatial domain and they exhibited a smaller increment in the 52–54<inline-formula><mml:math id="M314" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N band compared to the fringes of the domain
than in other seasons.</p>
</sec>
<sec id="Ch1.S3.SS2">
  <title>Diurnal variability</title>
      <p id="d1e5703">There were differences between day (defined arbitrarily as 09:00 to 18:00)
and night fluxes, particularly in spring and summer (Figs. 9 and 10). Median
daytime <inline-formula><mml:math id="M315" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> fluxes were negative for latitudes in the range 54.5
to 55.9<inline-formula><mml:math id="M316" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N in spring; in summer, negative <inline-formula><mml:math id="M317" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>
fluxes were found at 54.5 and 55.3–55.5<inline-formula><mml:math id="M318" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N. It
is important to note that air mass transit time between the inflow and outflow
points of the domain varied from a median of 11 h in winter to 19 h
in summer, which means that the day and night periods did overlap.</p>
      <p id="d1e5746">Seasonal and annual budgets were recalculated using day and night fluxes
weighted by day length (Table 3) in order to assess the impacts of uneven
day–night data density distributions over the spatial domain caused by the
relatively slow travel speed of the ship and the random data gaps introduced
by changing wind direction and measurement downtime. The annual budgets
calculated with day–night flux segregation were smaller than those obtained
without day–night partitioning, but the differences were not statistically
significant and, in general, separating fluxes into day and night components
increased the uncertainties on the final budgets both at the seasonal and
annual levels.</p>
      <p id="d1e5749">The annual budgets calculated using all available data were smaller than
those obtained from seasonal budgets (both with and without day–night
segregation); however, the only statistically significant difference was
between the annual budget of <inline-formula><mml:math id="M319" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> obtained from seasonal data and the
budget estimated with day–night weighting but without seasonality.</p>
      <p id="d1e5763">The annual budgets for both gases obtained without accounting for the
seasonality in data coverage were consistent with inventory data but the
measurement uncertainties were large (36 % and 32 % for <inline-formula><mml:math id="M320" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> with
and without day–night weighting, with counterpart uncertainties on <inline-formula><mml:math id="M321" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>
budgets of 42 % and 38 %, respectively). The annual budgets of <inline-formula><mml:math id="M322" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>
obtained from seasonal budgets were in good agreement with inventory data,
with uncertainties of 12 % and 19 % for estimates calculated with and
without day–night weighting, respectively. In contrast, <inline-formula><mml:math id="M323" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> budgets
were almost double the inventory value, with uncertainties of 14 % and
24 % for estimates calculated with and without day–night weighting.</p>
      <p id="d1e5811">The seasonal mass balance fluxes of <inline-formula><mml:math id="M324" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M325" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> calculated from
concentration measurements on the ferry were compared to known land sources
and meteorological drivers of these gases. For both gases, there was a
strong positive correlation between seasonal emissions measured on the
ferry and the consumption of natural gas in the UK (Fig. 11). The correlation
between GHG emissions and mean air temperature was negative and
statistically significant (Fig. 12).</p>
</sec>
</sec>
<?pagebreak page3054?><sec id="Ch1.S4">
  <title>Discussion</title>
      <p id="d1e5843">The mass balance approach presented here relies on simplifying assumptions
to derive GHG budgets for a large part of the British Isles. The main
assumptions are that (a) the air masses travel west to east, (b) the PBL
height is constant over the spatial domain for each nominal averaging
period, (c) there is no loss or input of mass into the domain other than from
land sinks–sources, and (d) the air is well-mixed over the entire PBL
height.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F10" specific-use="star"><label>Figure 10</label><caption><p id="d1e5848">Box and whisker plots of 5 min binned averages of <inline-formula><mml:math id="M326" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>
fluxes along the route of the ferry (latitude bin width: 0.2<inline-formula><mml:math id="M327" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>)
segregated into day and night contributions. The horizontal bar within each
box corresponds to the median for a given latitude bin, the upper and lower
hinges represent the 75th and 25th quantiles, respectively, and
the upper and lower whiskers indicate the largest–smallest observation
less–greater than or equal to upper–lower hinge <inline-formula><mml:math id="M328" display="inline"><mml:mrow><mml:mo>±</mml:mo><mml:msup><mml:mn mathvariant="normal">1.5</mml:mn><mml:mo>*</mml:mo></mml:msup></mml:mrow></mml:math></inline-formula> IQR
(inter-quantile range), respectively. The outliers are represented by solid
circles and arithmetic means by red diamonds. The flux is integrated over
the height of the planetary boundary layer and expressed in units of mass
flux per metre travelled crosswind within each latitude bin per unit time.</p></caption>
        <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://acp.copernicus.org/articles/19/3043/2019/acp-19-3043-2019-f10.png"/>

      </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F11" specific-use="star"><label>Figure 11</label><caption><p id="d1e5892">Seasonal budgets of <inline-formula><mml:math id="M329" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M330" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> as a function of UK
natural gas consumption (source: BEIS, 2018). The shaded area represents the
95 % confidence interval of the linear regression.</p></caption>
        <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://acp.copernicus.org/articles/19/3043/2019/acp-19-3043-2019-f11.png"/>

      </fig>

      <p id="d1e5924">The data were filtered for westerly flow based on air mass back trajectories
obtained from the HYSPLIT Trajectory Model (NOAA Air Resources Laboratory,
2018) daily 72 h runs at two coordinates: the Mace Head reference site
and one ferry position halfway along its route. The back trajectories were
run daily, commencing at midnight, and the air mass histories were assumed
to be valid for an entire 24 h period and for the entire spatial domain.
Of the four main assumptions listed above, points (c) and (d) are the most
subjective because they could not be verified nor quantified. Assumption (a) (air mass travel from west to east)
can be considered to be reasonably
well-constrained owing to the data screening procedure at the preprocessing
stage. Violations of the stationarity assumption (point b) due to
significant changes in the mean PBL height at a sub-hourly time step would
either be captured, in part or entirely, during the next hourly averaging
period or go unnoticed in the case of very transient non-stationary events.
Whilst the temporal variability of the mean PBL height for the spatial
domain considered can be quantified and propagated through the emissions
budget calculations as measurement uncertainty, the potential bias between
model output and observations is unknown. Recent studies have compared
different WRF parametrisation schemes with observed PBL height and found
that, in general, the YSU scheme used in this study performs reasonably well
in terms of predicting PBL height with minimum bias typically observed
before midday (Hu et al., 2010; Banks et al., 2016; Tyagi et al., 2018; Xu
et al., 2018); however, these studies also highlighted the fact that model performance
can vary significantly between sites and time of day and that YSU tends to
underestimate the PBL height over the sea (Tyagi et al., 2018). Comparisons
between observations and model outputs of wind speed profiles for different
parametrisation schemes also found substantial variability, both intra- and
inter-model, with the YSU scheme exhibiting a tendency to overestimate wind
speeds (Balzarini et al., 2014; Tyagi  et al., 2018). The formation of sea breezes adds
another level of complexity to the modelling of PBL height and wind speed,
in particular in the southern North Sea where the orientation of the
coastlines and their proximity to one another have been shown to induce sea
breeze formation and to influence sea breeze type and offshore extent
(Steele et al., 2013, 2015). Furthermore, not all WRF
parametrisation schemes are equal in performance with respect to sea breeze
conditions; recent studies show that the YSU scheme used here exhibited the
smallest bias for wind speeds measured onshore under complex sea breeze
conditions (Steele et al., 2015) and that it also captured the temporal
evolution of the atmospheric boundary layer height better than other schemes
(Salvador et al., 2016).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F12" specific-use="star"><label>Figure 12</label><caption><p id="d1e5929">Seasonal budgets of <inline-formula><mml:math id="M331" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M332" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> as a function of mean UK
air temperature derived from ca. 250 synoptic stations (source: Met Office,
2018). The shaded area represents the 95 % confidence intervals of the
linear regressions.</p></caption>
        <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://acp.copernicus.org/articles/19/3043/2019/acp-19-3043-2019-f12.png"/>

      </fig>

      <p id="d1e5960">Intrinsic, unquantifiable biases on the mixing layer heights and mean wind
speeds derived from the WRF model are hence likely. Wind speed and
enhancement above background concentration were found to be to dominant
uncertainty terms, jointly accounting for over 80 % of the total
uncertainty in all seasons (Table S2). In
contrast, nudging the baseline concentrations measured at Mace Head by a
time lag estimated from the mean air mass travel time had only a very modest
impact on the final budgets (Table S2). The two measures of errors proposed
in this paper (based on temporal variability and total uncertainty through
error propagation) yield on the whole comparable results, with the main
discrepancy found for the autumn budget (years used: 2015–2017) in which the
total uncertainty was almost four-fold the value obtained by considering the
temporal variability alone. The autumn uncertainty was brought in line with
the temporal variability estimate for both gases when the day–night
weighting was applied. Whilst the variability and the total uncertainty are
useful as first approximations for the confidence in the emission budgets,
they should be treated as potential lower limits because of the unquantified
bias between WRF model outputs and actual values of the PBL height and wind
speed.</p>
      <p id="d1e5963">The fluxes calculated under this data filtering regime were assumed to be
representative of surface emissions and uptake over the land masses bounded
by the spatial domain, and local influences (due to e.g. localised air
recirculation) were assumed to be negligible. This assumption could not be
tested on a point-per-point basis but the latitudinal trends for both
<inline-formula><mml:math id="M333" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M334" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> at the seasonal timescale (Figs. 7 and 8) are
consistent with the demographics and the known spatial distributions of
sources of GHGs over the latitudinal range considered. In particular, the
emission peaks for <inline-formula><mml:math id="M335" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> observed around 52.5 and 54<inline-formula><mml:math id="M336" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N coincide
with major urban centres in the British Midlands,
namely Birmingham and Manchester, Liverpool, Leeds, and Sheffield, as well as Dublin
further upwind in the Republic of Ireland. These conurbations are reported
to be significant sources of <inline-formula><mml:math id="M337" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> by the UK's official National
Atmospheric Emissions Inventory (NAEI, 2018a). The calculated <inline-formula><mml:math id="M338" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>
emissions were elevated in the 52.5–54<inline-formula><mml:math id="M339" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N
latitude band compared to the fringes of the domain. This agrees with the
NAEI UK <inline-formula><mml:math id="M340" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> map (NAEI, 2018a), which shows large emissions from the
western parts of England in that latitude band. The NAEI reports substantial
<inline-formula><mml:math id="M341" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> emissions from the Cornwall area (SW England; latitudes
&lt; 51.3<inline-formula><mml:math id="M342" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N), which might not always have registered in their
entirety by the measurement system on the ferry because the port of
Zeebrugge – the starting and end point of the vessel's route – lies at 51.21<inline-formula><mml:math id="M343" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F13" specific-use="star"><label>Figure 13</label><caption><p id="d1e6082">Seasonal fluxes of <inline-formula><mml:math id="M344" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M345" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> estimated by mass
balance from concentration measurements on board the ferry as a function of
mean regional air temperature (source: Met Office, 2018). The data are
presented for three latitudinal regions denoted MID, N, and S.
The MID region spans the latitude range 52.8–54.2<inline-formula><mml:math id="M346" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, N spans 54.2–56.1<inline-formula><mml:math id="M347" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N, and
S spans 52.0–52.8<inline-formula><mml:math id="M348" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N. The shaded area
represents the 95 % confidence intervals of the linear regressions.</p></caption>
        <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://acp.copernicus.org/articles/19/3043/2019/acp-19-3043-2019-f13.png"/>

      </fig>

      <p id="d1e6141">The negative daytime fluxes of <inline-formula><mml:math id="M349" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> registered in summer for latitudes
&gt; 54.5<inline-formula><mml:math id="M350" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N are consistent with the demographics,
topography, and land use of the northern parts of England and of Northern
Ireland; these areas are less populated than the southern parts, host the
hills and mountains of the Lake District and the North Pennines, and the
land use consists largely of grasslands. The combination of these factors
(lower density of anthropogenic sources and higher density of biogenic sinks
compared to southern parts of the UK) can explain the net negative fluxes of
<inline-formula><mml:math id="M351" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> measured during the daytime in spring and summer. Whilst the
observed lower emissions of <inline-formula><mml:math id="M352" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> in the northern parts of the spatial
domain are consistent with the spatial distribution of emissions from NAEI
data (NAEI, 2018a), Polson et al. (2011) reported substantial
summertime emissions from Ireland and Northern Ireland which should cancel
out the sink terms in northern England when integrating along a latitude
bin. The fact that negative and very low summer emissions were derived by
the ferry mass balance approach could indicate that measurements on board
the ferry were more sensitive to sources and sinks in the eastern parts of
the domain sampled because of (a) violation of the simplifying assumption
that there is no loss of mass out of the domain, (b) imperfect vertical
mixing, or (c) local air circulation which would not have been resolved by
the HYSPLIT air mass histories. Alternatively, the mass balance estimates
are real and the high <inline-formula><mml:math id="M353" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> emissions assigned to Ireland in the aircraft
inversion model are measurement<?pagebreak page3057?> artefacts caused by the venting of the
nocturnal boundary layer as postulated by Polson et al. (2011).</p>
      <p id="d1e6197">There was no statistically significant difference between day and night
fluxes for <inline-formula><mml:math id="M354" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, which could be because (a) the major sources of this
gas in the British Isles (livestock, including enteric fermentation and manure
management, and waste-treatment-related emissions, including landfills and waste
water; 52.8 % and 39.1 % of the total <inline-formula><mml:math id="M355" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> budget for the UK,
respectively; BEIS, 2017) do not have marked diurnal cycles, (b) the mass
balance approach could not resolve them, (c) the transit time of the air
masses over the spatial domain blurred the potential differences between day
and night emissions, or (d) the <inline-formula><mml:math id="M356" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> signal measured on the ferry
was contaminated and did not reflect emissions from the land surface. Due to
the temporal and spatial averaging carried out to derive emission estimates
from the ferry measurements, and due to the diffuse spatial distribution of
the dominant land sources of <inline-formula><mml:math id="M357" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, it seems likely that relatively small
diurnal variations (e.g. studies indicate diurnal cycles in <inline-formula><mml:math id="M358" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>
emissions from dairy farms and from landfills
sites; Van der Zaag et al., 2014, and Borjesson and Svensson, 1997, respectively) would not be resolved by the mass
balance approach.</p>
      <p id="d1e6255">At the seasonal timescale, the fluxes of <inline-formula><mml:math id="M359" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M360" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> were both
strongly correlated with UK natural gas usage (Fig. 11; BEIS, 2018); this
provides confidence that the fluxes calculated by the mass balance approach
can be related to physical emissions within the spatial domain and that the
data filtering and quality control criteria excluded data points potentially
contaminated by emissions from the ship. The statistically significant
linear correlations between derived <inline-formula><mml:math id="M361" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M362" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> fluxes and natural
gas usage do not demonstrate causality, but suggest that the sources of
these two GHGs within the domain sampled have seasonal dynamics similar to
those of natural gas usage. However, both <inline-formula><mml:math id="M363" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M364" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> emissions
exhibited a weaker correlation with mean seasonal air temperature than with
natural gas usage (Fig. 12), and this may indicate that natural gas
consumption is a causal driver rather than a proxy for another underlying
variable. Whilst it is reasonable to infer that both <inline-formula><mml:math id="M365" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M366" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>
would increase in line with an increasing demand for natural gas during the
colder months, the NAEI (NAEI, 2018b) attributes only 15 % of annual
<inline-formula><mml:math id="M367" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> emissions to fuel-related sources (combustion and fugitive
emissions); this does not tally with the <inline-formula><mml:math id="M368" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">100</mml:mn></mml:mrow></mml:math></inline-formula> % increase in
<inline-formula><mml:math id="M369" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> emissions between winter and summer, which is accompanied by a
similar increase in natural gas usage. An unexpectedly large diurnal and
seasonal variability in the <inline-formula><mml:math id="M370" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> flux was observed from direct flux
measurements above London (Helfter et al., 2016), and this suggested that
pressure variations in the gas supply network in response to gas demand may
have a significant impact on urban emissions. Fugitive emissions from the
network may be underestimated in the NAEI.</p>
      <p id="d1e6391">Seasonality in methane emissions from landfills has also been reported, with
higher emissions sometimes observed in winter and autumn (Borjesson and
Svensson, 1997; Chanton and Liptay, 2000). The explanation for this is that
net <inline-formula><mml:math id="M371" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> emissions from landfill emissions can be largely regulated by
methane oxidation in the top layer of the landfill cover soil: oxidation is
limited by soil temperature and the methane-oxidising potential decreases in
autumn and winter because of lower soil temperatures, which results in an
increase in methane emissions during the colder seasons. Riddick et al. (2017) reported a 71 % winter-to-summer reduction in
<inline-formula><mml:math id="M372" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> emissions from a waste treatment park near Haddenham, England.
Central England has the largest densities of waste treatment and landfill
sites, which might explain the statistically significant linear
anti-correlation between seasonal <inline-formula><mml:math id="M373" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> emissions and mean air
temperature found in this region (Fig. 13). This is a remarkable result,
which demonstrates the merit of this simple mass balance approach. In the
other two regions considered (N and S, i.e. north and south of the
central region denoted as MID), there was no compelling correlation
between <inline-formula><mml:math id="M374" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> emissions and mean air temperature. This suggests that the
dominant sources of this GHG in the N and S regions differ from the ones in
the central region.</p>
      <p id="d1e6438">For <inline-formula><mml:math id="M375" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, the seasonal emissions had statistically significant
correlations with mean air temperature in the central and northern regions,
whilst the linear correlation was only marginally non-significant in the
southern region. This is consistent with (a) the seasonality of natural gas
usage (the NAEI attributes <inline-formula><mml:math id="M376" display="inline"><mml:mrow><mml:mo>∼</mml:mo><mml:mn mathvariant="normal">50</mml:mn></mml:mrow></mml:math></inline-formula> % of annual <inline-formula><mml:math id="M377" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>
emissions to fuel combustion processes such as domestic and industrial gas
usage; NAEI, 2018b) and (b) the seasonality of <inline-formula><mml:math id="M378" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> uptake by
vegetation.</p>
      <p id="d1e6484">Contrary to our findings, the UK <inline-formula><mml:math id="M379" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> emissions derived by inverse
modelling using concentration data from four tall tower sites distributed
across the UK and Ireland did not exhibit any clear seasonality over the
period August 2012–August 2014 (Ganesan et al., 2015), but the range of
emissions (1.65 to 2.67 Tg) was consistent with the ferry measurements
(<inline-formula><mml:math id="M380" display="inline"><mml:mrow><mml:mn mathvariant="normal">1.52</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">1.0</mml:mn></mml:mrow></mml:math></inline-formula> to <inline-formula><mml:math id="M381" display="inline"><mml:mrow><mml:mn mathvariant="normal">3.56</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.32</mml:mn></mml:mrow></mml:math></inline-formula> Tg).</p>
      <p id="d1e6523">For <inline-formula><mml:math id="M382" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, all four annual budgets calculated using all the available
data for the 2015–2017 period were consistent with the inventory values for
the UK (excluding Scotland) and the Republic of Ireland, as well as with
top-down modelling estimates (Table 3). Temporal data aggregation (i.e. not
considering seasonality) increased the uncertainty on the final budget
(36 % and 32 % uncertainty for annual budgets derived with and without
considering differences in day and night emissions compared to 12 % and
19 % for the budgets into which seasonality was factored) and it therefore seems
that this approach should be discarded. The difference between the
annual <inline-formula><mml:math id="M383" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> budgets calculated with and without day–night segregation
but with seasonality was within the uncertainty of the individual estimates,
and since we found no compelling evidence of diurnal trends, we arrive at
<inline-formula><mml:math id="M384" display="inline"><mml:mrow><mml:mn mathvariant="normal">2.55</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.48</mml:mn></mml:mrow></mml:math></inline-formula> Tg yr<inline-formula><mml:math id="M385" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> as our final estimate of the methane emissions
from the UK (excluding Scotland) and the Republic of Ireland for the period
2015–2017.</p>
      <?pagebreak page3058?><p id="d1e6572">Following the same argument regarding temporal data aggregation, we derive
an annual emission budget for <inline-formula><mml:math id="M386" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> of <inline-formula><mml:math id="M387" display="inline"><mml:mrow><mml:mn mathvariant="normal">881.0</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">125.8</mml:mn></mml:mrow></mml:math></inline-formula> Tg yr<inline-formula><mml:math id="M388" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>,
which is the estimate obtained from seasonal budgets with day–night
segregation because we found indications of diurnal trends in some parts of
the spatial domain.</p>
      <p id="d1e6610">This value is more than twice the inventory estimate of 422.7 Tg, but
contrarily to <inline-formula><mml:math id="M389" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M390" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> has significant biogenic sources (e.g. the
<inline-formula><mml:math id="M391" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> exhaled by the 65 million-strong human population within the
spatial domain considered is of the order of 18 Tg yr<inline-formula><mml:math id="M392" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>; Moriwaki and
Kanda, 2004) and sinks (vegetation uptake) which are not accounted for by
anthropogenic atmospheric emissions inventories; a direct comparison
with the inventory is hence not possible. Polson et al. (2011) derived an
annual budget for <inline-formula><mml:math id="M393" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> of <inline-formula><mml:math id="M394" display="inline"><mml:mrow><mml:mn mathvariant="normal">620</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">105</mml:mn></mml:mrow></mml:math></inline-formula> Tg yr<inline-formula><mml:math id="M395" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula> from a series of
flights around Britain in the summer of 2005 and September 2006. Using only
summer data, in order to emulate the temporal upscaling done by Polson, we
arrive at an annual <inline-formula><mml:math id="M396" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> budget of <inline-formula><mml:math id="M397" display="inline"><mml:mrow><mml:mn mathvariant="normal">511</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">308</mml:mn></mml:mrow></mml:math></inline-formula> Tg yr<inline-formula><mml:math id="M398" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>, which
agrees with the 2011 aircraft study within measurement uncertainty. Whilst
the seasonality of <inline-formula><mml:math id="M399" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> emissions cannot be disregarded, comparing our
summertime budgets with the aircraft study provides an independent
validation of the ferry mass balance approach and gives us confidence in the
method despite the simplifying assumptions that underpin it. Finally, we
compared the ferry-derived summertime estimates for the southern region,
filtered with a narrow 260–280<inline-formula><mml:math id="M400" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> wind direction window,
to the fluxes of <inline-formula><mml:math id="M401" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M402" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> obtained in 2012 by airborne
measurements in the greater London area (O'Shea et al., 2014). The ferry
fluxes of both gases (<inline-formula><mml:math id="M403" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>: <inline-formula><mml:math id="M404" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.049</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.020</mml:mn></mml:mrow></mml:math></inline-formula>;
<inline-formula><mml:math id="M405" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>: <inline-formula><mml:math id="M406" display="inline"><mml:mrow><mml:mn mathvariant="normal">24</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">15</mml:mn></mml:mrow></mml:math></inline-formula> Tg season<inline-formula><mml:math id="M407" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>) compared reasonably well with the
ones from the airborne campaign (<inline-formula><mml:math id="M408" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>: <inline-formula><mml:math id="M409" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.034</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.002</mml:mn></mml:mrow></mml:math></inline-formula>; <inline-formula><mml:math id="M410" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>: <inline-formula><mml:math id="M411" display="inline"><mml:mrow><mml:mn mathvariant="normal">13.4</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">1.2</mml:mn></mml:mrow></mml:math></inline-formula> Tg season<inline-formula><mml:math id="M412" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>), but clearly
also include sources upwind and downwind of the greater London area. The
uncertainty was large for both gases, which is unsurprising considering the
length of the averaging period (summers of 2015 and 2016), but this
comparison with another independent measurement further consolidates the
confidence in the method and in the overall annual budgets for <inline-formula><mml:math id="M413" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and
<inline-formula><mml:math id="M414" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>.</p>
</sec>
<sec id="Ch1.S5" sec-type="conclusions">
  <title>Conclusions</title>
      <p id="d1e6918">Applying a mass balance approach to continuous measurements of <inline-formula><mml:math id="M415" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and
<inline-formula><mml:math id="M416" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> in the outflow and using a ship of opportunity, we estimated the net
annual emissions of <inline-formula><mml:math id="M417" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> from the UK (excluding Scotland) and the
Republic of Ireland, averaged over the 2015–2017 period, to be <inline-formula><mml:math id="M418" display="inline"><mml:mrow><mml:mn mathvariant="normal">2.55</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.48</mml:mn></mml:mrow></mml:math></inline-formula> Tg, which is consistent with the combined 2.29 Tg reported to the
United Nations Framework Convention on Climate Change. The annual <inline-formula><mml:math id="M419" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>
budget obtained by mass balance (<inline-formula><mml:math id="M420" display="inline"><mml:mrow><mml:mn mathvariant="normal">881.0</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">125.8</mml:mn></mml:mrow></mml:math></inline-formula> Tg) was more than twice
the inventory value (422.7 Tg), but a direct comparison is not possible for
this gas because the atmospheric inventory only accounts for anthropogenic
sources (BEIS, 2016). Instead we compared our <inline-formula><mml:math id="M421" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> budget estimate with
previous airborne studies, one for the UK as a whole and the second one for
the greater London area, and found good agreement with both. The mass balance
approach presented here does not provide direct source apportionment
information, but the latitudinal emission patterns observed for both
<inline-formula><mml:math id="M422" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M423" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> were generally consistent with known spatial
distributions of sources and sinks. Assuming that the atmospheric emissions
inventory captures all anthropogenic emissions, we estimate that the net
biogenic component of the measured <inline-formula><mml:math id="M424" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> annual budget was 458.7 Tg,
which corresponds to 52 % of the total emissions. We detected marked
seasonality in the emissions of both gases with lower values in the summer,
and the seasonal budgets had statistically significant correlations with
natural gas and mean air temperature. We attribute the two-thirds decrease
in <inline-formula><mml:math id="M425" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> emissions between winter and summer for <inline-formula><mml:math id="M426" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> to the
superposition of the reduction in demand for fossil fuels and an increase in
the biogenic sink during the summer. For <inline-formula><mml:math id="M427" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, we attribute the seasonal
variability of the measured fluxes to natural gas consumption and to the
waste management sector for which temperature has been shown to control the
methane-oxidising potential of landfill cover soil and thereby the net
emissions. With this study, we validated the atmospheric emissions inventory
of <inline-formula><mml:math id="M428" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> for the UK (excluding Scotland) and Ireland, quantified the
biogenic component of the annual <inline-formula><mml:math id="M429" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> budget, and derived seasonal
emissions budgets for both gases. Finally, we demonstrated that <inline-formula><mml:math id="M430" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">CH</mml:mi><mml:mn mathvariant="normal">4</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>
emissions are strongly seasonal even at such a relatively large spatial
scale, which highlights the importance of taking meteorological drivers such
as air temperature into account in future bottom-up budgets.</p>
</sec>

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

      <p id="d1e7105">The datasets are currently in the process of being archived with the Centre for
Environmental Data Analysis (CEDA; <uri>http://www.ceda.ac.uk</uri>, last access: 7 March 2019). They will be accessible
from
<uri>http://catalogue.ceda.ac.uk/uuid/9a1295858ff14fc6acea73e356a8842c</uri> (GAUGE project team, 2015).</p>
  </notes><app-group>
        <supplementary-material position="anchor"><p id="d1e7114">The supplement related to this article is available online at: <inline-supplementary-material xlink:href="https://doi.org/10.5194/acp-19-3043-2019-supplement" xlink:title="pdf">https://doi.org/10.5194/acp-19-3043-2019-supplement</inline-supplementary-material>.</p></supplementary-material>
        </app-group><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d1e7123">CH led the data analysis and writing of the paper with
contributions from all co-authors. Furthermore, NM and MR provided the calibrated time series of gas concentrations measured
on the ship and at the Mace Head site, respectively. SO'D led the
“round robin” inter-calibration of analysers used within the wider GAUGE
project, and MV carried out the WRF modelling. Finally, PP and EN advised on methodology and data interpretation.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <?pagebreak page3059?><p id="d1e7129">The authors declare that they have no conflict of
interest.</p>
  </notes><notes notes-type="sistatement"><title>Special issue statement</title>

      <p id="d1e7135">This article is part of the special
issue “Greenhouse gAs Uk and Global Emissions (GAUGE) project (ACP/AMT
inter-journal SI)”. It is not associated with a conference.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e7142">The GAUGE project was funded by the UK Natural Environment Research Council
under grant reference NE/K002449/1. This
work was also supported by the Natural Environment Research
Council award number NE/R016429/1 as part of the UK-SCAPE programme delivering National
Capability.</p><p id="d1e7144">We are grateful to DFDS Seaways for authorising the research activities on
board the Rosyth–Zeebrugge
commercial ferry, and we thank the captains and
crews of the <italic>Longstone</italic> (now the <italic>Finnmerchant</italic>) and <italic>Finlandia Seaways</italic> for
access to the ships and for assistance with the day-to-day research
operations. We also acknowledge the contributions of Gerry Spain (NUIG),
Victor Kazan (LSCE), and Damien Martin (EPA, Ireland) for the maintenance of
the analysers at the Mace Head measurement station.
<?xmltex \hack{\newline}?><?xmltex \hack{\newline}?>
Edited by: Dominik Brunner<?xmltex \hack{\newline}?>
Reviewed by: two anonymous referees</p></ack><ref-list>
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    <!--<article-title-html>Country-scale greenhouse gas budgets using shipborne measurements: a case study for the UK and Ireland</article-title-html>
<abstract-html><p>We present a mass balance approach to estimate the seasonal and annual
budgets of carbon dioxide (CO<sub>2</sub>) and methane (CH<sub>4</sub>) of the United
Kingdom (excluding Scotland) and the Republic of Ireland from concentration
measurements taken on a ferry along the east coast of the United Kingdom over
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881.0±125.8&thinsp;Tg, with a net biogenic contribution of 458.7&thinsp;Tg (taken
as the difference between the estimated net emissions and the inventory
value,
which accounts for anthropogenic emissions only). The largest emissions for
both gases were observed in a broad latitudinal band (52.5–54°&thinsp;N), which coincides with densely populated areas. The
emissions of both gases were seasonal (maxima in winter and minima in
summer), strongly correlated with natural gas usage and, to a lesser extent,
also anti-correlated with mean air temperature. Methane emissions exhibited a
statistically significant anti-correlation with air temperature at the
seasonal timescale in the central region spanning 52.8–54.2°&thinsp;N, which hosts a relatively high density of waste treatment
facilities. Methane emissions from landfills have been shown to sometimes
increase with decreasing air temperature due to changes in the
CH<sub>4</sub>-oxidising potential of the topsoil, and we speculate that the waste
sector contributes significantly to the CH<sub>4</sub> budget of this central
region. This study brings independent verification of the emission budgets
estimated using alternative products (e.g. mass balance budgets by aircraft
measurements, inverse modelling, inventorying) and offers an opportunity to
investigate the seasonality of these emissions, which is usually not possible.</p></abstract-html>
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