Abstract
This review focuses on the solar irradiance model chain for horizontal-to-tilted irradiance conversion at high latitudes. The main goals of the work are 1) to assess the extent to which the literature accounts for decomposition and transposition models specifically developed for high-latitude application; 2) to evaluate existing validation studies for these particular conditions; 3) to identify research gaps in the optimal solar irradiance model chain for high-latitude application (i.e., latitude ≥60°). In total, 112 publications are reviewed according to their publication year, country, climate, method, and keywords: 78 publications deal with decomposition models and 34 deal with transposition models. Only a few models (6) have been parameterized using data from Nordic countries. Here, we compare 57 decomposition models in terms of their performance in Nordic climate zones and analyze the geographical distribution of the data used to parametrize these models. By comparing the Normalized Root Mean Square Deviation coefficients for direct normal irradiation, the decomposition models Skartveit1 and Mondol1 are most effective on one-hour scale and Yang4 on one-minute scale. Recent studies on the empirical transposition models estimating the global tilted irradiation on vertical surfaces show the best performance for Perez4 and Muneer models. In addition, innovative methods such as artificial neural networks have been identified to further enhance the model chain. This review reveals that a validated model chain for estimating global tilted irradiation at high latitudes is missing from the literature. Moreover, there is a need for a universal validation protocol to ease the comparison of different studies.
Highlights
• In total, 47 one-hour and 10 one-minute decomposition models are parametrized for high latitudes.
• Skartveit1 and Yang4 are the most effective one-hour and one-minute models.
• Perez4 and Muneer can assess east-west vertical bifacial photovoltaics.
• Decomposition models can achieve sub-hour resolution, transposition models cannot.
• Validated model chains are lacking for east-west vertical surfaces at high latitudes.
1 Introduction
Achieving net-zero emissions by 2050 represents a milestone for the low-carbon built environment. However, reaching this target is hindered by continuously rising global energy consumption (). In response, different governments have proposed increasing the share of energy production from renewables and enhancing the efficiency of new energy power plants ().
To achieve climate targets, monofacial photovoltaics (MPV) and bifacial photovoltaics (BPV) have been exploited in recent decades. While MPV produces electricity by collecting sunlight only from the front side (i.e., the backside is covered with an opaque sheet), BPV collects sunlight from both sides of the panel. Using two active sides (i.e., the front and the rear side) increases overall energy production because the backside of the panel can harvest sunlight scattered by the atmosphere and reflected by the ground or other surfaces behind the panel. When not integrated into the building envelope, MPV and BPV are generally south oriented (in the Northern Hemisphere) and tilted at an optimal angle, which maximizes annual energy production, depending on the location. Therefore, the peak in energy production is usually observed at around solar noon. However, there is a mismatch between typical solar production and the average consumption profile of a residential sector which peaks in the early morning (around 7–8a.m.) and late afternoon (around 5–6p.m.) (). Such a temporal mismatch between solar power production and electricity load can be reduced by adopting east-west (E-W) vertically mounted BPV systems (VBPV) (; ), whose production peaks are specifically in the morning and in the afternoon or evening. Furthermore, the electricity spot price typically peaks during the evening, and therefore increasing the self-consumption of PV electricity should be prioritized. Increasing self-consumption and avoiding electricity use during peak price represent the main drivers for E-W VBPV.
E-W VBPV have the greatest potential at high latitudes () based on the low average Sun elevation, wide azimuth range, and long periods of high ground albedo due to snowfalls (; ). In these conditions, an E-W VBPV can outperform a south-facing photovoltaic (PV) system (; ). investigated the advantages and disadvantages of MPV and BPV installations from an economic perspective. Their analysis highlighted the importance of different parameters, such as latitude, weather data, albedo, and the applied model chain, when calculating global tilted irradiance (Egt) (; ). Knowing the Egt is a key factor for determining the potential energy production of a new PV plant (; ). To estimate the Egt, the amount of direct normal irradiance (Ebn) and diffuse horizontal irradiance (Edh) must be known. However, ground measurements of Ebn and Edh are uncommon, and these quantities are usually estimated from global horizontal irradiance (Egh) using empirical decomposition models (). Although the scientific community has improved and developed new decomposition models since they were first introduced in 1961, they continue to be strongly influenced by the selected location, as they are empirical models based on site-specific data (; ). The number of locations considered in the model parametrization has been increasing in the recent years by permitting to implement a group of quasi-universal models (i.e., decomposition models for global application) in contrast to local models (i.e., decomposition models for regional application). However, local models can outperform models presented as quasi-universal when applied to the location where the data originates ().
In contrast to decomposition models, transposition models allow Egt to be estimated based on solar irradiance (i.e., Ebn, Edh), Sun geometry (i.e., solar zenith angle, solar azimuth angle), and surface geometry (i.e., tilt angle, azimuth angle). These models have used different assumptions about the spatial distribution of sky radiance over the hemisphere, ranging from isotropic () to anisotropic (). Nowadays, the anisotropic assumption is used the most, as it accounts for the circumsolar and horizon brightening contribution beyond the isotropic sky radiance and the direct beam irradiance (Figure 1).
FIGURE 1
Within this framework, E-W VBPV systems in high-latitude application pose different challenges compared to south-facing PV systems. In particular, during the early and late hours of the day, when energy production peaks for E-W VBPV systems, the atmospheric thickness is high, which is a major source of error in many transposition models (). In addition, solar elevations less than five degrees are often omitted in the decomposition models because data quality check routines tend to filter them out as low-reliable datapoints (; ). This is only a minor drawback when modelling conventionally mounted PV systems. However, when modelling vertical E-W mounted systems at high latitudes, a significant part of the production is cut when solar elevations below five degrees are excluded (Figure 2). During 2021 in Trondheim (Norway), a direct solar irradiance of approximately 120 kWh/m2 reached the ground throughout the year (around 15% of the total yearly direct normal irradiance) when the Sun elevation angle was lower than five degrees. Moreover, another source of error is related to the estimation of the horizon brightness component of diffuse irradiance, which has a greater influence on E-W VBPV than on south-facing MPV systems.
FIGURE 2
1.1 Aims and structure of the study
The ability to accurately predict PV energy production is based on implementing a solar irradiance model chain which comprises suitable decomposition and transposition models. Knowing which combination of decomposition and transposition models should be used to estimate Egt in a new PV system is of primary importance. In fact, the accuracy of the model used for estimating the available solar energy is tied to uncertainty in the predicted energy production of the system. However, such models are usually created and validated for a specific geographical area (i.e., local, regional, global). Therefore, their accuracy can vary depending on where they are exploited.
Although a significant number of publications have validated decomposition and transposition models, the extent to which the literature covers the use of decomposition models in the Nordic geographical area is unclear. Moving from the extensive worldwide validation studies carried out by , and , the aim of this review is to explore decomposition models which can adequately estimate the Edh and Ebn at high latitudes. In addition, transposition model validation studies are investigated to provide a complete theoretical framework for a model chain for Egt estimation of E-W VBPV in Nordic setting. The paper is structured as follows: the materials and methods (Section 2) defines the literature search workflow, the statistical indicators, and the investigated location; the theory section (Section 3) outlines the theoretical framework behind the model chain for Egt estimation; the results section (Section 4) provides an overview of decomposition and transposition models; the discussion section (Section 5) comments on the results and analyses the strengths, weaknesses, opportunities, and threats (SWOT), literature gaps, and study limitations. The review concludes by considering future developments and summarises the most important findings and the implications for future advancements in model development and application to high-latitude locations (Section 6).
2 Material and methods
2.1 Literature search
A systematic review approach was followed to investigate decomposition and transposition models for predicting Egt on E-W VBPV in high-latitude locations. Relevant literature was identified using a keyword-based search on the Web of Science (WoS) and Scopus databases. Among the existing databases, these were selected as they return literature from highly reliable sources and provide wide geographic coverage. Identical search terms were used in both databases. Scientific journal articles that focused on the development and validation of methodologies for estimating Egt were selected through a three-step screening process similar to (). The first and the limited to selecting the best combination of search terms. Although using numerous search terms may be considered best, it can result in an unnecessarily high number of database hits which require longer and more extensive screening. In the third step, the eligibility of each database hit was “manually” assessed. The abstracts were screened to identify and exclude review articles and comparative studies which did not introduce new models.
Initially, all the possible combinations of three groups of terms were searched for in the titles, abstracts and keywords of the papers selected from both databases. The Boolean Operator “AND” was used to connect the three groups (A, B, and C) which included the following terms:
• Group A: “decomposition” and “transposition”;
• Group B: “*radia*“, and “solar”;
• Group C: “tilted”, “photovoltaic”, and “surface”.
Terms within the same group were mainly connected with the Boolean Operator “OR”. In particular, the query which was entered in both databases was: (“decomposition” OR “transposition”) AND (“*radia*” W/3 “solar”) AND (“tilted” OR “surface” OR “photovoltaic”). The operator W/3 (NEAR/3 in WoS) indicated that the search should only identify articles where the connected words appear within a range of 3 words in the selected search fields, while the asterisks were used to consider all the words including “radia” such as “irradiation”, “radiation”, “radiative”, and “irradiance”. The search was conducted in March 2022. The chosen search terms were found in more than 500 articles in Scopus and WoS. The order of the terms within the group and the order of the groups did not alter the returned literature: for example, (“decomposition” OR “transposition”) AND (“*radia*" W/3 “solar”) AND (“tilted” OR “surface” OR “photovoltaic”) and (“solar” W/3“*radia*”) AND (“photovoltaic” OR “tilted” OR “surface”) AND (“transposition” OR “decomposition”) returned the same publications. However, this search was deemed ineffective, as it returned a wide range of literature with topics beyond the scope of decomposition and transposition models. The search terms used in step two were refined with the help of the VOS Visualizer tool. This machine learning-based tool ranks the words contained in authors’ keywords from database hits and then applies clustering models to classify the most used words in groups. The resulting density visualization provided a quick overview of the main areas in the bibliometric network, highlighting the presence of journal articles about chemical photodegradation, photocatalysis, and x-ray diffraction. The density visualization in Figure 3 shows how the database hits belong to two different research areas that only share the “solar energy” term. Probably, using “decomposition” without “model” as well as including “photovoltaic” in the entered query led to such undesirable results.
FIGURE 3
In step two, the entered query was modified into: [(“decomposition” OR “transposition”) W/5 “model”] AND (“*radia*” W/3 “solar”). The density visualization map (Figure 4) highlights the exclusion of the unwanted scientific journal articles which appeared in step one. The chosen search terms were found in around 150 articles in Scopus and WoS. Finally, the screening process in the third step permitted the results to be further narrowed. Around 110 database hits were selected for a detailed review in this study. Among these, 78 research studies describe decomposition models, while 34 research studies focus on transposition models.
FIGURE 4
2.2 Climate zones
Studies related to Norway, Sweden and Finland were investigated in this work. According to the Köppen-Geiger climate classification () updated by , these countries mainly belong to subtypes of cold climate which begin with the letter D (Table 1). Alongside these, areas classified as subzones from polar climate (E) and mild temperate climate (C) are also present (Figure 5).
TABLE 1
| 1st | 2nd | 3rd | Description | Criteria |
|---|---|---|---|---|
| D | Cold | Thot>10 & Tcold≤0 | ||
| s | - Dry summer | Psdry<40 & Psdry < Pwwet/3 | ||
| w | - Dry winter | Pwdry < Pswet/10 | ||
| f | - Without dry season | Not (Ds) or (Dw) | ||
| a | - Hot summer | Thot≥22 | ||
| b | - Warm summer | Not (a) & Tmon10 ≥ 4 | ||
| c | - Cold summer | Not (a,b, or d) | ||
| d | - Very cold summer | Not (a or b) & Tcold < −38 |
Description of Köppen-Geiger climate symbols and defining criteria for the cold climate.
Thot is the temperature of the hottest month, Tcold is the temperature of the coldest month, Tmon10 is the number of months where the temperature is above 10, Psdry is the precipitation of the driest month in summer, Pwdry is the precipitation of the driest month in winter, Pswet is the precipitation of the wettest month in summer, Pwwet is the precipitation of the wettest month in winter.
FIGURE 5
Most Norwegian, Swedish, and Finnish regions belong to the “Dfc” sub-climate which corresponds to subarctic climates with the coldest month averaging below 0°C and up to 3 months averaging above 10°C. No significant precipitation difference is observed throughout the year. However, since only one weather station from the Dfc subzone is considered in the most relevant validation studies about decomposition models (
3 Theory
3.1 Global tilted irradiance calculation
This section outlines the theory behind decomposition and transposition models used to estimate Egt. Regarding the taxonomy applied to decomposition and transposition models, these are named after the main author’s name with the addition of a number in case more models from the same author exist. In this article, the only exception to this is represented by the BRL decomposition model which is named after the initial of the three scientists who developed this: Boland,
The total solar irradiance outside the Earth`s atmosphere (E0) is almost constant at 1,361.1 W/m2 (
As reported in Eq. 1, the sum of direct and diffuse irradiance incident to a horizontal plane is defined as Egh.where θz is the solar zenith angle (the angle between the direct line to the Sun and a vertical line).
The Egh is used to calculate the clearness index (kt) which is equal to the Egh to E0cosθz ratio. The diffuse fraction (kd) is the share of the diffuse horizontal irradiance from the global horizontal irradiance (Edh/Egh). Due to the atmosphere inhomogeneity, the kt and kd indices vary with space and time.
The Edh can be split into isotropic (Ed;iso), circumsolar (Ed;circ) and horizon brightening (Ed;hor) components. The Ed;iso is emanated uniformly from every point in the sky dome, while the Ed;circ originates from forward scattering rays near the path of sunrays. Finally, the Ed;hor consists of the brightness near the horizon and occurs when rays are scattered multiple times in the atmosphere in a band just above the horizon. Positive values for Ed;hor correspond to clear sky days (and they increase with the θz), while negative values are calculated for overcast days when the sky is not visible and the clouds near the horizon are darker than the rest of the hemisphere (
Determining the position of the Sun in relation to the investigated PV system is necessary to quantify the Egt. The position of the Sun can be easily estimated for a specific combination of date, time, latitude, longitude, and elevation. Numerous algorithms determine the Sun position with high accuracy (
Following this, Egt can be calculated with the following equation:where Edt is the calculated diffuse irradiance on the tilted surface and Er;gr is the incident irradiance from ground reflections. The fb and fd factors account for the shading phenomena of direct and diffuse irradiance, respectively. To calculate Egr, the View Factor (VF) from a specific ground area to the sky, the Edh for that ground area, the ground albedo (ρ), and the VF from the tilted surface to the ground area must be known.
The ground area is assumed as horizontal in Eq. 3.
3.2 Decomposition modeling
To estimate the solar irradiance collected by an oriented surface, Edh and Ebn in the chosen location, the surface geometry configuration, and the characteristics of the surroundings (i.e., buildings, vegetation) in terms of horizon profile and albedo must be known. Quantifying Edh and Ebn represents an issue due to the lack of measured data. Although it is feasible from a technological point of view, only Egh is usually monitored for economic reasons (
Decomposition models enable Edh and Ebn to be estimated by knowing Egh. The first decomposition models to be developed exploited experimental data to identify empirical correlations between kd and kt. The reliability of these models was limited to climate conditions similar to the one used in the model parametrization. Therefore, more complex models have been developed which correlate kd to more than one predictor. In general, such models calculate the kd index through the Eq. 4 that was originally proposed by
FIGURE 6

Measured and modelled kd vs. kt at Trondheim (Norway). Measurements are retrieved from the NTNU-SINTEF SolarNet in Trondheim (
Several databases provide solar radiation datasets based on satellite monitoring or reanalysis models from Numerical Weather Prediction (NWP). Alongside these, Typical Meteorological Year (TMY) datasets are commonly used to evaluate building energy performance. Nonetheless, the use of solar irradiation data from statistic-based weather data files may result in the incorrect computing of diffuse fractions as well as in systematic error within the evaluation of the potential benefits. Databases from satellite observation are characterized by a specific spatial resolution and are not available for each time-period and for each latitude. Moreover, they present limitations regarding the assessed solar radiation components and land cover. The major issue related to the use of satellite images is distinguishing between snow and cloud coverage because they usually have the same pixel values and spatial distribution patterns. Conversely, reanalysis databases are created by running modern NWP models on previous data before correcting the outcomes with ground-measured meteorological data. The main advantage is that the datasets usually cover the whole Earth, although with a low accuracy and spatial resolution compared to satellite observations. Since large parts of Norway, Sweden, and Finland lack coverage of satellite-derived datasets, reanalysis databases have potential if they are more accurate than using empirical decomposition models with ground-measured Egh. In this regard, the Copernicus Arctic Regional Reanalysis (CARRA) system, which is the first regional atmospheric reanalysis targeted for European parts of the Arctic areas, have been implemented in 2022 to specifically investigate the climate at high-latitude locations. Databases providing Egh and another radiative component for the Nordic zone are listed in Table 2.
TABLE 2
| Database | Source | Type | Spatial resolution | Availability | Estimated components | Latitude range |
|---|---|---|---|---|---|---|
| CAMS-RAD | SoDa | Satellite | ≈ 4 km | 2004-present | Egh, Ebn, Edh | From −66 to 66 |
| CERES | NASA | Satellite | 1° by 1° | 2000-present | Egh, Ebn, Edh | All |
| ERA5-Land | ECMWF | Reanalysis | 0.1° by 0.1° | 1979-present | Egh, Ebn | All |
| CARRA-East domain | ECMWF | Reanalysis | ≈ 2.5 km | 1990-2022 | Egh, Ebn | From 62 to 70 |
| PVGIS-ERA5 | PVGIS | Reanalysis | 0.25° by 0.25° | 2005-2016 | Egh, Edh, Egt, TMY | From −31 to 73 |
| PVGIS-SARAH | PVGIS | Satellite | ≈ 5 km | 2005-2016 | Egh, Edh, Egt, TMY | From −35 to 63 |
| PVGIS-SARAH-2 | PVGIS | Satellite | 0.05° by 0.05° | 2005-2020 | Egh, Edh, Egt, TMY | From −37 to 72 |
List of modelled databases which provide at least two irradiance components for a significant part of Norway, Sweden, and Finland. Metric conversion of 1° longitude is around 110 km, while 1° latitude can range between 63 km (at 55° latitude) and 36 km (at 71° latitude).
3.3 Transposition modeling
Once Edh and Ebn have been determined, Egt can be estimated by applying the transposition models in the next step of the model chain. Numerous transposition models have been implemented for quantifying Egt on south-oriented MPV (
Such tools usually assess the VF from the ground to the sky and from the tilted surface to the ground. The view factor describes the ratio of radiant energy emitted by a surface which is incident on another surface. This is calculated with Eq. 6:When it comes to PV systems, the VF can be estimated by considering only two dimensions.
Raytracing assessment can be applied as an alternative to the VF evaluation to estimate shading. Raytracing is a method to mathematically determine the ray’s path within a tridimensional environment (
4 Results
4.1 Decomposition models in the Nordic climate zone
4.1.1 Bibliometric analysis
Figure 7 shows the number of articles published per year along with the time resolution adopted for the model outputs. More than half of the studies were published in the last two decades, even though the first study about decomposition modeling was published in 1961. A turning point in this research topic occurred in the year 2015. In fact, decomposition models characterized by sub-hour time resolution, which first appeared in 1988, became increasingly frequent between 2013 and 2015, when they finally outnumbered one-hour models.
FIGURE 7

Number and distribution of time resolution of publications by year. The black and red dashed lines indicate, respectively, the yearly percentage of the study adopting a sub-hour and an hour time resolution.
After 2015, all the decomposition models included in this review had sub-hour resolution. This represents a significant improvement because it allows some instantaneous events to be investigated such as the CE and albedo enhancement (AE) effects, which cannot be detected when aggregating data hourly.
The analysis of weather stations whose data were used for the model validations in the reviewed studies highlighted the scarcity of decomposition models that are specifically developed for high latitudes. In fact, around three quarters of these models were implemented for dry climates (B) and temperate climates (C), while the rest were divided into tropical climates (A), continental climates (D), and polar climates (E). Figure 8 highlights that the most investigated climate zones were the humid sub-tropical climates (Cfa), the oceanic climate (Cfb), and the Mediterranean hot summer climates (Csa). Moreover, the tropical savanna climates with dry-winter characteristics (Aw), the cold semi-arid climates (Bsk), the warm summer continental climates (Dfb), and the tundra climate (ET) were the most common from the other main climate zones. Data from the sub-artic climates (Dfc), which is most common in the territories of Norway, Sweden, and Finland, were used in the validation of only five decomposition models.
FIGURE 8

Number of publications by Köppen-Geiger main climate zones (A) and sub-climate zones (B). The red crosses represent the percentage of studies for each bin with respect to the totality.
The geographical distribution of the studies is reported in Figure 9. Among the investigated countries, up to six decomposition models were proposed for Norway, while none was found for Sweden or Finland.
FIGURE 9

Number of studies by countries.
Decomposition model inputs were chosen from a wide group of predictors. The number of predictors varied and ranged from one to seven in the reviewed studies. A unique predictor was used by 71 decomposition models (kt in 70), while in 27 studies another predictor such as θz or V was added to kt. The number of publications per quantity of predictors is reported in Table 3 along with the number of publications for each predictor.
TABLE 3
| Number of predictors used | 1 | 2 | 3 | 4 | 5 | 6 | 7 |
|---|---|---|---|---|---|---|---|
| Number of publications | 71 | 27 | 9 | 5 | 15 | 5 | 1 |
Number of publications by number of predictors used as decomposition model input.
In total, around 20 different predictors were considered in the reviewed decomposition models. The analysis highlighted that the θz, the V, and the time of the day (t) are the three most used parameters after the clearness index (Figure 10).
FIGURE 10

Number of publications by used predictor.
A frequency analysis of the keywords associated with the reviewed scientific journal articles was carried out (Figure 11). On the one hand, the “diffuse solar radiation” and “clearness index” keywords were the most used and were found in 59 and 30 articles, respectively. On the other hand, the “clouds” and “statistical models” keywords were less frequent with only seven and six articles, respectively. The “other” category includes up to 26 different keywords that occurred less than five times.
FIGURE 11

Number of publications by authors’ keywords.
4.1.2 Meta-analysis
This section presents the decomposition models existing in the literature that were parameterized by considering solar radiation datasets from at least one of the climate zones characteristic of Norway, Sweden, and Finland (see Figure 5) (Tables 4, 5). Decomposition models which are characterized by an hourly time resolution are shown in the first part, while those having a one-minute time resolution are described in the second part.
TABLE 4
| Model | Reference | Year | Climate zones | NSFa | ||||
|---|---|---|---|---|---|---|---|---|
| A | B | C | D | E | ||||
| Tapakis1,2,3 | 2015 | - | 1 | - | - | - | - | |
| PerezBurgos | 2014 | - | 1 | 2 | - | - | 1 | |
| Kuo1,2,3,4 | 2014 | 1 | - | - | - | - | - | |
| Magarreiro | 2014 | - | - | 1 | - | - | - | |
| Lee | 2013 | - | - | 1 | - | - | - | |
| Yao1,2,3,4,5 | 2013 | - | - | 1 | - | - | - | |
| Boland5 | 2013 | 1 | - | 2 | - | - | - | |
| Lauret | 2013 | 1 | - | 3 | - | - | - | |
| Chikh1,2 | 2012 | - | 1 | - | - | - | - | |
| Chikh3 | 2012 | - | - | 1 | - | - | - | |
| Janjai | 2010 | 2 | - | - | - | - | - | |
| Karatasou | 2010 | - | - | 1 | - | - | - | |
| RuizArias1 | 2010 | 1 | 2 | 4 | 2 | - | 3 | |
| Torres1,2,3,4 | 2010 | - | - | 1 | - | - | 1 | |
| Helbig | 2010 | - | - | - | - | 1 | 1 | |
| Posadillo4,5,6 | 2010 | - | - | 1 | - | - | - | |
| RuizArias2 | 2010 | 1 | 2 | 4 | 2 | - | 3 | |
| Ridley2 | 2010 | 1 | - | 3 | - | - | 1 | |
| Pagola1,2,3,4 | 2009 | - | 1 | 1 | - | - | - | |
| Posadillo1,2,3,7 | 2009 | - | - | 1 | - | - | - | |
| Boland3,4 | 2008 | 1 | - | 3 | - | - | 1 | |
| Furlan | 2008 | - | - | 1 | - | - | - | |
| Mondol2 | 2008 | - | - | 1 | - | - | - | |
| Elminir1,2,3 | 2007 | - | 1 | - | - | - | - | |
| Jacovides | 2006 | - | 1 | - | - | - | - | |
| Mondol1 | 2005 | - | - | 1 | - | - | - | |
| Soares | 2004 | - | - | 1 | - | - | - | |
| Ridley1 | 2004 | 1 | - | 3 | - | - | 1 | |
| Tsubo1,2,3 | 2003 | - | 3 | 4 | - | - | 1 | |
| Tamura | 2003 | - | - | 1 | - | - | - | |
| Oliveira | 2002 | - | - | 1 | - | - | - | |
| Ulgen | 2002 | - | - | 1 | - | - | - | |
| Perez2 | 2002 | - | 2 | 3 | 3 | - | 1 | |
| Boland1 | 2001 | - | - | 1 | - | - | 1 | |
| DeMiguel | 2001 | - | - | 2 | - | - | 1 | |
| Li | 2001 | - | - | 1 | - | - | - | |
| Lopez1,2,3 | 2000 | 1 | 1 | 1 | - | - | 1 | |
| Gonzalez1,2,3,4,5,6,7,8 | 1999 | - | - | 1 | - | - | - | |
| Remund | 1998 | - | - | 2 | 2 | - | 3 | |
| Skartveit2,3 | 1998 | - | - | 1 | - | - | - | |
| Hijazin | 1997 | - | 1 | - | - | - | - | |
| Maduekwe1,2,3 | 1997 | 1 | - | - | - | - | - | |
| Muneer3 | 1997 | - | - | - | - | - | - | |
| Lam1,2 | 1996 | - | - | 1 | - | - | - | |
| Rerhrhaye | 1995 | - | - | 1 | - | - | - | |
| Chandrasekaran | 1994 | - | - | 1 | - | - | - | |
| Chendo1,2,3 | 1994 | 1 | - | - | - | - | - | |
| Macagnan | 1994 | - | 1 | - | - | - | - | |
| Alriahi | 1992 | - | 1 | - | - | - | - | |
| Perez1 | 1992 | - | 2 | 3 | 2 | - | 2 | |
| Louche1,2 | 1991 | - | - | 1 | - | - | - | |
| Reindl1,2,3 | 1990 | 1 | - | 3 | 1 | - | 2 | |
| Perez3 | 1990 | - | 2 | 3 | 2 | - | 2 | |
| Maxwell | 1987 | - | 1 | 1 | 1 | - | - | |
| Skartveit1 | 1987 | - | - | 1 | - | - | 1 | |
| Jeter | 1986 | - | - | - | 1 | - | - | |
| Muneer2 | 1986 | - | - | - | 1 | - | 1 | |
| Bakhsh | 1985 | - | 1 | - | - | - | - | |
| Hollands1,2 | 1985 | - | - | - | 1 | - | 1 | |
| Hawlader | 1984 | 1 | - | - | - | - | - | |
| Muneer1 | 1984 | - | 1 | - | - | - | - | |
| Turner | 1984 | - | - | 1 | - | - | - | |
| Erbs | 1982 | - | 1 | 3 | 1 | - | 1 | |
| Spencer | 1982 | - | 2 | 3 | - | - | 1 | |
| Bruno | 1978 | - | - | 1 | - | - | 1 | |
| Orgill | 1977 | - | - | - | 1 | - | 1 | |
| Bugler | 1977 | - | - | 1 | - | - | 1 | |
| Hay | 1976 | - | - | - | 1 | - | 1 | |
| Liu | 1961 | 1 | 2 | 4 | 3 | - | 3 | |
Distribution of the climate zones used in the parametrization of the reviewed one-hour decomposition models. Multiple models presented in the same publication are clustered in the same row.
NSF stands for “sub-climate zones from Norway, Sweden, and Finland territories”.
TABLE 5
| Model | Reference | Year | Climate zones | NSFa | ||||
|---|---|---|---|---|---|---|---|---|
| A | B | C | D | E | ||||
| Yang3,4 | 2021 | - | 2 | 4 | 2 | - | 2 | |
| Starke21 | 2021 | 2 | 4 | 3 | 1 | 2 | 3 | |
| Every1,2 | 2020 | 2 | 3 | 4 | - | - | 1 | |
| Yang1,2 | 2019 | - | 2 | 4 | 2 | - | 2 | |
| Paulescu | 2019 | 3 | 3 | 3 | 3 | - | 2 | |
| Abreu | 2019 | 2 | 4 | 3 | 1 | 2 | 3 | |
| Engerer4 | 2019 | - | 1 | 4 | - | - | 1 | |
| BRL1M | 2018 | 1 | 2 | 2 | - | - | - | |
| Hofmann | 2017 | 2 | 2 | 3 | 2 | - | 2 | |
| Engerer1,2,3 | 2015 | - | 1 | 4 | - | - | 1 | |
| Erusiafe | 2014 | 1 | - | - | - | - | - | |
| Oumbe | 2013 | - | 1 | 1 | - | - | - | |
| Boland2 | 2001 | - | - | 1 | - | - | 1 | |
| Suehrke | 1988 | - | - | 1 | - | - | - | |
Distribution of the climate zones used in the parametrization of the reviewed one-minute decomposition models. Multiple models presented in the same publication are clustered in the same row.
NSF stands for “sub-climate zones from Norway, Sweden, and Finland territories”.
Their performances were evaluated based on the extensive validation work carried out by
One-hour models which might be suitable for high-latitude locations were mostly climate-specific models. In fact, only one fourth of them were found to consider more than one location during the parametrization process. In this regard, the Skartveit model family was established in (
The Reindl model family was also parametrized with a solar radiation dataset from Norway, although it was used alongside datasets from the United States, Germany, Denmark, and Spain (
In addition, other decomposition models such as the ones from Hollands, Perez, Boland, and Ridley model families are evaluated in this section since they were developed for high-latitude climate zones. It is worth highlighting that the Yao model family (
The analysis of the nRMSD index is reported in Table 6 and visualized in Figure 12. The Skartveit1 model was identified as the most effective model at high latitudes, although it was outperformed by Spencer in the E zone. In addition to this, Mondol1, which was parametrized with solar radiation data from Northern Ireland, exhibited high performance levels being the second in the global ranking and the third in the D zone ranking.
TABLE 6
| C zone | D zone | E zone | Global | ||||
|---|---|---|---|---|---|---|---|
| Model | nRMSD [%] | Model | nRMSD [%] | Model | nRMSD [%] | Model | nRMSD [%] |
| Skartveit1 | 12.70 | Skartveit1 | 9.39 | Spencer | 12.70 | Skartveit1 | 11.32 |
| Perez2 | 13.16 | Perez3 | 9.62 | Muneer2 | 12.82 | Mondol1 | 11.76 |
| Skartveit3 | 13.26 | Mondol1 | 9.77 | Mondol2 | 12.87 | Muneer2 | 11.76 |
| Muneer2 | 13.35 | Perez1 | 9.88 | Mondol1 | 13.03 | Perez3 | 11.80 |
| Perez3 | 13.36 | Reindl2 | 9.90 | Skartveit1 | 13.05 | Reindl2 | 12.00 |
| Mondol1 | 13.44 | Muneer2 | 9.95 | Reindl3 | 13.23 | Skartveit3 | 12.01 |
| Reindl2 | 13.44 | Skartveit3 | 10.12 | Perez3 | 13.76 | Mondol2 | 12.12 |
| Mondol2 | 13.73 | Perez2 | 10.13 | Orgill | 13.79 | Perez1 | 12.35 |
| Perez1 | 13.91 | Orgill | 10.20 | Erbs | 13.85 | Orgill | 12.40 |
| Reindl3 | 14.15 | DeMiguel | 10.21 | DeMiguel | 13.85 | DeMiguel | 12.43 |
Error statistics about Ebn calculated for the high-latitude locations from Supplementary Material by
FIGURE 12

Error statistics about Ebn calculated for the high-latitude locations from Supplementary Material by
Regarding the analysis of one-minute models, those reviewed in the extensive validation study carried out by
Alongside this, the one-minute model from Paulescu and Blaga (
In
In 2019,
In 2021,
In Figure 13, the comparative analysis on models’ performance levels in the high-latitude locations confirmed that Yang4 is the best one-minute model. Alongside this, the Starke family model can represent an effective solution particularly when applied to C and D zones (Table 7).
FIGURE 13

Error statistics about Ebn calculated for the high-latitude locations from Supplementary Material by
TABLE 7
| C zone | D zone | E zone | Global | ||||
|---|---|---|---|---|---|---|---|
| Model | nRMSD [%] | Model | nRMSD [%] | Model | nRMSD [%] | Model | nRMSD [%] |
| Yang4 | 19.44 | Yang4 | 23.41 | Yang4 | 28.33 | Yang4 | 22.02 |
| Starke21 | 20.19 | Starke18A | 24.05 | Engerer2 | 29.68 | Starke18A | 23.05 |
| Starke18A | 20.44 | Starke21 | 24.18 | Starke18A | 30.07 | Engerer2 | 24.33 |
| Engerer2 | 21.94 | Engerer2 | 25.96 | Paulescu | 31.68 | Starke21 | 24.75 |
| Starke18B | 22.55 | Paulescu | 26.69 | Engerer4 | 32.07 | Paulescu | 25.71 |
| Paulescu | 23.43 | Starke18B | 26.89 | Starke18B | 34.92 | Starke18B | 25.83 |
| Engerer4 | 25.21 | Engerer4 | 28.93 | Abreu | 37.79 | Engerer4 | 27.37 |
| Abreu | 27.02 | Abreu | 31.01 | Every2 | 39.45 | Abreu | 29.93 |
| Every1 | 31.15 | Every2 | 33.57 | Starke21 | 40.42 | Every2 | 33.45 |
| Every2 | 31.56 | Every1 | 36.65 | Every1 | 42.05 | Every1 | 34.48 |
Error statistics about Ebn calculated for the high-latitude locations from Supplementary Material by
4.2 Transposition models
4.2.1 Bibliometric analysis
Figure 14 shows a timeline in which the reviewed studies about transposition modeling are distributed and clustered according to the model typology. Four model typologies were found in the literature: isotropic models, anisotropic models, artificial neural network (ANN) models, and probabilistic models. Isotropic models were the first model typology to be implemented in 1961; then, anisotropic models were developed (1977). ANN (e.g., multi-inputs convolutional neural networks, generalized regression neural networks, gradient-boosting frameworks for machine learning) and probabilistic models have been introduced recently in this research field (from 2013), but they are considered so promising that around 70% of the transposition models published since 2013 belong to these two groups. Conversely, the isotropic models have been investigated increasingly less over the last two decades. Nonetheless, ANN and probabilistic models have been presented in around 20% of the reviewed studies, while the isotropic and anisotropic models have occurred in 63% and 16% of the studies, respectively (Figure 15).
FIGURE 14

Number of publications and distribution of model typologies by year.
FIGURE 15

From the left: percentage distribution of model typologies, percentage distribution of sky conditions in the model validation, percent distribution of time resolution values. Percentage is calculated over all the reviewed transposition models.
When it comes to the simulated sky conditions, half of the reviewed transposition models were found to be validated in both clear and overcast sky conditions (Figure 15). Conversely, 18% of the models performed exclusively for overcast skies, while 16% of the models can operate only in case of a clear sky. Furthermore, most of the transposition models were found to provide hourly outputs (87%), and only three models could work with a sub-hour time resolution (8%). Contrary to decomposition modeling, there is a lack of trend in transposition modeling towards the reduction of the time resolution. Such a discrepancy might represent an issue and reduce the impacts of the decomposition model’s enhancement on the overall model chain. However, the hourly transposition models reviewed in (
TABLE 8
| Model | Reference | Year | Model typology | Diffuse radiation source(s) | Time resolution | |||||||
|---|---|---|---|---|---|---|---|---|---|---|---|---|
| Isotropic | Anisotropic | ANN | Probabilistic | Isotropic | Circumsolar | Horizontal bright | Ground reflection | Egt | ||||
| Liu1:22 | 2022 | ● | ● | ● | ● | 30 m | ||||||
| Pierce | 2021 | ● | ● | n.d. | ||||||||
| Quan1 | 2020 | ● | ● | h | ||||||||
| Quan2 | 2020 | ● | ● | h | ||||||||
| Li | 2020 | ● | ● | h | ||||||||
| Manni | 2020 | ● | ● | h | ||||||||
| Vàzquez | 2020 | ● | ● | M | ||||||||
| Pierro | 2016 | ● | ● | h | ||||||||
| Westbrook | 2015 | ● | ● | ● | ● | ● | h | |||||
| Yang | 2014 | ● | ● | ● | ● | h | ||||||
| Celik | 2013 | ● | ● | h | ||||||||
| Olmo2 | 2009 | ● | ● | h | ||||||||
| Bugler2 | 2007 | ● | ● | ● | h | |||||||
| Igawa | 2004 | ● | ● | ● | ● | h | ||||||
| Badescu | 2002 | ● | ● | ● | h | |||||||
| Tian | 2001 | ● | ● | h | ||||||||
| Olmo1 | 1999 | ● | ● | h | ||||||||
| Hay2 | 1993 | ● | ● | ● | h | |||||||
| Brunger | 1993 | ● | ● | ● | ● | m | ||||||
| Perez4 | 1990 | ● | ● | ● | ● | 15m | ||||||
| Muneer1 | 1990 | ● | ● | ● | ● | h | ||||||
| Muneer2 | 1990 | ● | ● | ● | ● | h | ||||||
| Reindl | 1990 | ● | ● | ● | ● | h | ||||||
| Perez3 | 1988 | ● | ● | ● | ● | h | ||||||
| Perez2 | 1987 | ● | ● | ● | ● | h | ||||||
| Gueymard | 1987 | ● | ● | ● | ● | h | ||||||
| Koronakis | 1986 | ● | ● | h | ||||||||
| Perez1 | 1986 | ● | ● | ● | ● | h | ||||||
| Skartveit | 1986 | ● | ● | ● | ● | ● | h | |||||
| Willmott | 1982 | ● | ● | ● | ● | h | ||||||
| Steven3 | 1980 | ● | ● | ● | h | |||||||
| Hooper | 1980 | ● | ● | ● | ● | h | ||||||
| Klucher | 1979 | ● | ● | ● | ● | h | ||||||
| Steven1 | 1979 | ● | ● | ● | h | |||||||
| Steven2 | 1979 | ● | ● | ● | h | |||||||
| Temps | 1977 | ● | ● | ● | ● | h | ||||||
| Bugler1 | 1977 | ● | ● | ● | h | |||||||
| Liu | 1961 | ● | ● | h | ||||||||
Tabular review of the reviewed transposition models according to the typology, the evaluated diffuse radiation sources, and the time resolution. For the time resolution: M stands for “month”, h stands for “hour”, and m stands for “minute”.
4.2.2 Research evaluation
The review study about transposition models from
An innovative sky-radiance model was conceptualized in
Up to 26 parametric models (isotropic and anisotropic) were designed through Artificial Neural Networks (ANNs) and machine learning techniques in (
5 Discussion
5.1 Inconsistencies in the decomposition modeling
The literature on decomposition modelling is evolving rapidly with new innovative models being presented and more validation studies carried out. The methodology and standards used are well documented in most cases, but not consistent among the studies. New methods are frequently being developed, and an overview of recent development as well as historical works are presented in many recent review studies (
Conversely, almost all of the reviewed studies assessed quantitative performance indicators such as nMBD and nRMSD. However, features of the used datasets such as time interval, quality control, and model implementation are not homogeneous throughout the studies, making it difficult to compare them. A nonparametric statistical procedure, based on the sum of ranks, is presented in
TABLE 9
List of weather stations, time period, model outputs, and statistical indicators used by
D datasets depend on which stations within the major climate zone D are used in a study.
Data availability varies between stations. E.g., PSU lacks 1-min data available before 2009.
Validation studies also differ in the models exploited to predict Ebn and the kd. Eq. 1 was applied by some authors to validate the models for calculating Ebn (
5.2 Inconsistencies of the transposition modeling
As observed for decomposition models, the existing literature about transposition models is characterized by some inconsistencies in the applied methodologies. In fact, there is a lack of shared protocols for the implementation of transposition models as well as in their validation. However, some methodologies such as the Taylor diagrams (
5.3 SWOT analysis
Even though the decomposition models require many inputs, the kt is commonly used since it can be measured. Alongside this, other parameters are used such as θz, V, and AM which are deterministic and can be easily calculated. In particular, the θz and the AM can be calculated from dataset timestamps, while the V is typically determined from a moving window of the kt values. As observed in Engerer2, decomposition models are usually comprised of a single function which makes them easy to implement in the Python environment. In this regard, the pvlib-python consists of a library of decomposition model implementations and supporting functions which can be used to calculate model parameters such as apparent solar time (AST), θz, and AM. This Python library is continuously developed and maintained and can be edited, so that new models can be implemented. Moreover, the kt can be used to combine different decomposition models by either choosing the output of a single model depending on the kt, or by summing the weighted outputs of multiple models, where the weight of each model depends again on the kt. Different approaches exist, and combining models is still a developing topic. Exploiting a combination of decomposition models which are defined through ANNs and machine learning-based models depending on the kt and time of year is also a solution. Model parameters can be re-fitted for local datasets to produce location tailored models. Major issues currently concern data availability and data quality-control routines. These have yet to be sufficiently discussed in the literature although this would improve the comparability of outcomes from different validation studies. Recent models such as the one presented in
TABLE 10
| Strengths | Weaknesses |
|---|---|
| 1-2 measured inputs | Specific temporal resolution |
| Easy to implement | Deterministic predictions |
| Developing machine learning methods | Lack of transportability |
| Opportunities | Threats |
|---|---|
| Open-source libraries | Climate change |
| Combining models can improve accuracy | Limited data availability |
| New and improved models are frequent |
SWOT analysis of decomposition modeling.
Empirical transposition models are usually less user-friendly than decomposition models. The pvlib-python tool includes the most common transposition models by allowing model chains to be built in Python. It is worth highlighting that transposition models such as Perez4 struggle with the hours of the day characterized by low solar elevation angles, making uncertainties high when the power production of the E-W VBPV system peaks. This issue is not addressed in the literature, as almost all the validation studies exclude the hours of low solar elevation (Table 11).
TABLE 11
| Strengths | Weaknesses |
|---|---|
| Varying degrees of complexity | Large uncertainties at low solar elevations |
| Open-source software tools | Raytracing simulations are time consuming |
| Developing machine learning methods | Tools have limited empirical transposition |
| Opportunities | Threats |
|---|---|
| Satellite derived inputs are improving | Climate change to a lesser degree |
| Rapidly increasing computation power | Often relies on a modelled input |
SWOT analysis of transposition modeling.
As mentioned in the above paragraph for decomposition models, numerous approaches exist that enable combining different transposition models to increase the model accuracy. Furthermore, machine learning-based methods can contribute to ANN-created transposition models and have shown improvements over empirical transposition models due to lower computation times (faster routines and faster hardware).
5.4 Literature gaps
The main literature gaps that were found in this review study are highlighted in this section. Firstly, the difference in temporal resolution of data between decomposition and transposition models is addressed. The former can provide one-minute estimations and validations, while the latter usually deals with hourly predictions which is also the same time resolution used when assessing PV energy production. Indeed, PV simulations tools aim to estimate the economic prospects of different system configurations, and if the system is contracted with a set price per kWh electricity produced, the hourly or sub hourly mismatch between production and load profiles is not a factor in the calculations. For this study, however, the penetration potential of E-W VBPV systems is investigated at a sub-hour temporal resolution for more accurate results enabling user to account for CE and AE effects.
Secondly, the numerical models implemented for assessing BPV systems mainly focuses on south-oriented cells with a tilt angle that can range between 30° and 45°. In such optimally exposed configurations, the diffuse fraction of solar radiation and the solar radiation reflected by the ground play a secondary role. Conversely, these factors are relevant in E-W VBPV, particularly when simulating solar irradiation with low Sun elevation angles (i.e., significant contribution from horizontal brightening). Being the reviewed models mostly empirical, their performances can reasonably worsen when applied to conditions different from the one considered for the model parametrization. Therefore, the use of models particularly accurate in the estimation of the horizontal brightening as well as with the ground albedo as input parameter should be recommended for E-W VBPV systems. Among the reviewed models, the transposition model from
Thirdly, there is an evident gap with high-latitude conditions. Decomposition models are mostly parametrized with datasets from climate zones which are not representative of the territories of Norway, Sweden, and Finland. In particular, only one weather station was considered from the Dfc climate in
5.5 Limitations of the study
The evaluation of decomposition models based on outcomes from
The data provided as Supplementary Material from
Finally, ensemble model output statistics such as the one described in
6 Conclusion
This systematic review investigated the solar irradiance model chain for horizontal-to-tilted irradiance conversion at high-latitude locations. Although a considerable number of publications exist on this topic, it is a scarcity of examples in the literature about the use of decomposition models at these latitudes. Moving from
This work demonstrates that validation studies lack in terms of their inter-comparability and relevance to E-W VBPV in Norway, Sweden, and Finland. The major issues are the variety in the applied methodologies in recent decomposition model validation studies, the lack of validation studies for empirical transposition models for E-W VBPV, and the absence of one-minute transposition models. While the newest decomposition models (i.e., Yang4, Engerer4, Starke21) show promising results, more data and climate-specific validation of these models are required. The development of a common and shared validation protocol should be prioritized to ease the inter-comparison of the numerous decomposition models. Such a gap has been partially covered by the recent work from
The main findings from the present review can be summarized as follows:
• Skartveit1 and Mondol1 are the most effective one-hour model at high latitudes, although they are outperformed by Spencer in the E zone;
• Yang4 is the best one-minute model followed by the Starke family model which represents an effective solution particularly when applied to C and D zones;
• Perez4 and Muneer transposition models perform best for East- and West-facing vertical surfaces;
• Hour time resolution is mostly adopted in transposition models, while decomposition models can already perform one-minute analyses;
• A validated model chain for Egt estimation on E-W VBPV in Norway, Sweden, and Finland was not found in the literature.
Therefore, the model chain resulting from the matching of Yang4 and Perez4 models could be recommended for performing one-minute analysis of E-W VBPV at high-latitude locations. Nonetheless, further insight into the best model choice for optical modelling is necessary. This includes:
• Validating the best performing decomposition models (see Table 5) with data from Norway, Sweden, and Finland by assessing decomposition model performance both on a seasonal level, and as a function of kt;
• Evaluating how well the model validation with other D-type climate zone data works for Dfc-zone;
• Validating transposition models with irradiance measurements from an E-W VBPV system;
• Assessing the potential of novel methods within the field such as ANN and probabilistic models.
Statements
Author contributions
MM, MDS, and GL contributed to conception and design of the study. MM and JT organized the database. MM and JT performed the statistical analysis. MM and JT wrote the first draft of the manuscript. SJ and KM wrote sections of the manuscript. All authors contributed to the article and approved the submitted version.
Acknowledgments
The authors acknowledge the financial support from the Norwegian Research Council (research project FRIPRO-FRINATEK No. 324243 HELIOS), the Finnish Cultural Foundation, and Emil Aaltonen Foundation.
Conflict of interest
The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.
Publisher’s note
All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors and the reviewers. Any product that may be evaluated in this article, or claim that may be made by its manufacturer, is not guaranteed or endorsed by the publisher.
Nomenclature
| Variables | |||
| E | Irradiance [W/m2] | ||
| MBD | Mean Bias Deviation | ||
| RMSD | Root Mean Square Deviation | ||
| R2 | Coefficient of determination | ||
| nMBD | Normalized Mean Bias Deviation [0-1] | ||
| nRMSD | Normalized Root Mean Square Deviation [0-1] | ||
| kt | Clearness Index [dimensionless] | ||
| kd | Diffuse Fraction [dimensionless] | ||
| ρ | Surface albedo [0-1] | ||
| V | Variability index [dimensionless] | ||
| t | Time of the day [0-24] | ||
| ktcs | Clear sky clearness index [dimensionless] | ||
| Greek letters | |||
| θ | Zenith angle [degree] | ||
| α | Azimuth angle [degree] | ||
| β | Surface tilt angle [degree] | ||
| Φ | Angle of incidence [degree] | ||
| Subscripts | |||
| g | Global | ||
| t | Tilted | ||
| b | Direct | ||
| n | Normal | ||
| d | Diffuse | ||
| h | Horizontal | ||
| 0 | Out of the atmosphere | ||
| z | Solar | ||
| iso | Isotropic | ||
| circ | Circumsolar | ||
| hor | Horizontal bright | ||
| r | Reflected | ||
| gr | Ground | ||
| s | Satellite-derived | ||
| cs | Clear sky | ||
| hour | Hourly | ||
| Acronyms | |||
| MPV | Monofacial Photovoltaic | ||
| BPV | Bifacial Photovoltaic | ||
| E-W | East-West | ||
| VBPV | Vertical Bifacial Photovoltaic | ||
| PV | Photovoltaic | ||
| SWOT | Strengths, weaknesses, opportunities, and threats | ||
| WoS | Web of Science | ||
| AM | Air Mass | ||
| CE | Cloud Enhancement | ||
| NREL | National Renewable Energy Laboratory | ||
| VF | View Factor | ||
| NWP | Numerical Weather Prediction | ||
| TMY | Typical Meteorological Year | ||
| AE | Albedo Enhancement | ||
| ANN | Artificial Neural Network | ||
| SVF | Sky View Factor | ||
| BSRN | Baseline Solar Radiation Network | ||
| AST | Apparent solar time [0–24] | ||
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Summary
Keywords
decomposition modelling, transposition modelling, solar energy, high latitudes, solar modelling
Citation
Manni M, Thorning JK, Jouttijärvi S, Miettunen K, Di Sabatino M and Lobaccaro G (2023) Horizontal-to-tilt irradiance conversion for high-latitude regions: a review and meta-analysis. Front. Built Environ. 9:1245223. doi: 10.3389/fbuil.2023.1245223
Received
23 June 2023
Accepted
12 September 2023
Published
28 September 2023
Volume
9 - 2023
Edited by
Cristina Piselli, University of Florence, Italy
Reviewed by
Marina Bonomolo, University of Palermo, Italy
Massimiliano Manfren, University of Southampton, United Kingdom
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Copyright
© 2023 Manni, Thorning, Jouttijärvi, Miettunen, Di Sabatino and Lobaccaro.
This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.
*Correspondence: Mattia Manni, mattia.manni@ntnu.no
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