<?xml version="1.0" encoding="UTF-8"?>
<!DOCTYPE article PUBLIC "-//NLM//DTD Journal Publishing with OASIS Tables v3.0 20080202//EN" "journalpub-oasis3.dtd">
<article xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:oasis="http://docs.oasis-open.org/ns/oasis-exchange/table" xml:lang="en" dtd-version="3.0"><?xmltex \bartext{17th EMS Annual Meeting: European Conference for Applied Meteorology and Climatology 2017}?>
  <front>
    <journal-meta><journal-id journal-id-type="publisher">ASR</journal-id><journal-title-group>
    <journal-title>Advances in Science and Research</journal-title>
    <abbrev-journal-title abbrev-type="publisher">ASR</abbrev-journal-title><abbrev-journal-title abbrev-type="nlm-ta">Adv. Sci. Res.</abbrev-journal-title>
  </journal-title-group><issn pub-type="epub">1992-0636</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/asr-15-51-2018</article-id><title-group><article-title>An approach for the estimation of the aggregated photovoltaic power generated in several European countries from meteorological data</article-title><alt-title>Estimation of the PV power generation  in several EU countries</alt-title>
      </title-group><?xmltex \runningtitle{Estimation of the PV power generation  in several EU countries}?><?xmltex \runningauthor{Y.-M.~Saint-Drenan et al.}?>
      <contrib-group>
        <contrib contrib-type="author" corresp="yes" rid="aff1">
          <name><surname>Saint-Drenan</surname><given-names>Yves-Marie</given-names></name>
          <email>yves-marie.saint-drenan@mines-paristech.fr</email>
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Wald</surname><given-names>Lucien</given-names></name>
          
        <ext-link>https://orcid.org/0000-0002-2916-2391</ext-link></contrib>
        <contrib contrib-type="author" corresp="no" rid="aff1">
          <name><surname>Ranchin</surname><given-names>Thierry</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff2 aff4">
          <name><surname>Dubus</surname><given-names>Laurent</given-names></name>
          
        </contrib>
        <contrib contrib-type="author" corresp="no" rid="aff3 aff4">
          <name><surname>Troccoli</surname><given-names>Alberto</given-names></name>
          
        </contrib>
        <aff id="aff1"><label>1</label><institution>MINES ParisTech, PSL Research University, O.I.E. – Centre Observation, <?xmltex \hack{\break}?> Impacts, Energy, 06904 Sophia Antipolis, France</institution>
        </aff>
        <aff id="aff2"><label>2</label><institution>EDF R&amp;D/MFEE, Applied Meteorology and Atmospheric Environment, CHATOU CEDEX, France</institution>
        </aff>
        <aff id="aff3"><label>3</label><institution>School of Environmental Sciences, University of East Anglia, Norwich, NR4 7TJ, UK</institution>
        </aff>
        <aff id="aff4"><label>4</label><institution>World Energy &amp; Meteorology Council (WEMC), Norwich, NR4 7TJ, UK</institution>
        </aff>
      </contrib-group>
      <author-notes><corresp id="corr1">Yves-Marie Saint-Drenan (yves-marie.saint-drenan@mines-paristech.fr)</corresp></author-notes><pub-date><day>2</day><month>May</month><year>2018</year></pub-date>
      
      <volume>15</volume>
      <fpage>51</fpage><lpage>62</lpage>
      <history>
        <date date-type="received"><day>16</day><month>January</month><year>2018</year></date>
           <date date-type="rev-recd"><day>2</day><month>April</month><year>2018</year></date>
           <date date-type="accepted"><day>6</day><month>April</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://asr.copernicus.org/articles/15/51/2018/asr-15-51-2018.html">This article is available from https://asr.copernicus.org/articles/15/51/2018/asr-15-51-2018.html</self-uri><self-uri xlink:href="https://asr.copernicus.org/articles/15/51/2018/asr-15-51-2018.pdf">The full text article is available as a PDF file from https://asr.copernicus.org/articles/15/51/2018/asr-15-51-2018.pdf</self-uri>
      <abstract>
    <p id="d1e135">Classical approaches to the calculation of the photovoltaic (PV) power
generated in a region from meteorological data require the knowledge of the
detailed characteristics of the plants, which are most often not publicly
available. An approach is proposed with the objective to obtain the best
possible assessment of power generated in any region without having to
collect detailed information on PV plants. The proposed approach is based on
a model of PV plant coupled with a statistical distribution of the prominent
characteristics of the configuration of the plant and is tested over Europe.
The generated PV power is first calculated for each of the plant
configurations frequently found in a given region and then aggregated taking
into account the probability of occurrence of each configuration. A
statistical distribution has been constructed from detailed information
obtained for several thousands of PV plants representing approximately
2 % of the total number of PV plants in Germany and was then adapted to
other European countries by taking into account changes in the optimal PV
tilt angle as a function of the latitude and meteorological conditions. The
model has been run with bias-adjusted ERA-interim data as meteorological
inputs. The results have been compared to estimates of the total PV power
generated in two countries: France and Germany, as provided by the
corresponding transmission system operators. Relative RMSE of 4.2 and
3.8 % and relative biases of <inline-formula><mml:math id="M1" display="inline"><mml:mo>-</mml:mo></mml:math></inline-formula>2.4 and 0.1 % were found with
three-hourly data for France and Germany. A validation against estimates of
the country-wide PV-power generation provided by the ENTSO-E for 16 European
countries has also been conducted. This evaluation is made difficult by the
uncertainty on the installed capacity corresponding to the ENTSO-E data but
it nevertheless allows demonstrating that the model output and TSO data are
highly correlated in most countries. Given the simplicity of the proposed
approach these results are very encouraging. The approach is particularly
suited to climatic timescales, both historical and future climates, as
demonstrated here.</p>
  </abstract>
    </article-meta>
  </front>
<body>
      

<sec id="Ch1.S1" sec-type="intro">
  <title>Introduction</title>
      <p id="d1e152">Time series of photovoltaic (PV) power generated within a region are needed
for prospective studies on the transformation of the electricity supply
system. Under classical approaches an accurate calculation of the power
generated by PV plants in a region requires the knowledge of the detailed
characteristics of the plants. A few cases can be found where enough
information is available, and can be used for the model development and/or
validation (see e.g. Jamaly et al., 2013; Lingfors and Widén, 2016;
Shaker et al., 2015, 2016). Plant production data are however most often
unavailable to the public. They may be collected from e.g. the operators of
PV plants but this represents a huge amount of work. Hence, an accurate
calculation of the PV power generated in any European region with a classical
method represents an<?pagebreak page52?> exhaustive and time-consuming task and is intractable.
Alternatively, statistical approaches may be used to train models from
historical time series of the aggregated PV generated power, such as those
published by the transmission system operators. In this case, the collection,
understanding and quality check of the training data is primordial to ensure
accurate model output. Though more practical than the classical approaches,
these statistical approaches are also time consuming because of the handling
of the data and they cannot be applied in regions where no training data is
available. Another common practice consists in estimating the total power
generated in a region by upscaling the power generated by a subset of
reference plants (Schierenbeck et al., 2010; Lorenz and Heinemann, 2012;
Shaker et al., 2015, 2016; Saint-Drenan et al., 2016; Bright et al., 2017;
Pierro et al., 2017; Killinger et al., 2017). The major obstacles to this
practice is on the one hand the establishment of criteria on the selection of
the plants that are statistically representative of the region and their
number, and on the other hand, the access to measurements of the selected
plants. In addition, those methods only allow estimating the PV power
generation for historical periods where measurements are available, and their
extrapolation to other periods is not straightforward. This can be a major
drawback for e.g. generation adequacy study or prospective analysis where
scenarios with long time series are needed. A further option consists in
selecting a simple PV model, with a very limited number of unknowns (Jerez et
al., 2015), whose implementation for any region is easy to do at the expense
of the model accuracy. Finally, several authors propose to consider a mix of
different key parameters, where the distributions are chosen by the authors
(Marinelli et al., 2015; Schubert, 2012). This requires a deep expertise of
the domain. This approach is limited to a few regions and cannot be used to
model all EU countries.</p>
      <p id="d1e155">This brief survey of the proposed approaches demonstrates the need for a new
approach that offers a better trade-off between implementation constraints
and model output accuracy. This paper describes a method addressing this
need. It has been developed in the framework of the EU-funded Copernicus
Climate Change Service ECEM<fn id="Ch1.Footn1"><p id="d1e158"><uri>http://ecem.climate.copernicus.eu</uri></p></fn>
(European Climate Energy Mixes) project which aims at producing, in close
collaboration with prospective users, a proof-of-concept climate service, or
demonstrator, whose purpose is to enable the energy industry and policy
makers to assess how well different energy supply mixes in Europe will meet
demand, over different time horizons (from seasonal to long-term decadal
planning), focusing on the role climate has on the mixes (Troccoli et al.,
2017).</p>
      <p id="d1e163">The innovation of our method is the extension of the regional PV model
proposed by Saint-Drenan (2015) and Saint-Drenan et al. (2017) to any region, without the need
for a priori knowledge of the characteristics of the installed PV plants. To
this end, the plant-related parameters which are needed as input to the PV
model are expressed as a function of known solar resource characteristics,
making thus the model generalizable to any region, namely beyond Germany
where the approach was originally tested. This is achieved in two steps:
firstly, by reducing the number of inputs to the PV model by the means of an
analytical function for the statistical distribution of the module
orientation and, secondly, by expressing the parameters of the chosen
analytical functions as a function of known geographically-dependent
information (optimal tilt angle).</p>
      <p id="d1e166">The paper is organized as follows. After a short summary of the regional PV
model proposed by Saint-Drenan (2015) and Saint-Drenan et al. (2017) in Sect. 2.1, the
reduction of the number of parameters achieved by the use of an analytical
function is detailed in Sect. 2.2. The approach chosen to relate the
parameters of the analytical function to known geographically-dependent
quantities is then explained in Sect. 2.3. Implementation details are
provided in Sect. 2.4. The results of a validation of the model are
described in Sect. 3, where the model output has been compared to
estimates of the total PV power generation of France and Germany provided by
transmission system operators (TSOs). Finally, the results and potential
improvements of the approach presented are discussed in Sect. 4.</p>
</sec>
<sec id="Ch1.S2">
  <title>Approach</title>
      <p id="d1e175">Our approach for modelling the PV power generation in any country use a
generic PV model which needs only the distribution of the two module
orientation angles as inputs. This model is introduced in Sect. 2.1 and
the methodology for estimating the distribution of the module orientation
angles in any location is described in the Sect. 2.2 and 2.3. Finally,
some implementation details are given in Sect. 2.4.</p>
<sec id="Ch1.S2.SS1">
  <title>Description of the model for the aggregated PV power produced in a
region</title>
      <?pagebreak page53?><p id="d1e183">The proposed method is built upon previous works by Saint-Drenan
(2015) and Saint-Drenan et al. (2017), where a model for the aggregated PV power produced by a fleet
of PV plants installed in a region is described. The authors have showed
that an accurate estimate of the German PV power generation can be obtained
by using the statistical distribution of the orientation angle of PV panels
as the sole plant-relevant input to the model (Fig. 1). The model is based
on the simple idea that the aggregated PV power generated in a region is the
sum of the normalized outputs of all plants with characteristics <inline-formula><mml:math id="M2" display="inline"><mml:mrow><mml:msub><mml:mi>A</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>
multiplied by the proportion <inline-formula><mml:math id="M3" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> of plants having the characteristics
<inline-formula><mml:math id="M4" display="inline"><mml:mrow><mml:msub><mml:mi>A</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> in the whole set of plants installed in the considered region. The
regional PV power generation can therefore be expressed as follows:
            <disp-formula id="Ch1.E1" content-type="numbered"><mml:math id="M5" display="block"><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mi mathvariant="normal">PV</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mi>t</mml:mi><mml:mo>)</mml:mo><mml:mo>=</mml:mo><mml:munderover><mml:mo movablelimits="false">∑</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow><mml:mi>n</mml:mi></mml:munderover><mml:msub><mml:mi>w</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msub><mml:mi>f</mml:mi><mml:mi mathvariant="normal">PV</mml:mi></mml:msub><mml:mfenced open="(" close=")"><mml:mrow><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">G</mml:mi><mml:mfenced close=")" open="("><mml:mrow><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:mfenced><mml:mo>,</mml:mo><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub><mml:mfenced open="(" close=")"><mml:mrow><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:mfenced><mml:mo>,</mml:mo><mml:msub><mml:mi>A</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:mfenced></mml:mrow></mml:math></disp-formula>
          Where
<inline-formula><mml:math id="M6" display="inline"><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mi mathvariant="normal">PV</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is an estimate of the aggregated power produced by all PV plants
located at <inline-formula><mml:math id="M7" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> at time <inline-formula><mml:math id="M8" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula> [W W<inline-formula><mml:math id="M9" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mi mathvariant="normal">p</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula>],
<inline-formula><mml:math id="M10" display="inline"><mml:mrow><mml:mi>G</mml:mi><mml:mo>(</mml:mo><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is the global horizontal irradiance (GHI) received at <inline-formula><mml:math id="M11" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M12" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula>
[W m<inline-formula><mml:math id="M13" display="inline"><mml:msup><mml:mi/><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:math></inline-formula>],
<inline-formula><mml:math id="M14" display="inline"><mml:mrow><mml:msub><mml:mi>T</mml:mi><mml:mi mathvariant="normal">a</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> (<inline-formula><mml:math id="M15" display="inline"><mml:mrow><mml:mi>x</mml:mi><mml:mo>,</mml:mo><mml:mi>t</mml:mi></mml:mrow></mml:math></inline-formula>) is the air temperature at <inline-formula><mml:math id="M16" display="inline"><mml:mi>x</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M17" display="inline"><mml:mi>t</mml:mi></mml:math></inline-formula>
[<inline-formula><mml:math id="M18" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>C],
<inline-formula><mml:math id="M19" display="inline"><mml:mrow><mml:msub><mml:mi>f</mml:mi><mml:mi mathvariant="normal">PV</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi mathvariant="normal">…</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> is a function representing the single PV plant model used to
calculate the normalized PV power [W W<inline-formula><mml:math id="M20" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mi mathvariant="normal">p</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula>].</p>
      <p id="d1e480">A first advantage of the chosen regional PV model is that each important
configuration is considered only once and the number of configurations
<inline-formula><mml:math id="M21" display="inline"><mml:mrow><mml:msub><mml:mi>A</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> can be optimized in order to limit the calculation costs. A second
advantage is the high flexibility offered by the use of an analytical
function to describe the statistical distribution of the characteristics of
the plants installed in a region.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F1"><caption><p id="d1e496">Flow chart of the single PV plant model.</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://asr.copernicus.org/articles/15/51/2018/asr-15-51-2018-f01.png"/>

        </fig>

      <p id="d1e505">The function <inline-formula><mml:math id="M22" display="inline"><mml:mrow><mml:msub><mml:mi>f</mml:mi><mml:mi mathvariant="normal">PV</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> in Eq. (1) represents a single plant model, which needs
to be chosen prior to the implementation of the proposed approach. In
Saint-Drenan (2015) and Saint-Drenan et al. (2017), the authors demonstrated that a simple
model with a limited number of input parameters yields good results for
regional application. With the chosen model, the set of characteristics
<inline-formula><mml:math id="M23" display="inline"><mml:mrow><mml:msub><mml:mi>A</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is only composed of the module tilt angle <inline-formula><mml:math id="M24" display="inline"><mml:mi mathvariant="italic">γ</mml:mi></mml:math></inline-formula> and azimuth angle
<inline-formula><mml:math id="M25" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula> or orientation. The <inline-formula><mml:math id="M26" display="inline"><mml:mrow><mml:msub><mml:mi>A</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>'s, which are a function of (<inline-formula><mml:math id="M27" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>,
<inline-formula><mml:math id="M28" display="inline"><mml:mrow><mml:mi mathvariant="italic">γ</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula>, are hereafter referred to as reference configurations. There are
two steps for the implementation of the regional PV model that are described
in the following section: the estimation of the weights <inline-formula><mml:math id="M29" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and the
choice of the reference configurations. A detailed description of the
chosen model which is illustrated in Fig. 1 can be found in e.g.
(Saint-Drenan, 2015).</p>
</sec>
<sec id="Ch1.S2.SS2">
  <?xmltex \opttitle{Modelling the weights $w_{{i}}$}?><title>Modelling the weights <inline-formula><mml:math id="M30" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula></title>
      <p id="d1e601">Saint-Drenan (2015) and Saint-Drenan et al. (2017) have created a dataset of
peak power and module orientation angles for 35 000 PV plants located in
Germany, which is used here. This amount of plants represents approximately
2 % of the number of plants installed in Germany. It is assumed that this
dataset is representative of all plants in Germany. A realistic example of
the relationship between <inline-formula><mml:math id="M31" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M32" display="inline"><mml:mrow><mml:msub><mml:mi>A</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> at country level may be derived
from this dataset. Figure 2 exhibits the share <inline-formula><mml:math id="M33" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> of installed capacity
per module orientation evaluated from this dataset. One may note the high
share of installed capacity for modules with a tilt of 20<inline-formula><mml:math id="M34" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>
southwards facing (orientation 180<inline-formula><mml:math id="M35" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>).</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F2"><caption><p id="d1e657">Share of the installed capacity per module orientation evaluated
from the 35 000 PV plants installed in Germany (coloured squares). Black
squares denote the set of 19 reference orientations used for the
implementation of the regional model.</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://asr.copernicus.org/articles/15/51/2018/asr-15-51-2018-f02.png"/>

        </fig>

      <?pagebreak page54?><p id="d1e666">The use of Eq. (1) requires that the space spanned by <inline-formula><mml:math id="M36" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula> and
<inline-formula><mml:math id="M37" display="inline"><mml:mi mathvariant="italic">γ</mml:mi></mml:math></inline-formula> is properly sampled in order to obtain a robust estimation of the
plant shares <inline-formula><mml:math id="M38" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> corresponding to the sampled orientations
<inline-formula><mml:math id="M39" display="inline"><mml:mrow><mml:msub><mml:mi>A</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>;</mml:mo><mml:msub><mml:mi mathvariant="italic">γ</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:math></inline-formula> in that equation. The smoothness and
form of the joint distribution displayed in Fig. 2 suggest that it may be
possible to fit an analytical relationship, therefore reducing the number of
parameters used to describe it. We propose to use the product of two
Gaussian distributions:

                <disp-formula specific-use="align" content-type="numbered"><mml:math id="M40" display="block"><mml:mtable displaystyle="true"><mml:mtr><mml:mtd><mml:mstyle class="stylechange" displaystyle="true"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:msub><mml:mover accent="true"><mml:mi>w</mml:mi><mml:mo mathvariant="normal">̃</mml:mo></mml:mover><mml:mi>i</mml:mi></mml:msub><mml:mfenced close=")" open="("><mml:mrow><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>;</mml:mo><mml:msub><mml:mi mathvariant="italic">γ</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:mfenced><mml:mo>=</mml:mo><mml:mfenced close="]" open="["><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">1</mml:mn><mml:msqrt><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mi mathvariant="italic">π</mml:mi><mml:msubsup><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="italic">α</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup></mml:mrow></mml:msqrt></mml:mfrac></mml:mstyle><mml:mi>exp⁡</mml:mi><mml:mfenced open="(" close=")"><mml:mrow><mml:mo>-</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msup><mml:mfenced close=")" open="("><mml:mrow><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi mathvariant="italic">μ</mml:mi><mml:mi mathvariant="italic">α</mml:mi></mml:msub></mml:mrow></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:msubsup><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="italic">α</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mfenced></mml:mrow></mml:mfenced></mml:mrow></mml:mtd></mml:mtr><mml:mlabeledtr id="Ch1.E2"><mml:mtd/><mml:mtd><mml:mstyle class="stylechange" displaystyle="true"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mspace linebreak="nobreak" width="0.25em"/><mml:mfenced open="[" close="]"><mml:mrow><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mn mathvariant="normal">1</mml:mn><mml:msqrt><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:mi mathvariant="italic">π</mml:mi><mml:msubsup><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="italic">γ</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup></mml:mrow></mml:msqrt></mml:mfrac></mml:mstyle><mml:mi>exp⁡</mml:mi><mml:mfenced open="(" close=")"><mml:mrow><mml:mo>-</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:msup><mml:mfenced close=")" open="("><mml:mrow><mml:msub><mml:mi mathvariant="italic">γ</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:msub><mml:mi mathvariant="italic">μ</mml:mi><mml:mi mathvariant="italic">γ</mml:mi></mml:msub></mml:mrow></mml:mfenced><mml:mn mathvariant="normal">2</mml:mn></mml:msup></mml:mrow><mml:mrow><mml:mn mathvariant="normal">2</mml:mn><mml:msubsup><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="italic">γ</mml:mi><mml:mn mathvariant="normal">2</mml:mn></mml:msubsup></mml:mrow></mml:mfrac></mml:mstyle></mml:mrow></mml:mfenced></mml:mrow></mml:mfenced><mml:mspace linebreak="nobreak" width="1em"/><mml:msub><mml:mi>A</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mo>(</mml:mo><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>;</mml:mo><mml:msub><mml:mi mathvariant="italic">γ</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>)</mml:mo></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

            In Eq. (2), the first product term corresponds to the normal distribution of
<inline-formula><mml:math id="M41" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>, characterised by a mean value <inline-formula><mml:math id="M42" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">μ</mml:mi><mml:mi mathvariant="italic">α</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and a standard
deviation <inline-formula><mml:math id="M43" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="italic">α</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>. The second product term corresponds to the
normal distribution of <inline-formula><mml:math id="M44" display="inline"><mml:mi mathvariant="italic">γ</mml:mi></mml:math></inline-formula>, characterised by a mean value <inline-formula><mml:math id="M45" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">μ</mml:mi><mml:mi mathvariant="italic">γ</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and a standard deviation <inline-formula><mml:math id="M46" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="italic">γ</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>. It appears reasonable to
assume that the distribution of <inline-formula><mml:math id="M47" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula> is centred on a southwards
orientation, so that <inline-formula><mml:math id="M48" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">μ</mml:mi><mml:mi mathvariant="italic">α</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> can be set to 180<inline-formula><mml:math id="M49" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>. In Eq. (2),
it is assumed that the distributions of the <inline-formula><mml:math id="M50" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula> and <inline-formula><mml:math id="M51" display="inline"><mml:mi mathvariant="italic">γ</mml:mi></mml:math></inline-formula> are
independent – from Fig. 2 this assumption is an acceptable first-order
approximation. A different notation has been used for the weights <inline-formula><mml:math id="M52" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> in
Eqs. (1) and (2) since, as further explained in Sect. 5, values
<inline-formula><mml:math id="M53" display="inline"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi>w</mml:mi><mml:mo mathvariant="normal">̃</mml:mo></mml:mover><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> calculated with Eq. (2) must be normalized before being
inserted into Eq. (1).</p>
      <p id="d1e1032">The use of the analytic form in Eq. (2) for the weights <inline-formula><mml:math id="M54" display="inline"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi>w</mml:mi><mml:mo mathvariant="normal">̃</mml:mo></mml:mover><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>
allows reducing the number of plant-relevant parameters down to three, which
are the mean and standard deviation of <inline-formula><mml:math id="M55" display="inline"><mml:mi mathvariant="italic">γ</mml:mi></mml:math></inline-formula> and the standard deviation
of <inline-formula><mml:math id="M56" display="inline"><mml:mi mathvariant="italic">α</mml:mi></mml:math></inline-formula>. This reduced form has been tested using the German solar
plants. We found an average value of 20.6<inline-formula><mml:math id="M57" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> for <inline-formula><mml:math id="M58" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">μ</mml:mi><mml:mi mathvariant="italic">γ</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and values of 19.3 and 10.8<inline-formula><mml:math id="M59" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> for <inline-formula><mml:math id="M60" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="italic">α</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M61" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">σ</mml:mi><mml:mi mathvariant="italic">γ</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>. The empirical histograms of the
tilt and azimuth angles are compared to their fitted normal distributions in
Fig. 3. The match between the histograms is not perfect but it seems an
acceptable first-order approximation.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F3"><caption><p id="d1e1117">Comparison of the experimental histograms of two module orientation
angles (blue bars) with the fitted normal distribution function (red lines)
for the module azimuth angle <bold>(a)</bold> and the module tilt angle
<bold>(b)</bold>. N(180, 19.3) <bold>(a)</bold> means that the average orientation is
180<inline-formula><mml:math id="M62" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> and the standard deviation is 19.3<inline-formula><mml:math id="M63" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>. N(20.6, 10.8)
<bold>(b)</bold> means an average tilt angle of 20.6<inline-formula><mml:math id="M64" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> and a standard
deviation of 10.8<inline-formula><mml:math id="M65" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>.</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://asr.copernicus.org/articles/15/51/2018/asr-15-51-2018-f03.png"/>

        </fig>

</sec>
<sec id="Ch1.S2.SS3">
  <title>Parameterisation of the relationship between the distribution of the
orientation of PV modules and the geographical location</title>
      <p id="d1e1181">The three plant-related parameters necessary to calculate the total PV power
produced in a given region from meteorological data has been determined
above in the specific case of Germany. How can these three parameters be
extended to other countries/regions? At this stage, one possibility may
consist in using ones own expertise on the characteristics of PV plants
installed in the considered regions as in Marinelli et al. (2015); Schubert
(2012); another is a detailed statistical analysis of a dataset of plant
information installed in the studied areas. Both ways hamper the easy use of
the regional model aimed at in this work. To address this issue a
parameterization of the three parameters is proposed in this section, which
makes the model implementable in any region without any prior knowledge on
the installed PV plants.</p>
      <p id="d1e1184">The statistical distribution of the plant capacity as a function of the
module orientation of a region is the result of individual choices on the
configurations of each single plant. It is affected by many factors of
different nature such as the characteristics of the solar resource, the
shading profile, architectural characteristics, different installation
practices, etc. All these factors cannot be taken into consideration and we
make the assumption that the most important one is the characteristics of
the solar resource. We propose to take this into consideration through the
use of an optimal tilt angle. The optimal tilt angle corresponds to the
value of the tilt angle of a southwards oriented module yielding the largest
annual output. In this work, we use the raster file of optimal tilt angles
available on the PV-GIS website (<uri>http://re.jrc.ec.europa.eu/pvgis/</uri>), which
is displayed in Fig. 4a as our starting point.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F4"><caption><p id="d1e1192"><bold>(a)</bold> Optimal tilt angles taken from the PV-GIS website
(<uri>http://re.jrc.ec.europa.eu/pvgis/</uri>). <bold>(b)</bold> Optimal tilt angles
used for the present work where high values present in mountainous regions
have been filtered out.</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://asr.copernicus.org/articles/15/51/2018/asr-15-51-2018-f04.png"/>

        </fig>

      <p id="d1e1209">It can be observed in Fig. 4 that the optimal tilt angle <inline-formula><mml:math id="M66" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">γ</mml:mi><mml:mi mathvariant="normal">opt</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> is
ranging between 30 and 35<inline-formula><mml:math id="M67" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> in Germany while the average
value for the tilt angle has been found equal to 20.6<inline-formula><mml:math id="M68" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> in the
previous section. The reason for this mismatch is that a tilt angle smaller
than the optimal tilt angle is commonly used to install more PV capacity per
unit of surface and maximize the economic output of the plant. This practice
has become more frequent with decreasing PV price and scarce available
surfaces for new installations. We propose to quantify the mismatch between
these two angles by a coefficient <inline-formula><mml:math id="M69" display="inline"><mml:mi>f</mml:mi></mml:math></inline-formula>. The average tilt angle <inline-formula><mml:math id="M70" display="inline"><mml:mrow><mml:msub><mml:mi mathvariant="italic">μ</mml:mi><mml:mi mathvariant="italic">γ</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>
can thus be expressed as
            <disp-formula id="Ch1.E3" content-type="numbered"><mml:math id="M71" display="block"><mml:mrow><mml:msub><mml:mi mathvariant="italic">μ</mml:mi><mml:mi mathvariant="italic">γ</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mi>f</mml:mi><mml:msub><mml:mi mathvariant="italic">γ</mml:mi><mml:mi mathvariant="normal">opt</mml:mi></mml:msub></mml:mrow></mml:math></disp-formula>
          The unknown factor <inline-formula><mml:math id="M72" display="inline"><mml:mi>f</mml:mi></mml:math></inline-formula> can vary from one plant to another since it depends on
numerous factors such as the solar resource, the plant cost per peak
capacity or the land price. It may thus exhibit spatial and time variation
and an accurate determination of this coefficient for all European countries
may be difficult. We assume that this factor is spatially constant.
Considering the average value of the tilt angles, which is equal to
20.6<inline-formula><mml:math id="M73" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>, the factor <inline-formula><mml:math id="M74" display="inline"><mml:mi>f</mml:mi></mml:math></inline-formula> should be chosen between 0.6 (20.6/35) and
0.7 (20.6/30). Given that the chosen dataset includes an
under-representative share of large solar park, that usually have an optimal
tilt angle (Saint-Drenan, 2015), we have chosen the upper bound for <inline-formula><mml:math id="M75" display="inline"><mml:mi>f</mml:mi></mml:math></inline-formula>
(<inline-formula><mml:math id="M76" display="inline"><mml:mrow><mml:mi>f</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.7</mml:mn></mml:mrow></mml:math></inline-formula>). Similarly, we<?pagebreak page55?> assume the standard deviations of the azimuth and
tilt angles spatially constant and set them to the values found with the set
of PV plants installed in Germany (19.3 and 10.8<inline-formula><mml:math id="M77" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> for
the azimuth and tilt angle).</p>
      <p id="d1e1333">The weights corresponding to the different orientation angles are finally
estimated using Eq. (2), where the mean tilt angle is taken equal to the
optimal tilt angle time the factor <inline-formula><mml:math id="M78" display="inline"><mml:mrow><mml:mi>f</mml:mi><mml:mo>=</mml:mo><mml:mn mathvariant="normal">0.7</mml:mn></mml:mrow></mml:math></inline-formula> and the standard deviations of
the azimuth and tilt angles are considered constant and equal to
19.3 and 10.8<inline-formula><mml:math id="M79" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> respectively.</p>
</sec>
<sec id="Ch1.S2.SS4">
  <title>Implementation details</title>
      <p id="d1e1364">Some implementation details have been intentionally omitted in the previous
sections for the sake of clarity and conciseness. This section provides some
important details for the implementation of our method.</p>
      <p id="d1e1367">For the implementation of Eq. (1), the identification of a limited number of
vectors <inline-formula><mml:math id="M80" display="inline"><mml:mrow><mml:msub><mml:mi>A</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> describing the reference module orientations is necessary.
The accuracy of the model output and the computation cost will depend on the
number of vectors chosen. It is thus an important step for an efficient use
of our model. We used a set of 19 module orientation angles: three azimuth
angles (170, 180 and 190<inline-formula><mml:math id="M81" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>) and 7 tilt
angles ranging from 0 to 60<inline-formula><mml:math id="M82" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> with a step of 10<inline-formula><mml:math id="M83" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>. These
are represented by black squares in Fig. 2.</p>
      <p id="d1e1408">Our parameterization of the distribution of the module orientation is a
function of the optimal tilt angle found on the PV-GIS website. This dataset
is displayed in the left map of Fig. 4, where it can be observed that
greater than average values are present in mountains (see e.g. regions of
the Alps or the Pyrenees). These high values are presumably stemming from
the high irradiation values present at high elevations. Since little PV
plants are installed in these regions and to avoid overestimation of the
tilt angle in the region neighbouring the mountains, these values have been
filtered out. The resulting data are displayed in the right map of Fig. 4.</p>
      <p id="d1e1411">As already mentioned in Sect. 3, the expression given in Eq. (2) cannot be
directly used to estimate the weights <inline-formula><mml:math id="M84" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> needed by Eq. (1). Indeed, for
a finite sample of orientation angles <inline-formula><mml:math id="M85" display="inline"><mml:mrow><mml:msub><mml:mi>A</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>, the sum of the values
<inline-formula><mml:math id="M86" display="inline"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi>w</mml:mi><mml:mo mathvariant="normal">̃</mml:mo></mml:mover><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> evaluated with Eq. (2) is not equal to unity. To address
this issue, <inline-formula><mml:math id="M87" display="inline"><mml:mrow><mml:msub><mml:mover accent="true"><mml:mi>w</mml:mi><mml:mo mathvariant="normal">̃</mml:mo></mml:mover><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> estimated with Eq. (2) is normalized as follows
to yield <inline-formula><mml:math id="M88" display="inline"><mml:mrow><mml:msub><mml:mi>w</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math></inline-formula>:

                <disp-formula specific-use="align" content-type="numbered"><mml:math id="M89" display="block"><mml:mtable displaystyle="true"><mml:mtr><mml:mtd><mml:mstyle displaystyle="true" class="stylechange"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle class="stylechange" displaystyle="true"/><mml:msub><mml:mi>w</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mo>∫</mml:mo><mml:mspace linebreak="nobreak" width="-0.125em"/><mml:mspace width="-0.125em" linebreak="nobreak"/><mml:mspace width="-0.125em" linebreak="nobreak"/><mml:munder><mml:mo movablelimits="false">∫</mml:mo><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:munder><mml:msub><mml:mover accent="true"><mml:mi>w</mml:mi><mml:mo mathvariant="normal">̃</mml:mo></mml:mover><mml:mi>i</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">γ</mml:mi><mml:mo>)</mml:mo><mml:mi mathvariant="normal">d</mml:mi><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">d</mml:mi><mml:mi mathvariant="italic">γ</mml:mi></mml:mrow><mml:mrow><mml:munder><mml:mo movablelimits="false">∑</mml:mo><mml:mi>i</mml:mi></mml:munder><mml:mfenced close=")" open="("><mml:mrow><mml:mo>∫</mml:mo><mml:mspace linebreak="nobreak" width="-0.125em"/><mml:mspace width="-0.125em" linebreak="nobreak"/><mml:mspace width="-0.125em" linebreak="nobreak"/><mml:munder><mml:mo movablelimits="false">∫</mml:mo><mml:mrow><mml:msub><mml:mi>D</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:munder><mml:msub><mml:mover accent="true"><mml:mi>w</mml:mi><mml:mo mathvariant="normal">̃</mml:mo></mml:mover><mml:mi>i</mml:mi></mml:msub><mml:mo>(</mml:mo><mml:mi mathvariant="italic">α</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="italic">γ</mml:mi><mml:mo>)</mml:mo><mml:mi mathvariant="normal">d</mml:mi><mml:mi mathvariant="italic">α</mml:mi><mml:mi mathvariant="normal">d</mml:mi><mml:mi mathvariant="italic">γ</mml:mi></mml:mrow></mml:mfenced></mml:mrow></mml:mfrac></mml:mstyle><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mtext>with</mml:mtext></mml:mrow></mml:mtd></mml:mtr><mml:mlabeledtr id="Ch1.E4"><mml:mtd/><mml:mtd><mml:mstyle displaystyle="true" class="stylechange"/></mml:mtd><mml:mtd><mml:mrow><mml:mstyle displaystyle="true" class="stylechange"/><mml:mspace width="0.25em" linebreak="nobreak"/><mml:mspace linebreak="nobreak" width="0.25em"/><mml:mspace linebreak="nobreak" width="0.25em"/><mml:msub><mml:mi>D</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mfenced close="]" open="["><mml:mrow><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mi mathvariant="italic">α</mml:mi></mml:mrow><mml:mn mathvariant="normal">2</mml:mn></mml:mfrac></mml:mstyle><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mo>;</mml:mo><mml:mspace linebreak="nobreak" width="0.125em"/><mml:msub><mml:mi mathvariant="italic">α</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mi mathvariant="italic">α</mml:mi></mml:mrow><mml:mn mathvariant="normal">2</mml:mn></mml:mfrac></mml:mstyle></mml:mrow></mml:mfenced><mml:mo>×</mml:mo><mml:mfenced close="]" open="["><mml:mrow><mml:msub><mml:mi mathvariant="italic">γ</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>-</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mi mathvariant="italic">γ</mml:mi></mml:mrow><mml:mn mathvariant="normal">2</mml:mn></mml:mfrac></mml:mstyle><mml:mspace width="0.125em" linebreak="nobreak"/><mml:mo>;</mml:mo><mml:mspace width="0.125em" linebreak="nobreak"/><mml:msub><mml:mi mathvariant="italic">γ</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo>+</mml:mo><mml:mstyle displaystyle="true"><mml:mfrac style="display"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mi mathvariant="italic">γ</mml:mi></mml:mrow><mml:mn mathvariant="normal">2</mml:mn></mml:mfrac></mml:mstyle></mml:mrow></mml:mfenced></mml:mrow></mml:mtd></mml:mlabeledtr></mml:mtable></mml:math></disp-formula>

            The scalars <inline-formula><mml:math id="M90" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mi mathvariant="italic">α</mml:mi></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M91" display="inline"><mml:mrow><mml:mi mathvariant="italic">δ</mml:mi><mml:mi mathvariant="italic">γ</mml:mi></mml:mrow></mml:math></inline-formula> in Eq. (6) represent
respectively the resolutions of the azimuth and tilt angles, which are both
equal to 10<inline-formula><mml:math id="M92" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> in our implementation.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F5"><caption><p id="d1e1720">Spatial distribution of the installed PV capacity in France and
Germany for the year 2014. The installed capacity is aggregated on the pixel
used for the calaculation which have a resolution of 0.5<inline-formula><mml:math id="M93" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>.</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://asr.copernicus.org/articles/15/51/2018/asr-15-51-2018-f05.png"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F6" specific-use="star"><caption><p id="d1e1740">Comparison of the model output (blue lines) with TSO estimates (red
lines) of the PV power generated in France <bold>(a)</bold> and Germany <bold>(b)</bold>.
The data are displayed over the year with a daily time
resolution in the two plots above and for two example weeks in a 3-hourly
time resolution in the two lower plots.</p></caption>
          <?xmltex \igopts{width=455.244094pt}?><graphic xlink:href="https://asr.copernicus.org/articles/15/51/2018/asr-15-51-2018-f06.png"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F7" specific-use="star"><caption><p id="d1e1757">Scatter plots of the TSO data against model outputs for France
<bold>(a)</bold> and Germany <bold>(b)</bold> for the calculation based on the
spatially resolved installed capacity of the year 2014.</p></caption>
          <?xmltex \igopts{width=398.338583pt}?><graphic xlink:href="https://asr.copernicus.org/articles/15/51/2018/asr-15-51-2018-f07.png"/>

        </fig>

</sec>
</sec>
<sec id="Ch1.S3">
  <title>Model evaluation</title>
<sec id="Ch1.S3.SS1">
  <title>Evaluation methodology</title>
      <p id="d1e1784">The model has been assessed by comparing its outputs to the PV power
generated within a country. Given the approach is influenced by
uncertainties in the input meteorological parameters, this comparison allows
only an indirect evaluation of our model and not a quantification of the
modelling accuracy. However, this approach offers a good balance between
accuracy and versatility. The goal of this evaluation is thus to verify the
plausibility of the model output for a particular model set up. Not only is
there a lack of certainty in the input meteorological data but also there
are various sources of uncertainty impacting the TSO data as well as the
installed capacity used by the model, both making the conclusion of the
validation difficult. To address these issues, we conduct the validation in
two steps. In the first step, the validation is conducted for two countries:
France and Germany, where we have long experience with both the installed
capacity and the TSO data. In this first step, the impact of the uncertainty
on the installed capacities and TSO estimates is under control but its
spatial extension is limited. We therefore conduct a second step, where TSO
data from 16 countries are considered. Given the lack of available
information on the installed PV capacity in these countries, it is assumed
spatially and temporally constant. The actual installed capacity<?pagebreak page56?> being
unknown, the validation is made by evaluating the correlation coefficient
between TSO data and model output.</p>
</sec>
<sec id="Ch1.S3.SS2">
  <title>Detailed evaluation of the model output for France and Germany</title>
      <p id="d1e1793">The assessment is first performed for Germany and France for the year 2014.
The choice of these two countries has been strongly motivated by the
comparatively high level of knowledge of their electricity supply structure
and the availability of the data to conduct the validation. The PV power
data was provided by the TSOs themselves with a time resolution ranging from
15 min to 1 h. A visual analysis of the time series was performed to control
the data. The data was aggregated into 3 h means to conform to the temporal
resolution of the meteorological data. Instants with no production by PV
(night time) were excluded from the comparison.</p>
      <p id="d1e1796">The German case is used to validate the assumption made that the statistical
quantities evaluated with 35 000 plants can be generalized to the ca. 1 500 000 plants
installed in Germany at that time. France has a different
level of PV<?pagebreak page57?> development compared to Germany and is located at slightly
different latitudes. This second case will test the validity of our approach
to generalize the statistical quantities evaluated in Germany to another
country with somewhat different meteorological conditions.</p>
      <p id="d1e1799">Gridded values of the normalized PV power were computed with the model using
the bias-adjusted ERA-interim data proposed by the ECEM project (Jones et
al., 2017) as meteorological inputs. A bias-adjusted dataset was preferred
to the original ERA-Interim re-analysis dataset in order to limit the effect
of error in the input meteorological data on the assessment of model
performance. The bias-adjusted ERA-Interim covers the period from 1 January 1979
to 31 December 2016 and is covering Europe with a spatial resolution of
0.5<inline-formula><mml:math id="M94" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> <inline-formula><mml:math id="M95" display="inline"><mml:mo>×</mml:mo></mml:math></inline-formula> 0.5<inline-formula><mml:math id="M96" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula>. The domain covered by the data extends
between 21.75 and 45.25<inline-formula><mml:math id="M97" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> in longitude and between 26.75 and
72.25<inline-formula><mml:math id="M98" display="inline"><mml:msup><mml:mi/><mml:mo>∘</mml:mo></mml:msup></mml:math></inline-formula> in latitude. The two meteorological variables used for the
calculation were the solar surface radiation downward (SSRD, also known as
GHI) and air temperature at 2 m. As the input meteorological data has a time
resolution of 3 h for SSRD and 6 h for temperature, an increase of the time
resolution was needed to properly estimate the PV power generation with
respect to the variation of the sun position with time. For this purpose,
the temperature and clearness index (the ratio of SSRD to the irradiation at
the top of atmosphere) were resampled down to a time resolution of 5 min by
a linear interpolation technique. The normalized PV power was calculated
with these resampled inputs and then summed up on 3 h periods, which is the
original time resolution of the solar radiation data.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F8"><caption><p id="d1e1847">Histograms of the ratio of actual plant tilt angles with the
corresponding optimal value for different classes of nominal capacity
(coloured lines). In the upper plot, the German case is calculated with the
IWES database. The French case is displayed in the lower plot where data from
BDPV are used.</p></caption>
          <?xmltex \igopts{width=241.848425pt}?><graphic xlink:href="https://asr.copernicus.org/articles/15/51/2018/asr-15-51-2018-f08.png"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F9" specific-use="star"><caption><p id="d1e1859">Spatial distribution of the tilt angle for plants smaller than
25 kW<inline-formula><mml:math id="M99" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">p</mml:mi></mml:msub></mml:math></inline-formula> <bold>(a)</bold> and greater than 25 kW<inline-formula><mml:math id="M100" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">p</mml:mi></mml:msub></mml:math></inline-formula>.</p></caption>
          <?xmltex \igopts{width=369.885827pt}?><graphic xlink:href="https://asr.copernicus.org/articles/15/51/2018/asr-15-51-2018-f09.png"/>

        </fig>

      <p id="d1e1889">By using gridded maps of the installed PV capacity in each country (Fig. 5),
the generated PV power was computed at each grid cell and then spatially
summed to yield the production for each country. The data on the installed
PV plants used for this purpose have been retrieved from the websites of the
four German TSOs (PV-DE 2014) and from a data portal of the French
government (PV-FR 2014). Finally, all time series have been normalized by
the total installed PV capacity, which is equal to 6.17 and 36.87 GW<inline-formula><mml:math id="M101" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">p</mml:mi></mml:msub></mml:math></inline-formula>
for France and Germany, respectively, in 2014 (PV-DE, 2014; PV-FR, 2014). Figure 6
exhibits the time series of both measured production and model outputs for
France and Germany daily and 3 h resolutions. It reveals that the seasonal
variations of the PV power are well assessed by the proposed model for the
two countries and that the match between model output and actual values is
qualitatively good. Scatter plots of the TSO data against the model outputs
are displayed in Fig. 7 for France and Germany for the 3 hourly resolution
and different error metrics are also displayed in Fig. 7. The data points
are well centred on the identity line for Germany while an underestimation
by the model can be observed for France. These observations are confirmed by
the bias, which are respectively equal to <inline-formula><mml:math id="M102" display="inline"><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2.4</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> and
<inline-formula><mml:math id="M103" display="inline"><mml:mrow><mml:mn mathvariant="normal">0.1</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> W W<inline-formula><mml:math id="M104" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mi mathvariant="normal">p</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula> for France and Germany. The correlation
coefficient is large in both countries: 0.987 and 0.975 respectively for
France and Germany. The MAE is respectively <inline-formula><mml:math id="M105" display="inline"><mml:mrow><mml:mn mathvariant="normal">3.8</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> and
<inline-formula><mml:math id="M106" display="inline"><mml:mrow><mml:mn mathvariant="normal">2.4</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> W W<inline-formula><mml:math id="M107" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mi mathvariant="normal">p</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula>; the RMSE is respectively
<inline-formula><mml:math id="M108" display="inline"><mml:mrow><mml:mn mathvariant="normal">4.2</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> and <inline-formula><mml:math id="M109" display="inline"><mml:mrow><mml:mn mathvariant="normal">3.0</mml:mn><mml:mo>×</mml:mo><mml:msup><mml:mn mathvariant="normal">10</mml:mn><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">2</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula> W W<inline-formula><mml:math id="M110" display="inline"><mml:mrow><mml:msubsup><mml:mi/><mml:mi mathvariant="normal">p</mml:mi><mml:mrow><mml:mo>-</mml:mo><mml:mn mathvariant="normal">1</mml:mn></mml:mrow></mml:msubsup></mml:mrow></mml:math></inline-formula>.</p>
      <p id="d1e2057">Some efforts were made to understand the reasons for the greater bias value
observed for France. During this investigation we obtained access to the
content of the bdpv.fr online portal (BDPV, 2018), which contains the main
information for more than 20 000 PV plants installed in France. We used this
new data source to compare the characteristics of the German and French PV
plants and to verify the validity of our assumption for France.</p>
      <p id="d1e2060">The strongest assumption made in this work is to consider that the mean tilt
angle is equal to the product of the optimal tilt angle and a constant <inline-formula><mml:math id="M111" display="inline"><mml:mi>f</mml:mi></mml:math></inline-formula>
equal to 0.7. In order to verify this assumption, the ratio between actual
and optimal module tilt angle has been analysed for the two countries. The
histograms of this ratio are displayed for the two countries and for
different classes of nominal capacity in Fig. 8. The assumed value for the
ratio <inline-formula><mml:math id="M112" display="inline"><mml:mi>f</mml:mi></mml:math></inline-formula> is displayed by a dashed black line in these two plots. We can
observe that the assumed ratio value matches well large German plants with
an installed capacity greater than 500 kW<inline-formula><mml:math id="M113" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">p</mml:mi></mml:msub></mml:math></inline-formula> (no information on large PV
plant is available in France). Data from both countries reveal that this
value is not fitting actual tilt values of medium and small plants: an
optimal ratio value of 0.4–0.6 would better match plants with an installed
capacity between 50 and 500 kW<inline-formula><mml:math id="M114" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">p</mml:mi></mml:msub></mml:math></inline-formula> and a ratio value of 0.9–1.3 would be
better for plants with an installed capacity smaller than 10 kW<inline-formula><mml:math id="M115" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">p</mml:mi></mml:msub></mml:math></inline-formula>. It is
interesting to note that the optimal ratio changes with the size<?pagebreak page58?> of the
plants in a similar way for both countries. These observations indicate,
that the variation of the share of PV plants according to their size between
countries can bring about a deviation from the assumed factor of 0.7. A
first possible explanation for bias observed in France may thus be that the
distribution of French plants according to their size is different from the
German one.</p>
      <p id="d1e2104">It would be interesting to exploit the trend observed in Fig. 8 in our
model. However, information on the size of installed PV plants is missing in
most European countries so that this is unfortunately impossible. Based on
these new results, one can wonder whether the choice of a value of 0.7 for
the ratio between actual and optimal tilt is still relevant? Given that
larger plants have more weight for the calculation of the regional PV power
generation than smaller plants, we consider that our estimate is not
unfounded and we decide to keep this value.</p>
      <p id="d1e2107">In Fig. 8, it can also be observed that for PV plants with an installed
capacity smaller than 10 kW<inline-formula><mml:math id="M116" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">p</mml:mi></mml:msub></mml:math></inline-formula>, the range of tilt angle values taken by
French plants is larger than for German plants. To understand this
difference, the tilt angle values of small plants have been displayed as a
function of their geographic position (Fig. 9). In this map, a very large
difference in tilt angles between North and South of France can be observed.
This spatial difference is much more pronounced than the spatial variation
that can be expected from the optimal tilt angle. Since such a marked
spatial difference is not present in Germany, it could bed a second possible
explanation to the observed bias in France.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F10" specific-use="star"><caption><p id="d1e2122">Scatter plots of three-hourly ENTSO-E solar generation data against
the corresponding model output for 16 European countries for the year 2016.
The modelled PV generation has been calculated with ERA-interim data assuming
a spatially constant installed capacity.</p></caption>
          <?xmltex \igopts{width=341.433071pt}?><graphic xlink:href="https://asr.copernicus.org/articles/15/51/2018/asr-15-51-2018-f10.jpg"/>

        </fig>

      <?xmltex \floatpos{t}?><fig id="Ch1.F11"><caption><p id="d1e2133">Spatial distribution of the correlation between ENTSO-E data and
model output for a three-hourly time resolution and for the year 2016.</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://asr.copernicus.org/articles/15/51/2018/asr-15-51-2018-f11.png"/>

        </fig>

      <p id="d1e2142">As reported in Saint-Drenan (2015), the spatial variations of the tilt angle
of small plants are resulting from regional architectural practices. It
would therefore be tempting to integrate this information into our model.
However, because this information is not commonly available (i.e. not even
for France), it could not be accounted for in a robust way.</p>
</sec>
<sec id="Ch1.S3.SS3">
  <title>Model evaluation for all European countries</title>
      <p id="d1e2151">Though the results of this first validation can be considered as
satisfactory, it is important to also demonstrate that results for Germany
and France can be extrapolated to other (European) countries, also with
different climates, engineering practices, etc. We therefore decided to
conduct an additional validation step, in which we compared the output of
our model to additional TSO data. To this end, we collected time series of
solar power generation on the ENTSO-E Transparency Portal for 16 countries
for the year 2015 and built 3-hourly averages to make the data comparable
with the model output. The model setup is the same than in the previous
validation except for the installed capacity, which is not known and thus
assumed spatially and temporally constant (even in France and Germany).
Indeed, the information available on the installed capacity is only updated
yearly and we experiment several situations where the time series of the
production were not matching with the given installed capacity (e.g.
situation with production values greater than the installed capacity).</p>
      <?pagebreak page60?><p id="d1e2154">The comparison of the model output with the ENTSO-E data has been conducted
for 16 countries. The scatter plot of the model output against ENTSO-E data
is given in Fig. 10 for each country. As mentioned before, since the
installed capacity is not known, the model output has not been scaled to the
actual capacity. As a result, one should not consider the absolute error
values in these plots but solely the correlation between the two time
series. Accordingly, only the correlation coefficient is given in Fig. 10 and
discussed in the remaining of this section. To facilitate the visualisation
of the results, the correlation coefficients evaluated for the different
countries are displayed as a map in Fig. 11.</p>
      <p id="d1e2157">With values greater than 0.97, the correlations are particularly high in
Italy, France and Germany. These results confirm those obtained for France
and Germany in the first validation. That the best correlation (0.982) is
found for Italy is a very good surprise since no information on the PV
plants installed in this country was considered in the model development. As
we can see in Fig. 12, the high installed capacity in Italy (ca. 19 GW<inline-formula><mml:math id="M117" display="inline"><mml:msub><mml:mi/><mml:mi mathvariant="normal">p</mml:mi></mml:msub></mml:math></inline-formula>
in 2016) may account for this good performance. The correlation coefficients
are high and comprised between 0.95 and 0.97 for six countries: Denmark,
Belgium, Czech Republic, Slovakia, Greece and Portugal. This demonstrates
that the proposed approach using the optimal tilt angle is valid at
different latitudes. The low performance of the model for Spain is explained
by the fact that the time series of solar generation available on the
ENTSO-E website includes both photovoltaic and concentrated solar power
generation. The reason for the medium performance in the remaining countries
is unclear: it may stem from an intra-yearly change of the installed
capacity, from lower performance of the re-analysis data in some regions or
from other unidentified issues, including in the ENTSO-E generation data. It
is however interesting to note that in the 16 countries, as shown in Fig. 8,
the greater the installed capacity, the better the performance of our model
performance. There may be several reasons to explain this observation:
firstly, the relative effect of the intra-yearly new installations is lower
when the installed capacity is high, and secondly, our assumption on the
distribution of plants may only become valid as the number of plants exceeds
a certain threshold.</p>

      <?xmltex \floatpos{t}?><fig id="Ch1.F12"><caption><p id="d1e2171">scatter plot of the correlation coefficients between model output
and ENTSO-E data against installed PV capacity for the 16 different
countries.</p></caption>
          <?xmltex \igopts{width=236.157874pt}?><graphic xlink:href="https://asr.copernicus.org/articles/15/51/2018/asr-15-51-2018-f12.png"/>

        </fig>

</sec>
</sec>
<sec id="Ch1.S4" sec-type="conclusions">
  <title>Conclusions</title>
      <p id="d1e2187">This paper describes an innovative approach that offers a trade-off between
implementation constraints and model output accuracy convenient for the
goals of the C3S ECEM service and that may be used in other contexts. The
validation of the model against country-aggregated production of electricity
by PV plants for France and Germany shows that the model is accurate enough
with a RMSE of 3–4 % of the installed capacity. In addition, the model has
been further validated against solar power generation time series from 16
countries, which give correlation coefficient above 0.94 except for 4
countries (Austria, Lithuania, Netherlands, and Switzerland). The reasons
for the under-average scores for these countries could unfortunately not be
identified, which represents a first possible continuation of the present
work. This validation revealed that the greater the installed capacity the
better the performance of our model is. This finding together with the
satisfying results of our performance analysis, confirm that the proposed
model is well suited for our targeted applications. Indeed, the goal of the
present work was not to make a perfect model for a single country but to
propose a generalized approach that can be implemented in any (European)
region without having to collect any specific information on the fleet of
plants installed in that country. We believe an under-optimal performance is
thus acceptable<?pagebreak page61?> with respect to the gain in flexibility offered by the
proposed approach.</p>
      <p id="d1e2190">Additional validation work would bring a better insight into the strengths
and weaknesses of the proposed methodology and identify possible
improvements. In addition, data on PV production is available from TSOs in
many European countries and the validation may be performed for these
countries thus confirming or not the performances of the model presented
here. The model may be refined with respect to its parameters using more
data from various countries. A possible approach to this end may consist in
estimating the probability function of the regional PV model using inversion
techniques, using the optimal tilt angle dependent distribution described in
this paper as a first guess.</p>
      <p id="d1e2193">Time series of PV power generation have been calculated in the framework of
the C3S ECEM service with the proposed approach using the ECEM bias-adjusted
ERA interim data and future climate projections for 33 countries in a 3 h
time resolution. These model output data are freely available on the
demonstrator of this project: <uri>http://ecem.climate.copernicus.eu/demo</uri></p>
</sec>

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

      <p id="d1e2203">The set of adjusted reanalysis data is available on ESSD
(Jones et al., 2017) and has the following DOI <ext-link xlink:href="https://doi.org/10.5194/essd-9-471-2017" ext-link-type="DOI">10.5194/essd-9-471-2017</ext-link>.
Times series of aggregated PV power generation are available at country level
for all EU countries on the following ftp server
<uri>ftp://ecem.climate.copernicus.eu/</uri>.</p>
  </notes><notes notes-type="competinginterests">

      <p id="d1e2215">The authors declare that they have no conflict of
interest.</p>
  </notes><notes notes-type="sistatement">

      <p id="d1e2221">This article is part of the special issue “17th EMS Annual
Meeting: European Conference for Applied Meteorology and Climatology 2017”.
It is a result of the EMS Annual Meeting: European Conference for Applied
Meteorology and Climatology 2017, Dublin, Ireland, 4–8 September 2017.</p>
  </notes><ack><title>Acknowledgements</title><p id="d1e2227">The authors would like to acknowledge funding for the European Climatic
Energy Mixes (ECEM) service by the Copernicus Climate Change Service, a
programme being implemented by the European Centre for Medium-Range Weather
Forecasts (ECMWF) on behalf of the European Commission. The specific grant
number is 2015/C3S_441_Lot2_UEA.<?xmltex \hack{\newline}?><?xmltex \hack{\newline}?> Edited by:
Sven-Erik Gryning<?xmltex \hack{\newline}?> Reviewed by: Sven Killinger, Hans Georg
Beyer, <?xmltex \hack{\newline}?> and one anonymous referee</p></ack><?xmltex \hack{\newpage}?><?xmltex \hack{\newpage}?><ref-list>
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  </ref-list></back>
    <!--<article-title-html>An approach for the estimation of the aggregated photovoltaic power generated in several European countries from meteorological data</article-title-html>
<abstract-html><p>Classical approaches to the calculation of the photovoltaic (PV) power
generated in a region from meteorological data require the knowledge of the
detailed characteristics of the plants, which are most often not publicly
available. An approach is proposed with the objective to obtain the best
possible assessment of power generated in any region without having to
collect detailed information on PV plants. The proposed approach is based on
a model of PV plant coupled with a statistical distribution of the prominent
characteristics of the configuration of the plant and is tested over Europe.
The generated PV power is first calculated for each of the plant
configurations frequently found in a given region and then aggregated taking
into account the probability of occurrence of each configuration. A
statistical distribution has been constructed from detailed information
obtained for several thousands of PV plants representing approximately
2&thinsp;% of the total number of PV plants in Germany and was then adapted to
other European countries by taking into account changes in the optimal PV
tilt angle as a function of the latitude and meteorological conditions. The
model has been run with bias-adjusted ERA-interim data as meteorological
inputs. The results have been compared to estimates of the total PV power
generated in two countries: France and Germany, as provided by the
corresponding transmission system operators. Relative RMSE of 4.2 and
3.8&thinsp;% and relative biases of −2.4 and 0.1&thinsp;% were found with
three-hourly data for France and Germany. A validation against estimates of
the country-wide PV-power generation provided by the ENTSO-E for 16 European
countries has also been conducted. This evaluation is made difficult by the
uncertainty on the installed capacity corresponding to the ENTSO-E data but
it nevertheless allows demonstrating that the model output and TSO data are
highly correlated in most countries. Given the simplicity of the proposed
approach these results are very encouraging. The approach is particularly
suited to climatic timescales, both historical and future climates, as
demonstrated here.</p></abstract-html>
<ref-html id="bib1.bib1"><label>1</label><mixed-citation>
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<a href="http://www.BDPV.fr" target="_blank">http://www.BDPV.fr</a>, last access: February 2018.
</mixed-citation></ref-html>
<ref-html id="bib1.bib2"><label>2</label><mixed-citation>
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satellite-derived PV power nowcasting using real-time power data from
reference PV systems, Sol. Energy, <a href="https://doi.org/10.1016/j.solener.2017.10.091" target="_blank">https://doi.org/10.1016/j.solener.2017.10.091</a>, in
press, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib3"><label>3</label><mixed-citation>
Jamaly, M., Bosch, J., and Kleissl, J.: Aggregate Ramp Rates Analysis of
Distributed PV Systems in San Diego County, 4, 519–526, 2013.
</mixed-citation></ref-html>
<ref-html id="bib1.bib4"><label>4</label><mixed-citation>
Jerez, S., Thais, F., Tobin, I., Wild, M., Colette, A., Yiou, P., and Vautard,
R.: The CLIMIX model: A tool to create and evaluate spatially-resolved
scenarios of photovoltaic and wind power development,
Renewable and Sustainable Energy Reviews, 42, 1–15, <a href="https://doi.org/10.1016/j.rser.2014.09.041" target="_blank">https://doi.org/10.1016/j.rser.2014.09.041</a>, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib5"><label>5</label><mixed-citation>
Jones, P. D., Harpham, C., Troccoli, A., Gschwind, B., Ranchin, T., Wald, L.,
Goodess, C. M., and Dorling, S.: Using ERA-Interim reanalysis for creating
datasets of energy-relevant climate variables, Earth Syst. Sci. Data, 9,
471–495, <a href="https://doi.org/10.5194/essd-9-471-2017" target="_blank">https://doi.org/10.5194/essd-9-471-2017</a>, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib6"><label>6</label><mixed-citation>
Killinger, S., Guthke, P., Semmig, A., Müller, B., Wille-Haussmann, B.,
and Fichtner, W.: Upscaling PV Power Considering Module Orientations, IEEE J.
Photovoltaics, 7, 941–944, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib7"><label>7</label><mixed-citation>
Lingfors, D. and Widén, J.: Development and validation of a wide-area
model of hourly aggregate solar power generation, Energy, 102, 559–566,
2016.
</mixed-citation></ref-html>
<ref-html id="bib1.bib8"><label>8</label><mixed-citation>
Lorenz, E. and Heinemann, D.: Prediction of Solar Irradiance and Photovoltaic
Power, in: Comprehensive Renewable Energy, 1, 239–292, <a href="https://doi.org/10.1002/pip.1224" target="_blank">https://doi.org/10.1002/pip.1224</a>,
2012.
</mixed-citation></ref-html>
<ref-html id="bib1.bib9"><label>9</label><mixed-citation>
Marinelli, M., Maule, P., Hahmann, A. N., Gehrke, O., Nørgård, P. B.,
and Cutululis, N. A.: Wind and Photovoltaic Large-Scale Regional Models for
Hourly Production Evaluation, IEEE Trans. Sustain. Energy, 6, 916–923, 2015.
</mixed-citation></ref-html>
<ref-html id="bib1.bib10"><label>10</label><mixed-citation>
Pierro, M., De Felice, M., Maggioni, E., Moser, D., Perotto, A., Spada, F.,
and Cornaro, C.: Data-driven upscaling methods for regional photovoltaic
power estimation and forecast using satellite and numerical weather
prediction data, Sol. Energy, 158, 1026–1038, 2017.
</mixed-citation></ref-html>
<ref-html id="bib1.bib11"><label>11</label><mixed-citation>
PV-DE: register of PV plants installed in France at the end of 2014 taken
from the 4 German transmission system operators,
<a href="https://www.tennettso.de/site/Transparenz/veroeffentlichungen/netzkennzahlen/tatsaechliche-und-prognostizierte-solarenergieeinspeisung" target="_blank">https://www.tennettso.de/site/Transparenz/veroeffentlichungen/netzkennzahlen/tatsaechliche-und-prognostizierte-solarenergieeinspeisung</a>,
<a href="http://www.amprion.net/photovoltaikeinspeisung" target="_blank">http://www.amprion.net/photovoltaikeinspeisung</a>,
<a href="http://www.50hertz.com/de/Kennzahlen/Photovoltaik" target="_blank">http://www.50hertz.com/de/Kennzahlen/Photovoltaik</a>,
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<ref-html id="bib1.bib12"><label>12</label><mixed-citation>
PV-FR: register of PV plants installed in France at the end of 2014,
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Saint-Drenan, Y.-M.: A Probabilistic Approach to the Estimation of Regional
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