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    Renewable Energy 33 (2008) 14061412

    Technical Note

    Evaluation of 12 models to estimate hourly diffuse irradiation on

    inclined surfaces

    Ali Mohammad Nooriana, Isaac Moradib,, Gholam Ali Kamalia

    aAtmospheric Science and Meteorological Research Center (ASMERC), IRIMO, Tehran, IranbDepartment of Physical Geography, Faculty of Geography, University of Tehran, Tehran, Iran

    Received 26 October 2006; accepted 30 June 2007

    Available online 7 September 2007

    Abstract

    This study evaluates the performance of 12 models to estimate hourly diffuse solar irradiation on inclined surfaces from those

    measured on horizontal surfaces. Total solar irradiation incident on a tilted surface consists of three components including: beam, diffuse

    and reflected from the ground. On a semi-hourly basis, the beam component can be calculated by the ratio of the incidence angle to the

    solar zenith angle. The reflected component has a small effect on calculations and may be calculated with an isotropic model. In contrast,

    models for estimating the diffuse component show major differences, which justify the validation study that this paper discusses. Twelve

    models were tested against recorded south- and west-facing slope irradiances at Karaj (351550N; 501560E), Iran. The following models

    were included: Badescu [Ba], Tian et al. [Ti], Perez et al. [P9], Reindl et al. [Re], Koronakis [Kr], Perez et al. [P8], Skartveit and Olseth

    [SO], Steven and Unsworth [SU], Hay [Ha], Klucher [Kl], Temps and Coulson [TC], and Liu and Jordan [LJ].

    The relative root mean square error (RMSE), for the south-facing surface ranges from 10.16% to 54.89% for the SO and TC models,

    respectively. For the west-facing surface, RMSE ranges from 30.71% for the P9 model to 63.53% for the TC model. Statistical indices

    show that all models produce large errors for the west-facing surface. Statistical indices for the south-facing surface show reasonably

    good agreement with measured data.

    r 2007 Elsevier Ltd. All rights reserved.

    Keywords: Diffuse irradiation; Isotropic models; Anisotropic models; Radiation modeling; Iran

    1. Introduction

    Solar energy is a sustainable, safe and abundant energy

    resource. Estimating solar irradiation incident on inclined

    surfaces of various orientations is necessary in order to

    calculate the building heat gain from the building envelope

    as well as the electric power generated by photovoltaics

    (PV) [1], design solar systems and to evaluate their long-term average performance. Despite the fact that many

    meteorological/radiometric stations measure global and

    diffuse irradiation received on horizontal surfaces the data

    on inclined surfaces are not available and are also

    estimated with different models from those measured on

    horizontal surfaces[2].

    Total radiation incident on a tilted plane consists of

    three components: beam radiation, diffuse radiation and

    reflected radiation from the ground. On an hourly basis the

    direct and reflected components can be computed with

    good accuracy by using simple algorithms but the nature of

    the diffuse component is more complicated and the desired

    algorithms need assessment and evaluation.

    Perez et al. [3,4] developed two new and more accuratebut considerably simpler versions of the original Perez

    diffuse irradiance model[5]. The original version has been

    used world wide to estimate short time step (hourly or less)

    irradiance on tilted surfaces based on global and direct (or

    diffuse) irradiance measured on horizontal surfaces. Li and

    Lam [6] evaluated the anisotropic models of Klucher [7],

    Hay [8] and Perez et al. [3] applied to two-years of

    measured data in Hong Kong (19961997). All three

    models produced large errors for north-facing surfaces.

    Predictions for south-facing surfaces showed reasonably

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    www.elsevier.com/locate/renene

    0960-1481/$- see front matter r 2007 Elsevier Ltd. All rights reserved.

    doi:10.1016/j.renene.2007.06.027

    Corresponding author. Tel.: +98 21 44580661; fax: +98 21 44580670.

    E-mail addresses: [email protected] (A.M. Noorian),isaac_moradi@

    yahoo.com (I. Moradi), [email protected] (G.A. Kamali).

    http://www.elsevier.com/locate/renenehttp://localhost/var/www/apps/conversion/tmp/scratch_3/dx.doi.org/10.1016/j.renene.2007.06.027mailto:[email protected]:[email protected]:[email protected]:[email protected]:[email protected]:[email protected]:[email protected]:[email protected]://localhost/var/www/apps/conversion/tmp/scratch_3/dx.doi.org/10.1016/j.renene.2007.06.027http://www.elsevier.com/locate/renene
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    good agreement with measured data. Kamali et al. [9]

    evaluated eight diffuse models to estimate solar irradiation

    on tilted surfaces using daily measured solar irradiation

    data in Iran and recommended the Reindl et al.[10]model

    for estimating solar irradiation on tilted surfaces. Notton

    et al. [11] evaluated the combination of some well-known

    models to estimate the hourly global solar irradiation on a

    tilted surface from those on a horizontal surface. They

    recommend the Klucher [7] model separately or in

    combination with other models to estimate diffuse solar

    irradiation on surfaces tilted towards the equator.The objective of this study is to compare the results of 12

    widely used models, for estimating total solar radiation on

    tilted surfaces, with measurements at Karaj, Iran for west-

    and south-facing surfaces inclined at 40 and 45,

    respectively. The models used the same method for

    calculating beam and ground reflected radiation on the

    tilted surface. The only difference was in the treatment of

    diffuse radiation.

    2. Data

    The measuring station was located on the roof-top of the

    Faculty of Agriculture, University of Tehran, Karaj

    35550N; 50560E), Iran. The measurements have been

    carried out using two CM5 pyranometers with solarimeter

    integrator CC2 manufactured by Kipp and Zonen, Hol-

    land. The solar radiation data measured by the authors,

    during the period from June to October 2002 were used in

    this study. This consisted of semi-hourly global solar

    radiation on a horizontal and two tilted surfaces (45

    south-facing and 40 west-facing). Also for testing the

    diffuse model, semi-hourly global and diffuse radiation on

    a horizontal surface was measured by the previously

    mentioned radiometers from February to June 2006. This

    represents the only measured data available for tilted

    surfaces in Iran[12].

    3. Theory and models

    The hourly total irradiation incident on a tilted surface

    GTh is composed of direct BTd, ground reflected RTh

    and sky-diffuse DTh components:

    GTh BThDThRTh, (1)

    The amount of direct radiation on a surface tilted S

    degrees from the horizontal and rotated aT degrees from

    the northsouth axis can be calculated by multiplying the

    direct horizontal irradiation by the ratio of cosy= cosZ,where y is solar incidence angle on a tilted plane and Z is

    solar zenith angle. Also, the measuring station was located

    on a roof-top with very low reflectance, and the reflected

    component was very much lower than the direct and the

    diffuse components so an isotropic model can be used to

    compute the reflected component on the tilted surface. So,

    Eq. (1) can be written again as follows:

    GTh Bh: cosy= cosZ rdDh Gh:r:1cosS=2,

    (2)where Bh, Dh and Gh are hourly direct, diffuse and total

    solar radiation on a horizontal surface, either measured

    directly or estimated from each other,rd is the ratio of the

    hourly diffuse irradiation incident on a tilted surface to

    that on a horizontal surface, r is ground reflectivity, and Z

    and y are calculated by well-known formulae:

    cosZ sinf sind cosf cosd coso,

    cosy sinS sinZ cosaS aT cosS cosZ, (3)

    where f is the latitude of the location, d is the solar

    declination, ando is the solar hour angle[13]. Calculation

    of the diffuse ratio is more complicated and many

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    Nomenclature

    Bh hourly direct solar radiation on a horizontal

    surface MJ m2

    BTh hourly direct solar radiation on a tilted surface

    MJ m

    2

    Dh hourly diffuse solar radiation on a horizontal

    surface MJ m2

    DTh hourly diffuse solar radiation on a tilted surface

    MJ m2

    Gh hourly total solar radiation on a horizontal

    surface MJ m2

    Goh hourly extraterrestrial solar radiation on a

    horizontal surface MJ m2

    GTh hourly total solar radiation on a tilted surface

    MJ m2

    kT atmospheric transmissivity and equals the ratio

    ofGh=Goh (dimensionless)

    rb beam ratio factor, the ratio of cosy= cosZ(dimensionless)

    rd ratio of the hourly diffuse solar radiation

    incident on a tilted surface to that on a

    horizontal surface (dimensionless)

    RTh hourly reflected solar radiation on a tiltedsurface MJ m2

    S tilted plane slope angle (deg.)

    Z solar zenith angle (deg.)

    aS solar azimuth angle (deg.)

    aT tilted plane azimuth angle (deg.)

    d solar de clination (deg.)

    f latitude of the site and positive for the northern

    hemisphere (deg.)

    r ground reflectivity (dimensionless)

    y solar incidence angle on tilted surface (deg.)

    o solar hour angle and clockwise from south is

    positive (deg.)

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    the west-facing surface the absolute MBE ranges from

    2.43% (Kl model) to 38.52% (TC model). For all

    the models studied covering south-facing surfaces, except

    for SU (47.18%) and TC (54.89%), the RMSE values

    do not differ a great deal. The SO, Ha, Re and P9 models

    give the most accurate predictions for the south-facing

    surface, and P9 model performs better for the west-facing

    surface. The MBE shows that all models, with the

    exception of SU model, underestimate values for west-

    facing surfaces.

    Graphical residual analysis of each model (residuals are

    estimates of experimental error obtained by subtracting the

    observed irradiation from the estimated one) for the south-

    facing-surface is reported in Fig. 1 which shows that the

    values of residuals for the SO, Ha, Re, P9 and P8 models,

    exhibit generally small differences and are very close to

    zero. This suggests that these models estimate of irradia-

    tion compare well with measured data. Residual analysis

    for the west-facing surface (Fig. 2) shows that only the

    values of residuals for P9 model show relatively small

    values with a distribution near to normal distribution. The

    residual analysis for both surfaces confirms the result of the

    statistical indices, RMSE and MBE.

    For the west-facing surface, although the correlation

    coefficients between the measured and estimated irradia-

    tion are significant at 0.05 level (Table 3) the frequency of

    the residuals (Fig. 2) shows that the high correlation is due

    to the scattering of residuals around zero and high positiveand negative values of the residuals neutralize the effect of

    each other. Statistical indices show that all models produce

    large errors for the west-facing surface. The statistical and

    graphical results for the south-facing surface show reason-

    ably good agreement with measured data.

    5. Conclusions

    An evaluation of the predicted tilted solar irradiance

    based on 12 inclined surface models and measured

    horizontal solar data in Karaj, Iran has been carried out.

    It has been observed that relatively high MBE and RMSEvalues are found for the west-facing surfaces, which receive

    much less direct radiation than south-facing surfaces; and

    the tilted components predicted for south-facing surface

    are more accurate. The Skartveit and Olseth[20], Hay[8],

    Reindl et al.[10]and Perez et al. [3]models give the most

    accurate predictions for the south-facing surface and the

    Perez et al. [3] model performs best for the west-facing

    surface. The RMSE values for the south-facing surface

    range from 10.16% to 54.89% and for west-facing surface

    range from 30.71% to 63.53%. In general, the Perez et al.

    [3] model shows the best agreement with the measured

    tilted data.

    Acknowledgments

    The authors would like to give their sincere thanks to

    Dr. Helfried Scheifinger (Vienna) for his helpful advices

    and recommendations, Dr. Peter Mayes (NJDEP) for

    improving the English text, and anonymous referees for

    carefully reading the manuscript and giving a number of

    useful suggestions for improvement.

    Appendix A

    A.1. Computing the semi-hourly total extraterrestrial solar

    irradiation, Goh

    For a given time, Goh in unit of MJ m2 is given by[23]:

    Goh 37:595

    d2 cosf cosdsino2sino1

    p

    180o2o1 sinf sind

    n o,

    (A.1)

    wheredis the earthsun distance in astronomical units,f is

    latitude,d is solar declination, o1 is the hour angle for the

    beginning time, o2 is the hour angle for the ending time

    and all angles are given in degrees. The solar constant is

    taken as 1367 W m2 [24,25].

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    Table 2

    Comparison of regression (model abmeasured) and correlation

    (R) coefficients, root mean square (RMSE) and mean bias errors (MBE) of

    different hourly diffuse models for south-facing surface

    Model a b R RMSE MBE %RMSE %MBE

    LJ 0.07 0.93 0.99 0.07 0.03 13.4 6.16

    Kr 0.08 0.95 0.99 0.08 0.05 14.89 9.54

    Ba 0.06 0.88 0.99 0.08 0.01 13.95 1.00

    Ti 0.06 0.88 0.99 0.08 0.01 13.95 1.00

    Ha 0.06 0.94 1.00 0.06 0.02 10.37 4.47

    SO 0.06 0.94 1.00 0.06 0.02 10.16 4.27

    Re 0.06 0.95 1.00 0.06 0.03 10.87 6.07

    SU 0.09 1.23 0.99 0.26 0.22 47.18 40.62

    P8 0.02 0.94 0.99 0.07 0.01 12.44 2.07

    P9 0.04 0.94 0.99 0.06 0.01 11.17 1.44

    Kl 0.08 0.96 0.99 0.08 0.06 15.43 10.40

    TC 0.1 0.5 0.94 0.3 0.18 54.89 31.86

    RMSE and MBE are in units of MJ m2.

    Table 3

    Same asTable 2but for west-facing surface

    Model a b R RMSE MBE %RMSE %MBE

    LJ 0.12 0.72 0.89 0.24 0.04 42.49 7.70

    Kr 0.12 0.74 0.89 0.24 0.03 42.10 5.20

    Ba 0.1 0.69 0.89 0.25 0.08 44.17 13.45

    Ti 0.1 0.68 0.89 0.26 0.08 44.57 14.46

    Ha 0.08 0.76 0.92 0.21 0.06 37.18 10.04

    SO 0.08 0.76 0.92 0.21 0.06 37.25 10.23

    Re 0.09 0.76 0.92 0.21 0.05 36.85 8.95

    SU 0.13 1.03 0.95 0.24 0.15 40.90 26.26

    P8 0.02 0.76 0.95 0.24 0.16 41.80 28.23

    P9 0.05 0.81 0.95 0.18 0.07 30.71 11.50

    Kl 0.11 0.78 0.91 0.22 0.01 37.97 2.43

    TC 0.07 0.5 0.89 0.37 0.22 63.53 38.52

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    d180

    p 0:0069180:399912 cosG0:070257 sinG

    0:006758 cos 2G0:000907 sin 2G0:002697 cos 3G0:00148 sin 3G, A:2

    1

    d2 1:000110:034221 cosG0:00128 sinG

    0:000719 cosG0:00077 sin 2G, A:3

    G360

    365dn 1, (A.4)

    o 18012TST=12, (A.5)

    wherednis day of the year, e.g. 1 Jan 1, 20 Feb 51, etc.

    and TST is true solar time.

    A.2. Computing hourly diffuse and direct components from

    hourly global irradiance

    A simple, physically based method proposed by Miguel

    et al. [15] was used for estimating hourly diffuse and direct

    components from hourly global irradiance. For three different

    ranges of atmospheric transmissivity kT Gh=Goh, theresulting correlations are given by the following expression:

    Dh

    Gh

    0:9950:081kT if kTo0:21;

    0:7242:738kT8:32k2T4:967k

    3T if 0:21pkTp0:76;

    0:180 if kT40:76:

    8>:

    (A.6)

    ThenBh can be calculated as follows:

    Bh GhDh. (A.7)

    ARTICLE IN PRESS

    Fig. 1. Percent frequency of the deviations of the daily global radiation on south-facing tilted surface, calculated with different models to the experimental

    data.

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    A.3. Statistical methods of comparison

    The statistical error tests are as follows [26]:

    RMSE ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiSC

    i M

    i2

    ns

    , (A.8)

    MBE

    PCi Mi

    n , (A.9)

    where Ci and Mi are the ith calculated and measured

    values on a tilted surface, respectively, and n is the total

    number of observations for a specific period of time.

    Relative RMSE (%RMSE) and MBE (%MBE), which

    are a dimensionless measure of RMSE and MBE, can be

    defined as follows.

    %RMSERMSE

    M100, (A.10)

    %MBE MBE

    M100, (A.11)

    where M is the mean of measured values on the tilted

    surface.

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    ARTICLE IN PRESS

    Fig. 2. Same asFig. 1but for west-facing surface.

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