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  <front>
    <journal-meta><journal-id journal-id-type="publisher">ASCMO</journal-id><journal-title-group>
    <journal-title>Advances in Statistical Climatology, Meteorology and Oceanography</journal-title>
    <abbrev-journal-title abbrev-type="publisher">ASCMO</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Adv. Stat. Clim. Meteorol. Oceanogr.</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">2364-3587</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/ascmo-6-31-2020</article-id><title-group><article-title>Possible impacts of climate change on fog in the Arctic and subpolar North Atlantic</article-title><alt-title>Possible impacts of climate change on fog in the Arctic and subpolar North Atlantic</alt-title>
      </title-group><?xmltex \runningtitle{Possible impacts of climate change on fog in the Arctic and subpolar North Atlantic}?><?xmltex \runningauthor{R.~E.~Danielson et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1 aff2">
          <name><surname>Danielson</surname><given-names>Richard E.</given-names></name>
          <email>rickedanielson@gmail.com</email>
        <ext-link>https://orcid.org/0000-0002-2025-0707</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Zhang</surname><given-names>Minghong</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2">
          <name><surname>Perrie</surname><given-names>William A.</given-names></name>
          
        </contrib>
        <aff id="aff1"><label>1</label><institution>Danielson Associates Office Inc., Halifax, Nova Scotia, Canada</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>Fisheries and Oceans Canada, Bedford Institute of Oceanography, Dartmouth, Nova Scotia, Canada</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Richard E. Danielson (rickedanielson@gmail.com)</corresp></author-notes><pub-date><day>30</day><month>April</month><year>2020</year></pub-date>
      
      <volume>6</volume>
      <issue>1</issue>
      <fpage>31</fpage><lpage>43</lpage>
      <history>
        <date date-type="received"><day>31</day><month>December</month><year>2019</year></date>
           <date date-type="rev-recd"><day>25</day><month>March</month><year>2020</year></date>
           <date date-type="accepted"><day>26</day><month>March</month><year>2020</year></date>
      </history>
      <permissions>
        <copyright-statement>Copyright: © 2020 Richard E. Danielson et al.</copyright-statement>
        <copyright-year>2020</copyright-year>
      <license license-type="open-access"><license-p>This work is licensed under the Creative Commons Attribution 4.0 International License. To view a copy of this licence, visit <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/4.0/">https://creativecommons.org/licenses/by/4.0/</ext-link></license-p></license></permissions><self-uri xlink:href="https://ascmo.copernicus.org/articles/6/31/2020/ascmo-6-31-2020.html">This article is available from https://ascmo.copernicus.org/articles/6/31/2020/ascmo-6-31-2020.html</self-uri><self-uri xlink:href="https://ascmo.copernicus.org/articles/6/31/2020/ascmo-6-31-2020.pdf">The full text article is available as a PDF file from https://ascmo.copernicus.org/articles/6/31/2020/ascmo-6-31-2020.pdf</self-uri>
      <abstract><title>Abstract</title>
    <p id="d1e101">A conventional parameterization of midlatitude warm fog occurrence,
based on in situ observations, is employed to estimate marine
surface visibility in the Arctic and North Atlantic from three
datasets: an ensemble member of the Hadley Earth System (HadGEM2)
model and a nested regional WRF simulation that follow historical
and future emissions scenarios for 1979–2100, and the ERA-Interim
reanalysis for 1979–2004.  Over large scales (of an entire year and
region), all three gridded datasets agree well in terms of variables
like surface air temperature, whose systematic differences seem
small by comparison with its predicted change over the course of
this century.  On the other hand, systematic differences are more
apparent in large-scale estimates of relative humidity and
visibility.  Large differences are attributed to a sensitivity to
representation bias that is inherent in the formulation of each
individual model and analysis.</p>
    <p id="d1e104">Two simple linear calibrations are examined, both of which assume
that an in situ based parameterization is broadly consistent with
the use of marine (ICOADS) observations of air and dew point
temperature as an error-free reference.  A single-step calibration
is considered that takes the mean and variance of ICOADS frequency
distributions as a reference.  A two-step calibration is also
performed in which ICOADS collocations are taken as a reference for
the ERA reanalysis, which in turn is taken as a large-scale
reference for the 1979–2004 HadGEM2 and WRF simulations.  Both
linear calibrations are applied (locally in time and space to air
and dew point temperature) to the future climate scenarios of
HadGEM2 and WRF.  Although ICOADS observations are not error-free
and parameterized visibility estimates are unlikely to capture much
more than half the variance found in observations, attempts are made
to present consistent regional changes in the frequency of high
relative humidity, as a proxy for warm fog occurrence.  The
large-scale decrease in visibility over the 21st century is in the
range of 8 %–12 % in the Arctic and 0 %–5 % in the North Atlantic.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <label>1</label><title>Introduction</title>
      <p id="d1e116">Available global records reveal regions of increasing fog occurrence
over the ocean over long timescales and decreasing occurrence over
land.  <xref ref-type="bibr" rid="bib1.bibx47" id="text.1"/> connect a reduction in dense
fog to a decrease in European aerosol loading during 1976–2006.
Marine visual observations for 1950–2007 reveal a positive summertime
trend in at least two parts of the world where fog is most frequent:
expansive regions of the western North Pacific and North Atlantic,
centered on the Kuril Islands and the Grand Banks, respectively
<xref ref-type="bibr" rid="bib1.bibx16" id="paren.2"/>.  A relative paucity of observations in the
Arctic prohibits similar historical analyses, but observed and
expected increases in moisture availability and temperature motivate
an exploration of both warm and cold fog occurrence (relative to
0 <inline-formula><mml:math id="M1" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C) in this region as well <xref ref-type="bibr" rid="bib1.bibx25" id="paren.3"/>.</p>
      <p id="d1e137">This study seeks to identify baseline long-term changes in warm fog
and visibility that might be expected in the Arctic and North Atlantic
marine regions.  We assert that a growing number of climate
simulations (e.g., <xref ref-type="bibr" rid="bib1.bibx11 bib1.bibx33 bib1.bibx46 bib1.bibx31 bib1.bibx49 bib1.bibx50" id="altparen.4"/>)
permit an initial multiyear prediction.  Our pragmatic assumption is
that the processes resolved by different climate models, explicitly
including sub-synoptic and<?pagebreak page32?> larger scales, provide a basis for
estimating the future trend in fog occurrence.  Contemporary studies,
both observed and modelled <xref ref-type="bibr" rid="bib1.bibx16 bib1.bibx51 bib1.bibx45 bib1.bibx34" id="paren.5"/>, highlight that fog formation and
dissipation are indeed sensitive to these resolved scales.  In an
attempt to approach the fog-process scales, we apply a regional model
downscaling of Hadley Center Earth System model (HadGEM2) global
climate simulations <xref ref-type="bibr" rid="bib1.bibx49 bib1.bibx50" id="paren.6"/> to
provide an enhanced representation of radiative processes and moist
energy transports.  As in situ observations provide a complementary
measure of such processes, this study can be seen as an extension (by
simple statistical modelling) of physical model downscaling.</p>
      <p id="d1e149">It is convenient to estimate visibility for various climate scenarios,
insomuch as parameterizations are available that employ common climate
model variables like surface temperature or relative humidity (e.g.,
<xref ref-type="bibr" rid="bib1.bibx22" id="altparen.7"/>).  With multiple combinations of
models and parameterizations, however, there are at least two related
challenges to identifying a reasonably consistent baseline change.
First, it is well known that different models may seek to represent or
support a variable like surface temperature in subtly different ways.
Bayesian data assimilation, for example, acknowledges a separate
target analysis for each model grid <xref ref-type="bibr" rid="bib1.bibx35 bib1.bibx14 bib1.bibx32" id="paren.8"/>.  Another familiar inconsistency relates to
spatiotemporal representations of a variable by models versus
observations (e.g., <xref ref-type="bibr" rid="bib1.bibx36 bib1.bibx43" id="altparen.9"/>).  Based
on a prior averaging of cloud observations, <xref ref-type="bibr" rid="bib1.bibx23" id="text.10"/>
conclude that input data representation is critical for tuned
parameterizations of fog and visibility.  Of course, differences in
representation by separate models, for example, are prevalent even at
a common resolution.  That is, any aspect of a model may ultimately
determine its representation, from initialization and core numerics to
physical parameterizations and a final vertical extrapolation to the
surface.  We may recognize a need to map between two representations,
but given sometimes subtle differences in the <italic>target</italic> of distinct
observations, models, and analyses, as well as the challenges of
mapping (e.g., <xref ref-type="bibr" rid="bib1.bibx17 bib1.bibx37" id="altparen.11"/>), representation
differences are to be expected nonetheless.</p>
      <p id="d1e171">A related challenge to identifying a baseline change in relative
humidity and visibility is that rudimentary and advanced estimates
alike can be sensitive to a representation of the variables used to
calculate them.  Observational support is given by <xref ref-type="bibr" rid="bib1.bibx26" id="text.12"><named-content content-type="post">their
Fig. 10</named-content></xref>, where visibility varies during the
course of a day between 50 km and a few meters within a relative
humidity range of 92 %–98 %.  By convention, fog is defined as
visibility of less than 1 km and is often identified with a
relative humidity of greater than 95 %.
<xref ref-type="bibr" rid="bib1.bibx22" id="text.13"/> note that the lack of a consistent
representation of surface relative humidity has led to numerous
proposed visibility parameterizations, perhaps applicable to one model
each.  In our search for a baseline change among multiple models,
because the calculation of relative humidity and visibility are
sensitive to a representation of their input variables, it is
instructive to explore whether systematic differences among models can
be adjusted to yield so-called homogeneous datasets.  In other words,
we seek a baseline that nominally employs a common reference of
visibility to which all our estimates can be calibrated.</p>
      <p id="d1e183">We begin with a parameterization of visibility based on in situ
observations of relative humidity with respect to water.  Because
marine observations (e.g., ships) generally include air and dew point
temperature (and thus relative humidity), they provide a proxy
representation for the climate models of interest.  Following
<xref ref-type="bibr" rid="bib1.bibx25" id="text.14"/>, however, a parameterization of warm fog can
be more accurately expressed in terms of condensation nuclei, liquid
water content, and drop size distribution (among other variables).  By
comparison, rudimentary parameterizations are sometimes described as
yielding a form of “relative humidity mist”.  We also acknowledge
that a model approximation of warm fog can cover a domain (i.e., a
grid box) that is larger than an entire marine fog event.  Our chosen
parameterization is expected to capture neither the intensity of warm
fog events nor processes that govern cold fog below 0 <inline-formula><mml:math id="M2" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C nor ice
fog below about <inline-formula><mml:math id="M3" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">20</mml:mn></mml:mrow></mml:math></inline-formula> <inline-formula><mml:math id="M4" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C <xref ref-type="bibr" rid="bib1.bibx24 bib1.bibx25" id="paren.15"/>.  Finally, in selecting an in situ based
parameterization, we consider the corresponding in situ representation
(i.e., of the input variables air and dew point temperature) to be our
target or true representation.  Although any estimate of visibility
involves a parameterization that is at least partly empirical, and
almost as challenging to relate to prognostic model variables as fog
itself <xref ref-type="bibr" rid="bib1.bibx10 bib1.bibx48 bib1.bibx34" id="paren.16"/>, this
in situ representation is not necessarily optimal.  However, it is a
separate ongoing challenge that, even for a precise instrument,
measurement error ranging from 10 % to 50 % (and more in Arctic winter
conditions) is common <xref ref-type="bibr" rid="bib1.bibx25" id="paren.17"/>.</p>
      <p id="d1e227">A somewhat broader accommodation of targets for truth and error is
explored in the context of more than one visibility parameterization
by <xref ref-type="bibr" rid="bib1.bibx12" id="text.18"/>.  This parallel exercise points to
relative humidity as a key source of information and allows us to
focus on an in situ based, midlatitude parameterization.  To establish
consistent baseline 21st century trends for either the Arctic or North
Atlantic, we focus on a homogeneous calibration of gridded historical
estimates of surface air and dew point temperature.  Such a
calibration is called homogeneous because it seeks to make one dataset
as consistent as possible with another.  In accordance with our assumption
of an error-free ICOADS reference, we adopt ordinary linear regression
as our statistical calibration model (a justification is given in the
Appendix).  Ship and fixed platform marine observations are then taken
as a large-scale reference for all model simulations, either directly
or indirectly via surface variables of the ERA-Interim reanalysis
<xref ref-type="bibr" rid="bib1.bibx43 bib1.bibx44" id="paren.19"/>.  Individual datasets
that nominally overlap with each other during the 1979–2004 historical
period are described in Sect. 2.  A visibility<?pagebreak page33?> parameterization and
two exploratory methods of linearly reconciling climate model
simulations to observations are discussed in Sect. 3.  The resulting
high relative humidity and low visibility estimates are then used in
Sect. 4 to indicate possible 21st century trends in fog.
Conclusions are provided in Sect. 5.</p>
</sec>
<sec id="Ch1.S2">
  <label>2</label><title>Data</title>
<sec id="Ch1.S2.SS1">
  <label>2.1</label><title>Regional WRF simulations</title>
      <p id="d1e251">The HadGEM2 model family is a comprehensive global Earth System model
including terrestrial and ocean ecosystems and their carbon cycling,
aerosols, and selected chemical constituents
<xref ref-type="bibr" rid="bib1.bibx11" id="paren.20"/>.  The model employs 38 levels above the
ocean surface and 40 levels below, without the need for flux
corrections in daily coupled simulations of its atmospheric
(discretized at 1.25<inline-formula><mml:math id="M5" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> latitude by 1.875<inline-formula><mml:math id="M6" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> longitude,
i.e., with a resolution of O[100 km]) and oceanic (discretized at
1<inline-formula><mml:math id="M7" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> poleward of 30<inline-formula><mml:math id="M8" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>) components.  Comments on physical
parameterizations of HadGEM2 in relation to downscaled WRF simulations
are provided by <xref ref-type="bibr" rid="bib1.bibx49" id="text.21"/>.  This study focuses on two
regional configurations of the Weather Research and Forecasting (WRF)
model, which are driven at lateral and lower boundaries by a selected
ensemble member of the HadGEM2 Earth System CMIP5 simulations.
Lateral boundaries can be seen in Fig. <xref ref-type="fig" rid="Ch1.F1"/>, at least where in
situ collocations exist poleward of 60<inline-formula><mml:math id="M9" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N in the Arctic and
30<inline-formula><mml:math id="M10" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N in the Atlantic.  A computation of dew point temperature
and essential mass, motion, and surface boundary conditions for WRF
are obtained from the HadGEM2 database of historical (6-hourly for
1979–2004) and representative concentration pathway (RCP) 4.5 and 8.5
emissions scenario (6-hourly for 2005–2100, but with surface variables
archived daily) simulations <xref ref-type="bibr" rid="bib1.bibx46 bib1.bibx31" id="paren.22"/>.</p>
      <p id="d1e320">Two slightly different configurations of the Weather Research and
Forecasting (WRF) model are employed for the Arctic and North Atlantic
domains.  These are subject to 6-hourly boundary forcing and a minor
nudging on the interior toward the HadGEM2 upper tropospheric,
large-scale flow <xref ref-type="bibr" rid="bib1.bibx21" id="paren.23"/>.  Both configurations employ
the polar-optimized version (3.6) of WRF <xref ref-type="bibr" rid="bib1.bibx30" id="paren.24"/> and
the same dynamical core (called ARW) with 38 vertical sigma levels,
but on 25 km polar stereographic and 30 km Lambert conformal grids,
respectively.  Parameterizations common to the two domains include
those of longwave radiation (Rapid Radiative Transfer Model), land
surface (Unified NOAH scheme), planetary boundary layer
(Mellor–Yamada–Janjic scheme), and cloud microphysics (Morrison
two-moment scheme).  The Arctic and North Atlantic simulations differ in
terms of their parameterizations of shortwave radiation (respectively,
new Goddard scheme versus Rapid Radiative Transfer Model) and cumulus
parameterization (Kain–Fritsch versus Grell–Devenyi ensemble scheme).
For both the Arctic and North Atlantic simulations, an evaluation of
cyclone statistics reveals good agreement with the ERA-Interim
reanalysis in comparison to the original HadGEM2 forcing fields
<xref ref-type="bibr" rid="bib1.bibx49 bib1.bibx50" id="paren.25"/>.  During the course of each
multidecadal WRF simulation, snapshots of 2 m (surface) variables are
obtained every 6 h by extrapolation from the lowest model level
(close to 30 m).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1" specific-use="star"><?xmltex \currentcnt{1}?><label>Figure 1</label><caption><p id="d1e334">Ship and fixed platform marine observations of <bold>(a, b)</bold> fog and
<bold>(c, d)</bold> non-fog visibility taken between January 1979 and December 2004 to the north of <bold>(a, c)</bold> 60<inline-formula><mml:math id="M11" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N in the Arctic and
<bold>(b, d)</bold> 30<inline-formula><mml:math id="M12" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N in the North Atlantic and within regional WRF
model domains.  Titles show the total number of ICOADS positions
and observations, given at 0.1<inline-formula><mml:math id="M13" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> resolution with
order-of-magnitude color labels in <bold>(a)</bold>.</p></caption>
          <?xmltex \igopts{width=355.659449pt}?><graphic xlink:href="https://ascmo.copernicus.org/articles/6/31/2020/ascmo-6-31-2020-f01.png"/>

        </fig>

</sec>
<sec id="Ch1.S2.SS2">
  <label>2.2</label><title>ERA-Interim reanalysis</title>
      <p id="d1e394">A 12-hourly sequential data assimilation system is used in the
European Centre for Medium-Range Weather Forecasting Reanalysis (ERA)
Interim production of a global atmosphere and ocean surface wave
evolution from 1979 onward <xref ref-type="bibr" rid="bib1.bibx15" id="paren.26"/>.  For the atmosphere
above the surface, a four-dimensional variational (4D-Var) analysis is
performed to obtain model initial conditions and adjustments for
selected satellite radiance observations.  Within this system, an
accommodation of evolving systematic differences between the model and
observations is thus made <xref ref-type="bibr" rid="bib1.bibx14" id="paren.27"/>.  The 4D-Var cost function
minimization includes a time-varying specification of error covariance
for the prognostic variables and a fixed error covariance for a wide
range of observations.  A spectral model with 60 vertical levels and
an effective horizontal resolution of about 80 km is employed.  It is
notable that the ERA-Interim 2 m surface variables are not just
extrapolated from the lowest model level (like WRF snapshots), but,
following <xref ref-type="bibr" rid="bib1.bibx36" id="text.28"/>, are also combined with in situ
observations using an optimal interpolation that is separate from the
4D-Var analysis <xref ref-type="bibr" rid="bib1.bibx43 bib1.bibx44" id="paren.29"/>.
Six-hourly surface analyses from 1979 to 2004 are obtained from an
archive <xref ref-type="bibr" rid="bib1.bibx4" id="paren.30"/> that is oversampled at
0.25<inline-formula><mml:math id="M14" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> in latitude and longitude and facilitates land–ocean
boundary matching on the WRF Arctic and North Atlantic domains.</p>
</sec>
<sec id="Ch1.S2.SS3">
  <label>2.3</label><title>ICOADS observations</title>
      <p id="d1e430">In situ surface marine observations of the International Comprehensive
Ocean-Atmosphere Data Set (ICOADS Version 3;
<xref ref-type="bibr" rid="bib1.bibx18" id="altparen.31"/>) are taken as a reference for diagnoses of
visibility between January 1979 and December 2004.  To ensure that
observations are of high quality, we consider only a full range of
valid variables (wind speed and direction, sea level pressure, air,
dew point, and sea surface temperature, present weather, and
visibility) and the strictest ICOADS trimming (i.e., values of air and
sea surface temperature, zonal and meridional wind component, sea-level pressure, and relative humidity are within 2.8 standard
deviations of a smoothed monthly climatology).  About 1 % of
these observations are excluded if any duplication of all variables
(including latitude and longitude) is found within a few hours of an
existing observation.  Also, observations are excluded if any type of
precipitation was falling at the time visibility was observed.
This is done to emphasize hydrometeors of less than about 30 <inline-formula><mml:math id="M15" display="inline"><mml:mrow class="unit"><mml:mi mathvariant="normal">µ</mml:mi><mml:mi mathvariant="normal">m</mml:mi></mml:mrow></mml:math></inline-formula>
(i.e., fog) in determining visibility <xref ref-type="bibr" rid="bib1.bibx25" id="paren.32"/>.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2"><?xmltex \currentcnt{2}?><label>Figure 2</label><caption><p id="d1e451">Simulated HadGEM2 (blue), WRF (black), and analyzed ERA
(red) areal average trends in Arctic (left panels) and North
Atlantic (right panels) <bold>(a, b)</bold> air temperature (<inline-formula><mml:math id="M16" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C), <bold>(c, d)</bold> dew
point temperature (<inline-formula><mml:math id="M17" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C), <bold>(e, f)</bold> specific humidity
(g kg<inline-formula><mml:math id="M18" 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>), <bold>(g, h)</bold> relative humidity (%), and <bold>(i, j)</bold> visibility
(km) at 2 m above the surface.  The WRF and ERA averages are taken
over fixed ocean domains (regardless of sea ice) of 15 (Arctic)
and 13 (North Atlantic) million square kilometers.  The HadGEM2
domains are about 25 % larger and include coastal overlap as these
data are at lower resolution.  Note that ordinate scales differ on
the left and right, but their spans are equal.</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://ascmo.copernicus.org/articles/6/31/2020/ascmo-6-31-2020-f02.png"/>

        </fig>

      <?pagebreak page34?><p id="d1e506"><?xmltex \hack{\newpage}?>Visibility is recorded in the ICOADS dataset as one of 10 categories
ranging from less than 50 m to over 50 km (5 categories of 1 km or
less and 5 of 2 km or more).  An observer may judge the densest
fog categories by the visibility of shipboard objects on large ships,
and otherwise by the appearance of the horizon, whose distance is a
function of height above the sea <xref ref-type="bibr" rid="bib1.bibx39" id="paren.33"/>.  All
observations of a given category are selected, but only to a maximum
of 10 000 (randomly selected) so as not to emphasize the more common
non-fog conditions.  Total numbers of fog and non-fog observations,
taken from within WRF domains and north of 60<inline-formula><mml:math id="M19" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N in the Arctic
and 30<inline-formula><mml:math id="M20" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> N in the North Atlantic, are shown in Fig. <xref ref-type="fig" rid="Ch1.F1"/>.
Non-fog observations (Fig. <xref ref-type="fig" rid="Ch1.F1"/>c, d) are more distributed
geographically and the Arctic fog-only categories (Fig. <xref ref-type="fig" rid="Ch1.F1"/>a)
are fewer in number.  The greatest frequency of observations are at
fixed oil platforms and along major shipping routes.  High-latitude
observations are preferentially from the warm season
<xref ref-type="bibr" rid="bib1.bibx16" id="paren.34"/> and data voids occur where sea ice cover is
typical.  The resulting collocation archive is given by
<xref ref-type="bibr" rid="bib1.bibx13" id="text.35"/>.</p>
</sec>
</sec>
<sec id="Ch1.S3">
  <label>3</label><title>Methods</title>
<sec id="Ch1.S3.SS1">
  <label>3.1</label><title>Visibility parameterization</title>
      <p id="d1e560">Uncalibrated estimates of 21st century visibility (Fig. <xref ref-type="fig" rid="Ch1.F2"/>)
are diagnosed directly from the HadGEM2 and WRF models, following
historical emissions (1979–2004) and two future (2005–2100)
representative concentration pathway (RCP 4.5 and 8.5) emissions
scenarios <xref ref-type="bibr" rid="bib1.bibx38 bib1.bibx33 bib1.bibx46 bib1.bibx49 bib1.bibx50" id="paren.36"/>.  Corresponding ERA-Interim
visibility estimates are included for the historical period.  All
variables are averaged over marine regions of the Arctic or North
Atlantic model domains using a centered 365 d window.  Locally in
time and space, surface visibility (Fig. <xref ref-type="fig" rid="Ch1.F2"/>i, j) is first
diagnosed from relative humidity (Fig. <xref ref-type="fig" rid="Ch1.F2"/>g, h), which in turn
is derived from temperature (Fig. <xref ref-type="fig" rid="Ch1.F2"/>a, b) and dew point
(Fig. <xref ref-type="fig" rid="Ch1.F2"/>c, d).  We estimate visibility using the median curve
fit of <xref ref-type="bibr" rid="bib1.bibx22" id="text.37"><named-content content-type="post"><inline-formula><mml:math id="M21" display="inline"><mml:mrow><mml:mn mathvariant="normal">40.1</mml:mn><mml:mo>-</mml:mo><mml:mn mathvariant="normal">5.19</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">10</mml:mn></mml:mrow></mml:msup><mml:mspace width="0.25em" linebreak="nobreak"/><mml:msup><mml:mtext>[relative
humidity]</mml:mtext><mml:mn mathvariant="normal">5.44</mml:mn></mml:msup></mml:mrow></mml:math></inline-formula></named-content></xref> to be consistent
with <xref ref-type="bibr" rid="bib1.bibx12" id="text.38"/>, but by their definition of
performance, slightly reduced and improved performance is available
using the bracketing curve fits that <xref ref-type="bibr" rid="bib1.bibx22" id="text.39"/>
provide (i.e., their 5 % and 95 % curves, respectively).  All curve
fits are based on instrument<?pagebreak page35?> observations of relative humidity and
visibility taken during the summers of 2006 and 2007 in Lunenburg,
Nova Scotia.</p>
      <p id="d1e614">Positive 100-year trends in temperature, dew point, and specific
humidity are generally larger than the difference between simulations
and the ERA-Interim reanalysis during the historical period, both in
the Arctic and North Atlantic.  On the other hand, the increase in
relative humidity and decrease in visibility (with greater 100-year
changes in the Arctic) can be smaller than historical differences
among simulations and the ERA analysis.  Such a large discrepancy in
historical diagnoses of visibility begs the question of how to
interpret corresponding future trends.  For instance, the HadGEM2 air
and dew point temperature estimates are low in part because, in lieu
of an interpolation to higher resolution, we opt to average over a
larger area that includes some overlap with land.  The WRF relative
humidity and visibility estimates are different in part because, as
snapshots of a long integration, they represent localized
supersaturation to a greater extent than other estimates (and in situ
observations in particular).  Given that our chosen parameterization
of visibility itself targets a particular in situ and warm fog
representation, which is not necessarily accommodating of such
differences, a mapping between each input dataset and an in situ
representation is explored.</p>
</sec>
<sec id="Ch1.S3.SS2">
  <label>3.2</label><title>Historical linear calibration</title>
      <p id="d1e625">The large-scale differences in Fig. <xref ref-type="fig" rid="Ch1.F2"/> seem relatively
constant in time, which suggests that representation bias in each
gridded dataset is also relatively constant.  A reconciliation of
gridded data to a highly resolved representation (historical ICOADS
observations) is often sought by some combination of physical (e.g.,
<xref ref-type="bibr" rid="bib1.bibx49 bib1.bibx50" id="altparen.40"/>) and statistical
calibration <xref ref-type="bibr" rid="bib1.bibx17 bib1.bibx37" id="paren.41"/>, both of which can be
considered nonlinear in general.  A notable advance in statistical
calibration by <xref ref-type="bibr" rid="bib1.bibx19" id="text.42"/> established a mapping
between two measures of marine wind speed by matching their cumulative
distribution functions (CDFs).  Mapping between satellite and ERA-Interim soil moisture is examined by <xref ref-type="bibr" rid="bib1.bibx29" id="text.43"/>, who finds
that a linear mapping (by matching the distribution mean and variance)
is similar in performance to a nonlinear mapping (including higher
moments).  <xref ref-type="bibr" rid="bib1.bibx17" id="text.44"/> and <xref ref-type="bibr" rid="bib1.bibx37" id="text.45"/> discuss the
benefits and limitations of a range of approaches, such as quantile
mapping, which <xref ref-type="bibr" rid="bib1.bibx2" id="text.46"/> employ in a separate
calibration of each variable in a multivariate regional climate
dataset.  More recent studies highlight the importance of simultaneous
multivariate calibration <xref ref-type="bibr" rid="bib1.bibx8 bib1.bibx9" id="paren.47"/>.</p>
      <p id="d1e655">Although nonlinear calibration may be appropriate, we explore two
linear adjustments because their physical interpretation is direct and
the ICOADS reference is assumed to be error-free (comments on
calibration to an error-free reference are given in the Appendix).
Perhaps the simplest strategy is a two-step calibration, in which we
calibrate ERA using the ICOADS collocations in Fig. <xref ref-type="fig" rid="Ch1.F1"/> (step
one) and then calibrate HadGEM2 and WRF to ERA (after adjustment)
using the values in Fig. <xref ref-type="fig" rid="Ch1.F2"/> (i.e., using large-scale annual
and areal averages; step two).  Although relative humidity estimates
in Fig. <xref ref-type="fig" rid="Ch1.F2"/> could be adjusted to ICOADS directly, instead
univariate linear calibrations are applied (locally in space and time)
to air and dew point temperature and the remaining variables are
calculated from these.  We note that an alternate estimate of HadGEM2
visibility is also possible, in which archived daily averages of
specific humidity are first calibrated before a dew point estimate is
obtained (cf. dew point archival for WRF, ERA, and ICOADS).  Unless the
HadGEM2 dew point is calculated before it is calibrated, however,
differences in Fig. <xref ref-type="fig" rid="Ch1.F2"/> seem to persist (not shown).</p>

<?xmltex \floatpos{t}?><table-wrap id="Ch1.T1" specific-use="star"><?xmltex \currentcnt{1}?><label>Table 1</label><caption><p id="d1e669">Homogeneous single- and two-step calibrations of Arctic and
North Atlantic 2 m air temperature (AT) and dew point temperature
(DPT) for 1979–2004.  Shown are additive and multiplicative
adjustments (left/right numbers) of the ERA reanalysis with
reference to all ICOADS collocations in Fig. <xref ref-type="fig" rid="Ch1.F1"/>.
Similarly, adjustments in WRF and HadGEM2 are with reference to
ICOADS in the single-step calibration and with reference to the
ERA time series in Fig. <xref ref-type="fig" rid="Ch1.F2"/> (after adjustment) in the
two-step calibration.  The additive adjustment unit is <inline-formula><mml:math id="M22" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C.</p></caption><oasis:table frame="topbot"><oasis:tgroup cols="5">
     <oasis:colspec colnum="1" colname="col1" align="left"/>
     <oasis:colspec colnum="2" colname="col2" align="right"/>
     <oasis:colspec colnum="3" colname="col3" align="right" colsep="1"/>
     <oasis:colspec colnum="4" colname="col4" align="right"/>
     <oasis:colspec colnum="5" colname="col5" align="right"/>
     <oasis:thead>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1"/>
         <oasis:entry namest="col2" nameend="col3" align="center" colsep="1">Single-step </oasis:entry>
         <oasis:entry namest="col4" nameend="col5" align="center">Two-step </oasis:entry>
       </oasis:row>
     </oasis:thead>
     <oasis:tbody>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">Arctic</oasis:entry>
         <oasis:entry colname="col2">AT</oasis:entry>
         <oasis:entry colname="col3">DPT</oasis:entry>
         <oasis:entry colname="col4">AT</oasis:entry>
         <oasis:entry colname="col5">DPT</oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">ERA</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M23" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.18</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">1.01</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M24" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.34</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">1.00</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M25" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.36</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">0.98</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M26" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.53</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">0.96</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">WRF</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M27" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.98</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">0.92</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M28" display="inline"><mml:mrow><mml:mn mathvariant="normal">2.04</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">0.82</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M29" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.67</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">1.00</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M30" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.02</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">1.00</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">HadGEM2</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M31" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.43</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">1.08</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M32" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.64</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">1.02</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M33" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1.73</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">1.00</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M34" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1.78</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">1.00</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row rowsep="1">
         <oasis:entry colname="col1">North Atlantic</oasis:entry>
         <oasis:entry namest="col2" nameend="col5" align="center"/>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">ERA</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M35" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.41</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">0.97</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M36" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.83</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">0.95</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M37" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.65</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">0.95</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M38" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.97</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">0.94</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">WRF</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M39" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1.93</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">1.06</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M40" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1.97</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">1.11</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M41" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">0.38</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">1.00</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M42" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.48</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">1.00</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
       <oasis:row>
         <oasis:entry colname="col1">HadGEM2</oasis:entry>
         <oasis:entry colname="col2"><inline-formula><mml:math id="M43" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">3.72</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">1.14</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col3"><inline-formula><mml:math id="M44" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">4.07</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">1.16</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col4"><inline-formula><mml:math id="M45" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2.10</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">1.00</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
         <oasis:entry colname="col5"><inline-formula><mml:math id="M46" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2.05</mml:mn><mml:mo>/</mml:mo><mml:mn mathvariant="normal">1.00</mml:mn></mml:mrow></mml:math></inline-formula></oasis:entry>
       </oasis:row>
     </oasis:tbody>
   </oasis:tgroup></oasis:table></table-wrap>

      <p id="d1e1120">By construction, the ERA reanalysis has a synoptic correlation with
ICOADS observations.  The HadGEM2 and<?pagebreak page36?> nested WRF models follow a
distinct synoptic evolution and thus match observations of the
1979–2004 historical period only by coincidence
<xref ref-type="bibr" rid="bib1.bibx46 bib1.bibx37" id="paren.48"/>.  However, a single-step
calibration is also feasible that matches the distributions of HadGEM2
and WRF air and dew point temperature to those of ICOADS.  Our
ordinary linear regression implementation of CDF matching
<xref ref-type="bibr" rid="bib1.bibx19 bib1.bibx29" id="paren.49"/> adjusts the mean and
variance of the gridded in situ collocations over the historical
period, after separately ranking both by magnitude.  For consistency,
ranking is also applied to the ERA and ICOADS collocations, although
in a shared synoptic sense, ERA-ICOADS pairings are largely ranked to
begin with.  In summary, both the single-step and two-step linear
calibrations can be considered large-scale adjustments based on the
historical collocations of Fig. <xref ref-type="fig" rid="Ch1.F1"/> and the historical areal
and annual averages of Fig. <xref ref-type="fig" rid="Ch1.F2"/>, respectively.</p>
</sec>
</sec>
<sec id="Ch1.S4">
  <label>4</label><title>Future trends in relative humidity and visibility</title>
      <p id="d1e1142">A linear calibration of collocated air or dew point temperature is
capable of matching the mean and variance of HadGEM2, WRF, and ERA
distributions to those of ICOADS.  In spite of a preexisting
conformity of ERA surface variables to in situ observations
<xref ref-type="bibr" rid="bib1.bibx36 bib1.bibx43 bib1.bibx44" id="paren.50"/>, the
assumption of no ICOADS error yields, unsurprisingly, a slight
adjustment of ERA temperature and dew point (Table <xref ref-type="table" rid="Ch1.T1"/>).  Also
as expected, adjustment is smaller (i.e., the additive component is
closer to zero and the multiplicative component is closer to one) when
the ICOADS and ERA collocation data are separately ranked
(single-step) than when they are unranked (two-step, where the first
step preserves synoptic pairing).  The single-step adjustment of
HadGEM2 and WRF generally involves non-negligible additive and
multiplicative components, whereas in two-step adjustment (to ERA),
the multiplicative component is negligible (equal to one) and the
additive component is similar in the Arctic and North Atlantic
(cf. Fig. <xref ref-type="fig" rid="Ch1.F2"/>).  For brevity in the remainder of this section,
single-step calibration is discussed in the context of our two-step
results.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3"><?xmltex \currentcnt{3}?><label>Figure 3</label><caption><p id="d1e1154">Distribution shifts under a homogeneous two-step
calibration.  Shown are the fraction of 59 966 Arctic (left panels)
and 94 703 North Atlantic (right panels) collocations of
Fig. <xref ref-type="fig" rid="Ch1.F1"/>, as a function of calibrated (solid lines) and
uncalibrated (dashed lines) <bold>(a, b)</bold> air temperature, <bold>(c, d)</bold> dew point
temperature, and <bold>(e, f)</bold> relative humidity with respect to water (at
0.5 <inline-formula><mml:math id="M47" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C and 1 % intervals, respectively, with a three-point
smoothing) for the 26-year historical period.  Fractions are shown
on a logarithmic scale for the ICOADS observations (green lines),
ERA reanalysis (red lines), and WRF (black lines) and HadGEM2
(blue lines) models.  Note that WRF boundaries are constrained to
the HadGEM2 freely evolving synoptic evolution, whereas the ICOADS
and ERA collocations sample the observed 1979–2004 synoptic
evolution.</p></caption>
        <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://ascmo.copernicus.org/articles/6/31/2020/ascmo-6-31-2020-f03.png"/>

      </fig>

      <p id="d1e1183">Figure <xref ref-type="fig" rid="Ch1.F3"/>a–d reveal good similarity in ERA (red) and ICOADS
(green) distributions of air and dew point temperature, both before
(dashed) and after (solid) calibration.  As in Fig. <xref ref-type="fig" rid="Ch1.F2"/>, WRF
is a nested model whose representation of temperature differs from the
HadGEM2 driving model, and both differ somewhat from the ERA and
ICOADS distributions.  The calibration of HadGEM2 is more apparent
than for WRF, with a shift of about 2 <inline-formula><mml:math id="M48" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C in all temperature
distributions (Table <xref ref-type="table" rid="Ch1.T1"/>).  Essentially by design, however,
differences in the shape of each distribution are unchanged after both
the single-step and two-step calibrations.  Figure <xref ref-type="fig" rid="Ch1.F3"/>e, f
reveal greater variation in the representations of relative humidity
and less similarity with ICOADS.  The contrast with WRF is most
apparent, but in general, ICOADS observations sample more evenly a
range in relative humidity from 45 % to 50 % to a limit of just over 95 %.
In turn, a linear calibration of temperature has the desired impact of
shifting all gridded relative humidity distributions towards drier
conditions, but because uncalibrated WRF relative humidity is quite
frequently high, linear calibration shifts the peak of its
distribution by as much as 5 % to 10 %. This occurs following both the
single-step and two-step calibrations and highlights the challenge of
conserving relationships between variables in univariate (marginal)
adjustments <xref ref-type="bibr" rid="bib1.bibx17 bib1.bibx37 bib1.bibx9" id="paren.51"/>.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4"><?xmltex \currentcnt{4}?><label>Figure 4</label><caption><p id="d1e1210">As in Fig. <xref ref-type="fig" rid="Ch1.F2"/> but after a homogeneous two-step
calibration of the WRF and HadGEM2 simulations to the analyzed ERA
time series, which in turn is calibrated to the ICOADS
collocations of the historical period (1979–2004).</p></caption>
        <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://ascmo.copernicus.org/articles/6/31/2020/ascmo-6-31-2020-f04.png"/>

      </fig>

      <p id="d1e1221">Comparison of the single-step and two-step calibrations suggests that,
in this study, it is more appropriate to employ an additive
calibration.  As noted above, if ERA-ICOADS differences are ignored,
then the single-step calibration is multiplicative, whereas the
two-step calibration is additive (Table <xref ref-type="table" rid="Ch1.T1"/>).  Both are
applied locally in time and space, but unfortunately, the annual and
areal averages of a single-step calibration (not shown) do not yield
the degree of similarity shown in Fig. <xref ref-type="fig" rid="Ch1.F4"/>.  Both before
(Fig. <xref ref-type="fig" rid="Ch1.F2"/>) and after (Fig. <xref ref-type="fig" rid="Ch1.F4"/>)<?pagebreak page37?> two-step calibration,
we find that divergence of the RCP4.5 and RCP8.5 trends occurs more so
in the Arctic than in the North Atlantic, after 2050, and for
temperature, dew point, and specific humidity.  The RCP4.5 and RCP8.5
relative humidity and visibility trends are quite similar throughout
these simulations.  To the extent that relative humidity increases and
visibility decreases, this is predominantly found in the Arctic.  We
estimate the 21st century visibility decrease (in kilometers) to be in the
range of 8 %–12 % in the Arctic and 0 %–5 % in the North Atlantic.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5"><?xmltex \currentcnt{5}?><label>Figure 5</label><caption><p id="d1e1234">Predicted (RCP4.5) distribution shifts in relative humidity
with and without a homogeneous two-step calibration.  Shown are
the fraction of marine coverage as a function of calibrated (solid
lines) and uncalibrated (dashed lines) relative humidity with
respect to water (at 1 % intervals) for the years 2006–2035 (red
lines) and 2069–2098 (blue lines).  Fractions are shown on a
logarithmic scale for the WRF <bold>(a, c)</bold> and HadGEM2 <bold>(b, d)</bold> simulations in the Arctic <bold>(a, b)</bold> and North
Atlantic <bold>(c, d)</bold>.  Calibrated positive differences for
2006–2035 minus 2069–2098 (red) and 2069–2098 minus 2006–2035
(blue) are shaded.  Note that HadGEM2 relative humidity is
obtained from daily averages of air and dew point temperature.</p></caption>
        <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://ascmo.copernicus.org/articles/6/31/2020/ascmo-6-31-2020-f05.png"/>

      </fig>

      <p id="d1e1255">Marine environments of the Arctic and North Atlantic can be
characterized by an observed peak in relative humidity that is near
saturation, followed by an abrupt limit beyond this value that
represents the physical process of condensation, which often includes
the fog formation process of interest (Fig. <xref ref-type="fig" rid="Ch1.F1"/>a, b).  Thus,
although our large-scale calibration aligns each distribution with an
ICOADS distribution in some mean sense (e.g., with a slight shift in
ERA and HadGEM2 relative humidity), accompanying our linear
calibration of WRF is the following interpretive burden: there is a
notable impact on the frequency of relative humidity near 100 % (i.e.,
a decrease of about an order of magnitude) and on peak relative
humidity (a drying of 5 %–10 %) in the Arctic and North Atlantic.  The
occurrence of fog is often associated with relative humidity above
95 % <xref ref-type="bibr" rid="bib1.bibx22" id="paren.52"/>, and while this is somewhat
unchanged in the HadGEM2 calibrated distributions (Fig. <xref ref-type="fig" rid="Ch1.F3"/>),
its frequency is considerably reduced for WRF.</p>
      <?pagebreak page38?><p id="d1e1265">Figure <xref ref-type="fig" rid="Ch1.F5"/> depicts the impact of linear calibration on the WRF
and HadGEM2 RCP4.5 distributions and their 21st century trends in
relative humidity (i.e., as a fraction of marine coverage in early and
late 30-year periods).  The RCP8.5 distributions are nearly the same
(not shown).  The number of gridded marine samples is 2 to 4
orders of magnitude larger than the number of ICOADS collocations, but
as expected, two-step calibration has the same impact as on the
historical distributions (Fig. <xref ref-type="fig" rid="Ch1.F3"/>).  In other words, if we
allow that condensational processes are shifted from near 100 % to
just greater than 90 % relative humidity in the calibrated WRF RCP
distributions, then differences in the early and late 30-year
distributions are otherwise the same before and after our simple
linear calibration.  By accommodating this shift, we find the same
signal in Fig. <xref ref-type="fig" rid="Ch1.F5"/> that we find at large scales in
Fig. <xref ref-type="fig" rid="Ch1.F4"/>.  That is, both WRF and HadGEM2 reveal an increase in
the frequency of fog-producing (high) relative humidity.  The Arctic
enhancement in each model (blue shading) is over 10 % of the peak
frequency and is roughly double that of the North Atlantic.</p>
</sec>
<sec id="Ch1.S5" sec-type="conclusions">
  <label>5</label><title>Conclusions</title>
      <p id="d1e1285">The basic premise of this study is that models, observations, and
analyses target distinct representations of the marine surface, with
similarly distinct forms of bias relative to an unknown, fully
supported representation (i.e., the “broad” definition of truth in
<xref ref-type="bibr" rid="bib1.bibx17" id="altparen.53"/>).  Because we recognize different target
representations, there is not <italic>necessarily</italic> a need to calibrate
them.<fn id="Ch1.Footn1"><p id="d1e1294">Homogeneous linear calibration to a singular in situ
reference is prompted by our choice of visibility parameterization,
but the symmetry recognized by <xref ref-type="bibr" rid="bib1.bibx28" id="text.54"/>,
<xref ref-type="bibr" rid="bib1.bibx41" id="text.55"/>, <xref ref-type="bibr" rid="bib1.bibx5" id="text.56"/>, and others invites us to
consider the reverse calibration of in situ air and dew point
temperature using a numerical model or gridded analysis as
a reference.  Moreover, this accommodation of symmetry may facilitate
a less restrictive form of linear calibration.</p></fn>  We identified a
large-scale visibility decrease of about 8 %–12 % in the Arctic and
0 %–5 % in the North Atlantic using HadGEM2 global and WRF nested
regional 21st century RCP4.5 climate model simulations.  We also
identified trends in the frequency of high values of relative
humidity, with increases of over 10 % in the Arctic and 5 % in the
North Atlantic.  Although these represent baseline (calibrated)
trends, they are also given directly by the two uncalibrated models.
This is desirable because if a calibration is employed, it should not
change such trends arbitrarily <xref ref-type="bibr" rid="bib1.bibx17 bib1.bibx37" id="paren.57"/>.</p>
      <p id="d1e1310">The ERA-Interim reanalysis and ICOADS in situ observations provided
estimates of marine surface variables complementary to the HadGEM2
global climate model and WRF nested regional model, with its enhanced
resolution <xref ref-type="bibr" rid="bib1.bibx49 bib1.bibx50" id="paren.58"/>.  Temporally
constant large-scale differences (Fig. <xref ref-type="fig" rid="Ch1.F2"/>) suggested that
representation bias in each gridded dataset is also relatively
constant.<fn id="Ch1.Footn2"><p id="d1e1318">Linear calibration is useful to address dataset
differences that invariably remain, but in a more effective way,
some physical differences have already been addressed.  Our WRF
downscaling of HadGEM2, for instance, reduces differences with the
<italic>scale</italic> of in situ observations.  The treatment of other gridded
and in situ data (resolution) limits, and their impact on visibility
estimation, can also be attempted.  Although calibration is not a
prescription for how this treatment might be done, it can aid in
identifying more direct methods.</p></fn>  We proposed two methods of
calibrating linearly (and locally in time and space) air and dew point
temperature, from which all other calibrated variables were derived.
Estimates of relative humidity and visibility were found to be
sensitive to the representation of these two variables.  Since our
chosen visibility parameterization was formulated based on in situ
observations <xref ref-type="bibr" rid="bib1.bibx22" id="paren.59"/>, we were motivated to take
in situ marine observations as an error-free reference.  Although this
assumption is unrealistic, it is consistent with our focus on linear
calibration (cf. Appendix), and in turn enabled a simple physical
interpretation.  Of the two methods, a single-step calibration was
considered that takes the mean and variance of ICOADS frequency
distributions as a reference <xref ref-type="bibr" rid="bib1.bibx29" id="paren.60"/>.  A two-step
calibration was also performed in which ICOADS collocations were taken
as a reference for the ERA reanalysis, which in turn was taken as a
large-scale reference for the 1979–2004 HadGEM2 and WRF simulations.
Although the single-step calibration offered more freedom in
distribution matching, the two-step calibration provided a greater
degree of consistency in the large-scale trends (Fig. <xref ref-type="fig" rid="Ch1.F4"/>).</p>
      <?pagebreak page39?><p id="d1e1334">Our rudimentary parameterization of warm fog is applied on relatively
large scales and questions remain concerning trends in cold fog
occurrence and warm fog intensity.  The Appendix also addresses
nonlinear calibration and our assumption of an error-free in situ
reference, which we have good reason to explore
<xref ref-type="bibr" rid="bib1.bibx19 bib1.bibx2 bib1.bibx8" id="paren.61"/>, along
with the need (or lack thereof) for an ERA calibration.  A related
caveat of this study that is developed separately
<xref ref-type="bibr" rid="bib1.bibx12" id="paren.62"/> is that about half of the variance in
observed visibility might be associated with physical processes that
are not captured by either climate models or reanalyses.  Moreover,
there may be a more informed division of collocations by which to
refine an ERA calibration or a physical justification for calibrating
HadGEM2 or WRF more locally than on the entire Arctic or North
Atlantic domains (cf. <xref ref-type="bibr" rid="bib1.bibx17 bib1.bibx37" id="altparen.63"/>).  This
includes consideration of fog formation in relation to changes in sea
ice coverage and possibly distinct trends for the Grand Banks during
summer and winter.  Another question that remains to be explored,
following <xref ref-type="bibr" rid="bib1.bibx47" id="text.64"/>, is possible trends in
aerosol loading.</p><?xmltex \hack{\clearpage}?>
</sec>

      
      </body>
    <back><app-group>

<?pagebreak page40?><app id="App1.Ch1.S1">
  <?xmltex \currentcnt{A}?><label>Appendix A</label><title/>
      <p id="d1e1360">Two measurement models are identified here to highlight that ordinary
linear regression, as used in this study, is consistent with linear
calibration, whereas an experimental but otherwise quite similar
model is consistent with nonlinear calibration
<xref ref-type="bibr" rid="bib1.bibx12" id="paren.65"/>.  We write the familiar ordinary linear
regression model as
          <disp-formula id="App1.Ch1.S1.E1" content-type="numbered"><label>A1</label><mml:math id="M49" display="block"><mml:mtable rowspacing="0.2ex" columnspacing="1em" class="split" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mi>C</mml:mi><mml:mo>=</mml:mo><?xmltex \hack{\hspace*{1.35cm}}?><mml:mi>t</mml:mi><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mi>U</mml:mi><mml:mo>=</mml:mo><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mi>U</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mi>U</mml:mi></mml:msub><mml:mi>t</mml:mi><mml:mo>+</mml:mo><mml:msub><mml:mi mathvariant="italic">ϵ</mml:mi><mml:mi>U</mml:mi></mml:msub><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
        where <inline-formula><mml:math id="M50" display="inline"><mml:mi>C</mml:mi></mml:math></inline-formula> (calibrated ICOADS or ERA) is an error-free reference for
<inline-formula><mml:math id="M51" display="inline"><mml:mi>U</mml:mi></mml:math></inline-formula> (uncalibrated HadGEM2, WRF, or ERA) and both are either ranked or
unranked.  Error (<inline-formula><mml:math id="M52" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ϵ</mml:mi><mml:mi>U</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) exists only in the uncalibrated data
<inline-formula><mml:math id="M53" display="inline"><mml:mi>U</mml:mi></mml:math></inline-formula> and the scalars <inline-formula><mml:math id="M54" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mi>U</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M55" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mi>U</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> represent a linear
adjustment by additive and multiplicative components, respectively.
Homogeneous calibration by ordinary linear regression seeks to make
<inline-formula><mml:math id="M56" display="inline"><mml:mi>U</mml:mi></mml:math></inline-formula> as consistent as possible with <inline-formula><mml:math id="M57" display="inline"><mml:mi>C</mml:mi></mml:math></inline-formula>, but insofar as <inline-formula><mml:math id="M58" display="inline"><mml:mi>C</mml:mi></mml:math></inline-formula> may have
errors, this calibration also uses those errors as a reference.  To
address this, we include an error (<inline-formula><mml:math id="M59" display="inline"><mml:mi mathvariant="italic">ϵ</mml:mi></mml:math></inline-formula>) that is shared between
<inline-formula><mml:math id="M60" display="inline"><mml:mi>C</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M61" display="inline"><mml:mi>U</mml:mi></mml:math></inline-formula> and an error (<inline-formula><mml:math id="M62" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ϵ</mml:mi><mml:mi>C</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>) for <inline-formula><mml:math id="M63" display="inline"><mml:mi>C</mml:mi></mml:math></inline-formula> that is unshared with
<inline-formula><mml:math id="M64" display="inline"><mml:mi>U</mml:mi></mml:math></inline-formula> to write a similar measurement model as
          <disp-formula id="App1.Ch1.S1.E2" content-type="numbered"><label>A2</label><mml:math id="M65" display="block"><mml:mtable class="split" rowspacing="0.2ex" columnspacing="1em" displaystyle="true" columnalign="right left"><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mi>C</mml:mi><mml:mo>=</mml:mo><?xmltex \hack{\hspace*{1.35cm}}?><mml:mi>t</mml:mi><mml:mo>+</mml:mo><mml:mi mathvariant="italic">ϵ</mml:mi><mml:mo>+</mml:mo><mml:msub><mml:mi mathvariant="italic">ϵ</mml:mi><mml:mi>C</mml:mi></mml:msub><mml:mo>,</mml:mo></mml:mrow></mml:mtd></mml:mtr><mml:mtr><mml:mtd/><mml:mtd><mml:mrow><mml:mi>U</mml:mi><mml:mo>=</mml:mo><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mi>U</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mi>U</mml:mi></mml:msub><mml:mi>t</mml:mi><mml:mo>+</mml:mo><mml:mi mathvariant="italic">ϵ</mml:mi><mml:mo>+</mml:mo><mml:msub><mml:mi mathvariant="italic">ϵ</mml:mi><mml:mi>U</mml:mi></mml:msub><mml:mo>.</mml:mo></mml:mrow></mml:mtd></mml:mtr></mml:mtable></mml:math></disp-formula>
        <?xmltex \hack{\newpage}?>This model differs from the standard errors-in-variables model
<xref ref-type="bibr" rid="bib1.bibx20" id="paren.66"/> in its explicit accommodation of a so-called
nonlinear shared error (<inline-formula><mml:math id="M66" display="inline"><mml:mi mathvariant="italic">ϵ</mml:mi></mml:math></inline-formula>).  Regardless of whether shared
error is written as part of the unshared errors (<inline-formula><mml:math id="M67" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ϵ</mml:mi><mml:mi>C</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and
<inline-formula><mml:math id="M68" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">ϵ</mml:mi><mml:mi>U</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>), however, Eq. (<xref ref-type="disp-formula" rid="App1.Ch1.S1.E2"/>) avoids the common assumptions
of linear measurements with independent errors (cf. <xref ref-type="bibr" rid="bib1.bibx27" id="altparen.67"/>).</p>
      <p id="d1e1645">Although calibration may involve confirmation of improved
association<fn id="App1.Ch1.Footn1"><p id="d1e1648">Whereas <xref ref-type="bibr" rid="bib1.bibx40" id="text.68"/> use the word
“agreement”, we use the word “association” here, with both
concepts appearing as terms in Eqs. (<xref ref-type="disp-formula" rid="App1.Ch1.S1.E1"/>) and (<xref ref-type="disp-formula" rid="App1.Ch1.S1.E2"/>).
Specifically, measurement in medicine often concerns agreement
<xref ref-type="bibr" rid="bib1.bibx1 bib1.bibx7" id="paren.69"/>, where calibration
coefficients <inline-formula><mml:math id="M69" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mi>U</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M70" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mi>U</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> are taken as the <italic>linear</italic>
agreement between <inline-formula><mml:math id="M71" display="inline"><mml:mi>C</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M72" display="inline"><mml:mi>U</mml:mi></mml:math></inline-formula>.  Measurement in philosophy often
concerns meaningful association <xref ref-type="bibr" rid="bib1.bibx40" id="paren.70"/>, where
shared truth <inline-formula><mml:math id="M73" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> can be taken as the <italic>linear</italic> association
between <inline-formula><mml:math id="M74" display="inline"><mml:mi>C</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M75" display="inline"><mml:mi>U</mml:mi></mml:math></inline-formula>.  While <inline-formula><mml:math id="M76" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mi>U</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, <inline-formula><mml:math id="M77" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">β</mml:mi><mml:mi>U</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, and <inline-formula><mml:math id="M78" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> are
distinct and identifiable, terminology and meaning may vary across
fields.</p></fn>  <xref ref-type="bibr" rid="bib1.bibx40" id="paren.71"/>, under a strictly linear
calibration that follows from a solution of either Eqs. (<xref ref-type="disp-formula" rid="App1.Ch1.S1.E1"/>) or
(<xref ref-type="disp-formula" rid="App1.Ch1.S1.E2"/>), no change in association is expected
<xref ref-type="bibr" rid="bib1.bibx3" id="paren.72"/>.  However, we suggest that improved
association would be expected under a nonlinear calibration.  But if
the association between <inline-formula><mml:math id="M79" display="inline"><mml:mi>C</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M80" display="inline"><mml:mi>U</mml:mi></mml:math></inline-formula> is presumed to be nonlinear, then
we propose that improvements be confirmed by a measurement model that
accommodates nonlinearity.  Of the two models (<xref ref-type="disp-formula" rid="App1.Ch1.S1.E1"/>) and
(<xref ref-type="disp-formula" rid="App1.Ch1.S1.E2"/>), the latter explicitly accommodates a broad
interpretive scope for truth and error, nonlinearity in both <inline-formula><mml:math id="M81" display="inline"><mml:mi>C</mml:mi></mml:math></inline-formula> and
<inline-formula><mml:math id="M82" display="inline"><mml:mi>U</mml:mi></mml:math></inline-formula>, as well as a genuine nonlinear association (<inline-formula><mml:math id="M83" display="inline"><mml:mi mathvariant="italic">ϵ</mml:mi></mml:math></inline-formula>) between
them (cf. <xref ref-type="bibr" rid="bib1.bibx42" id="altparen.73"/>).  Demonstration of improved
association using a simple neural network is given by
<xref ref-type="bibr" rid="bib1.bibx12" id="text.74"/>.  The present study (e.g.,
Fig. <xref ref-type="fig" rid="Ch1.F3"/> distribution differences) supports the notion that
for common measures of relative humidity and visibility (if not for
other processes of interest), perhaps only rarely is association
expected to be strictly linear.</p><?xmltex \hack{\clearpage}?>
</app>
  </app-group><notes notes-type="dataavailability"><title>Data availability</title>

      <p id="d1e1823">The ICOADS, ERA-Interim, and HadGEM2 data are
available from separate online archives.  Collocations employed by
this study for the historical period (1979–2004) are also available
online (<ext-link xlink:href="https://doi.org/10.21963/13169" ext-link-type="DOI">10.21963/13169</ext-link>, <xref ref-type="bibr" rid="bib1.bibx13" id="altparen.75"/>).</p>
  </notes><notes notes-type="authorcontribution"><title>Author contributions</title>

      <p id="d1e1835">RED proposed the linear calibration approach and
provided an initial literature review and interpretation.  MZ and
WAP contributed to the literature review and MZ supplied the WRF
data.  RED prepared the Julia code to identify collocations and
perform baseline estimates.  All the authors contributed to proofreading
and fine-tuning the paper.</p>
  </notes><notes notes-type="competinginterests"><title>Competing interests</title>

      <p id="d1e1841">The authors declare that they have no conflict of
interest.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e1847">We thank Ismail Gultepe and an anonymous reviewer for insightful
comments on earlier drafts and acknowledge those developing the
NCAR/NOAA WRF model, the Met Office Hadley Centre Earth System model
family, as well as an international effort over many years to
assemble and analyze marine observations, as given by the ERA-Interim and ICOADS datasets.  Encouragement from Zhenxia Long,
Changshuo Chen, George Isaac, and Bjarne Hansen and beneficial
contributions from the Julia language <xref ref-type="bibr" rid="bib1.bibx6" id="paren.76"/> and
Wikipedia communities are also appreciated.</p></ack><notes notes-type="financialsupport"><title>Financial support</title>

      <p id="d1e1855">This research has been supported by the Ocean Frontier Institute via the Marine Atmospheric Composition and Visibility project (module A grant), from a Belmont Forum project on Fog Variability in a Warming Arctic and its Impact on Maritime Human Activities (AFV grant), from the Aquatic Climate Change Adaptation Services Program of Fisheries and Oceans Canada, and from the Canadian Office of Energy Research and Development (grant no. 1B00.003C).</p>
  </notes><notes notes-type="reviewstatement"><title>Review statement</title>

      <p id="d1e1861">This paper was edited by William Hsieh and reviewed by Ismail Gultepe and one anonymous referee.</p>
  </notes><ref-list>
    <title>References</title>

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    <!--<article-title-html>Possible impacts of climate change on fog in the Arctic and subpolar North Atlantic</article-title-html>
<abstract-html><p>A conventional parameterization of midlatitude warm fog occurrence,
based on in situ observations, is employed to estimate marine
surface visibility in the Arctic and North Atlantic from three
datasets: an ensemble member of the Hadley Earth System (HadGEM2)
model and a nested regional WRF simulation that follow historical
and future emissions scenarios for 1979–2100, and the ERA-Interim
reanalysis for 1979–2004.  Over large scales (of an entire year and
region), all three gridded datasets agree well in terms of variables
like surface air temperature, whose systematic differences seem
small by comparison with its predicted change over the course of
this century.  On the other hand, systematic differences are more
apparent in large-scale estimates of relative humidity and
visibility.  Large differences are attributed to a sensitivity to
representation bias that is inherent in the formulation of each
individual model and analysis.</p><p>Two simple linear calibrations are examined, both of which assume
that an in situ based parameterization is broadly consistent with
the use of marine (ICOADS) observations of air and dew point
temperature as an error-free reference.  A single-step calibration
is considered that takes the mean and variance of ICOADS frequency
distributions as a reference.  A two-step calibration is also
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the ERA reanalysis, which in turn is taken as a large-scale
reference for the 1979–2004 HadGEM2 and WRF simulations.  Both
linear calibrations are applied (locally in time and space to air
and dew point temperature) to the future climate scenarios of
HadGEM2 and WRF.  Although ICOADS observations are not error-free
and parameterized visibility estimates are unlikely to capture much
more than half the variance found in observations, attempts are made
to present consistent regional changes in the frequency of high
relative humidity, as a proxy for warm fog occurrence.  The
large-scale decrease in visibility over the 21st century is in the
range of 8&thinsp;%–12&thinsp;% in the Arctic and 0&thinsp;%–5&thinsp;% in the North Atlantic.</p></abstract-html>
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