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<!DOCTYPE article PUBLIC "-//NLM//DTD Journal Publishing with OASIS Tables v3.0 20080202//EN" "journalpub-oasis3.dtd">
<article xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:oasis="http://docs.oasis-open.org/ns/oasis-exchange/table" xml:lang="en" dtd-version="3.0" article-type="research-article"><?xmltex \bartext{Research article}?>
  <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-22-3891-2022</article-id><title-group><article-title>Assessing vehicle fuel efficiency using a dense network of CO<inline-formula><mml:math id="M1" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>
observations</article-title><alt-title>Assessing vehicle fuel efficiency using a dense network of CO<inline-formula><mml:math id="M2" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>
observations</alt-title>
      </title-group><?xmltex \runningtitle{Assessing vehicle fuel efficiency using a dense network of CO${}_{{2}}$
observations}?><?xmltex \runningauthor{H. L. Fitzmaurice et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Fitzmaurice</surname><given-names>Helen L.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Turner</surname><given-names>Alexander J.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-1406-7372</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Kim</surname><given-names>Jinsol</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Chan</surname><given-names>Katherine</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4">
          <name><surname>Delaria</surname><given-names>Erin R.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-6033-848X</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4">
          <name><surname>Newman</surname><given-names>Catherine</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff4">
          <name><surname>Wooldridge</surname><given-names>Paul</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="yes" rid="aff1 aff4">
          <name><surname>Cohen</surname><given-names>Ronald C.</given-names></name>
          <email>rccohen@berkeley.edu</email>
        <ext-link>https://orcid.org/0000-0001-6617-7691</ext-link></contrib>
        <aff id="aff1"><label>1</label><institution>Department of Earth and Planetary Science, University of California
Berkeley, <?xmltex \hack{\break}?>Berkeley, CA 94720, USA</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Department of Atmospheric Sciences, University of Washington, Seattle,
WA 98195, USA</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>Program Coordination Division, Sacramento Metro Air Quality Management District, <?xmltex \hack{\break}?>Sacramento, CA 95814,
USA</institution>
        </aff>
        <aff id="aff4"><label>4</label><institution>Department of Chemistry, University of California Berkeley, Berkeley, CA
94720, USA</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Ronald C. Cohen (rccohen@berkeley.edu)</corresp></author-notes><pub-date><day>24</day><month>March</month><year>2022</year></pub-date>
      
      <volume>22</volume>
      <issue>6</issue>
      <fpage>3891</fpage><lpage>3900</lpage>
      <history>
        <date date-type="received"><day>28</day><month>September</month><year>2021</year></date>
           <date date-type="rev-request"><day>5</day><month>October</month><year>2021</year></date>
           <date date-type="rev-recd"><day>23</day><month>January</month><year>2022</year></date>
           <date date-type="accepted"><day>10</day><month>February</month><year>2022</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2022 </copyright-statement>
        <copyright-year>2022</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="d1e188">Transportation represents the largest sector of anthropogenic
CO<inline-formula><mml:math id="M3" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions in urban areas in the United States. Timely reductions in
urban transportation emissions are critical to reaching climate goals set by
international treaties, national policies, and local governments.
Transportation emissions also remain one of the largest contributors to both
poor air quality (AQ) and to inequities in AQ exposure. As municipal and
regional governments create policy targeted at reducing transportation
emissions, the ability to evaluate the efficacy of such emission reduction
strategies at the spatial and temporal scales of neighborhoods is
increasingly important; however, the current state of the art in emissions
monitoring does not provide the temporal, sectoral, or spatial resolution
necessary to track changes in emissions and provide feedback on the efficacy
of such policies at the abovementioned scale. The BErkeley Air Quality and
CO<inline-formula><mml:math id="M4" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> Network (BEACO<inline-formula><mml:math id="M5" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N) has previously been shown to provide constraints on emissions from the vehicle sector in aggregate over a
<inline-formula><mml:math id="M6" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 1300 km<inline-formula><mml:math id="M7" display="inline"><mml:msup><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:math></inline-formula> multicity spatial domain. Here, we focus on a
5 km, high-volume, stretch of highway in the San Francisco Bay Area. We show that inversion of the BEACO<inline-formula><mml:math id="M8" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N measurements can be used to understand two
factors that affect fuel efficiency: vehicle speed and fleet composition.
The CO<inline-formula><mml:math id="M9" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emission rate of the average vehicle (in grams per vehicle kilometer) is shown to vary by as much as 27 % at different times of a typical weekday because of
changes in these two factors. The BEACO<inline-formula><mml:math id="M10" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N-derived emission estimates
are consistent to within <inline-formula><mml:math id="M11" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 3 % of estimates derived from
publicly available measures of vehicle type, number, and speed, providing
direct observational support for the accuracy of the EMission FACtor model (EMFAC) of vehicle fuel efficiency.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d1e278">Urban emissions currently account for <inline-formula><mml:math id="M12" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 75 % of all
anthropogenic CO<inline-formula><mml:math id="M13" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions  (Seto et al., 2014). By 2050,
roughly two-thirds of the Earth's projected population of 9.3 billion is
expected to reside within urban areas  (Seto et al., 2014), meaning
that effective greenhouse gas (GHG) emission reduction strategies must focus on urban emission reductions.</p>
      <p id="d1e297">The transportation sector is responsible for <inline-formula><mml:math id="M14" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 23 % of
global GHG emissions worldwide  (Seto et al., 2014) and
represents the greatest sectoral percentage (<inline-formula><mml:math id="M15" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula> 25 %–66 %) of
emissions from within the boundaries of urban areas in the United States
(City of Oakland, 2020; Gurney et al., 2021). Although the
fuel efficiency of new internal combustion engine vehicles has increased by
<inline-formula><mml:math id="M16" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 30 % over the last 20 years, and electric vehicles (EVs) are
becoming more prevalent (e.g., <uri>https://arb.ca.gov/emfac/emissions-inventory</uri>, last access: 12 January 2022),
emission reductions resulting from fuel efficiency gains in newer vehicles
are negated by an increasing percentage of heavy-duty vehicles (HDVs)
(Moua, 2020), speed-related reductions in fuel efficiency
resulting from increases in congestion, and an increase in the total vehicle
kilometers traveled. Over the past 20 years, even in locations with
aggressive climate change policies, these factors have resulted in CO<inline-formula><mml:math id="M17" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>
emissions from vehicles that have increased or stayed nearly constant. For
example, the California Air Resources Board estimates that per capita vehicle emissions in the state of
California in 2015 were only 2 % lower than
in 2000, and per capita vehicle kilometers traveled increased
<inline-formula><mml:math id="M18" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 2.5 % over that time period  (California Air
Resources Board, 2018). In addition to GHG emissions, the transportation
sector is responsible for a significant share of fine particulate matter (PM<inline-formula><mml:math id="M19" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula>) and NO<inline-formula><mml:math id="M20" display="inline"><mml:msub><mml:mi/><mml:mi>x</mml:mi></mml:msub></mml:math></inline-formula> emissions, exacerbating PM<inline-formula><mml:math id="M21" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula> and ozone exposure in BIPOC already experiencing disproportionate
health burdens associated with poor air quality
(Tessum et al., 2021).</p>
      <p id="d1e368">Municipal and regional governments have increasingly shown interest in
tracking and reducing CO<inline-formula><mml:math id="M22" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions from all sectors, including
transportation. For example, Boswell et al. (2019) found that
64 % of Californians live in a city with a climate action plan. For urban
and regional governments to plan, monitor, and responsively adjust emission
reduction policies, an up-to-date understanding of the spatial and temporal
variations in total emissions and in emissions by sector and subsector
processes is key.</p>
      <p id="d1e380">For transportation, reductions in vehicle kilometers, congestion mitigation, and rules
affecting fleet composition (e.g., limiting road access to HDVs,
incentivizing use of electric vehicles, or buy-backs of older vehicles) are
three levers that can be employed to reduce CO<inline-formula><mml:math id="M23" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> and AQ emissions from
vehicles, thereby affecting the climate footprint, air quality (AQ), and
environmental justice (EJ) in a region. However, the current state of the
art in emission monitoring and modeling do not provide the temporal,
sectoral, or spatial resolution necessary to track changes in urban
emissions and provide feedback on the efficacy of each lever separately.
Furthermore, current estimates of the magnitude and sectoral apportionment
of urban CO<inline-formula><mml:math id="M24" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions can vary widely. For example, Gurney et al. (2021) show how a consistent approach to total emissions from cities across
the United States differs from locally constructed inventories in magnitude and
sector by sector.</p>
      <p id="d1e402">Spatial and temporal process-level maps of emissions are needed to improve
the scientific basis for emission control strategies. The current state of
the art involves finding aggregate emissions over large regions (e.g., counties or
states) using economic data and then downscaling those totals using proxies such
as road length, building type, or population density. These models meet the
need for high spatial resolution (<inline-formula><mml:math id="M25" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula> 500 m) and capture
emissions from many detailed subsectors (Gately et
al., 2015; Gurney et al., 2012; McDonald et al., 2014). Because fuel sales
are well characterized, these models are also likely to produce accurate
region-wide CO<inline-formula><mml:math id="M26" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emission totals from the transportation sector.</p>
      <p id="d1e421">However, even the most detailed of these inventories do not presently describe
the temporal variability in processes that affect emissions, such as the
direct response of home heating or air conditioning to ambient temperature
or, with one exception  (Gately et
al., 2017), the variations in emissions per kilometer when comparing free-flowing
with stop-and-go traffic. These models often disagree with one another
spatially  (Gately and Hutyra,
2017), have been subject to only limited testing against observations of
the atmosphere, and are not designed to be consistent with separately
constructed AQ inventories that have been subject to much more extensive
testing against observations.</p>
      <p id="d1e424">Mobile monitoring campaigns and high-density measurement networks highlight
the importance of characterizing and identifying the processes contributing
to sharp neighborhood-scale AQ and GHG hot spots and point to the importance
of traffic emissions at neighborhood scales. For example, Apte et al. (2017) showed that concentrations of NO<inline-formula><mml:math id="M27" display="inline"><mml:msub><mml:mi/><mml:mi>x</mml:mi></mml:msub></mml:math></inline-formula> and black carbon (BC) can
vary by as much as a factor of <inline-formula><mml:math id="M28" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 8 on the scale of tens to hundreds
of meters. Caubel et al. (2019) showed BC concentrations to be
<inline-formula><mml:math id="M29" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 2.5 times higher on trucking routes than on neighboring
streets. Such gradients are not represented in inventories based on
downscaled economic data.</p>
      <p id="d1e450">Observations of CO<inline-formula><mml:math id="M30" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> and other GHGs can play an important
role in improving and maintaining the accuracy of emission
models – especially during a time of rapid proposed changes. CO<inline-formula><mml:math id="M31" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>
measurements paired with Bayesian inverse models have been shown to provide
a quantitative assessment of emissions
(Lauvaux
et al., 2016, 2020; Turner  et al., 2020a). To date, most
attempts at quantifying urban CO<inline-formula><mml:math id="M32" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions have focused on extracting
a temporally averaged (often a full year) total of the anthropogenic
CO<inline-formula><mml:math id="M33" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> across the full extent of city. A few studies have attempted to
disaggregate emissions by sector or fuel type or to describe large shifts in
aggregate emissions (Newman et al., 2016;
Nathan et al., 2018; Lauvaux et al., 2020; Turner et al., 2020a), but none
characterize the subsector processes of vehicle emissions.</p>
      <p id="d1e489">High-spatial-density observations offer promise as a means to explore
process-level emission details. The BErkeley Air Quality and CO<inline-formula><mml:math id="M34" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>
Network (BEACO<inline-formula><mml:math id="M35" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N) is an observing network deployed in the San Francisco
Bay Area and other cities with a measurement spacing of <inline-formula><mml:math id="M36" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 2 km
(Fig. 1, left). In a prior analysis, Turner et al. (2020a) showed that BEACO<inline-formula><mml:math id="M37" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N measurements
can detect variation in CO<inline-formula><mml:math id="M38" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions with time of the day and day of the week
in addition to the dramatic changes in CO<inline-formula><mml:math id="M39" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions due to the
COVID-related decrease in driving.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1" specific-use="star"><?xmltex \currentcnt{1}?><?xmltex \def\figurename{Figure}?><label>Figure 1</label><caption><p id="d1e548">The left panel presents a map of the BEACO<inline-formula><mml:math id="M40" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N network, showing all sites (blue dots)
for which there are more than 4 weeks of data during the period analyzed
(January to June from 2018 to 2020). Red stars indicate the location of the PeMS monitors used in
this study. The top right panel presents CO<inline-formula><mml:math id="M41" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> values shown for a “typical week” during the
time period observed. The dark line represents the median value observed across
all sites and times, and the shaded envelope represents <inline-formula><mml:math id="M42" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mi mathvariant="italic">σ</mml:mi></mml:mrow></mml:math></inline-formula> variance across the
network and over the 2-year period. The bottom right panel presents CO<inline-formula><mml:math id="M43" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions on
all highway pixels in the domain as derived from the inversion of
BEACO<inline-formula><mml:math id="M44" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N observations (blue), BEACO2N prior (black), and the
PeMS-EMFAC-based estimate (red). The shaded envelope shows variance in emissions
during the 18-month analysis window.</p></caption>
        <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://acp.copernicus.org/articles/22/3891/2022/acp-22-3891-2022-f01.png"/>

      </fig>

      <p id="d1e603">Here, we analyze hourly, spatially allocated CO<inline-formula><mml:math id="M45" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions derived from
the inversion of BEACO<inline-formula><mml:math id="M46" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N observations
(Turner et al., 2020a) to explore how well they
constrain the CO<inline-formula><mml:math id="M47" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions from a 5 km stretch of highway. This stretch was
chosen because of its location upwind of consistently active BEACO<inline-formula><mml:math id="M48" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N
sites, for completeness of traffic data, and because emission rates are
highly affected by speed (vehicles use more fuel per kilometer at very low and high
speeds) and fleet composition (HDVs emit more CO<inline-formula><mml:math id="M49" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> per kilometer than light-duty
vehicles, LDVs). The variation in the ratio of total fleet CO<inline-formula><mml:math id="M50" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions
per vehicle kilometer traveled (grams of CO<inline-formula><mml:math id="M51" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> per vehicle kilometer) is used to explore variations
in on-road fuel efficiency and the factors responsible for that variation.
We show that the average fuel efficiency of the vehicle fleet on the road varies
by as much as 27 % over the course of a typical weekday.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Methods and data</title>
<sec id="Ch1.S2.SS1">
  <label>2.1</label><?xmltex \opttitle{The Berkeley Air quality and CO${}_{{2}}$ Network}?><title>The Berkeley Air quality and CO<inline-formula><mml:math id="M52" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> Network</title>
      <p id="d1e695">We use hourly CO<inline-formula><mml:math id="M53" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> observations from the Berkeley Air quality and
CO<inline-formula><mml:math id="M54" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> Network (BEACO<inline-formula><mml:math id="M55" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N) (Shusterman et al., 2016; Kim et al., 2018;
Delaria et al., 2021). The BEACO<inline-formula><mml:math id="M56" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N network includes more than 70
locations in the San Francisco Bay Area, spaced at <inline-formula><mml:math id="M57" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 2 km, and measures
CO<inline-formula><mml:math id="M58" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> with a network instrument error of 1.6 ppm or less
(Delaria et al., 2021). All available data from January to June during the
2018–2020 period are included in this analysis. During this time, more than 50
distinct locations had nodes that were active for a month or more (including
19 sites within 10 km of our highway stretch of interest). The number of
nodes active at any given time ranged from 7 to 41, with a mean of 17. Figure 1
shows sites in operation at some point during analysis period, and Fig. S1 in the Supplement
shows a time series of the number of nodes available throughout the study
period.</p>
</sec>
<sec id="Ch1.S2.SS2">
  <label>2.2</label><?xmltex \opttitle{The BEACO${}_{{2}}$N Stochastic-Time Inverted Lagrangian Transport inversion system (BEACO${}_{{2}}$N-STILT)}?><title>The BEACO<inline-formula><mml:math id="M59" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N Stochastic-Time Inverted Lagrangian Transport inversion system (BEACO<inline-formula><mml:math id="M60" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N-STILT)</title>
      <p id="d1e778">To infer CO<inline-formula><mml:math id="M61" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions from within the BEACO<inline-formula><mml:math id="M62" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N footprint, we use
the Stochastic-Time Inverted Lagrangian Transport (STILT) model, coupled
with a Bayesian inversion as described in detail in Turner et al. (2020a).
Briefly, we use meteorology from the National Oceanic and Atmospheric Administration (NOAA) High-Resolution Rapid Refresh (HRRR) product at a 3 km resolution to
calculate footprints from each hour at each site, weighted by a priori
CO<inline-formula><mml:math id="M63" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions. The overall region of influence, the network footprint,
as defined by a contour representing 40 % of the CO<inline-formula><mml:math id="M64" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> influence, is
shown in Fig. S2 (left). We construct a spatially gridded prior emission
inventory using point sources provided by the Bay Area Air Quality
Management District (BAAQMD) (2015), home heating emissions as reported by BAAQMD (2011) and distributed spatially according to population density, on-road
emissions from the High-resolution Fuel Inventory for Vehicle Emissions
(McDonald et al., 2014) varying by hour of week and
scaled by year using fuel sales data, and a biogenic inventory derived using
solar-induced fluorescence (SIF) satellite data
(Turner et al., 2020b).</p>
      <p id="d1e817">To ensure a focus on highway emissions, we subtract prior estimates
associated with non-highway sources from posterior BEACO<inline-formula><mml:math id="M65" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N-STILT
fluxes. Non-highway sources are small (<inline-formula><mml:math id="M66" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula> 12 %) in comparison
with highway emissions for the pixels corresponding to the highway stretch
analyzed in this study (Fig. 2, left). We assume the error in prior
estimates of these sources to be an even smaller fraction of the total. For
reference, a diel cycle of sector-specific, weekday prior emissions for the
pixels analyzed in this study is shown in Fig. S3.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2" specific-use="star"><?xmltex \currentcnt{2}?><?xmltex \def\figurename{Figure}?><label>Figure 2</label><caption><p id="d1e838">The left panel shows the <inline-formula><mml:math id="M67" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 5 km stretch over which we analyze grams of CO<inline-formula><mml:math id="M68" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> per vehicle kilometer (vkm). Points show the location of PeMS stations, and squares show the pixels
associated with BEACO<inline-formula><mml:math id="M69" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N-STILT output that we use for comparison for the
5 km stretch. The top right panel presents the hourly average speed shown for two opposite (west
in red, and east in blue) PeMS measurement stations for a typical week. The middle right panel presents the PeMS-EMFAC-derived emission rates calculated for two opposite
(west in red, and east in blue) PeMS measurement stations for a typical week.
The bottom right panel presents the aggregate PeMS-EMFAC-derived estimated emission rates from
the two directions of traffic for a typical week for this highway stretch.</p></caption>
          <?xmltex \igopts{width=455.244094pt}?><graphic xlink:href="https://acp.copernicus.org/articles/22/3891/2022/acp-22-3891-2022-f02.png"/>

        </fig>

      <p id="d1e873">We estimate the BEACO<inline-formula><mml:math id="M70" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N-STILT inversion to be precise to at least
30 % for a line source. This estimate is based on the results of Turner et
al. (2016), who used observation system simulation experiments to demonstrate
that a 45 tC h<inline-formula><mml:math id="M71" 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> line source could be
constrained to 15 tC h<inline-formula><mml:math id="M72" 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> with 7 d of observations at 30 sites. However, this paper also demonstrated that error
in the posterior decreased as results were averaged over a longer period of
time. Here, as we are using 18 months (rather than 7 d) of observations, we
expect and observe better precision than 30 %.</p>
</sec>
<sec id="Ch1.S2.SS3">
  <label>2.3</label><?xmltex \opttitle{PeMS-EMFAC-derived CO${}_{{2}}$ emission estimates}?><title>PeMS-EMFAC-derived CO<inline-formula><mml:math id="M73" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emission estimates</title>
      <p id="d1e927">Total hourly vehicle flow, the HDV (truck) percentage, and speed were retrieved
from <uri>http://pems.dot.ca.gov</uri> (last access: 12 January 2022) for the period from January to June for the years from 2018 to 2020.
There are <inline-formula><mml:math id="M74" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 1800 traffic counting stations hosted by the
Caltrans Performance Measurement System (PeMS) in the San Francisco Bay Area, including
more than 400 sites (Fig. S2) within the 2020 footprint of the BEACO<inline-formula><mml:math id="M75" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N network,
as described in Turner et al. (2020a). These stations count vehicle flow
using magnetic loops imbedded in roadways and estimate the HDV fraction using
calculated vehicle speed and assumptions about vehicle length
(Kwon et al., 2003). For hours during which fewer than
50 % of measurements were reported, we fill in the total speed and light-duty
vehicle (LDV) flow gaps using linear fits to nearest-neighbor sites, and we fill in
gaps in the HDV flow using hour-of-day-specific and weekend/weekday-specific median
ratios between neighboring sites. Using this imputation method, we find that
mean absolute errors in speed are 5–10 km h<inline-formula><mml:math id="M76" 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>, mean absolute errors in the LDV flow are 500 vehicles per hour, and mean absolute errors in the HDV flow are 50 vehicles per hour (see Fig. S4).</p>
      <p id="d1e961">We calculate both LDV and HDV vehicle kilometers for each highway segment during each hour
using downloaded flow data at each sensor location and segment lengths
obtained from the PeMS database. For highway segments within the
BEACO<inline-formula><mml:math id="M77" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N footprint, vehicle kilometers are summed to obtain regional highway HDV and
LDV vehicle kilometers for every hour. Figure S2 (left) shows the extent of the PeMS
network in comparison to the BEACO<inline-formula><mml:math id="M78" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N-STILT footprint as well as the total
HDV vehicle kilometers and the total LDV vehicle kilometers.</p>
      <p id="d1e982">Vehicle fuel efficiency is dependent on both fleet composition and vehicle
speed. We calculate an emission rate at each location by combining the speed
and the HDV percentage with fuel efficiency estimates provided by the
California Air Resources Board EMission FACtor model (EMFAC2017). The
EMFAC2017 model provides yearly fuel efficiency estimates for the San Francisco Bay Area
for 41 vehicle classes as a function of speed. We group these 41 vehicle
types into the LDV or HDV categories (Table S1). The PeMS vehicle-type
classification system is length based, assuming that LDVs have a median
length of 3.7 m and HDVs have a median length of 18.3 m
(Kwon et al., 2003). As a result, we group most light-duty trucks into the LDV category. To find speed-dependent emission rate
values for the LDV and HDV groups, we find a vehicle-kilometer-weighted mean of emission
rates across all vehicle classes within a group at a given speed:
            <disp-formula id="Ch1.E1" content-type="numbered"><label>1</label><mml:math id="M79" display="block"><mml:mrow><mml:msub><mml:mi mathvariant="normal">er</mml:mi><mml:mrow><mml:mi mathvariant="normal">speed</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">group</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><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:mi>n</mml:mi></mml:msubsup><mml:msub><mml:mi mathvariant="normal">vkm</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">speed</mml:mi></mml:mrow></mml:msub><mml:msub><mml:mi mathvariant="normal">er</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">speed</mml:mi></mml:mrow></mml:msub></mml:mrow><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:mi>n</mml:mi></mml:msubsup><mml:msub><mml:mi mathvariant="normal">vkm</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">speed</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          where er denotes the total emission rate, <inline-formula><mml:math id="M80" display="inline"><mml:mi>i</mml:mi></mml:math></inline-formula> is a vehicle class, and vkm denotes vehicle kilometers. From this, we generate LDV and HDV emission rates at 8.02 km h<inline-formula><mml:math id="M81" 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> (5 mph) intervals (see Fig. S5). EMFAC does not provide
data for several LDV vehicle classes at and above 96.8 km h<inline-formula><mml:math id="M82" 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> (60 mph).
To fill this gap, we estimate emission rates for the LDV group by employing the
emission rate to speed slopes (grams of CO<inline-formula><mml:math id="M83" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> per vehicle kilometer per hour) for high
speeds (88–145 km h<inline-formula><mml:math id="M84" 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>), using data from
Davis et al. (2021).</p>
      <p id="d1e1117">We calculate emission rates (grams of CO<inline-formula><mml:math id="M85" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> per vehicle kilometer) for each (<inline-formula><mml:math id="M86" display="inline"><mml:mi mathvariant="italic">&lt;</mml:mi></mml:math></inline-formula> 1 km)
road segment between the PeMS sensors at a moment in time:
            <disp-formula id="Ch1.E2" content-type="numbered"><label>2</label><mml:math id="M87" display="block"><mml:mrow><mml:mi mathvariant="normal">er</mml:mi><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">seg</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mstyle scriptlevel="+1"><mml:mtable class="substack"><mml:mtr><mml:mtd><?xmltex \hack{\textstyle}?><mml:msub><mml:mi mathvariant="normal">vkm</mml:mi><mml:mi mathvariant="normal">LDV</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">seg</mml:mi><mml:mo>)</mml:mo><mml:msub><mml:mi mathvariant="normal">er</mml:mi><mml:mi mathvariant="normal">LDV</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">seg</mml:mi><mml:mo>)</mml:mo><mml:mo>+</mml:mo><mml:msub><mml:mi mathvariant="normal">vkm</mml:mi><mml:mi mathvariant="normal">tHDV</mml:mi></mml:msub></mml:mtd></mml:mtr><mml:mtr><mml:mtd><?xmltex \hack{\textstyle}?><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">seg</mml:mi><mml:mo>)</mml:mo><mml:msub><mml:mi mathvariant="normal">er</mml:mi><mml:mi mathvariant="normal">tHDV</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">seg</mml:mi><mml:mo>)</mml:mo></mml:mtd></mml:mtr></mml:mtable></mml:mstyle><mml:mrow><mml:msub><mml:mi mathvariant="normal">vkm</mml:mi><mml:mi mathvariant="normal">LDV</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">seg</mml:mi><mml:mo>)</mml:mo><mml:mo>+</mml:mo><mml:msub><mml:mi mathvariant="normal">vkm</mml:mi><mml:mi mathvariant="normal">HDV</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">seg</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:mfrac></mml:mstyle><mml:mo>,</mml:mo></mml:mrow></mml:math></disp-formula>
          where the emission rates for cars and trucks are found via a spline fit between the
reported speed for that segment and time with our curves for the emission
rates of each vehicle group. A fit is used rather than individual bins,
due to the sharp gradients that exist at low speeds for LDVs. From the
emission rate for each (<inline-formula><mml:math id="M88" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula> 1 km) segment, we calculate an
emission rate for a stretch of highway including several segments to find the
total emission rate (er) along a “stretch” over a period of time:
            <disp-formula id="Ch1.E3" content-type="numbered"><label>3</label><mml:math id="M89" display="block"><mml:mrow><mml:mi mathvariant="normal">er</mml:mi><mml:mfenced close=")" open="("><mml:mrow><mml:mi>t</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">stretch</mml:mi></mml:mrow></mml:mfenced><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mstyle scriptlevel="+1"><mml:mtable class="substack"><mml:mtr><mml:mtd><?xmltex \hack{\textstyle}?><mml:msub><mml:mo>∑</mml:mo><mml:mrow><mml:mi mathvariant="normal">all</mml:mi><mml:mspace linebreak="nobreak" width="0.25em"/><mml:mi mathvariant="normal">segments</mml:mi></mml:mrow></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="normal">vkm</mml:mi><mml:mi mathvariant="normal">LDV</mml:mi></mml:msub><mml:mo>)</mml:mo><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>,</mml:mo><mml:mi>s</mml:mi><mml:mo>)</mml:mo><mml:msub><mml:mi mathvariant="normal">er</mml:mi><mml:mi mathvariant="normal">LDV</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>,</mml:mo><mml:mi>s</mml:mi><mml:mo>)</mml:mo></mml:mtd></mml:mtr><mml:mtr><mml:mtd><?xmltex \hack{\textstyle}?><mml:mo>+</mml:mo><mml:msub><mml:mi mathvariant="normal">vkm</mml:mi><mml:mi mathvariant="normal">HDV</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">seg</mml:mi><mml:mo>)</mml:mo><mml:msub><mml:mi mathvariant="normal">er</mml:mi><mml:mi mathvariant="normal">HDV</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>,</mml:mo><mml:mi>s</mml:mi><mml:mo>)</mml:mo></mml:mtd></mml:mtr></mml:mtable></mml:mstyle><mml:mstyle scriptlevel="+1"><mml:mtable class="substack"><mml:mtr><mml:mtd><?xmltex \hack{\textstyle}?><mml:msub><mml:mo>∑</mml:mo><mml:mrow><mml:mi mathvariant="normal">all</mml:mi><mml:mspace linebreak="nobreak" width="0.25em"/><mml:mi mathvariant="normal">segments</mml:mi></mml:mrow></mml:msub><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="normal">vkm</mml:mi><mml:mi mathvariant="normal">LDV</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>,</mml:mo><mml:mi>s</mml:mi><mml:mo>)</mml:mo></mml:mtd></mml:mtr><mml:mtr><mml:mtd><?xmltex \hack{\textstyle}?><mml:mo>+</mml:mo><mml:msub><mml:mi mathvariant="normal">vkm</mml:mi><mml:mi mathvariant="normal">HDV</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>t</mml:mi><mml:mo>,</mml:mo><mml:mi>s</mml:mi><mml:mo>)</mml:mo><mml:mo>)</mml:mo></mml:mtd></mml:mtr></mml:mtable></mml:mstyle></mml:mfrac></mml:mstyle><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>
          The total CO<inline-formula><mml:math id="M90" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emission rates for the highway stretch analyzed in this work
are shown in Fig. 2 (bottom right).</p>
</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Results</title>
      <p id="d1e1452">To gain insight into the relative impacts of congestion and fleet
composition, we first calculate fleet-wide vehicle emission rates (in grams of CO<inline-formula><mml:math id="M91" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> per vehicle kilometer)
using two different methods. For both methods, the Caltrans Performance
Measurement System (PeMS; <uri>http://pems.dot.ca.gov</uri>, last access: 12 January 2022) provides vehicle counts, speed, and vehicle category (HDVs
or LDVs). Using these data and estimates of fuel consumption per
kilometer from the EMission FACtor 2017 (EMFAC) model, we calculate the CO<inline-formula><mml:math id="M92" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions per kilometer for the average vehicle with an hourly time resolution, as
described above. Second, we use the PeMS data in combination with the grams of CO<inline-formula><mml:math id="M93" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>
per unit area derived from the BEACO<inline-formula><mml:math id="M94" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N-STILT inversion system. We focus
on the <inline-formula><mml:math id="M95" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 5 km stretch of Interstate 80 just north of the San
Francisco–Oakland Bay Bridge (Fig. 2). Interstate 80 is an east–west Highway
whose orientation along this stretch is mainly north–south, with eastbound
lanes traveling north and westbound lanes traveling south. The road has five
lanes in each direction and is often subject to high congestion (vehicles
traveling slower than the posted speed).</p>
      <p id="d1e1502">PeMS-EMFAC-derived emission rates give us insight into (1) the expected
variation in emission rates across a typical day (Fig. 2) and (2) the
relative impacts of congestion vs. the HDV percentage as factors leading to this
variation (Fig. S6). For example, while the westbound segment experiences
speeds significantly below free-flow during both morning and evening rush
hours, the eastbound segment experiences significant congestion only during
the evening. Because of a steep gradient in LDV emission rates between 20
and 50 km h<inline-formula><mml:math id="M96" 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> (Fig. S5), the westbound congestion in this segment
occurs at speeds that are more fuel efficient than free flow. The overall
variance in emission rates over the whole stretch is significantly smaller
than in either of the directions shown individually.</p>
      <p id="d1e1517">From PeMS-EMFAC-derived emission factors, we predict a median diel cycle
with the emissions per kilometer traveled ranging from <inline-formula><mml:math id="M97" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 247 to
<inline-formula><mml:math id="M98" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 314 g CO<inline-formula><mml:math id="M99" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> per vehicle kilometer. For reference, if all vehicles were
driving at the speed limit of 104.6 km h<inline-formula><mml:math id="M100" 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> (65 mph) and the fleet mix
was 6 % HDVs and 94 % LDVs, we calculate an emission rate of 265 g CO<inline-formula><mml:math id="M101" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> per vehicle kilometer. The range of predicted emissions is narrower on the weekend
(238–276 g CO<inline-formula><mml:math id="M102" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> per vehicle kilometer), as fewer HDVs use the road and there is a smaller range with respect to speed.</p>
      <p id="d1e1574">Figure S6 shows the hourly variation in the relative contributions of LDV
speed, HDV percentage, and HDV speed to the deviation in grams of CO<inline-formula><mml:math id="M103" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> per vehicle kilometer
from the reference value of 265 g CO<inline-formula><mml:math id="M104" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> per vehicle kilometer. The solid line is the mean,
and the shaded envelope represents the day-to-day variance. In the morning
and at midday, the HDV percentage and LDV speed have opposite impacts on the grams of CO<inline-formula><mml:math id="M105" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> per vehicle kilometer, leading to small variations in the grams of CO<inline-formula><mml:math id="M106" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> per vehicle kilometer over the day,
despite substantial variations in the separate effects of speed and HDV percentage. During evening rush hour, low vehicle speeds result in higher emission
rates, leading to large positive deviations. High day-to-day variance in
vehicle speed contributes to high day-to-day variance in emission rates. At
times near midnight, large, positive deviations are observed, mostly as a
consequence of a high HDV percentage but also because traffic flows at rates
higher than 104.6 km h<inline-formula><mml:math id="M107" 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>, leading to higher emission rates. Night-to-night
variance in the HDV percentage is low; thus, variance in the nighttime predicted grams of CO<inline-formula><mml:math id="M108" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> per vehicle kilometer is small. The HDV speed has little impact on the grams of CO<inline-formula><mml:math id="M109" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> per vehicle kilometer.</p>
      <p id="d1e1645">We use CO<inline-formula><mml:math id="M110" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> measurements from 50 BEACO<inline-formula><mml:math id="M111" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N sites across the San Francisco Bay Area
combined with the BEACO<inline-formula><mml:math id="M112" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N-STILT inversion system to assess highway
emissions from our stretch of interest. In Fig. 1, we show the location of
BEACO<inline-formula><mml:math id="M113" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N sites, the stretch of interest, and emission estimates for
this stretch. Note that the posterior emissions move substantially from
prior emissions towards what is estimated from PeMS-EMFAC, particularly
during the evening rush hour, when the prior overestimates emissions by
<inline-formula><mml:math id="M114" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 20 %.</p>
      <p id="d1e1691">We compare BEACO<inline-formula><mml:math id="M115" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N-derived and PeMS-EMFAC-derived emission rates
(grams CO<inline-formula><mml:math id="M116" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> per vehicle kilometer) and find remarkable agreement. The PeMS-EMFAC-derived emission rates range from 225 to 300 g CO<inline-formula><mml:math id="M117" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> per vehicle kilometer and include the effects of
both fleet composition and variation in speed. For BEACO<inline-formula><mml:math id="M118" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N, we use the
total CO<inline-formula><mml:math id="M119" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions from the inversion at times corresponding to narrow
bins of PeMS-EMFAC (grams of CO<inline-formula><mml:math id="M120" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> per vehicle kilometer). Figure 3a shows an example of
data selected at times with PeMS-EMFAC-derived fuel efficiency in the
range of 271.4 to 279 g CO<inline-formula><mml:math id="M121" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> per vehicle kilometer. There is a range of emissions at each vehicle kilometer because of noise in the inversion, variation in speed, and variation in the
fleet composition. The slope of a fit to the data in Fig. 3a is an
estimate of the emission rate (Eq. 4), where CO<inline-formula><mml:math id="M122" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions are defined as hourly emissions
summed over BEACO<inline-formula><mml:math id="M123" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N pixels corresponding to our highway stretch of
interest (Fig. 2):
          <disp-formula id="Ch1.E4" content-type="numbered"><label>4</label><mml:math id="M124" display="block"><mml:mrow><mml:mi mathvariant="normal">er</mml:mi><mml:mfenced open="(" close=")"><mml:mrow><mml:mi mathvariant="normal">g</mml:mi><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msub><mml:mi mathvariant="normal">CO</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msup><mml:mi mathvariant="normal">vkm</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:mfenced><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msub><mml:mrow class="chem"><mml:mi mathvariant="normal">CO</mml:mi></mml:mrow><mml:mn mathvariant="normal">2</mml:mn></mml:msub><mml:mspace linebreak="nobreak" width="0.125em"/><mml:mi mathvariant="normal">emissons</mml:mi></mml:mrow><mml:mi mathvariant="normal">vkm</mml:mi></mml:mfrac></mml:mstyle><mml:mo>.</mml:mo></mml:mrow></mml:math></disp-formula>
        Using 18 months of data for weekdays between 04:00 and 22:00 local time, we compare PeMS-EMFAC-derived and BEACO<inline-formula><mml:math id="M125" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N-derived CO<inline-formula><mml:math id="M126" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> per vehicle kilometer (Fig. 3b).
These hours were chosen, because they represent the hours for which we
expect traffic emissions to be substantially larger than emissions from
other sources in our area of interest (see Fig. S3). When fitting to a line
forced through the origin, emission rates found via the BEACO<inline-formula><mml:math id="M127" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N
inversion are within 3 % (<inline-formula><mml:math id="M128" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.97</mml:mn><mml:mo>±</mml:mo><mml:mn mathvariant="normal">0.01</mml:mn></mml:mrow></mml:math></inline-formula>) of those predicted using
PeMS-EMFAC traffic counts. A more complete description of this fitting and
error calculation process can be found in Sect. S8, and a comparison to the
results from applying this method to the prior can be found in Sect. S9. Using the
definition of the limit of detection as 3 times our uncertainty, we
calculate that we would be able to detect an 11 % change in individual
points (representing bins of fuel efficiency from a combination of HDV
percentage and speed) and a 3 % change in the slope. Because 18 months of
data was required to reach this level of certainty, if we assume the
2.3 %–3.8 % yr<inline-formula><mml:math id="M129" 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> decrease in the emission rate found by Kim et al. (2021), we
should be able to detect a change in the overall fuel efficiency with 3 full
years of BEACO<inline-formula><mml:math id="M130" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N-STILT output.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3" specific-use="star"><?xmltex \currentcnt{3}?><?xmltex \def\figurename{Figure}?><label>Figure 3</label><caption><p id="d1e1884"><bold>(a)</bold> BEACO<inline-formula><mml:math id="M131" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N-derived emissions vs. vehicle kilometers (vkm) for times
corresponding to modeled emission rates of 271.4–279 g CO<inline-formula><mml:math id="M132" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> per vehicle kilometer. Red
points represent binned medians used in fitting. <bold>(b)</bold> BEACO<inline-formula><mml:math id="M133" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N-derived
vs. PeMS-EMFAC-derived emission rates with the uncertainty estimate. The black line
shows the fit weighted by variance: <inline-formula><mml:math id="M134" display="inline"><mml:mrow><mml:mi>y</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.97</mml:mn><mml:mo>(</mml:mo><mml:mn>.01</mml:mn><mml:mo>)</mml:mo><mml:mi>x</mml:mi></mml:mrow></mml:math></inline-formula>. The gray envelope is the 5 %
deviation from fit, and the red line represents the <inline-formula><mml:math id="M135" display="inline"><mml:mrow><mml:mn mathvariant="normal">1</mml:mn><mml:mo>:</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:math></inline-formula> line.</p></caption>
        <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://acp.copernicus.org/articles/22/3891/2022/acp-22-3891-2022-f03.png"/>

      </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4"><?xmltex \currentcnt{4}?><?xmltex \def\figurename{Figure}?><label>Figure 4</label><caption><p id="d1e1960"><bold>(a)</bold> Emission rates by time of day on weekdays for PeMS-derived
(red), BEACO2N prior (blue), and BEACO<inline-formula><mml:math id="M136" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N posterior (green) data. Probability density functions of the HDV (truck) fraction <bold>(b)</bold> and speed <bold>(c)</bold>
from a weekday morning (05:00–09:00) and evening (16:00–20:00) rush hour period on the
segment of Interstate 80 analyzed in Sect. 3. The <inline-formula><mml:math id="M137" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> axis represents the
relative probability of the HDV fraction <bold>(b)</bold> or averaged hourly speed
<bold>(c)</bold>. Speeds are from individual PeMS sensors, whereas the HDV fraction is
aggregated over the whole stretch under consideration (both directions).</p></caption>
        <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://acp.copernicus.org/articles/22/3891/2022/acp-22-3891-2022-f04.png"/>

      </fig>

      <p id="d1e2000">We also consider how emission rates compare throughout the day (Fig. 4a). During the evening, PeMS-EMFAC-derived and BEACO<inline-formula><mml:math id="M138" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N-derived
emission rates are in good agreement. The BEACO<inline-formula><mml:math id="M139" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N grams of CO<inline-formula><mml:math id="M140" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> per vehicle kilometer
increases from 256 g CO<inline-formula><mml:math id="M141" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> per vehicle kilometer before rush hour (14:00) to 324 g CO<inline-formula><mml:math id="M142" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> per vehicle kilometer during peak rush hour (17:00). Likewise, the PeMS-EMFAC-derived
CO<inline-formula><mml:math id="M143" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> per vehicle kilometer increases from 256  to 320 CO<inline-formula><mml:math id="M144" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> per vehicle kilometer over
the same time period. The BEACO<inline-formula><mml:math id="M145" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N prior has a slightly larger increase
in the emission rate over this period (256 g CO<inline-formula><mml:math id="M146" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> per vehicle kilometer at 14:00 to 361 g CO<inline-formula><mml:math id="M147" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> per vehicle kilometer at 17:00). In contrast, during the morning rush hours, we see
less agreement between PeMS-EMFAC-derived and BEACO<inline-formula><mml:math id="M148" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N-derived emission
rate estimates. The BEACO<inline-formula><mml:math id="M149" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N inversion is similar to the PeMS-EMFAC
estimate at 05:00 local time (280 g CO<inline-formula><mml:math id="M150" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> per vehicle kilometer), and the BEACO2N
estimate then increases over the morning rush hour to 330 g CO<inline-formula><mml:math id="M151" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> per vehicle kilometer at 8:00. This behavior is different from both the BEACO<inline-formula><mml:math id="M152" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N prior (175 g CO<inline-formula><mml:math id="M153" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> per vehicle kilometer at 05:00 and 275 g CO<inline-formula><mml:math id="M154" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> per vehicle kilometer at 08:00) and the PeMS-EMFAC calculation which decreases over this
period (275 g CO<inline-formula><mml:math id="M155" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> per vehicle kilometer at 05:00 and 250 g CO<inline-formula><mml:math id="M156" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> per vehicle kilometer at 08:00).</p>
      <p id="d1e2178">The discrepancy in the morning between emissions derived from PeMS-EMFAC and
BEACO<inline-formula><mml:math id="M157" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N can potentially be reconciled by congestion. There is a
nonlinear relationship between vehicle speed and the rate of emissions. As
such, congestion involving nonconstant speeds can result in higher
emissions than would be estimated using the average vehicle speed. This can
be seen from a simple example. Consider two cases: (1) an LDV traveling at a
constant 50 km h<inline-formula><mml:math id="M158" 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> for 1 h and (2) an LDV traveling at 100 km h<inline-formula><mml:math id="M159" 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> for 20 min and at 25 km h<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> for 40 min. Both vehicles
travel 50 km in 1 h and, therefore, have the same average speed; however,
the emission rate is 461.5 g CO<inline-formula><mml:math id="M161" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> per vehicle kilometer at 25 km h<inline-formula><mml:math id="M162" 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>, 195 g CO<inline-formula><mml:math id="M163" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> per vehicle kilometer at 50 km h<inline-formula><mml:math id="M164" 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>, and 221 g CO<inline-formula><mml:math id="M165" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> per vehicle kilometer at 100 km h<inline-formula><mml:math id="M166" 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>.
Using these emission rates, the vehicle in the first case would emit 9.75 kg of CO<inline-formula><mml:math id="M167" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>, whereas the vehicle with the variable speed in the second case
would emit 15 kg of CO<inline-formula><mml:math id="M168" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>.</p>
      <p id="d1e2309">Contrasting the speeds (Fig. 4c) during these two periods, we
see that while both show a bimodal speed distribution, a greater fraction
of morning speeds fall into the 40–100 km h<inline-formula><mml:math id="M169" 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> range, whereas a greater fraction
of evening speeds are <inline-formula><mml:math id="M170" display="inline"><mml:mi mathvariant="italic">&lt;</mml:mi></mml:math></inline-formula> 40  or <inline-formula><mml:math id="M171" display="inline"><mml:mi mathvariant="italic">&gt;</mml:mi></mml:math></inline-formula> 100 km h<inline-formula><mml:math id="M172" 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>. In Fig. S8, we show that emission rate estimates based on hourly
averaged speeds between 0 and 40 km h<inline-formula><mml:math id="M173" 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> and between 100 and 140 km h<inline-formula><mml:math id="M174" 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> (more
common in evening rush hour) are likely an upper bound on possible emission rates corresponding to those hourly averaged speeds, whereas emission rate
estimates based on hourly averaged speeds between 40 and 100 km h<inline-formula><mml:math id="M175" 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> (more
common in morning rush hour) likely represent a lower bound of emissions.
The predicted range in the emission rate, resulting from nonconstant speeds
combined with a larger HDV percentage, in the morning (Fig. 4c) is
large enough to explain the mismatch observed during the morning rush hour.</p>
</sec>
<sec id="Ch1.S4">
  <label>4</label><title>Discussion</title>
      <p id="d1e2395">The strategic reduction of emissions from transportation is important for both
reducing total GHG emissions and improving AQ. To make informed decisions
that reduce GHGs and exposure to poor AQ, policy makers need to know (1) how
much is being emitted, (2) the location and timing of emissions, and (3) the
relative impact of various subsector processes (e.g., vehicle kilometers and fleet composition).</p>
      <p id="d1e2398">To effectively capture emissions from subsector processes, models are also
reliant on emission factor models, such as the EMFAC2017 model used in this paper. While our BEACO<inline-formula><mml:math id="M176" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N-STILT-based estimates largely
agree with EMFAC2017 with respect to CO<inline-formula><mml:math id="M177" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>, tracking on-road
changes in emission factors will be especially important as the impacts of
congestion and fleet composition evolve rapidly, making timely updates
essential to creating spatially accurate inventories. For example, the EMFAC
model predicts an 18 % decrease in overall CO<inline-formula><mml:math id="M178" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emission rates by
2030, resulting from the improved fuel efficiency of combustion engine
vehicles and a transition to hybrid vehicles and EVs (<inline-formula><mml:math id="M179" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula> 6.8 % of LDV vehicle kilometers and <inline-formula><mml:math id="M180" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 6 % of HDV vehicle kilometers are expected to be traveled by EVs
by 2030). While the increased share of hybrid vehicles and EVs should work to decrease
the impact of congestion, a projected increase in total congestion and the
congested vehicle kilometer share by HDVs (Texas A&amp;M Transportation Institute,
2019) is likely to work against that trend, making the overall result
difficult to predict.</p>
      <p id="d1e2442">To our knowledge, this paper represents the first demonstration that a
high-density atmospheric observing network can both diagnose and quantify the
relative contributions of subsector processes at the neighborhood scale. We
demonstrate that the BEACO<inline-formula><mml:math id="M181" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N network (<inline-formula><mml:math id="M182" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula> 2 km spacing) of
low-cost CO<inline-formula><mml:math id="M183" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> sensors can be used to quantify emission rates at a
specific location (a <inline-formula><mml:math id="M184" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 5 km stretch) and by time of day. We show
that, on the highway stretch examined, activity-based emission estimates that account
for speed and HDV percentage match the inference from atmospheric measurements to
within 3 %. Finally, we demonstrate that the BEACO<inline-formula><mml:math id="M185" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N-STILT system
detects daily changes in fuel efficiency that range from 200 to 300 g CO<inline-formula><mml:math id="M186" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> per vehicle kilometer and that this system would be capable of detecting fleet-wide changes in
fuel efficiency in <inline-formula><mml:math id="M187" display="inline"><mml:mo>∼</mml:mo></mml:math></inline-formula> 3 years.</p>
</sec>
<sec id="Ch1.S5" sec-type="conclusions">
  <label>5</label><title>Outlook</title>
      <p id="d1e2512">In this work, we have demonstrated that the BEACO<inline-formula><mml:math id="M188" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N-STILT system was
able to infer emission rates from vehicles along a specific stretch of
highway. To understand the extent to which this method can be applied to
other contexts, future work should investigate the extent to which various
elements of the BEACO<inline-formula><mml:math id="M189" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N-STILT system, including measurement density,
error in meteorology used to calculate STILT trajectories, and the quality
of the prior, impact the ability of similar systems to estimate emissions.</p>
      <p id="d1e2533">For example, it is possible that the mismatch that we observe during the morning
rush hour may be due to a larger relative meteorological model error in
the morning compared with the afternoon and early evening, during which time the
boundary layer is relatively well mixed. Because a highly mixed boundary
layer is important for minimizing discrepancies between particle
trajectories in the STILT model and real transport (Lin et al., 2003),
inversions typically use only measurements taken during the afternoon,
(Lauvaux et al., 2016, 2020; Nathan et al., 2019) when the
boundary layer is relatively well mixed. However, as discussed by Martin et
al. (2019), the impacts of meteorological mismatch during the morning may be
offset by a stronger signal, and future work should explore the extent to
which averaging results over long time periods or strategic filtering of
meteorological mismatches can combat emission error.</p>
      <p id="d1e2536">Beyond further exploration of the elements influencing the sensitivity and
precision of the BEACO<inline-formula><mml:math id="M190" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N-STILT system, because each BEACO<inline-formula><mml:math id="M191" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula>N node
measures CO, NO<inline-formula><mml:math id="M192" display="inline"><mml:msub><mml:mi/><mml:mi>x</mml:mi></mml:msub></mml:math></inline-formula>, and PM<inline-formula><mml:math id="M193" display="inline"><mml:msub><mml:mi/><mml:mrow><mml:mn mathvariant="normal">2.5</mml:mn><mml:mspace width="0.125em" linebreak="nobreak"/></mml:mrow></mml:msub></mml:math></inline-formula>in addition to CO<inline-formula><mml:math id="M194" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> (Kim et al.,
2018), the method presented in this paper has the potential to shed light on subsector processes impacting the emission factors of these co-emitted species.
This is salient because plume-based emission factor measurements of
co-emitted pollutants show that various emission factor models systematically
underestimate emissions  (Bishop, 2021), fail to capture
spatial heterogeneity in these factors due to fleet composition (age and
compliance with control technologies) for PM (Haugen
et al., 2018; Park, et al., 2016) and black carbon
(Preble et al., 2018), or fail to capture
the impact of temperature on emission factors.</p>
      <p id="d1e2586">Applying these methods across a broader spatial area and to other species
(e.g., PM<inline-formula><mml:math id="M195" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2.5</mml:mn></mml:msub></mml:math></inline-formula>, NO<inline-formula><mml:math id="M196" display="inline"><mml:msub><mml:mi/><mml:mi>x</mml:mi></mml:msub></mml:math></inline-formula>, and CO) should yield information of interest to both
scientists and policy makers by</p>
      <p id="d1e2608"><list list-type="order">
          <list-item>

      <p id="d1e2613">revealing spatial and temporal trends in emission rates and emission factors
across an urban area and quantifying the contributions of congestion, fleet
composition, or other factors to spatial variations;</p>
          </list-item>
          <list-item>

      <p id="d1e2619">identifying and diagnosing the causes of traffic-related AQ hot spots that
contribute to exposure inequities;</p>
          </list-item>
          <list-item>

      <p id="d1e2625">tracking trends in the above over periods of years to decades.</p>
          </list-item>
        </list></p>
</sec>

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

      <p id="d1e2634">The CO<inline-formula><mml:math id="M197" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> data used for this study are publicly
available at <uri>http://beacon.berkeley.edu</uri> (Cohen Research – University of California Berkeley, 2022). Raw data can
be provided upon request. The traffic data used for this study are publicly
available at <uri>https://pems.dot.ca.gov/</uri> (California Department of Transportation, 2022).</p>
  </notes><app-group>
        <supplementary-material position="anchor"><p id="d1e2652">The supplement related to this article is available online at: <inline-supplementary-material xlink:href="https://doi.org/10.5194/acp-22-3891-2022-supplement" xlink:title="pdf">https://doi.org/10.5194/acp-22-3891-2022-supplement</inline-supplementary-material>.</p></supplementary-material>
        </app-group><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d1e2661">HLF derived the CO<inline-formula><mml:math id="M198" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> emissions from traffic data, conceived the idea for the project
design, wrote the paper, and collected CO<inline-formula><mml:math id="M199" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> data. AJT created and ran the
CO<inline-formula><mml:math id="M200" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> inversion code. HLF, JK, KC, ERD, CN, and PW collected CO<inline-formula><mml:math id="M201" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">2</mml:mn></mml:msub></mml:math></inline-formula> data.
RCC gave feedback on the project design and assisted with writing the paper.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d1e2703">The contact author has declared that neither they nor their co-authors have any competing interests.</p>
  </notes><?xmltex \hack{\newpage}?><notes notes-type="disclaimer"><title>Disclaimer</title>

      <p id="d1e2710">Publisher’s note: Copernicus Publications remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e2716">The authors are grateful to Kristin Lauter and the MSR Urban Innovation group for
support with thinking through PeMS data acquisition. This research used the Savio
computational cluster resource provided by the Berkeley Research Computing
program at UC Berkeley (supported by the UC
Berkeley Chancellor, Vice Chancellor for Research, and Chief Information
Officer). The authors wish to acknowledge  Hannah S. Kenagy for reading through and offering organizational
suggestions on the manuscript.</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d1e2721">This research has been supported by the NSF, the Adolph C. and Mary Sprague Miller Institute for Basic Research in Science, UC Berkeley, and the Koret Foundation.</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d1e2727">This paper was edited by Christoph Gerbig and reviewed by two anonymous referees.</p>
  </notes><ref-list>
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