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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-18-8373-2018</article-id><title-group><article-title>Maximizing ozone signals among chemical, meteorological,<?xmltex \hack{\newline}?> and climatological
variability</article-title><alt-title>Maximizing ozone signals</alt-title>
      </title-group><?xmltex \runningtitle{Maximizing ozone signals}?><?xmltex \runningauthor{B. Brown-Steiner et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1 aff2 aff7">
          <name><surname>Brown-Steiner</surname><given-names>Benjamin</given-names></name>
          <email>bbrownst@aer.com</email>
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2 aff4 aff5">
          <name><surname>Selin</surname><given-names>Noelle E.</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-6396-5622</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2 aff5">
          <name><surname>Prinn</surname><given-names>Ronald G.</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1 aff2">
          <name><surname>Monier</surname><given-names>Erwan</given-names></name>
          
        <ext-link>https://orcid.org/0000-0001-5533-6570</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff6">
          <name><surname>Tilmes</surname><given-names>Simone</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-6557-3569</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff6">
          <name><surname>Emmons</surname><given-names>Louisa</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-2325-6212</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3">
          <name><surname>Garcia-Menendez</surname><given-names>Fernando</given-names></name>
          
        <ext-link>https://orcid.org/0000-0003-0235-5692</ext-link></contrib>
        <aff id="aff1"><label>1</label><institution>Center for Global Change Science, Massachusetts Institute of Technology, 77 Massachusetts Ave, Cambridge, <?xmltex \hack{\newline}?> MA 02139, USA</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Joint Program on the Science and Policy of Global Change, Massachusetts Institute of Technology, 77 Massachusetts Ave, Cambridge, MA 02139, USA</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>Department of Civil, Construction, and Environmental Engineering, North Carolina State University, Raleigh,<?xmltex \hack{\newline}?>  NC 27695, USA</institution>
        </aff>
        <aff id="aff4"><label>4</label><institution>Institute for Data, Systems, and Society, Massachusetts Institute of Technology, 77 Massachusetts Ave, Cambridge,<?xmltex \hack{\newline}?>  MA 02139, USA</institution>
        </aff>
        <aff id="aff5"><label>5</label><institution>Department of Earth, Atmospheric, and Planetary Sciences, Massachusetts Institute of Technology, 77 Massachusetts Ave, Cambridge, MA 02139, USA</institution>
        </aff>
        <aff id="aff6"><label>6</label><institution>Atmospheric Chemistry Observations and Modeling Lab, National Center for Atmospheric Research, 3450 Mitchell Lane, Boulder, CO 80301, USA</institution>
        </aff>
        <aff id="aff7"><label>a</label><institution>now at: Atmospheric and Environmental Research, 131 Hartwell Avenue, Lexington, MA 02421, USA</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Benjamin Brown-Steiner (bbrownst@aer.com)</corresp></author-notes><pub-date><day>15</day><month>June</month><year>2018</year></pub-date>
      
      <volume>18</volume>
      <issue>11</issue>
      <fpage>8373</fpage><lpage>8388</lpage>
      <history>
        <date date-type="received"><day>12</day><month>October</month><year>2017</year></date>
           <date date-type="rev-request"><day>28</day><month>November</month><year>2017</year></date>
           <date date-type="rev-recd"><day>19</day><month>May</month><year>2018</year></date>
           <date date-type="accepted"><day>26</day><month>May</month><year>2018</year></date>
      </history>
      <permissions>
        
        
      <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>
    <p id="d1e184">The detection of meteorological, chemical, or other signals in modeled or
observed air quality data – such as an estimate of a temporal trend in
surface ozone data, or an estimate of the mean ozone of a particular region
during a particular season – is a critical component of modern atmospheric
chemistry. However, the magnitude of a surface air quality signal is
generally small compared to the magnitude of the underlying chemical,
meteorological, and climatological variabilities (and their interactions)
that exist both in space and in time, and which include variability in
emissions and surface processes. This can present difficulties for both
policymakers and researchers as they attempt to identify the influence or
signal of climate trends (e.g., any pauses in warming trends), the impact
of enacted emission reductions policies (e.g., United States
<inline-formula><mml:math id="M1" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> State Implementation Plans), or an estimate of the mean
state of highly variable data (e.g., summertime ozone over the northeastern
United States). Here we examine the scale dependence of the variability of
simulated and observed surface ozone data within the United States and the
likelihood that a particular choice of temporal or spatial averaging scales
produce a misleading estimate of a particular ozone signal. Our main
objective is to develop strategies that reduce the likelihood of
overconfidence in simulated ozone estimates. We find that while increasing
the extent of both temporal and spatial averaging can enhance signal
detection capabilities by reducing the noise from variability, a
strategic combination of particular temporal and spatial averaging scales can
maximize signal detection capabilities over much of the continental US. For
signals that are large compared to the meteorological variability (e.g.,
strong emissions reductions), shorter averaging periods and smaller spatial
averaging regions may be sufficient, but for many signals that are smaller
than or comparable in magnitude to the underlying meteorological variability,
we recommend temporal averaging of 10–15 years combined with some level of
spatial averaging (up to several hundred kilometers). If this level of
averaging is not practical (e.g., the signal being examined is at a local
scale), we recommend some exploration of the spatial and temporal variability
to provide context and confidence in the robustness of the<?pagebreak page8374?> result. These
results are consistent between simulated and observed data, as well as within a
single model with different sets of parameters. The strategies selected in
this study are not limited to surface ozone data and could potentially
maximize signal detection capabilities within a broad array of climate and
chemical observations or model output.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <title>Introduction</title>
      <p id="d1e205">The capability to detect air quality signals – be they meteorological,
chemical, or of some other type – is a fundamental component of modern
climate science and atmospheric chemistry. The debate over the existence or
length of a global warming hiatus (Lewandowsky et al., 2015; Roberts et al.,
2015; Medhaug et al., 2017) and research examining the time of emergence of
climatological (Weatherhead et al., 2002; Deser et al., 2012; Hawkins and
Sutton, 2012; de Elía et al., 2013; Schurer et al., 2013), meteorological
(Giorgi and Bi, 2009; King et al., 2015), chemical (Camalier et al., 2007;
Strode and Pawson, 2013; Barnes et al., 2016; Garcia-Menendez et al., 2017),
and other sectoral signals (e.g., Monier et al., 2016) embody an accumulation
of techniques and strategies for filtering noise (due to natural
variability) and maximizing the capability to detect statistically
significant signals and trends in noisy data. It is well established that
temporal averaging (e.g., Lewandowsky et al., 2015) and spatial averaging
(e.g., Frost et al., 2006; Hawkins and Sutton, 2012; Barnes et al., 2016) can
enhance signal detection capabilities in atmospheric data. Here we extend
this research by quantifying the impact of both spatial and temporal
averaging – individually and in combination – of surface ozone on the
magnitude of the calculated variability, which is largely driven by the
influence of meteorological variability on atmospheric chemistry (e.g., Jacob
and Winner, 2009). We offer recommendations for strategically averaging in
space and time to maximize signal detection capabilities. In particular, we
examine estimates of mean ozone and of the ozone variability that results
from meteorology, although our approach can be generalized to other air
quality applications.</p>
      <p id="d1e208">For observed ozone data, strategies for reducing spatial and temporal noise
are limited: a longer time series is needed, more observations need to be
made, or the spatial region over which the ozone observations are being
averaged needs to be enlarged. For surface ozone estimates using models,
however, there exist a variety of strategies for reducing the noise (due to
chemical and meteorological variability) relative to the strength of the
signal, although they cluster into three main types. The first strategy is
to average or combine multiple runs of structurally different models under
the assumption that errors, biases, and uncertainties within the individual
models are reduced and the multi-model or multi-dataset mean is a best
estimate of the actual, aggregated ozone field. This is most notably done
with multi-model ensembles within the Atmospheric Chemistry and Climate
Model Intercomparison Project (ACCMIP) framework (Lamarque et al., 2013;
Young et al., 2013; Stevenson et al., 2013), and this approach tends to
assume that all members in the ensemble are independent and equally
skillful. This assumption, however, may result in a loss of some valuable
information (Knutti, 2010). Another form of this strategy is to run multiple
model runs within a single model, but under different initial conditions or
sets of parametric assumptions (e.g., Deser et al., 2012; Monier et al., 2013,
2015; Kay et al., 2015; Garcia-Menendez et al., 2015, 2017). This approach
cannot address structural uncertainties and internal (unforced) variability
between models, but is capable of identifying parametric uncertainties
within a single model.</p>
      <p id="d1e211">The second strategy to reduce ozone variability is to expand the temporal
averaging window, which can influence the interpretation of the determined
ozone value (e.g., Brown-Steiner et al., 2015). The Environmental Protection
Agency (EPA) National Ambient Air Quality Standard (NAAQS) for ozone (US
EPA, 2015) explicitly takes this into account, both in the length of the
averaging period (daily maximum 8 h average) and the selection criteria
for the standard (fourth highest over the previous 3 years). The calculated
ozone variability can be further reduced by utilizing even longer averaging
periods, such as monthly (e.g., Rasmussen et al., 2012), seasonal (e.g., Fiore
et al., 2014; Barnes et al., 2016), annual, or decadal mean values (e.g.,
Garcia-Menendez et al., 2017). This strategy is analogous to the averaging
of meteorological data to derive a climate signal, and, just as Lewandowsky
et al. (2015) recommend averaging 17 or more years in order to achieve
climatological estimates of temperature trends, there is a growing body of
literature recommending averaging short-timescale chemical variability
(what could be called chemical weather, see Lawrence et al., 2005) for 15 or more
years (e.g., Garcia-Menendez et al., 2017) in order to achieve an estimate of
what could be called the chemical climate (see Möller, 2010).</p>
      <p id="d1e214">The third strategy to reduce ozone variability is to average surface ozone
values over larger spatial regions, and, while there is a significant body of
literature discussing the capability and interpretation of coarse-resolution
model representations of the sub-grid-scale heterogeneity (Pyle and Zavody,
1990; Searle et al., 1998; Wild and Prather, 2006), there are few that
strategically expand the spatial scale over which averaging is applied in
order to maximize signal detection capabilities. This strategy has been
applied in other fields of the atmospheric sciences as well as for general
gridded datasets (e.g., Pogson and Smith, 2015), and spatial averaging has
been suggested as a means of reducing temperature variability and smoothing
biases at the smallest spatial scales within a single model run
(Räisänen and Ylhäsi, 2011). This “scale problem” has also
been noted as an important consideration when analyzing aerosol indirect
effects (McComiskey and Feingold, 2012) and for the detection and
attribution of extreme weather events (Angélil et al., 2017).</p>
      <?pagebreak page8375?><p id="d1e218">Our objective in this study is to provide a framework for selecting spatial
and temporal averaging scales that reduces the uncertainty in analyzing
ozone signals and limits the likelihood of overconfidence in an estimate of
surface ozone that arises from meteorological variability. This type of
framework can be useful from two different research perspectives. The first
research perspective has a priori an ozone estimate (either observed or
modeled) at a certain spatial and temporal scale (e.g., a 3-year simulation
of surface ozone over the northeastern US) and aims to quantify the
likelihood that this estimate is representative of the long-term ozone
behavior (rather than overly sensitive to meteorological variability of that
particular 3-year period). Since ozone is strongly influenced by natural
fluctuations in meteorology (Jacob and Winner, 2009; Jhun et al., 2015) and
since extremes in surface ozone and temperature tend to co-occur (Schnell
and Prather, 2017), atypically hot or cold periods can strongly influence
ozone behavior over short timescales.</p>
      <p id="d1e221">The second research perspective is to identify an ozone signal of a certain
magnitude (or threshold) and decide what spatial and temporal averaging
scales are needed to best identify that signal. The ozone signal could be
large (e.g., determining the effectiveness or compliance with a 5 ppbv
incremental reduction of the EPA NAAQS for ozone; US EPA, 2015) or small
(e.g., identifying annual ozone trends within the US, which Cooper et
al., 2012, show can be on the order of 0.10–0.45 ppbv) and can be highly
sensitive to spatial and temporal heterogeneity and meteorological
variability. Barnes et al. (2016) found that surface ozone trends over
20-year periods can vary by <inline-formula><mml:math id="M2" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula>2 ppbv due solely to climate
variability, while interannual variability can be on the order of <inline-formula><mml:math id="M3" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula>15 ppbv
(Fiore et al., 2003; Tilmes et al., 2012; Lin et al., 2014) and
day-to-day variability can be even larger, extending regularly from
near-background levels of 40–50 ppbv up to 100 ppbv during the summertime
(Fiore et al., 2014).</p>
      <p id="d1e238">In this study, we quantify the impact of both temporal and spatial averaging
on the calculated ozone variability – due solely to meteorological
variability – in order to maximize the capability to detect signals. We use
simulated ozone (with the Community Atmosphere Model with Chemistry,
CAM-chem) and observational data (with the EPA's Clean Air Status and Trends
Network, CASTNET) within the United States in order to answer the following
four questions. (1) Within a given dataset (model or observations), with
both spatial and temporal coverage, what is the magnitude of the ozone
variability due to meteorology at the smallest scale, and how does spatial
and temporal averaging reduce this variability? (2) Are there combinations
of temporal and spatial averaging scales that maximize the signal detection
capability for surface ozone data? (3) How sensitive are the above
strategies to different configurations (i.e., emissions, meteorology, and
climate) of the CAM-chem modeling framework? And (4) how could they be
applied to other datasets (chemical, meteorological, or climatological)? We
limit our focus to spatial scales within the United States as it has high
spatial and temporal variability and numerous observations, and since
averaging over larger regions (e.g., the Northern Hemisphere, or the globe)
would produce a smaller calculated variability.</p>
      <p id="d1e241">In Sect. 2, we describe the CAM-chem model and our simulations, as well as
the CASTNET observational database and the regional definitions used
throughout this paper. In Sect. 3 we quantify the temporal and spatial
variability of surface ozone, show how temporal and spatial averaging
reduces the calculated ozone variability, and demonstrate the spatial
heterogeneity of the calculated ozone variability. In Sect. 4, we discuss
the potential strategies that could be used to maximize ozone signal
detection due to meteorological variability, explore uncertainties, and make
recommendations for future research.</p>
</sec>
<sec id="Ch1.S2">
  <title>Methods</title>
      <p id="d1e250">We examine both present-day (one simulation and one observed dataset) and
future (two simulations) surface ozone in this study. For present-day
analysis, we simulate surface ozone using CAM-chem, a component of the
Community Earth System Model (CESM) and available observations within the US
from the EPA CASTNET database. For future analysis, and in order to examine
the potential for patterns of variability to change in the future, we
utilize two existing simulations of CAM-chem conducted by Garcia-Menendez et
al. (2017). Much of this analysis is conducted using the R language
(R Project, <uri>https://www.r-project.org/</uri>, last access: 7 June 2018). Here we summarize each of the three datasets
and our approach to our analysis in Sect. 3.</p>
<sec id="Ch1.S2.SS1">
  <title>CAM-chem</title>
      <p id="d1e261">The present-day simulation (MOZ_2000) was conducted using
CAM-chem model version 1.2.2, with the CAM4 atmospheric component (see
Tilmes et al., 2015, 2016, for model description and evaluation). The model
has been used extensively for a wide range of atmospheric chemistry research
and is included in the ACCMIP (Lamarque et al., 2012; Young et al., 2013, and
references therein). We conduct our simulations using the Model for Ozone
and Related chemical Tracers version 4 (MOZART-4) chemical mechanism
(Emmons et al., 2010), which is a full tropospheric chemical mechanism
integrated into CAM-Chem (e.g., Lamarque et al., 2012; Tilmes et al., 2015).
Offline forced meteorology is taken from
the Modern-Era Retrospective analysis for Research and Applications (MERRA)
reanalysis product (Rienecker et al., 2011) for 26 meteorological years
(1990–2015). Additional model evaluation and comparisons to surface and
ozonesonde observations can be found in Brown-Steiner et al. (2018).
This simulation has 56 vertical levels – adopted from MERRA meteorology –
as well as 96 latitudinal and 144 longitudinal grid cells. We aim to isolate<?pagebreak page8376?> the
variability to the meteorologically driven impact on atmospheric chemistry
so we repeat year-2000 anthropogenic emissions from the ACCMIP inventory (Lamarque et
al., 2012) as well as all non-biogenic emissions for all meteorological years and
include specified long-lived stratospheric species (<inline-formula><mml:math id="M4" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M5" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>,
<inline-formula><mml:math id="M6" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">HNO</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M7" 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>, <inline-formula><mml:math id="M8" 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:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">5</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) as in MOZART-4 (Emmons et al., 2010),
an online biogenic emissions model MEGAN (Guenther et al., 2012), and forced
sea ice and sea surface temperatures to year-2000 historical conditions.
Like many state-of-the-art chemical tracer models, the CAM-chem exhibits
some biases, most notably for our purposes a high bias in simulated surface
ozone in the eastern US (e.g., Lamarque et al., 2012; Brown-Steiner et al.,
2015; Travis et al., 2016; Barnes et al., 2016). Recent efforts have been
successful in partially reducing these biases (e.g., Sun et al., 2017).</p>
      <p id="d1e326">We also include two reference simulations of the future climate,
MOZ_2050 and MOZ_2100 (simulating the
meteorological years 2035–2065 and 2085–2115, respectively), using the
CESM CAM-chem simulations described in detail by Garcia-Menendez et
al. (2017) with one set of initial condition data and a climate sensitivity of
3.0 <inline-formula><mml:math id="M9" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C. These simulations do not include projections of any
changes in future emissions. Compared to the present-day simulation
(MOZ_2000), these future simulations (MOZ_2050
and MOZ_2100) have several parametric differences: the model
version is 1.1.2 (see Tilmes et al., 2015, and references for information on
model development), the atmospheric component is CAM3, the emissions (which
are held constant at year-2000 levels) are from the Precursors of Ozone and
their Effects in the Troposphere database (see Garcia-Menendez et al.,
2017), and the meteorology is derived from a linkage between the
Massachusetts Institute of Technology Integrated Global System Model (MIT
IGSM) and the CESM CAM model (Monier et al., 2013), and as such has 26
vertical levels. For a full description of these simulations, see
Garcia-Menendez et al. (2017).</p>
</sec>
<sec id="Ch1.S2.SS2">
  <title>CASTNET</title>
      <p id="d1e344">The observational database comes from the EPA Clean Air Status and Trends
Network (CASTNET), which has more than 90 surface observational sites within
the United States and has been collecting hourly surface meteorological and
chemical data since 1990 (US EPA, 2016 and <uri>https://www.epa.gov/castnet</uri>, last access: 7 June 2018). We
collected data from all sites that reported complete ozone data from each
year and removed data that was marked invalid within the downloaded EPA
files. The number of sites that matched these criteria varied from year to
year, but generally we have between 55 and 94 sites throughout the 1991–2014
period. The CASTNET observational network is located primarily in rural
sites and thus is considered to be a reasonable comparison to coarse grid-cell model output (e.g., Brown-Steiner et al., 2015; Phalitnonkiat et al.,
2016). Since a notable trend in observed ozone data exists, especially in
the northeastern US (Frost et al., 2006), and since the simulations have no
change in anthropogenic emissions, and thus no ozone trend, we detrended the
CASTNET data for each of the four averaging regions (described below) using
a simple linear regression.</p>
</sec>
<sec id="Ch1.S2.SS3">
  <title>Telescoping regional definitions</title>
      <p id="d1e356">In order to isolate the impact of the size of the spatial scale over which
ozone data are averaged, we analyze ozone data at different spatial scales.
The largest region considered is the entire continental US, while the
smallest regions considered are at the individual grid-cell level of the
CESM CAM-chem model (1.9 <inline-formula><mml:math id="M10" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 2.5<inline-formula><mml:math id="M11" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> latitude and longitude).
Data and statistics for the other regions (i.e., the midwestern and
southeastern US) are included in the Supplement but do not alter
the conclusions we draw from the northeastern US. For CESM CAM-chem data, we
averaged all grid cells within each region, while for the CASTNET data we
first average sites within each corresponding CESM CAM-chem grid cell and
then average these data together. These telescoping regions are shown in Fig. 1.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1"><caption><p id="d1e377">Telescoping spatial regions included in this study. The largest
scale we consider is the continental US (outer border). We focus on the
eastern US by subdividing into three subregions: the midwest (blue),
northeast (black), and southeast (red). Within each subregion we telescope
into a 3 <inline-formula><mml:math id="M12" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 3 grid cell (yellow) a 2 <inline-formula><mml:math id="M13" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 2 grid cell (purple), and a 1 <inline-formula><mml:math id="M14" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 1 grid cell
(green). In the paper, we only show a subset of these telescoping regions,
and we include the rest in the Supplement.</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/8373/2018/acp-18-8373-2018-f01.jpg"/>

        </fig>

</sec>
<sec id="Ch1.S2.SS4">
  <title>Temporal averaging windows</title>
      <p id="d1e414">To explore the impact of temporal averaging, we examine ozone across a range
of temporal averaging windows, from 1 day up to the full 26 years for the
CESM data (1990–2015), the full 24 years for the detrended CASTNET data
(1991–2014), and the 30 years available from the future scenarios of
Garcia-Menendez et al. (2017). Each averaging window, therefore, can be
considered to be a sample of possible realizations of meteorology. For
instance, a selection of an averaging window of 1 year has 26 possible
slices within the 1990–2015 MOZ_2000 data, while a
selection of an<?pagebreak page8377?> averaging window of 10 years has 17 possible slices within
the CESM data (<inline-formula><mml:math id="M15" display="inline"><mml:mi>N</mml:mi></mml:math></inline-formula> <inline-formula><mml:math id="M16" display="inline"><mml:mo>=</mml:mo></mml:math></inline-formula> # years – length of window <inline-formula><mml:math id="M17" display="inline"><mml:mo>+</mml:mo></mml:math></inline-formula>1). In this study, we
consider all realizations to be equally likely and compare them to each
other and to the long-term trend. However, if we were only able to simulate
5 years, we would not be able to compare to the long-term trend, and so we would be
unable to completely quantify the likelihood of error in the context of the
long-term behavior.</p>
</sec>
</sec>
<sec id="Ch1.S3">
  <title>Results</title>
      <p id="d1e445">Here we examine the spatial and temporal behavior of MOZ_2000, MOZ_2050, and MOZ_2100 and compare
MOZ_2000 to present-day CASTNET observations. We introduce
the moving temporal averaging windows, explore possible thresholds of
acceptable error or signal strength, and examine the influence of expanding
spatial averaging regions. Finally, we combine these temporal and spatial
averaging techniques into a single framework.</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1" specific-use="star"><caption><p id="d1e451">Statistical Summary of the CASTNET observations and the three
CAM-chem simulations for different spatial averaging regions within the US.
Variability is defined as the standard deviation divided by the mean value
(in percent). Biases are only included for the present-day CAM-chem
simulation compared to the CASTNET data. Similar tables for the other
regions in this study are included in the Supplement.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="7">
     <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:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <oasis:colspec colnum="6" colname="col6" align="right"/>
     <oasis:colspec colnum="7" colname="col7" align="right"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2"/>
         <oasis:entry colname="col3"/>
         <oasis:entry colname="col4">CASTNET</oasis:entry>
         <oasis:entry colname="col5">MOZ_2000</oasis:entry>
         <oasis:entry colname="col6">MOZ_2050</oasis:entry>
         <oasis:entry colname="col7">MOZ_2100</oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Mean</oasis:entry>
         <oasis:entry colname="col3">ppbv</oasis:entry>
         <oasis:entry colname="col4">52.4</oasis:entry>
         <oasis:entry colname="col5">56.7</oasis:entry>
         <oasis:entry colname="col6">56.8</oasis:entry>
         <oasis:entry colname="col7">57.4</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Continental</oasis:entry>
         <oasis:entry colname="col2">Standard deviation</oasis:entry>
         <oasis:entry colname="col3">ppbv</oasis:entry>
         <oasis:entry colname="col4">5.04</oasis:entry>
         <oasis:entry colname="col5">3.08</oasis:entry>
         <oasis:entry colname="col6">3.54</oasis:entry>
         <oasis:entry colname="col7">3.73</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">US</oasis:entry>
         <oasis:entry colname="col2">Variability</oasis:entry>
         <oasis:entry colname="col3">%</oasis:entry>
         <oasis:entry colname="col4">10%</oasis:entry>
         <oasis:entry colname="col5">5%</oasis:entry>
         <oasis:entry colname="col6">6%</oasis:entry>
         <oasis:entry colname="col7">7%</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Bias</oasis:entry>
         <oasis:entry colname="col3">ppbv</oasis:entry>
         <oasis:entry colname="col4"/>
         <oasis:entry colname="col5">4.31</oasis:entry>
         <oasis:entry colname="col6"/>
         <oasis:entry colname="col7"/>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Mean</oasis:entry>
         <oasis:entry colname="col3">ppbv</oasis:entry>
         <oasis:entry colname="col4">50.7</oasis:entry>
         <oasis:entry colname="col5">58.6</oasis:entry>
         <oasis:entry colname="col6">55.5</oasis:entry>
         <oasis:entry colname="col7">56.5</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Eastern</oasis:entry>
         <oasis:entry colname="col2">Standard deviation</oasis:entry>
         <oasis:entry colname="col3">ppbv</oasis:entry>
         <oasis:entry colname="col4">5.78</oasis:entry>
         <oasis:entry colname="col5">5.77</oasis:entry>
         <oasis:entry colname="col6">5.80</oasis:entry>
         <oasis:entry colname="col7">6.50</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">US</oasis:entry>
         <oasis:entry colname="col2">Variability</oasis:entry>
         <oasis:entry colname="col3">%</oasis:entry>
         <oasis:entry colname="col4">11%</oasis:entry>
         <oasis:entry colname="col5">10%</oasis:entry>
         <oasis:entry colname="col6">10%</oasis:entry>
         <oasis:entry colname="col7">12%</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Bias</oasis:entry>
         <oasis:entry colname="col3">ppbv</oasis:entry>
         <oasis:entry colname="col4"/>
         <oasis:entry colname="col5">7.91</oasis:entry>
         <oasis:entry colname="col6"/>
         <oasis:entry colname="col7"/>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Mean</oasis:entry>
         <oasis:entry colname="col3">ppbv</oasis:entry>
         <oasis:entry colname="col4">48.3</oasis:entry>
         <oasis:entry colname="col5">74.4</oasis:entry>
         <oasis:entry colname="col6">68.4</oasis:entry>
         <oasis:entry colname="col7">73.0</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">Northeastern</oasis:entry>
         <oasis:entry colname="col2">Standard deviation</oasis:entry>
         <oasis:entry colname="col3">ppbv</oasis:entry>
         <oasis:entry colname="col4">6.89</oasis:entry>
         <oasis:entry colname="col5">11.4</oasis:entry>
         <oasis:entry colname="col6">11.1</oasis:entry>
         <oasis:entry colname="col7">12.7</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">US</oasis:entry>
         <oasis:entry colname="col2">Variability</oasis:entry>
         <oasis:entry colname="col3">%</oasis:entry>
         <oasis:entry colname="col4">14%</oasis:entry>
         <oasis:entry colname="col5">15%</oasis:entry>
         <oasis:entry colname="col6">16%</oasis:entry>
         <oasis:entry colname="col7">17%</oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Bias</oasis:entry>
         <oasis:entry colname="col3">ppbv</oasis:entry>
         <oasis:entry colname="col4"/>
         <oasis:entry colname="col5">26.1</oasis:entry>
         <oasis:entry colname="col6"/>
         <oasis:entry colname="col7"/>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Mean</oasis:entry>
         <oasis:entry colname="col3">ppbv</oasis:entry>
         <oasis:entry colname="col4">49.6</oasis:entry>
         <oasis:entry colname="col5">84.9</oasis:entry>
         <oasis:entry colname="col6">81.1</oasis:entry>
         <oasis:entry colname="col7">85.1</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">1 <inline-formula><mml:math id="M18" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 1 Northeastern</oasis:entry>
         <oasis:entry colname="col2">Standard deviation</oasis:entry>
         <oasis:entry colname="col3">ppbv</oasis:entry>
         <oasis:entry colname="col4">10.2</oasis:entry>
         <oasis:entry colname="col5">12.8</oasis:entry>
         <oasis:entry colname="col6">16.7</oasis:entry>
         <oasis:entry colname="col7">17.3</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">US</oasis:entry>
         <oasis:entry colname="col2">Variability</oasis:entry>
         <oasis:entry colname="col3">%</oasis:entry>
         <oasis:entry colname="col4">21%</oasis:entry>
         <oasis:entry colname="col5">15%</oasis:entry>
         <oasis:entry colname="col6">21%</oasis:entry>
         <oasis:entry colname="col7">20%</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1"/>
         <oasis:entry colname="col2">Bias</oasis:entry>
         <oasis:entry colname="col3">ppbv</oasis:entry>
         <oasis:entry colname="col4"/>
         <oasis:entry colname="col5">35.3</oasis:entry>
         <oasis:entry colname="col6"/>
         <oasis:entry colname="col7"/>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2"><caption><p id="d1e893">Continental US surface maps of <bold>(a)</bold> present-day CAM-chem mean MDA8
<inline-formula><mml:math id="M19" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, <bold>(b)</bold> CAM-Chem (<inline-formula><mml:math id="M20" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> axis) comparison to CASTNET observations (<inline-formula><mml:math id="M21" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> axis)
for the year 2000 (see Brown-Steiner et al., 2018, for additional
comparisons), <bold>(c)</bold> present-day CAM-chem standard deviation of MDA8
<inline-formula><mml:math id="M22" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>,
<bold>(d)</bold> present-day CAM-chem variability (standard deviation divided by mean,
as a percent), <bold>(e)</bold> future CAM-chem year-2050 mean MDA8 <inline-formula><mml:math id="M23" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>, and <bold>(f)</bold>
future CAM-chem year-2100 mean MDA8 <inline-formula><mml:math id="M24" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>. All model results are averaged
over every JJA day in the time series, while the CASTNET results are only
for the year 2000. The numbers in <bold>(b)</bold> are slopes (left) and <inline-formula><mml:math id="M25" display="inline"><mml:mrow><mml:msup><mml:mi>R</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula>
values (right).</p></caption>
        <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/8373/2018/acp-18-8373-2018-f02.pdf"/>

      </fig>

<?xmltex \hack{\newpage}?>
<sec id="Ch1.S3.SS1">
  <title>Spatial and temporal comparisons</title>
      <p id="d1e1002">Figure 2 compares summertime (JJA) maximum daily 8 h average ozone (MDA8
<inline-formula><mml:math id="M26" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>) from the present-day model simulation (MOZ_2000,
Fig. 2a) to the year-2000 CASTNET observations (Fig. 2b). Figure 2c and
d plot the MDA8 <inline-formula><mml:math id="M27" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> standard deviation and variability for
MOZ_2000, while Fig. 2d and e compare the mean summertime
MDA8 <inline-formula><mml:math id="M28" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> for the future simulations (MOZ_2050 and
MOZ_2100). Some of the averaging strategies we present can
average away the high ozone behavior this MDA8 <inline-formula><mml:math id="M29" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> metric is intended to
quantify, but it is such a well-reported metric that focusing our analysis
on it allows for ready comparisons to other studies. The well-known high
ozone bias in the eastern US (e.g., Lamarque et al., 2012; Travis et al.,
2016; Barnes et al., 2016) is apparent, but otherwise the spatial
variability over the entire continental US is well captured. While we do
examine the magnitude of surface ozone in this paper, most of our analysis
is focused on the variability around the mean value (the anomaly), and as we
show below, the CASTNET observations and CESM results are largely consistent
in their representation of ozone variability (Fig. 2, Table 1). The
standard deviation of the simulated MDA8 <inline-formula><mml:math id="M30" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> is large over the eastern
US and the Pacific Coast, with peak values of <inline-formula><mml:math id="M31" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula>25 ppbv over the
highly populated Atlantic Coast (Fig. 2c). The variability (defined as the
standard deviation divided by the mean, expressed as a percentage) is lowest
over the western US (<inline-formula><mml:math id="M32" display="inline"><mml:mo lspace="0mm">∼</mml:mo></mml:math></inline-formula> 15 %), only slightly higher over the
eastern US (up to 25 %), and highest (up to 50 %) over the coastal
regions (Fig. 2d). We consider both the standard deviation (ppb) and a
mean-normalized standard deviation (as a percentage). The normalized
standard deviation allows for a more direct comparison of the shape of the
MDA8 <inline-formula><mml:math id="M33" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> distributions between the simulations and available
observations, which accounts for the noted ozone biases (Fig. 2b, c and
Table 1). The future climate simulations, MOZ_2050 and
MOZ_2100 (Fig. 2e and  f, respectively), although run with
different parametric settings than MOZ_2000 (see Sect. 2),
simulate a similar spatial distribution of surface ozone, although under the
warmer simulated climate of 2050 and 2100. These future climate simulations
have a similar spatial pattern to the present-day simulation (Fig. 2a),
with high ozone levels in the eastern US that increase from 2050 to 2100
(see Garcia-Menendez et al., 2017, for more details).</p>
      <p id="d1e1086">Figure 3 compares box plots over the four telescoping regions (Fig. 1) for
MOZ_2000, the CASTNET data, the detrended CASTNET data, and
for the single year 2000 for the CASTNET data (Fig. 3a–d), and Table 1
summarizes relevant statistics. In order to compare CASTNET ozone to the
simulated ozone, which does not have a trend over time, we detrend the CASTNET
data in order to remove the impact of any temporal trends (e.g.,
<inline-formula><mml:math id="M34" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> emissions reductions) on ozone. The northeastern US ozone bias is apparent
at the smaller spatial scales (Fig. 3c, d) and is less apparent when
averaging over larger regions (Fig. 3a, b). Figure 3e compares the
year-to-year box plots of the JJA MDA8 O<inline-formula><mml:math id="M35" display="inline"><mml:msub><mml:mi/><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:math></inline-formula> for the<?pagebreak page8378?> MOZ_2000 and
the detrended CASTNET data and demonstrates the variability both
in the median and spread of the ozone values in both the modeled and
simulated data. While the MOZ_2000 ozone is generally higher
than the CASTNET data, there are years in which the CASTNET data has higher
ozone extremes. The red box plot in Fig. 3e, which corresponds to the red
box plot in Fig. 3b, indicates that the year 2000 was an anomalously low
year for observed ozone, although not the lowest.</p>
      <p id="d1e1109">While all the CESM CAM-chem simulations have high ozone biases in the
northeastern US (Figs. 2 and 3, Table 1), their capability to simulate
ozone variability is consistent with the available observations (for present
day) and for expectations of ozone variability changes in the future climate
(for MOZ_2050 and MOZ_2100). It is clear that
variability increases when the size of the averaging region decreases – a
fact that is well noted in the literature, as in Hawkins and Sutton (2012)
for climate variables and Barnes et al. (2016) for ozone. As can be seen
in Table 1, the CASTNET variability increases as the spatial scale decreases
(10, 13, 16, and 20 % for our telescoping regions from
continental to a single northeastern US grid box), and MOZ_2000
largely captures this trend, albeit with lower overall variability
(5, 10, 15, and 15 %). This increase in ozone variability with
decreasing spatial scale is maintained in the future climate simulations
(6, 10, 16, and 21 % for MOZ_2050 and 7,
12, 17, and 20 % for MOZ_2100). Table S1 contains
statistics for the other telescoping regions.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3" specific-use="star"><caption><p id="d1e1114"><bold>(a–d)</bold>: Box plots for surface MDA8 <inline-formula><mml:math id="M36" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> for every summertime
(JJA) day from 1991 to 2014 averaged over the continental US, the eastern
US, the northeastern US, and a single grid cell in the northeastern US from
CAM-chem (grey), CASTNET observations (blue), detrended CASTNET observations
centered at the year 2000 (green), and, since the CAM-chem simulations have
cycled year-2000 emissions and boundary conditions, the CASTNET values for
the year 2000 only (red). <bold>(e)</bold> Comparison of the yearly JJA MDA8 <inline-formula><mml:math id="M37" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> estimates
averaged over the eastern US for CAM-chem (grey) and the detrended CASTNET
(green) from 1991 to 2014. The single red box plot coincides with the red
box plot in <bold>(b)</bold>. The units are in ppbv and for each box plot the box contains
the interquartile range (IQR); the horizontal line within the box is the
median; and the whiskers extend out to the farthest point, which is within
1.5 times the IQR with circles indicating any outliers.</p></caption>
          <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/8373/2018/acp-18-8373-2018-f03.pdf"/>

        </fig>

</sec>
<sec id="Ch1.S3.SS2">
  <title>Variability, averaging windows, and thresholds</title>
      <p id="d1e1159">As we aim to quantify the potential tradeoffs that result from a particular
choice of temporal and spatial scales on the assessment of ozone variability
within the US, we represent the spatial scale by applying the telescoping
regions (see Fig. 1 and Sect. 2.3) and we represent the temporal scale
through the use of moving averaging windows (see Sect. 2.4). We frame much
of the following analysis from the perspective of limited simulation length
in order to approximate the question that decision-makers and modelers face
when constrained by limited computational capabilities or available data:
what is the likelihood that a particular estimate (of both the mean and the
variability) is not a true representation of the true mean and variability
but rather a product of the underlying variability at the particular choice
of spatial and temporal scale?</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4" specific-use="star"><caption><p id="d1e1164">Comparisons of the variability represented by the summertime MDA8
<inline-formula><mml:math id="M38" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> anomaly (from the long-term summertime mean) for the four datasets
in this study (CASTNET, MOZ_2000, MOZ_2050,
MOZ_2100, shown in columns) averaged over the four telescoping regions
(the continental US, the eastern US, the northeastern US, and a
single grid cell within the northeastern US).
In each panel, the horizontal axis is the
number of years in the dataset (24 years, 1991–2014, for CASTNET; 26 years, 1990–2015, for MOZ_2000; and 30 years, 2036–2065 and
2086–2115, for MOZ_2050 and MOZ_2100), and the
vertical axis represents the length of the averaging window (ranging from
1 day, bottom row, up to the entire time series, top
pixel, upper right corner of each triangle). Each pixel
represents the estimate of the ozone anomaly for a given averaging window
(vertical axis) ending at a given time (horizontal axis). Horizontal lines
indicate the length of averaging window required to guarantee that the
variability drops below thresholds of 5 ppbv (solid), 1 ppbv (dashed), and
0.5 ppbv (dotted).</p></caption>
          <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/8373/2018/acp-18-8373-2018-f04.jpg"/>

        </fig>

      <p id="d1e1184">Figure 4 presents this likelihood by plotting all possible estimates of MDA8
<inline-formula><mml:math id="M39" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> (as anomalies from the long-term mean) over all possible selections
of averaging window (from 1 day up to the complete time series) for our
telescoping regions. The semi-cyclical and highly autocorrelated nature of
surface ozone is apparent at all spatial scales, with alternating cycles of
anomalously high and low ozone. The temporal impact of anomalous ozone
events is indicated by the vertical and right-leaning diagonal striations,
which show that anomalous ozone events can impact estimates of ozone values
within averaging windows up to 15 or 20 years. Figure 4 demonstrates how
small-scale anomalously high or low ozone values (that come only from
meteorological<?pagebreak page8379?> variability) can impact temporal averages of 5, 10, or even
20 years. For instance, a selected 5-year averaging window within the
MOZ_2000 simulation averaged over the northeastern US could
be 2.5 ppbv higher or lower than the 25-year mean value of 74 ppbv, a
potential error of 7 %. Horizontal lines in Fig. 4 mark the length of
averaging windows that are needed to ensure that ozone anomaly for any
selection of averaging window does not exceed a given threshold (5, 1, and
0.5 ppbv for solid, dashed, and dotted lines, respectively). This potential
error is larger within smaller regions and at the shorter selections of the
averaging window. While the high and low ozone anomalies differ in time
between CASTNET, MOZ_2000, MOZ_2050, and
MOZ_2100 in Fig. 4, the impact of spatial and temporal
averaging is consistent.</p>
      <p id="d1e1198">We also quantify this variability in Figs. S1 and S2, which
plots the likelihood (as a percentage) that a particular selection of
spatial (rows) and temporal (<inline-formula><mml:math id="M40" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> axis) scale estimates ozone values that
exceed a particular threshold (colored lines) away from the true mean value.
For instance, if we were interested in characterizing ozone behavior (e.g.,
estimating a trend, or the mean value) in the northeastern US, but were
limited to a 5-year simulation, there is more than a 50 % likelihood that
the simulated ozone is 1 ppbv away from the 26-year mean and an 80 %
likelihood that the discrepancy is greater than 0.5 ppbv. However, these
data indicate that there is a virtual certainty that the estimate will be
within 2.5 ppbv of the true mean value. We should note that, at the
grid-cell level and within a 10-year period, the surface ozone variability
can exceed 1 ppbv but is unlikely to exceed 2.5 ppbv (Fig. 4) and that a
20-year trend is very likely to be able to identify significant ozone
signals among the impact of meteorological variability on atmospheric
chemistry. Our results also align with the results from Garcia-Menendez et
al. (2017), which recommended that simulations need to be at least 15 years
long to identify anthropogenically forced ozone signals on the order of 1 ppbv.</p>
      <p id="d1e1209">Figures 4, S1, and S2 compare the CASTNET
observations to the three CESM CAM-chem simulations, and, while there are
minor differences, there are broad features that are consistent. First,
using longer temporal averaging windows reduces the influence of small-scale
ozone variability at all spatial scales, and, depending on the acceptable
threshold, one can select a temporal scale that effectively reduces the
likelihood of exceeding that threshold to zero. Second, larger spatial
scales also reduce this likelihood of exceeding a given threshold, but not
as effectively as longer temporal scales. Finally, the impact of both
temporal and spatial averaging on ozone variability is largely consistent
for the CASTNET observations and for all three CESM CAM-chem simulations.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5" specific-use="star"><caption><p id="d1e1214">Spatial plots over the continental US plotting the likelihood
(%) that an estimate of ozone exceeds a given threshold due to
meteorological variability (rows) at the grid-cell level when using
different lengths of averaging windows (columns) for the present-day CESM
simulation (MOZ_2000).</p></caption>
          <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/8373/2018/acp-18-8373-2018-f05.pdf"/>

        </fig>

</sec>
<sec id="Ch1.S3.SS3">
  <title>Selection of temporal averaging scales</title>
      <p id="d1e1229">Figure 5 extends this analysis to examine the spatial heterogeneity of this
likelihood of the meteorological variability causing ozone anomalies
exceeding particular thresholds<?pagebreak page8380?> at the grid-cell level. Here we plot four
thresholds (0.5, 1, 2.5, and 5 ppbv) and four averaging windows (1, 5, 10,
and 20 years) for the MOZ_2000 simulation. Ozone variability
is highest in the eastern US. At the grid-cell level, there are two
strategies for filtering out the noise associated with natural
meteorological variability (and thus enhancing signal detection
capabilities): either average over longer periods, or acknowledge the level
of noise and increase the threshold. For these data, it is virtually certain
that any 20-year average will be within 5 ppbv of a full 25-year mean value
(which itself may not be an accurate representation of a longer simulation)
and virtually certain that any 1-year average will be at least 0.5 ppbv away
from the mean.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6" specific-use="star"><caption><p id="d1e1234">As in Fig. 5, but only the second row (1 ppbv threshold), for
present-day CAM-chem (MOZ_2000), future CAM-chem 2050
(MOZ_2050), and future CAM-chem 2100 (MOZ_2100).</p></caption>
          <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/8373/2018/acp-18-8373-2018-f06.pdf"/>

        </fig>

      <p id="d1e1243">Figure S3 extends the analysis of Fig. 5 by comparing the
MOZ_2000, MOZ_2050, and MOZ_2100 simulations across the four thresholds for the 5-year averaging window.
Figure 6 similarly compares the 1 ppbv ozone threshold across the four
averaging windows for MOZ_2000, MOZ_2050, and
MOZ_2100. Interpreting Figs. 6 and S3
gives largely consistent interpretations compared to the analysis above
(Fig. 5) – namely, that at the grid-scale level increasing the temporal averaging
window (Fig. 6) or increasing the acceptable ozone threshold (Fig. S3) is effective at reducing the impact of the meteorological
variability on estimates of the ozone signal. Shorter windows (or smaller
thresholds) are needed in the western US (where variability is smaller, see
Fig. 2d) than in the eastern US (where variability is larger) as well as
over coastal and highly populated regions. Finally, the 1 ppbv threshold and
the 5-year averaging window plots (in either Figs. 5 and S3) indicate
that the spatial distribution and location of the peak
variability may shift into the future, although this may be due to
parametric differences between MOZ_2000, MOZ_2050, and MOZ_2100. Future<?pagebreak page8382?> simulations will be needed to
check this shift in peak ozone variability.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7" specific-use="star"><caption><p id="d1e1249">Combined impact of temporal and spatial averaging on reducing
ozone variability on the likelihood (%) of exceeding the 0.5 ppbv
threshold (as in Figs. 5, 6, and S3) for the
present-day MOZ_2000 simulation. The top row is the same as
in Fig. 6, while the lower rows have averaged the values within a 3 <inline-formula><mml:math id="M41" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 3,
5 <inline-formula><mml:math id="M42" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 5, 7 <inline-formula><mml:math id="M43" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 7, and 9 <inline-formula><mml:math id="M44" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 9 grid box surrounding each individual grid cell.</p></caption>
          <?xmltex \igopts{width=426.791339pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/8373/2018/acp-18-8373-2018-f07.pdf"/>

        </fig>

</sec>
<sec id="Ch1.S3.SS4">
  <title>Selection of spatial averaging scales</title>
      <p id="d1e1292">We examine the impact of increasing the spatial averaging region (Fig. 7)
at four different temporal averaging windows (1, 5, 10, and 20 years) and
for the smallest ozone threshold from the previous section (0.5 ppbv). It is
evident that, at all temporal averaging windows, expanding the number of
surrounding grid cells that are averaged together consistently decreases the
likelihood of exceeding the 0.5 ppbv threshold, although these reductions
are relatively small at the 1-year window, especially over the eastern US.
While increasing the spatial averaging from a single grid cell up to include
the surrounding 81 grid cells (bottom row in Fig. 7) manages to
essentially smooth away much of the spatial heterogeneity in surface ozone
(by moving down any column in Fig. 7); it does not eliminate the
likelihood of exceeding the 0.5 ppbv threshold over much of the eastern US.
For instance, even at a 20-year averaging window, and by averaging together
the surrounding 81 grid cells over locations in the eastern US, there is
still a 20–70 % likelihood of exceeding the 0.5 ppbv threshold due to the
small-scale impact of the meteorological variability on atmospheric
chemistry.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F8"><caption><p id="d1e1297">The maximum potential calculated MDA8 <inline-formula><mml:math id="M45" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> anomaly (ppbv) from
the long-term mean for <bold>(a)</bold> the continental US average and three individual
grid cells taken from <bold>(b)</bold> southern California, demonstrating effective
temporal and spatial averaging; <bold>(c)</bold> the northeast, where spatial averaging
is ineffective; and <bold>(d)</bold> the Rocky Mountains, where spatial averaging
initially reduces the anomaly but then increases the anomaly as surrounding
regions get included in the spatial average. The number of years included in
the temporal averaging window increase along the <inline-formula><mml:math id="M46" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> axis and the number of
grid cells included in the spatial averaging window increase along the
<inline-formula><mml:math id="M47" display="inline"><mml:mi>y</mml:mi></mml:math></inline-formula> axis. A full map of the continental US can be found in the Supplement (Fig. S4).
Note that the color scale is nonlinear, and the color
transitions are selected to match the thresholds established throughout this
paper.</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://acp.copernicus.org/articles/18/8373/2018/acp-18-8373-2018-f08.pdf"/>

        </fig>

</sec>
<sec id="Ch1.S3.SS5">
  <title>Combination of spatial and averaging scales</title>
      <p id="d1e1350">We now examine the combined impact of temporal and spatial averaging on
reducing the influence of small-scale ozone variability in order to enhance
ozone signal detection capabilities. Table S2 summarizes our analysis by
dividing the likelihood of the ozone variability estimates exceeding
selected thresholds away from the long-term mean into four categories: (1) the
length of the averaging window over which ozone is averaged (columns),
(2) the magnitude of the ozone threshold of interest (rows), (3) the
observed (CASTNET) and modeled (MOZ_2000, MOZ_2050, and MOZ_2100) ozone data (sub-columns), and (4) the
size of the spatial extent over which ozone is averaged (sub-rows). A
graphical representation consistent with the data presented in Table S2 is
plotted in Fig. 8 for the continental US average and for three grid cells
that represent various cases. In each plot in Fig. 8, by moving along
columns from left to right, we can see the influence of increasing the size
of the temporal averaging window, and, by moving along rows (from the bottom
to the top), we can see the influence of increasing the spatial averaging
scale. By taking in the entire plot as a whole, we can get a feel for the
combined influence of both temporal and spatial averaging. Figure S4 contains a plot for each grid cell in the continental US.</p>
      <p id="d1e1353">On average within the continental US, both temporal and spatial averaging
are effective at reducing the calculated MDA8 <inline-formula><mml:math id="M48" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> anomaly, although
temporal averaging is more effective (Fig. 8a). There are many grid cells
in the eastern and western US coasts (Fig. 8b and S4),
where both spatial and temporal averaging are effective, but their combined
usage is especially effective. There are also many grid cells where temporal
averaging is effective but spatial averaging is barely effective or not
effective at all (Figs. 8c and  S4). Finally, there are
some grid cells, particularly in the central US (Figs. 8d and  S4), where spatial averaging over smaller regions is effective, but
spatial averaging of larger regions actually increases the calculated MDA8
<inline-formula><mml:math id="M49" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> anomaly by including surrounding grid cells that have higher
variability.</p>
</sec>
</sec>
<sec id="Ch1.S4">
  <title>Discussion</title>
      <p id="d1e1385">We now return to the original four research questions posed in Section 1.
First, what is the magnitude of ozone variability due to meteorology alone
at the smallest scale and what is the impact of increasing the scale of
temporal and spatial averaging? In both observed and modeled MDA8 <inline-formula><mml:math id="M50" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula>
surface data, the small-scale variability driven solely by the
meteorological variability impact on atmospheric chemistry (expressed as the
standard deviation as a percentage of the mean) can exceed 20 % (Table 1,
Fig. 2d). The chemical variability examined here is the result of
fluctuations in meteorology, which itself results from larger-scale
climatological drivers. While variability in emissions also influences
atmospheric chemistry, our analysis has removed the influence of emissions
variability and isolated the variability due to meteorology. A more
comprehensive analysis of chemical variability will need to account for both
meteorological and emission variability, which is complicated by temporal
trends in both the emissions of ozone precursor species and the climate.</p>
      <p id="d1e1399">There is high temporal and spatial heterogeneity of surface ozone
variability (Fig. 2d), with the lowest values found in the western US
(<inline-formula><mml:math id="M51" display="inline"><mml:mo lspace="0mm">&lt;</mml:mo></mml:math></inline-formula> 10%), higher values found in the eastern US (up to 20 %),
and the highest values found over coastal or heavily populated regions (up to
30 %). Averaging over longer temporal scales (by increasing the averaging
window) and over larger spatial scales (by expanding the averaging region)
can reduce the magnitude of the calculated variability, with temporal
averaging proving to be more effective than spatial averaging in most cases
(Fig. 8). In this study, we performed simple spatial averaging, but there
are other methodologies for smoothing two-dimensional signals (e.g.,
Räisänen and Ylhäisi, 2011; Pogson and Smith, 2015) that could
potentially increase signal detection capabilities.</p>
      <p id="d1e1409">Second, are there combinations of temporal and spatial averaging that
maximize the filtration of calculated ozone variability and thus maximize
the potential for signal detection? Figure 8 (and Fig. S4)
demonstrates clearly that there are cases in which the combined usage of
temporal and spatial averaging can reduce the calculated variability better
than either strategy alone (see Fig. 8b), although there are many regions
within the eastern US in which spatial averaging has little to no impact on
reducing the calculated<?pagebreak page8383?> variability (Fig. 8c) or even results in an
increase in the calculated variability (Fig. 8d). There are no such cases
(see  Fig. S4) in which expanding the temporal averaging scale
increases the calculated ozone variability. This could potentially enable
region-specific averaging strategies that help decision-makers identify and
meet regional air quality objectives.</p>
      <p id="d1e1412">Third, are these results dependent on the particular parameterizations of
the CESM CAM-chem model and are they consistent with the available CASTNET
observations? The three CESM CAM-chem simulations exhibited consistent
representations of ozone variability, consistent with our understanding of
future changes to the climate (and meteorology) and the resulting impact on
atmospheric chemistry (Table 1, Figs. 4, S1, and S2). Compared to the
CASTNET observations (which we detrended to remove the influence of changing
precursor emissions), the present-day simulation (MOZ_2000)
exhibited a high ozone bias in the eastern US, while the representation of
the ozone variability is comparable (Table 1).</p>
      <p id="d1e1416">Fourth, how may these strategies be applied to other datasets, be they
chemical, meteorological, or climatological? Much of this analysis could be
applied to any dataset that has spatial and temporal coverage, as long as
some set of acceptable thresholds is provided. While our time step in this
analysis is daily (given the MDA8 <inline-formula><mml:math id="M52" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> metric), and applied only to
summertime (JJA) days, any time step (i.e., hourly, monthly, annual, decadal)
could be utilized as long as cyclical trends (e.g., diurnal or seasonal
cycles) are removed. Indeed, the sliding-scale presentation in Figs. 8 and
S4 can specifically be utilized to identify particular
spatial and temporal scales that are sufficient to identify signals at
particular thresholds and to identify particular geographic regions that are
best suited to identify a given signal. For example, Sofen et al. (2016)
identified regions across the globe where additional observations would be
particularly suited to improve our understanding of surface ozone behavior,
and our analysis could potentially be used to identify particular temporal
and spatial averaging scales that could further maximize the capability for
trend detection. In particular, Sofen et al. (2016) noted that the peak in
the power spectrum of the El Niño–Southern Oscillation (ENSO) on surface
ozone is at the 3.8-year timescale, and that, within some regions within<?pagebreak page8384?> the
US, the amplitude of the ENSO influence on surface ozone approached 0.5 ppbv
(and up to 1.1 ppbv globally). Our analysis shows that there are no grid
cells within the continental US where a 0.5 ppbv signal can be identified at
the 5-year (or shorter) temporal averaging scale (Fig. S4),
but that there are many regions – especially within the western US – in
which even a modest amount of spatial averaging can identify surface ozone
signals below the 1 ppbv level with a 5-year or shorter averaging window.
The type of sliding-scale analysis – in which spatial and temporal
averaging are utilized individually and in combination – as presented in
Figs. 8 and S4 could readily be applied to a wide range
of atmospheric (and other) topics to aid in the capability to identify
signals that exist both in space and in time. In particular, low-frequency
oscillations (e.g., ENSO, and others) and other forms of internally or
externally forced trends (e.g., anthropogenic and natural changes in
emissions) are readily adaptable to this type of analysis, which could
address signals pertaining to precipitation, biogenic emissions, boundary
layer variables, cloud properties, and many others.</p>
      <p id="d1e1430">We did not quantify statistical significance (as in Lewandowsky et al.,
2015) as our goals were to understand the general nature of ozone
variability at all scales and for all signal strengths. Statistical
significance testing (and other statistical techniques) can certainly
provide additional information as to the strengths of ozone signals within
the underlying variability and can be used to extend these results in a
case-by-case manner, but we leave this testing to future studies that can
focus on particular air quality objectives at particular temporal and
spatial scales. Furthermore, future research examining the impact of spatial
and temporal averaging using regional-scale models, models with different
resolutions, and the inclusion of urban observations could provide
additional insight into understanding chemical variability and averaging
techniques.</p>
      <p id="d1e1433">Smaller signals require longer temporal averaging periods to identify.
Figure 4 shows that a 0.5 ppb MDA8 <inline-formula><mml:math id="M53" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> signal will emerge after
15–20 years of temporal averaging. The range here reflects different spatial
averaging domains, with larger domains requiring shorter temporal averaging
windows than smaller domains (i.e., 15 years for averaging over the
continental US and 20 years for averaging over the northeastern US). This
would mean that an average trend of 0.25–0.33 ppb year<inline-formula><mml:math id="M54" 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> would require a
time series of at least 15 years to identify. Similarly, a 1.0 ppb MDA8
<inline-formula><mml:math id="M55" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> signal emerges after 7–15 years, which indicates an average trend
of 0.14–0.67 ppb year<inline-formula><mml:math id="M56" 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> would take at least 7 years to identify. Finally, a
5 ppb signal can be identified in less than 3 years, which indicates that an
average trend of 1.67 ppb year<inline-formula><mml:math id="M57" 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> or greater would only require a 3-year time
series. This presents particular difficulties if the ozone signal of
interest is a trend spanning a time period on the same order. The 10–15 year
averaging timescale we propose translates into a length of time beyond
which you are likely to not see spurious trends above 0.5 ppb, but there are
many cases in which the identification of a small trend is desired with less
than 10–15 years of available data.  For instance, Jiang et al. (2018)
have found that <inline-formula><mml:math id="M58" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">NO</mml:mi><mml:mi>x</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> emissions reductions since 2005 are not as strong
as previously expected, showing a significant slowdown beginning in 2011.
This has large implications for ozone and for short-term decisions for air
quality managers within the United States, who have to promulgate policies
on short-term scales without the luxury of postponing action until longer
and more complete datasets become available. As we have shown, spatial and
temporal variability due to meteorology is high, and the identification and
quantification of trends over 5, 10, or 15 years is difficult, particularly
at small spatial scales.</p>
      <p id="d1e1506">However, as we have shown, a consideration of the impact on variability –
and how variability changes over time – is often pivotal to understanding the
nature of the signals being examined. In this paper, we have provided
methods for quantifying the spatial and temporal variability and strategies
for determining which types of signals are likely detectable at particular
temporal and spatial scales. Some signals,<?pagebreak page8385?> especially small signals at small
scales, are simply not large enough to emerge from the variability and thus
may not be detectable without additional data or expanding the temporal and
spatial averaging scales used for analysis.  Quantifying the signal-to-noise
ratio at a variety of spatial scales, and determining an acceptable
threshold of a particular signal, could be one accessible method for
providing this context. The risk in neglecting the quantification and
contextualization of the magnitude of the ozone signal relative to the
magnitude of the variability induced by the internal meteorology – and the
impact of temporal and spatial averaging – is primarily the risk of drawing
conclusions that are more sensitive to a particular peculiarity in the
underlying variability rather than the signal itself.</p>
</sec>
<sec id="Ch1.S5" sec-type="conclusions">
  <title>Conclusions</title>
      <p id="d1e1516">We quantified the impact of spatial and temporal averaging at different
scales – both individually and combined – on estimates of summertime
surface ozone variability and the resulting likelihood of overconfidence in
estimates of chemical signals over the United States using CASTNET
observations and the CESM CAM-chem model. We simulate three multi-decadal
time periods, each with constant surface emissions, and find that this
analysis is consistent across our simulated time periods and that our
results are not sensitive to particular configurations and parametric
choices within the CESM CAM-chem (i.e., emissions, meteorology, and climate).
We also provide a conceptual framework for gaining understanding of the
influence of spatial and temporal averaging that may be adapted to a wide
range of atmospheric and surface phenomena, provided sufficient spatial and
temporal coverage. Here we focus on summertime surface ozone, a highly
variable (in both space and time) atmospheric constituent with severe human
health impacts and implications for planetary climate, which is the focus of
many local, regional, and national policies. However, these ozone signals
(e.g., temporal trends or regional averages) are frequently small when
compared to the magnitude of the day-to-day ozone variability, and thus
detecting these signals can be challenging. In particular, it would be
impractical to delay interpreting observations for 10–15 years or
alternatively to expand the spatial averaging such that small-scale features
are smoothed away. Nonetheless, it is unwise to over-interpret trends and
signals based on observations from a limited spatial area and over a short
temporal period. Our analysis and conceptual framework presented here cannot
solve this tension, but it does demonstrate some strategies which can allow
for a selection of spatial and temporal averaging scales, and a
consideration of the error threshold, that can aid in this signal detection
on a case-by-case basis. Taking into account the complex interactions
involving trends and variability between emissions, chemistry, meteorology,
and climatology necessitates a variety of strategies. This work quantifies
the impact of spatial and temporal averaging in signal detection, which can
be used in conjunction with ensembles of simulations, statistical
techniques, and other strategies to further our understanding of the
chemical variability in our atmosphere.</p>
      <p id="d1e1519">In order to quantify the impact of spatial and temporal averaging on
summertime ozone variability, we start by selecting four telescoping spatial
regions (the continental US, the eastern US, the northeastern US, and a
single grid cell within the northeastern US) and examine all possible
choices for averaging windows (ranging from daily to multi-decadal windows),
although we focused primarily on averaging windows of 1, 5, 10, and
20 years. We find that – consistent with previous studies – summertime MDA8
<inline-formula><mml:math id="M59" display="inline"><mml:mrow class="chem"><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn mathvariant="normal">3</mml:mn></mml:msub></mml:mrow></mml:math></inline-formula> variability is largest at the smallest spatial and temporal scales
and is frequently on the order of <inline-formula><mml:math id="M60" display="inline"><mml:mo>±</mml:mo></mml:math></inline-formula>10–20 ppbv or which is roughly
15–20 % of the mean ozone signal. In order to minimize the chemical noise
that results from meteorological variability – and thus enhance the signal
– we find averaging windows of 10–15 years (and sometimes longer at the
smaller spatial scales) combined with modest (nearest-neighbor) spatial
averaging substantially improve the capability for signal detection. For
signals that are large compared to the underlying meteorological variability
(e.g., strong emissions reductions), shorter averaging windows and smaller
spatial regions may be used. We recognize that achieving a 10–15 year
temporal averaging window is difficult, but this recommendation is
consistent with recent literature (e.g., Barnes et al., 2016; Garcia-Menendez
et al., 2017). For studies where 10–15 years of averaging is impractical,
we recommend that some spatial and temporal context is provided that
demonstrates that the signals being examined are robust and not the result
of internal variability or noise. We also recognize that our analysis is
just one strategy for enhancing signal detection capabilities and will
ideally be used alongside others, such as perturbed initial condition
ensembles, running simulations with either internal or forced meteorology,
and examining a region or time period with different models or
parameterizations.</p>
      <p id="d1e1540">We show that the largest summertime ozone variability is found in the
eastern US (Figs. 5 and S4), and subsequently there are many regions
within the eastern US where even a 20-year averaging window has a
non-negligible likelihood of estimating ozone variability that is dependent
(with possible error in the 1–3 ppbv range) on the particular years
selected. In addition, over much of the eastern US, simulations of 5 years
or less have a substantial likelihood (40–90 %, Figs. S1 and S2)
of reflecting the influence of meteorological variability on chemistry
rather than the mean state of surface ozone, with the possibility of 5–10 ppbv
error (Fig. S4). While we have detrended the CASTNET observations to
compare to the constant year-2000 cycled emissions in the simulations, the
CASTNET time series inherently includes the compounded variability of both
meteorological and emission sources. Future studies will need to expand this
analysis to include trends and variability in the emissions, as well as in
the meteorology.</p>
      <?pagebreak page8386?><p id="d1e1543">Finally, we demonstrate a conceptual framework that allows for a
sliding-scale view of surface ozone variability, in which both temporal
and spatial averaging is examined at every grid cell within the continental
US. We show that the magnitude of estimates of ozone variability can be
reduced with both temporal and spatial averaging, although temporal
averaging tends to be more effective. While there are many regions in which
both temporal and spatial averaging used in conjunction substantially reduce
the estimate of ozone variability, there are some regions where spatial
averaging is ineffective or even counter-effective. In contrast, this is
not the case for temporal averaging, which consistently reduces the
magnitude of estimated ozone variability. Our analysis could be combined
with other studies (e.g., Sofen et al., 2016) to guide observational and
modeling strategies and identify regions and scales at which particular
signals are most likely to be identified.</p>
</sec>

      
      </body>
    <back><notes notes-type="codedataavailability">

      <p id="d1e1550">The CESM CAM-Chem code is available through the National Center for Atmospheric
Research/University Corporation for Atmospheric Research (NCAR/UCAR)
website (<uri>http://www.cesm.ucar.edu/models/cesm1.2/</uri>, last access: 7 June 2018), and this
project made no code modifications from the released model version.</p>

      <p id="d1e1556">The raw model output is archived on the NCAR servers, and processed data are
archived at <uri>https://dspace.mit.edu/handle/1721.1/114467</uri>, last access: 7 June 2018.</p>
  </notes><app-group>
        <supplementary-material position="anchor"><p id="d1e1562">The supplement related to this article is available online at: <inline-supplementary-material xlink:href="https://doi.org/10.5194/acp-18-8373-2018-supplement" xlink:title="pdf">https://doi.org/10.5194/acp-18-8373-2018-supplement</inline-supplementary-material>.</p></supplementary-material>
        </app-group><notes notes-type="authorcontribution">

      <p id="d1e1571">BBS ran the present-day simulation, analyzed the data, and wrote the
manuscript. EM ran the future climate simulations, while FGM ran the future
atmospheric chemistry simulations and made the data available to BBS. NS,
RP, EM, ST, and LE guided and reviewed the scientific modeling and analysis
process. All authors provided feedback throughout the project and
development of the manuscript.</p>
  </notes><notes notes-type="competinginterests">

      <p id="d1e1577">The authors declare that they have no conflict of interest.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e1583">This model development work was supported by the U.S. Department of Energy
(DOE) grant DE-FG02-94ER61937 to the MIT Joint Program on the Science and
Policy of Global Change. Computational resources for this project were
provided by DOE and a consortium of other government, industry, and
foundation sponsors of the Joint Program. For a complete list of sponsors,
see <uri>http://globalchange.mit.edu</uri> (last access: 7 June 2018). Additional computing
resources were provided by the Climate Simulation Laboratory at NCAR's
Computational and Information Systems Laboratory (CISL), sponsored by the
National Science Foundation and other agencies. The National Center for
Atmospheric Research is funded by the National Science Foundation. The
authors would also like to thank Daniel Rothenberg for efficient processing
of the ozone files.<?xmltex \hack{\newline}?><?xmltex \hack{\newline}?>
Edited by: Jayanarayanan Kuttippurath<?xmltex \hack{\newline}?>
Reviewed by: two anonymous referees</p></ack><ref-list>
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    <!--<article-title-html>Maximizing ozone signals among chemical, meteorological, and climatological variability</article-title-html>
<abstract-html><p>The detection of meteorological, chemical, or other signals in modeled or
observed air quality data – such as an estimate of a temporal trend in
surface ozone data, or an estimate of the mean ozone of a particular region
during a particular season – is a critical component of modern atmospheric
chemistry. However, the magnitude of a surface air quality signal is
generally small compared to the magnitude of the underlying chemical,
meteorological, and climatological variabilities (and their interactions)
that exist both in space and in time, and which include variability in
emissions and surface processes. This can present difficulties for both
policymakers and researchers as they attempt to identify the influence or
signal of climate trends (e.g., any pauses in warming trends), the impact
of enacted emission reductions policies (e.g., United States
NO<sub><i>x</i></sub> State Implementation Plans), or an estimate of the mean
state of highly variable data (e.g., summertime ozone over the northeastern
United States). Here we examine the scale dependence of the variability of
simulated and observed surface ozone data within the United States and the
likelihood that a particular choice of temporal or spatial averaging scales
produce a misleading estimate of a particular ozone signal. Our main
objective is to develop strategies that reduce the likelihood of
overconfidence in simulated ozone estimates. We find that while increasing
the extent of both temporal and spatial averaging can enhance signal
detection capabilities by reducing the noise from variability, a
strategic combination of particular temporal and spatial averaging scales can
maximize signal detection capabilities over much of the continental US. For
signals that are large compared to the meteorological variability (e.g.,
strong emissions reductions), shorter averaging periods and smaller spatial
averaging regions may be sufficient, but for many signals that are smaller
than or comparable in magnitude to the underlying meteorological variability,
we recommend temporal averaging of 10–15 years combined with some level of
spatial averaging (up to several hundred kilometers). If this level of
averaging is not practical (e.g., the signal being examined is at a local
scale), we recommend some exploration of the spatial and temporal variability
to provide context and confidence in the robustness of the result. These
results are consistent between simulated and observed data, as well as within a
single model with different sets of parameters. The strategies selected in
this study are not limited to surface ozone data and could potentially
maximize signal detection capabilities within a broad array of climate and
chemical observations or model output.</p></abstract-html>
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