CMNSEM 1107 13 Estimating Global Diffuse Solar Radiation Sunshine Duration

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    Canadian Journal on Computing in Mathematics, Natural Sciences, Engineering and Medicine Vol. 2 No.9, December 2011

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    Estimating Global and Diffuse Solar Radiation from Sunshine Duration at Qena/

    Egypt

    S.M. El Shazly , A. A. Hassan, Kh. O. Kassem*, M. E. Adam and Z.M. Ahmed

    Physics Dept., Faculty of Science at Qena, South Valley University, Qena, Egypt

    Abstract

    The clearness index (Kt) and diffuse fraction (KD) at Qena / Upper Egypt have

    been expressed in terms of the sunshine fraction (n/N) with the aim of using them to

    estimate the values of global (G) and diffuse (D) solar radiation in the study region. A

    variety of regression forms, namely linear, exponential, power, second and third orderpolynomial has been applied in this process. The significance and performance of these

    regression forms have been evaluated with the aid of several procedures of statistical

    analysis. In view of this analysis it has been found that all of them can reasonably be used

    to represent the effect of (n/N) on both (Kt) and (KD). In this paper the simple linear

    forms are applied to estimate both (G) and (D), since the other forms of the regressions

    do not improve the accuracy of the estimation. Comparison between measured and

    estimated values of (G) and (D) are performed. The accuracy of estimation of these

    components is tested by calculating the mean bias error (MBE), absolute bias errors

    (MAE), root mean square errors (RMSE), model efficiency (ME), modeling index (d)

    and t-statistic test. The obtained values of these parameters indicate the performance and

    validity of the suggested empirical models in estimating (G) and (D). Few estimates is

    found to fall beyond 10% accuracy level.

    Key words: Global solar radiation - Diffuse solar radiation - Sunshine fraction Daily

    values Monthly averages statistical analysis

    ____________________________________________________________

    * Corresponding author:

    E-mail: [email protected]

    Introduction

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    The interest in the applications of solar energy has increased largely in the last

    years owing to the expected demands in energy resulting from the increase in the world

    population. This demand can not be met from traditional sources of energy, which will be

    depleted by the year 2050 (El sayigh, 1992). Renewable energy must and can meet this

    challenge. Solar energy is one of the most promising renewable sources. It is

    environmentally kindly, plentiful and easy to utilize. For optimal exploitation of the solar

    energy, a detailed and accurate knowledge of the solar radiation data at a location is

    necessary for engineering design of collectors and storage systems and evaluation of its

    efficiency. In the other hand, at any location on the earth's surface, the solar radiation is

    also a function of various atmospheric variables such as: the nature and extent of cloud

    cover, the aerosol and water vapor contents of the atmosphere --- etc. Therefore solar

    radiation data can also enable the scientist to study the atmospheric and environmental

    properties that attenuate them and affect its amount received at the ground. Review

    through a lot numbers of references (e.g. Benghanem and Joraid, 2007; Zekai, 2007;

    Almorox and Hontoria, 2004; Tarhan and Sari, 2005; Ahmed and Ulfat, 2004) has shown

    that the "best" measurements to be used in the above utilities of solar energy are those

    measured at the location of interest. However, these in-situ measurements, including

    global solar radiation and its direct and diffuse components, are not always available in

    all locations. Accordingly, development of calculation procedures has been prompted to

    provide estimates for places where measurements are not made and places where there

    are gaps in the measurement record. This paper aims mainly to calculate the global (G)

    and diffuse (D) solar radiation components at Qena, Upper Egypt, a city of abundant

    solar radiation, at which data are not always available. These calculations were made for

    the first time at Qena, since the solar radiation observations were not feasible at this city

    before the establishment of the meteorological station at the south valley university in 1 /

    4 / 2000 . The calculation process has carried out using different correlations between

    the sunshine fraction (n/N) with each of the clearness index kt (G/G 0) and the diffuse

    fraction kd (D/G), where G0 is the daily extraterrestrial solar radiation. Daily values as

    well as monthly averages of these components have been calculated. These types of

    results are needed to satisfy the requirements of the solar energy utilities in the study

    region either for engineers or for scientists. Some of these utilities, at least in this time,

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    are using this energy as a source of thermal energy, that can be used in homes and water

    heating projects as well studying the atmospheric contaminants in view of the attenuation

    caused by it in the incoming solar radiation before it reaches the earth's surface. These

    data may be used to some extend in the adjoining locations of similar atmospheric

    characteristics.

    2. Data and methodology

    Daily data of global (G) and diffuse (D) solar radiation components as well as the

    sunshine duration (n) were obtained from Egypt meteorological department in south

    valley university station at Qena /upper Egypt ( 26 17N, 32 43E, Height 78 asl) in the

    period from 2001 to 2004. Global solar radiation is measured by "first class' precise

    spectral pyranometer, Eppley No. 163171S (WMO 1996) with errors around 3-4%.

    Diffuse solar radiation is measured by shading the direct beam from similar pyranometer

    using anodized aluminum shadow band. The sunshine duration is measured using

    Campbellstokes sunshine recorder (burn method) with uncertainty 0.1 h and a

    resolution of 0.1 h. The extraterrestrial possible solar radiation G0 and the day length N

    are calculated using standard procedure (Duffi and Beckman, 1991, 1994; El-shazly,

    1994; and Aljamal, 1987).The following essentials regression forms are used in fitting the

    measured data:

    Y = a + bx (1)

    Y = a +bx + cx2 (2)

    Y = a +bx + cx2 + dx3 (3)

    Y = ax b (4)

    Y = a e bX (5),

    where a, b, c and d are regression coefficients. They were determined by regression

    analysis using the well known least mean square method and they depend on the location.

    In the above equations the terms Y represent Kt andkd; while the x terms are the sunshine

    fraction (n/N).The obtained correlations are then used to estimate the three solar radiation

    components G and D in the study region. Different performance measures are used to

    ensure the accuracy of estimation of these components such as the mean bias error

    (MBE), absolute bias errors (MAE), root mean square errors (RMSE), model efficiency

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    (ME), modeling index (d) and t-statistic test. The following formulae are used to

    calculate these errors

    = mc YYn

    MBE1

    (6)

    ( ) = mc YYn

    MAE1

    (7)

    ( )5.0

    21

    = mc YY

    nRMSE (8)

    ( )

    ( )

    =

    2

    2

    1

    mm

    cm

    YY

    YYME (9)

    ( )

    ( )

    +

    =

    2

    2

    1

    mcmm

    cm

    YYYY

    YYd (10)

    ( ) 5.022

    21

    =

    MBERMSE

    MBEnt (11)

    In all the above statistical tests of accuracy, except ME and d, the smaller value,

    the better is the model performance, while values of ME and d closer to 1 indicate the

    superior model performance (Willmott, 1982; Mayer and Butler, 1993; Stone, 1993;

    Torul et al, 2000; Torul, 1998). For any equation estimates to be significant, the t-

    values produced by eq. (11) must be smaller than the values for that confidence level in

    standard statistical tables.

    3. Results and discussion

    3.1 Correlation between clearness index (Kt) and sunshine fraction (n/N)

    Figs. 1 and 2 show the percentage of the frequency distribution of daily K t and(n/N) through the study period (2001-2004). It is clear that more than 98 % of Kt values

    are > 0.5 and more than 89 % of (n/N) lies in the range > 0.7. This reflects the abundance

    of solar energy and semi cloudless weather characterizing the study region through the

    year months and consequently the importance of using it in solar energy projects.

    Relation between the daily values of K t and (n/N) is presented in Fig. 3. This relation has

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    been described and analyzed quantitatively using the above given equations 1-5. The

    obtained values of the regression constants a, b, c and d as well as the results of the

    statistical analysis of these equations are summarized in Table 1. According to this table,

    the high values of the correlation coefficients and F- value (compared to its critical value

    given in this table) illustrate that all these formulae can compute the daily global solar

    radiation (Gd) with a good accuracy. Also the T-ratio for each coefficient has values

    greater than zero, reflecting the significance of their great contribution and high certainty

    to the fitting process.

    In view of the above statistical analysis, the following simple linear correlation:

    Kt = 0.33 + 038 (n/N) (12),

    is used in our calculation process to calculate the daily and monthly averages of global

    solar radiation at Qena in the study period (2001 -2004).

    3.1.1 Daily global solar radiation (Gd)

    3.1.1.1 Model performance

    Fig. 4 represents a regression form for the variation of both the daily measured (Gdm)

    and calculated (Gdc) values of global solar radiation in this period. All data are used in

    this figure. In spite of the apparent small deviations between the measured and calculated

    values of Gd

    in some months in spring and summer seasons, the suggested model (eq.12)

    can estimate Gd with a very good accuracy. The high effect of atmospheric constituents in

    these months such as aerosols, clouds etc. may be the reason for these deviations(El-

    Shazly, 1989). Fig.5a, b represents the percentages of the relative deviation and its

    frequency distribution of calculated global solar radiation (Gdc) from measured ones

    (Gdm) atQena through the study period. From this fig., about 68% and 94% of the relative

    deviation percentage of the results lie in the ranges < 5% and < 10%, respectively.

    To confirm the performance of eq. (12) in estimating the daily global solar

    radiation Gd, some statistical analysis has been done. The result is summarized in Table

    2. It is evident in this table that, the percentages of MBE, RMSE, and MAE are in the

    acceptable range with respect to the mean value of Gd, while the values of ME and d are

    closed to unity. Also t- value is less than its critical one (2.57). Accordingly, one can

    conclude that this equation can estimate the daily global solar radiation with a high

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    accuracy and indicates the model performance.

    3.1.1.2 Model validation

    To test the validity of the proposed equation, it was used to calculate Gd for new

    measurements of sunshine fraction at Qena during the period from May 2005 to April2006. Fig. 6 shows the relation between their calculated and measured values in this

    period. A very good correlation between both of them (r = 0.99) is clear in this figure.

    The statistical analysis of the results is shown in Fig.7a, b and Table 2. The figure and the

    table give an evidence for using the proposed equation in calculating Gd, where 73% of

    the results have relative deviation percentage < 5% and 96% of them lie in the range

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    3.2 Correlation between the diffuse fraction (KD) and sunshine fraction (n/N)

    In this section the same techniques as in sec 3.1 was applied to study the correlation

    between KD and n/N. Fig. 10 shows the percentage of the frequency distribution of KD

    through the study period. The figure indicates that 95.67% of the results have the values

    0.7.These results support the above

    mentioned conclusion in sec. 3.1 related to the semi cloudless weather in the study region

    (Adam and El-Shazly, 2007; EL- Nouby 2006, and EL-Shazly et al., 1997).

    Fig. 11 represents the relation between the daily values of the diffuse fraction

    (KD) and sunshine fraction (n/N) in the study area through the study period (2001-2004).

    This figure clearly indicates that the values of KD decrease with increasing (n/N). Least

    mean square method is used to analyze this relation in view of the above suggested

    formulae 1-5. The resultant values of the different regression and statistical parameters

    are summarized in Table (3). Similar to what done in section 3.1.1, all of these formulae

    may estimate the diffuse solar radiation with a high accuracy. In this work the following

    linear one is used to calculate the daily values and monthly averages of diffuse solar

    radiation at Qena.

    ( ) ( )13............................................079.1/945.0 += NnKD

    3.2.1 Daily diffuse solar radiation (Dd)

    3.2.1.1 Model performance

    The relation between the calculated (Ddc)and the measured (Ddm)values of daily

    diffuse solar radiation using this equation are represented in Fig. 12 for all daily data (D d)

    through the study period. This figure indicates the high correlation between the two

    parameters.

    To verify whether the obtained relationship (eq.13) allows a reliable estimate of

    daily diffuse solar radiation Dd, the percentage of the frequency distribution of the

    relative deviation (RD) of its calculated values (Ddc) from the measured ones (Ddm)

    through the study period is computed as shown in Fig. 13. According to this figure one

    can conclude that 40.29% of the results lie in the range < 10%; 74.11% lie in the range

    < 20% and 25.9% only have relative deviation > 20%. These results demonstrate an

    acceptable accuracy of the calculation.

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    Statistical analysis of the calculated daily diffuse solar radiation (Ddc) during the whole

    period (2001-2004) is summarized in Table 4. According to the values of the different

    parameters given in this table one can conclude that this equation can estimate the daily

    diffuse solar radiation with a good accuracy.

    3.2.1.2 Model validation

    Measured data of available sunshine fraction during new periods at Qena (Jan.

    2006 Apr. 2006; May 2000Aug. 2000 and Sep. 2005Dec. 2005) which are not used

    in the fitting process, are introduced in equation 13 to calculate the corresponding values

    of daily diffuse solar radiation. The calculated values (Ddc) were compared with the

    corresponding measured ones (Ddm) during the mentioned periods as shown in Fig. 14. It

    can be observed from this figure that there is a strong correlation between the calculated

    and measured values of Dd (0.87). The percentage of the frequency distribution of

    relative deviation of its calculated values from the measured ones is also computed as

    indicated in Fig. 15. It is clear that the used equation provide best estimates for Dd where

    27.40% of the results lie in the range < 5%; 44.18% lie in the range < 10%; 37.67% lie

    in the range (10%) (20%) and only 18.15% of the results have relative deviation >

    20%.

    Statistical analysis has been done with the aim of supporting the validity of the used

    model in calculating daily diffuse solar radiation Dd in the new period (Jan. 2006 Apr.

    2006; May 2000Aug. 2000 and Sep. 2005Dec. 2005). The results are summarized in

    Table 4. These results indicate that equation 13 is eligible to calculate the diffuse solar

    radiation in the study region with high accuracy.

    3.2.2 Monthly averages of diffuse solar radiation (m

    D )

    The relation between the calculated (mc

    D ), using equation 13, and the measured

    (mm

    D ) values of monthly averages of diffuse solar radiation through the study period is

    shown in Fig. 16 . It is clear from this figure that both parameters change in a similar

    pattern through the months of the year with a high degree of correlation (corr. = 0.97). As

    shown in Fig. 17, the percentage of the frequency distribution of the relative deviation of

    calculated monthly averages of diffuse solar radiation from the experimental ones in the

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    study period indicates that 50% of the results lie in the range < 5%; 91.67% lie in the

    range < 10%; while 8.33% only lie in the range > 10%. Also Table 4 summarizes the

    statistical study of the calculation process. In view of the above discussions in the

    previous sections, equation (13) proofs its validity in calculating (m

    D ) with a high

    accuracy.

    4. Comparison of the constants of the linear regression forms at different locations

    in Egypt

    Comparison of the linear regression constants of equations (12) and (13) with that

    estimated at different locations in Egypt (El-sebaii and Trabea, 2003, 2005) is given in

    Table (5). It is obvious from this table that both the constants (a) and (b) change from

    location to another, especially with respect to KD correlations. This is due to the different

    geographic and climatic conditions as well as the nature and the concentration of the

    atmospheric constituents (e.g. aerosols and water vapor) characterizing these locations.

    Near values of (a) and (b) are found at Qena and Aswan (288 Km south of Qena) owing

    to their quasi similar climatic conditions.

    5. Conclusions

    On the light of the preceding results, the following conclusions can be deducted:

    1. The necessity of using solar radiation as an alternative source of energy at

    Qena/Egypt to help in solving the problem of energy demand, since this region is

    characterized with abundant solar radiation and semi cloudless weather. On the

    average more than 98% of the values of K t > 0.5 and more than 89% of the

    sunshine periods can extend to > 70% of the maximum possible bright hours.

    2. Several equations of different types (1-5) have been developed and performed for

    use in estimating (G) and (D) at the study region. All of them can be used with a

    good accuracy in the estimation process. The simple first order relations (12) and

    (13) are proposed for estimating both of them in this work.

    3. The proposed equations are found to be valid to estimate (G) and (D) in the study

    region with high accuracy. Few estimates are found to fall beyond accuracy level

    10%. They can also be used to some extend in the adjoining locations of

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    similar atmospheric characteristics. This conclusion is somewhat different with

    respect to (D), because it depends largely on the impact of atmospheric

    constituents (e.g. aerosols and water vapor) on the solar radiation incident on the

    Earth's surface, which varies from region to region according to their nature of

    man- and industrial activities.

    References

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    E. El Nobi, 2006. Surface Ultraviolet Radiation Measurements in Qena Upper

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    Table 1 Calculated regression constants of equations 1-5 and its statistical analysis, with

    respect to Kt, in the period (2001-2004) in the study region

    Statistical parameters

    Models

    LinearSec.order

    Thirdorder

    Power Exponential

    Correlation 0.75 0.75 0.76 0.76 0.79

    F- statistics 1054.4 532.31 364.27 1133.6 1323.1

    F critical 254.31 19.496 8.526 254.31 254.31

    parameters

    a 0.33 0.29 0.37 0.7 0.36b 0.38 0.513 -0.09 0.34 0.69

    c - -0.1 1.03 - -

    d - - -0.61 - -

    St.Deviation

    a 0.011 0.02 0.03 0.002 0.006

    b 0.012 0.059 0.178 0.01 0.019

    c - 0.042 0.318 - -

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    d - - 0.171 - -

    T- ratio

    a 31.1 14.52 12.55 376.9 58.83

    b 32.47 8.698 0.51 33.67 36.37

    c - 2.25 3.25 - -

    d - - 3.58 - -

    Table 2 Statistical analysis of calculated global solar radiation (Gc) during different

    periods

    Statistical parametersDaily values(2001-2004)

    Daily values ( May2005 Apr 2006)

    Monthly averages(2001-2004)

    MBE% -0.476 2.39 -0.0749

    RMSE% 5.809 4.794 2.799

    MAE% 4.687 3.83 2.407ME

    0.963 0.966 0.986

    D 0.985 0.992 0.996

    t- test (critical value) 2.358 (2.57) 9.824 (12.706) 0.088 (2.57)

    Table 3Calculated regression constants of equations 1-5 and its statistical analysis, with

    respect to KD, in the period (2001-2004) in the study region

    Statistical parameters

    Models

    Linear Quadratic Cubic Power Exponential

    Correlation 0.92 0.67 0.71 0.68 0.82

    F- statistics 4464.12 2550.45 1699 638.96 1598.03

    F critical 254.31 19.496 8.526 254.31 254.31

    parameters

    a 1.08 0.19 0.11 0.18 2.46

    b - 0.95 1.62 3.86 - 1.12 - 2.74

    c - - 1.73 - 6.99 - -

    d - - 3.16 - -

    St.Deviation

    a 0.013 0.022 0.033 0.002 0.153

    b 0.014 0.067 0.202 0.044 0.069

    c - 0.049 0.363 - -d - - 0.196 - -

    T- ratio

    a 84.14 8.74 3.37 84.52 16.08

    b 66.81 24.30 19.11 25.23 39.97

    c - 35.52 19.26 - -

    d - - 16.14 - -

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    Table 4 Statistical analysis of calculated daily diffuse solar radiation (Dc) during different

    periods

    Statisticalparameters

    Daily values(2001-2004)

    Daily values (Jan. 2006 Apr.2006, May 2000Aug. 2000 and

    Sep. 2005Dec. 2005)

    Monthly averages(2001-2004)

    MBE% 1.04 0.68 -2.03

    RMSE% 18.85 16.53 6.94

    MAE% 14.52 12.57 5.59

    ME 0.88 0.84 0.93

    d 0.94 0.93 0.98

    t- statistics(criticalvalue) 1.53(1.65) 0.705(1.65) 1.02(1.79)

    Table 5 Comparison of constants of the linear regression equations (12&13) at

    different locations in Egypt

    Locations Type of

    correlation

    Correlation

    coefficients

    Regression constants

    a b

    Rafah (3113

    N, 34

    12E, 73 m)

    Kt & (n/N) 0.965 0.367 0.342

    KD & (n/N) 0.67 0.730 -0.433

    AL Arish (31 07N,

    3345

    E, 32 m)

    Kt & (n/N) 0.970 0.295 0.423

    KD & (n/N) 0.78 0.941 -0.683

    Matruh (31 21N, Kt & (n/N) 0.973 0.508 0.186

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    2713

    E, 38 m) KD & (n/N) 0.85 0.618 -0.335

    Tanta (30 47N, 31

    E, 8 m)

    Kt & (n/N) 0.960 0.247 0.489

    KD & (n/N) - - -

    Aswan (23 58N,

    32 47E, 191.7 m)

    Kt & (n/N) 0.950 0.334 0.389

    KD & (n/N) 0.78 0.886 -0.618

    Qena (26 10N, 32

    43E,78 m)

    Kt & (n/N) 0.99 0.330 0381

    KD & (n/N) 0.97 1.08 -0.95

    Fig. 1 Percentage of the frequency distribution of daily clearness index KtatQena through the study period (2001-2004).

    1.18%

    95.04%

    3.78%

    0%

    10%

    20%

    30%

    40%

    50%

    60%

    70%

    80%

    90%

    100%

    percentageofclearnessindex(%)

    < 0.5 0.5 ? 0.7 > 0.7

    clearness index (Kt)

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    Fig. 2 Percentage of the frequency distribution ofdailysunshine fraction(n/N) at Qena through the study period (2001-2004).

    0.0

    0.2

    0.4

    0.6

    0.8

    1.0

    0.0 0.2 0.4 0.6 0.8 1.0

    sunshine fraction (n/N)

    clearnessindex(Kt)

    Fig. 3 Relationship between the daily values of clearness index

    (Kt) and sunshine fraction (n/N) at Qena through the

    study period (2001-2004).

    1.72%

    8.33%

    89.94%

    0%

    10%

    20%

    30%

    40%

    50%

    60%

    70%

    80%

    90%

    percentageofsunshin

    efraction(%)

    < 0.5 0.5 ? 0.7 > 0.7

    sunshine fraction (n/N)

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    Figure 4 Variation of the daily measured (Gdm) and calculated (Gdc) global solarradiation values through the study period at Qena /Egypt

    Julian day

    Dailyglobalsolarradia

    tion(Gd)in

    Wh/m2

    0

    2000

    4000

    6000

    8000

    10000

    1 31 61 91 121 151 181 211 241 271 301 331 361

    Jan. Feb. Mar. Apr. May Jun. Jul. Aug. Sep. Oct. Nov. Dec.

    winter spring summerAutumn

    (Gdc) (Gd m)

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    -40

    -30

    -20

    -10

    0

    10

    20

    30

    40

    1 31 61 91 121 151 181 211 241 271 301 331 361

    Julian day

    Relativedeviation

    (R.D.)

    %

    68.17%

    26.25%

    5.35%

    0.24%

    0%

    10%

    20%

    30%

    40%

    50%

    60%

    70%

    Fr e

    quencydist ribut ioni n

    Per c

    ent age

    ( %)

    0 (5) (5) (10) (10) (20) > 20

    Relative deviation (R.D.) (%)

    N= 561

    N= 216

    N= 44N= 2

    Figure 5: Percentages of the relative deviation (a) and its frequency distribution(b) of calculated daily global solar radiation (Gdc)from measured ones(Gdm) atQena through the study period

    ( b )

    ( a )

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    0

    2000

    4000

    6000

    8000

    10000

    0 2000 4000 6000 8000 10000

    measured daily global solar radiation (Gdm) in Wh/m2.day

    Ca

    lcu

    latedda

    ilyg

    loba

    lso

    larra

    diatio

    n(G

    dc

    )inWh/m

    2.d

    ay

    Figure 6 Relation between the daily values of the measured (Gdm) and the calculated

    (Gdc) global solar radiation values through the period (May 2005 April 2006)

    at Qena /Egypt.

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    Figure 7 Percentages of the relative deviation (a) and its frequency distribution(b) of calculated daily global solar radiation (Gdc)from measured ones(Gdm) atQena through the period (May 2005 Apr 2006)

    73.04%

    22.87%

    3.41%0.68%

    0%

    10%

    20%

    30%

    40%

    50%

    60%

    70%

    80%

    FrequencydistributioninPercentage(%)

    0 ? (5) (5) ? (10) (10) ? (15) (15) ? (20)

    Relative deviation (R.D.) (%)

    N= 214

    N= 67

    N= 10N 2

    -40

    -30

    -20

    -10

    0

    10

    20

    30

    40

    1 31 61 91 121 151 181 211 241 271 301 331 361

    Julian day

    Relativedeviation(R.D.)

    %

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    0

    2000

    4000

    6000

    8000

    10000

    Jan. Feb Mar Apr May Jun Jul Aug Sep Oct Nov Dec

    monthlyaverageglobalsolarradiation(G

    m)inWh/m

    2

    Gmc Gmm --------

    Fig. 8 Relation between the measured (Gmm) and calculated (Gmc) values ofmonthly average of global solar radiation through the study period (2001-

    2004) at Qena /Egypt.

    -25

    -20

    -15

    -10

    -5

    0

    5

    10

    15

    20

    25

    1 2 3 4 5 6 7 8 9 10 11 12

    months

    Re

    lative

    devia

    tion

    %

    Figure 9 Percentage of the relative deviation of calculated monthly average of

    global solar radiation from experimental ones through the study period

    at Qena / Egypt..

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    95.67%

    2.77%

    1.56%

    0%

    10%

    20%

    30%

    40%

    50%

    60%

    70%

    80%

    90%

    100%

    per c

    entageofdif fus ef rac ti o

    n( %

    )

    < 0.5 0.5

    0.7 > 0.7Diffuse fraction (KD)

    N= 1106

    N= 32N= 18

    Figure 10: Percentage of the frequency distribution of the diffuse fraction (KD) at

    Qena through the study period (2001- 2004).

    Figure 11: Relation between the daily values of diffuse fraction (K D ) andsunshine fraction (n/N) at Qena through the study period (2001-2004).

    0.0

    0.2

    0.4

    0.6

    0.8

    1.0

    0.0 0.2 0.4 0.6 0.8 1.0

    Sunshine fraction (n/N)

    Diffusefraction(K

    D)

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    0

    1000

    2000

    3000

    4000

    5000

    0 1000 2000 3000 4000 5000

    Measured daily diffuse solar radiation Ddm in Wh/m2.day

    Ca

    lcu

    latedda

    ilydiffuseso

    larrad

    iation

    Ddc

    inWh/m

    2.d

    ay

    Figure 12 Relation between daily values of the measured (Ddm) and calculated (Ddc)

    diffuse solar radiation through the study period (2001-2004) at Qena / Egypt.

    40.29%

    33.82%

    17.97%

    6.74%

    1.19%

    0%

    5%

    10%

    15%

    20%

    25%

    30%

    35%

    40%

    45%

    Frequencydist ri b

    ut ioni nP

    er c

    ent age( %

    )

    0 (10) (10)(20) (20) (30) (30) (40) > 40

    Relative deviation (R.D.)%

    N= 305

    N= 136

    N= 51

    N= 9

    N= 256

    Figure 13 Percentage of the frequency distribution of relative deviation of daily

    calculated values (Ddc ) of diffuse solar radiation from measured ones

    (Ddm) at Qena through the study period (2001-2004).

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    0

    1000

    2000

    3000

    4000

    5000

    6000

    0 1000 2000 3000 4000 5000 6000

    measured diffuse solar radiation (Ddm) in Wh/m2.day

    calculateddiffusesolarradia

    tion(D

    dc)

    inWh/m

    2.day

    Figure 14: Relation between daily values of the measured (Ddm) and calculated

    (Ddc) diffuse olar radiation through the periods (Jan. 2006 Apr.

    2006, May 2000Aug 2000 and Sep 2005Dec. 2005) at Qena /Egypt.

    27.40%

    44.18%

    37.67%

    18.15%

    0%

    5%

    10%

    15%

    20%

    25%

    30%

    35%

    40%

    45%

    Fre q ue ncy d i s t ri butio n

    inp e r ce nta g e ( %

    )

    0(5) < (10) (10) (20) > 20

    Relative deviation (RD) %

    N= 129

    N=53

    N= 110

    N= 80

    Figure 15 Percentage of the frequency distribution of relative deviation of daily

    calculated values (Ddc ) of diffuse solar radiation from measured ones

    (Ddm) at Qena through the periods (Jan. 2006 Apr. 2006, May 2000

    Aug. 2000 and Sep. 2005Dec. 2005) at Qena /Egypt.

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    0

    500

    1000

    1500

    2000

    2500

    Jan. Feb Mar Apr May Jun Jul Aug Sep Oct Nov Dec

    Months

    Monthlyaveragediffusesolarradiation(Dm

    )inWh/m2

    Figure 16 Relation between the values of the measured (Dmm) and calculated

    (Dmc) monthly average of the diffuse solar radiation through the

    study period (2001- 2004) at Qena /Egypt.

    50.00%

    91.67%

    8.33%

    0%

    10%

    20%

    30%

    40%

    50%

    60%

    70%

    80%

    90%

    100%

    Frequenc y di s t ribution

    inperc entag

    e( %)

    0 (5) < (10) >(10)

    Relative deviation (R.D.)%

    N= 6

    N= 11

    N= 1

    Figure 17 Percentage of frequency distribution of relative deviation of calculated

    (Dmc) monthly average diffuse solar radiation from measured ones at

    Qena through the study period (2001- 2004).