# Study of Temperature Coefficients for Parameters of Photovoltaic Cells.

1. IntroductionAn increasing number of countries have introduced renewable energy policies to reduce the greenhouse gas emissions and to avoid an energetic crisis created by the exhaustion of the fossil fuels. Most of them have fixed targets for using different types of renewable energy, and for this, they offer financial support [1]. The ways to improve the renewable energy domain are to develop hybrid renewable energy systems [2, 3], to solve the problems created when the renewable energy is inserted in the electrical power system [3], to achieve a very good integration of the renewable energy in buildings [4], to solve the storage problem, and to increase the efficiency of the existing ones.

The important role that the photovoltaic technology plays in the renewable energy domain is demonstrated by the dynamics, by the photovoltaic capacity installed worldwide (which is over 40 GW each year over the last years), and by the growth in the number of jobs created, which is over 2.8 million and represents 30% from the total new jobs created in the renewable energy domain [1].

Due to the major interest for photovoltaic technology, the researchers have developed various types of photovoltaic cells, such as multijunction, perovskite, and quantum well [5-9]. Although these types of photovoltaic cells are very promising, the monocrystalline, polycrystalline, and the amorphous silicon photovoltaic cells and panels are still more widely used in terrestrial applications. The multijunction photovoltaic cells are highly efficient, but because of their rather high price, they are generally used in space applications and in concentrated light applications.

The photovoltaic cells and panels can be characterized using their important dc parameters: the photogenerated current, [I.sub.ph]; the short-circuit current, [I.sub.sc]; the open-circuit voltage, [V.sub.oc]; the maximum power, [P.sub.max]; the fill factor, FF; the efficiency, [eta]; the series resistance, [R.sub.s]; the shunt resistance, [R.sub.sh]; the ideality factor of diode, m; and the reverse saturation current, [I.sub.o] [10]. Using the I-V characteristic, the equivalent circuit and one or more of the methods developed by researchers in the last 40 years, [10], the important parameters of the photovoltaic cells can be determined.

All the photovoltaic cell parameters are influenced by the temperature variation. If the temperature of the photovoltaic cells increases, most of them being influenced negatively--they decrease. The others increase with temperature, such as the short-circuit current, which slightly increases, and the reverse saturation current which increases exponentially [11-14].

The temperature of the photovoltaic cells in most of the locations varies from 0[degrees]C to 60[degrees]C. There are locations where the lower limit of the working temperature can be below -20[degrees]C and the upper limit can be over 80[degrees]C in semiarid areas [15]. These limits can be exceeded in other applications such as the spatial applications and concentrated light applications or extreme locations [16, 17].

The behavior of the photovoltaic cell parameter function of the temperature is very well described by the temperature coefficients [11-21]. The temperature coefficients, TC, can be absolute and normalized as in the following [13, 18, 21]:

[TC.sub.a](p) = dp/dT,

[TC.sub.n](p) = 1/p dp/dT|[sub.T=25[degrees]C] (1)

where p represents the parameter of the photovoltaic cell and T is the temperature.

The dependence of the photovoltaic cell parameter function of the temperature is approximately linear [21], and thus, the temperature coefficients of the parameters can be determined experimentally using the linear regression method [22]. The mechanisms which influence the performance of the photovoltaic cell can be better studied if the normalized temperature coefficient of the [P.sub.max] is considered as a sum of the normalized temperature coefficients of the [I.sub.sc], [V.sub.oc], and FF [12,21].

Four types of commercial photovoltaic cells are taken into consideration for this study: three from the silicon family--the monocrystalline, polycrystalline, and the amorphous silicon photovoltaic cells--and one from the multijunction family--InGaP/InGaAs/Ge photovoltaic cell. The important parameters of these photovoltaic cells, like [I.sub.sc], [V.sub.oc], [P.sub.max], FF, [eta], [R.sub.s], and m were studied related to the temperature, which was varied from 25[degrees]C to 87[degrees]C. The temperature coefficients of the photovoltaic cell parameters are determined and compared with the reference ones found in the related literature. The dependence of the temperature coefficients for [I.sub.sc], [V.sub.oc], [P.sub.max], FF, and [eta] upon the irradiance was also studied.

2. Theoretical Considerations

The I-V characteristic and the equivalent circuit with the suitable mathematical model are important tools to study and to determine the parameters of the photovoltaic cells in different conditions. There are three models: one-, two-, and three-diode model function of the electric current conduction mechanism from the photovoltaic cell as the diffusion mechanism, the generation-recombination mechanism, and the thermionic mechanism [10]. The generally accepted model is the one-diode model [10,23]. The equivalent circuit for this model can be seen in Figure 1, and the model is described mathematically by the following equation:

[mathematical expression not reproducible], (2)

where [V.sub.T] = kT/q is the thermal voltage, T is the temperature, k is the Boltzmann constant, and q represents the elementary charge.

The generally used equivalent circuit and the model for analyzing the multijunction InGaP/InGaAs/Ge photovoltaic cell consist of three one-diode models, one for each junction, connected in series [24].

The open-circuit voltage can be obtained using (2) where I = 0 and [I.sub.ph] [approximately equal to] [I.sub.sc], m is equal to 1, and the shunt resistance is considered very high. In this case, the last term of (2) tends towards zero and can be neglected. Deriving the equation obtained in function of the temperature, the absolute temperature coefficient of the open-circuit voltage is given by the following equation [13]:

d[V.sub.oc]/dT = [V.sub.oc]/T + [V.sub.T] (1/[I.sub.sc] d[I.sub.sc]/dT - 1/[I.sub.o] d[I.sub.o]/dT). (3)

The reverse saturation current of the photovoltaic cell is a parameter strongly dependent on the temperature. This dependence is given by the following empirical equation which was simplified by Green [25]:

[mathematical expression not reproducible], (4)

where A is a constant equal to 1.5 x [10.sup.8] mA [cm.sup.-2] and [E.sub.g] represents the band gap energy.

The variation of the reverse saturation current function of the temperature [16] is given as follows:

1/[I.sub.o] d[I.sub.o]/dT = 1/[V.sub.T] ([E.sub.g]/T + d[E.sub.g]/dT). (5)

The fill factor temperature coefficient can be calculated using the fill factor formula given by Green [25] or using the formula which takes into account the series resistance [12]. Using the Green formula, the absolute temperature coefficient is obtained as follows:

[mathematical expression not reproducible]. (6)

The absolute temperature coefficient of the photovoltaic cell efficiency can be determined by linear fitting of the efficiency dependence on the temperature. The efficiency is calculated as follows:

[eta] = [P.sub.max]/[I.sub.t] x A, (7)

where A represents the area of the photovoltaic cell and It is the irradiance.

The [V.sub.oc], [I.sub.sc], and [P.sub.max] are parameters which can be determined very easily from the I-V characteristic of the photovoltaic cell and also FF using (8). The normalized temperature coefficient of the reverse saturation current, [TC.sub.n]([I.sub.o]), can be calculated, using (3), and the temperature coefficients, [TC.sub.n]([V.sub.oc]) and [TC.sub.n]([I.sub.sc]) can be determined experimentally. The advantage of this method is that it does not require the determination of [I.sub.o]. Also, the absolute coefficient of the energy band gap, [TC.sub.n]([E.sub.g]), can be determined using (5), [TC.sub.n]([I.sub.o]) and the value of [E.sub.g] at 25[degrees]C from the literature [26] without determination of the [E.sub.g].

FF = [P.sub.max]/[I.sub.sc] x [V.sub.oc]. (8)

The influence magnitude of the series resistance and the ideality factor of diode can be found by the comparison of the results obtained for [TC.sub.a](FF) using (6) and by linear regression of the dependency FF versus T obtained experimentally.

3. Experimental Set-Up

Four types of commercial photovoltaic cells--monocrystalline silicon 3 cm/3 cm, polycrystalline silicon 2.7 cm/1.3 cm, amorphous silicon 3 cm/3 cm, and triple junction InGaP/ InGaAs/Ge 1 cm/1 cm--were measured function of temperature and irradiance and also analyzed and compared. The band gap energies of the InGaP/InGaAs/Ge photovoltaic cell junctions are 1.86 eV/1.40 eV/0.67 eV. For each type of photovoltaic cells, several ones were measured in order to choose a representative one.

The I-V characteristics of the photovoltaic cells were measured using the SolarLab system developed by the authors [27] (see Figure 2).

The SolarLab system allows varying the temperature of the photovoltaic cells, and the I-V characteristic is measured at constant temperature. The temperature was maintained constant using a PID (proportional-integral-derivative controller) algorithm which is implemented in the software which serves the system.

The system is covered with a black box to avoid the reflection or other light sources and to minimize the temperature variation of the photovoltaic cell under test.

The I-V characteristics of the four photovoltaic cells are measured at different levels of illuminations from 400 W/[m.sup.2] to 1000 W/[m.sup.2], and for each level of illumination, the temperature of the photovoltaic cell was varied from 25[degrees]C to 87[degrees]C.

The temperature of the photovoltaic cell and the irradiance are measured simultaneously with the I-V characteristics. The accuracy of the temperature measurement is [+ or -]0.5[degrees]C, and the accuracy of the irradiance is [+ or -]3 W/[m.sup.2].

The SolarLab software is used to control the measurement system, to make the data acquisition, and it has modules implemented to determine the important parameters of the photovoltaic cells using different methods developed by researchers [10,27]. The software application was created in the graphical programming language LabVIEW, and its interface is presented in Figure 3.

4. Results

The important parameters of the four photovoltaic cells are obtained using the SolarLab system, the I-V characteristics, the-one diode model, and the analytical five-point method [10, 28] at different temperatures and different irradiance.

The I-V characteristics measured under illumination at 1000 W/[m.sup.2] irradiance and at different temperatures, which varies from 26[degrees]C to 87[degrees]C, are presented in Figure 4(a) for mSi photovoltaic cell and in Figure 4(b) for InGaP/InGaAs/ Ge photovoltaic cell.

The open-circuit voltage is strongly affected by the temperature variation. The increase in temperature led to decreasing the value of the band gap energy (see (9)). The intrinsic carrier concentration, [n.sub.i], increases because it depends inversely exponentially on the band gap energy [14]. Due to the proportionality of the [I.sub.o] with [n.sub.i.sup.2], the reverse saturation current increases with temperature. The increase is exponential (see (4)), leading to the decrease of the open-circuit voltage and the fill factor.

[E.sub.g](T) = [E.sub.g](0) - [alpha][T.sup.2]/T + [beta] (9)

where [E.sub.g](0), [alpha], and [beta] are material constants [14].

The behavior of the open-circuit voltage function of the temperature and irradiance is presented in Figure 5(a) for the monocrystalline photovoltaic cell, Figure 5(b) for the polycrystalline photovoltaic cell, Figure 5(c) for the amorphous photovoltaic cell, and Figure 5(d) for the InGaP/ InGaAs/Ge photovoltaic cell.

The absolute temperature coefficients for the important parameters of the photovoltaic cells at different levels of illumination are presented in Table 1.

The short-circuit current slightly increases with temperature, as a consequence of the band gap energy reduction. In this case, the number of photons which have enough energy to create electron-hole pairs is higher. The behavior of the open-circuit voltage temperature coefficient and the short circuit current temperature coefficient function of the irradiance is reverse.

The maximum power of the photovoltaic cells decreases when the temperature of the photovoltaic cells increases because the increase in the maximum current does not compensate for the decrease in the maximum voltage.

The values of the absolute and normalized temperature coefficients for different types of photovoltaic cells under 1000 W/[m.sup.2] illumination obtained in this paper (TI) and the ones from literature [13, 18, 20, 29, 30] are presented in Table 2.

Analyzing the values of the temperature coefficients, a good matching can be observed for the [TC.sub.a]([V.sub.oc]) and [TC.sub.n]([V.sub.oc]), but there are differences for the [TC.sub.a]([I.sub.sc]). This difference influences the matching for the other temperature coefficients. The differences can be explained by the differences in fabrication process for the same type of photovoltaic cells and the difference between the measurement conditions, and a very important role is played by the illumination source. The differences for [TC.sub.a]([I.sub.sc]) can be higher than 50% due to the spectral mismatch between the light sources used [18]. A very good matching is observed for the multijunction photovoltaic cell.

Analyzing the open-circuit voltage absolute temperature coefficient variation with the irradiance, for all types of the analyzed photovoltaic cells, a linear dependence is observed (see Figure 6(a)) and also, a linear dependency is obtained for the absolute temperature coefficient of the maximum power (see Figure 6(b)).

The positive slope of the linear dependency of the absolute temperature coefficient of the open-circuit voltage upon the irradiance shows a reduction in voltage drop if the temperature increases when the irradiance increases. The highest slope is obtained for the InGaP/InGaAS/Ge photovoltaic cell. The absolute temperature coefficient of the short-circuit current has the same behavior.

The negative slope of the linear dependency of the absolute temperature coefficient of the maximum power upon the irradiance shows a growth in power drop if the temperature increases when the irradiance increases. The best slope of photovoltaic cells' efficiency is obtained for the InGaP/ InGaAS/Ge photovoltaic cell. The amorphous silicon has a very good behavior, but it has a minor impact because the amorphous photovoltaic cell has the smallest maximum power from all photovoltaic cells taken into account in this study. The similar results are obtained for the dependence [TC.sub.a]([V.sub.oc]), [TC.sub.a]([I.sub.sc]), and [TC.sub.a](FF) on the irradiance for two photovoltaic cells polycrystalline silicon and Elkem Solar Silicon by Tayyib et al. [31].

Prediction of the photovoltaic cell and panel output in real work conditions is very important for the final users. There are some models developed which can give the maximum power generated by the photovoltaic panels, the short-circuit current and the open-circuit voltage function of the irradiance and temperature using the values given for the manufacturers in the data sheet, determined at standard test conditions (STC)--global irradiance 1000 W/[m.sup.2], AM 1.5, and panel temperature 25[degrees]C [32-36]. These models take into account the absolute temperature coefficients obtained at 1000 W/[m.sup.2] irradiance. Using the results obtained by the data analyzed, these models can be improved if the variation function of the irradiance is taken into account for the absolute temperature coefficients. The improved models to predict the maximum power generated by the photovoltaic panel at different irradiances and temperatures are given by (10), for the short-circuit current by (11) and for the open-circuit voltage by (12).

[P.sub.max] = [P.sub.max(STC)] G/1000 [1 + TC([P.sub.max], G)([T.sub.c] - 25)], (10)

where [P.sub.max](STC) is the maximum power at STC conditions, G is the irradiance, [T.sub.c] represents the temperature of the photovoltaic cells, and TC([P.sub.max], G) is the normalized temperature coefficient for the maximum power at irradiance G.

[I.sub.sc] = [I.sub.sc(STC)] G/1000 [1 + TC([I.sub.SC], G)([T.sub.c] - 25)], (11)

where [I.sub.SC(STC)] is the short-circuit current at STC conditions and TC([I.sub.sc], G) is the normalized temperature coefficient for the short-circuit current at irradiance G.

[V.sub.oc] = [V.sub.oc(STC)][1 + TC([V.sub.OC], G) ([T.sub.c] - 25)] + TC(G)ln G/1000, (12)

where [V.sub.OC(STC)] is the open-circuit voltage at STC conditions, TC([V.sub.oc], G) is the normalized temperature coefficient for the open-circuit voltage at irradiance G and TC(G) represents the temperature coefficient for the irradiance.

The I-V characteristics for all photovoltaic cells under test were performed at temperature room which is 21[degrees]C and at 1000 W/[m.sup.2] irradiance (Figure 7). Using (11) and (12), the short-circuit current and the open-circuit voltage were calculated to compare the obtained results with measured ones. The results obtained for the representative photovoltaic cells are presented in Table 3.

The difference between the measured and calculated value with (11) and (12) of the short-circuit current and the open-circuit voltage for all photovoltaic cells under test is under 0.1%. Better results are obtained for mSi photovoltaic cell.

Two additional experiments were performed to verify the results obtained for the short-circuit current and the open-circuit voltage, one in lab conditions using a mSi photovoltaic cell with sizes 6 cm x 8 cm (Figure 8). Both photovoltaic cells, 3 cm x 3 cm and 6 cm x 8 cm, were cut from the mSi by the same lot. The halogen bulbs used to illuminate the photovoltaic cells are the same with halogen bulb of SolarLab. The other experiment was performed in natural sunlight conditions using mSi from the same lot with the cells tested with SolarLab, and the sizes are 12.5 cm x 12.5 cm (Figure 9). The photovoltaic cells, in lab and outside, are cooled using Peltier module and water collector.

The I-V characteristics were measured for two levels of irradiance 900 W/[m.sup.2] and 1000 W/[m.sup.2], and at 30[degrees]C temperature of the photovoltaic cells. The results obtained are presented in Table 4.

The difference between [V.sub.oc] calculated and measured is under 1.1 mV which means a 0.5[degrees]C temperature difference in laboratory conditions and over 1[degrees]C in sunlight conditions. For [I.sub.sc], this difference increases, almost doubling. The short-circuit current is very sensitive to the level of illumination. The irradiance was measured with three different sensors, one for each case. This can be explained by the increasing difference for [I.sub.sc]. The difference between the results in laboratory and sunlight conditions can be due to the spectral difference between the light sources.

The extrapolation from the monocrystalline photovoltaic cells considered to a 15.6 cm x 15.6 cm one is as follows: the open-circuit voltage temperature coefficient is the same, and the short-circuit current and maximum power temperature coefficients can be obtained by multiplying the determined temperature coefficient with the ratio between the areas of the two cells.

The maximum power generated by the photovoltaic cells is very important from the energy point of view. The decreasing percent in [degrees]C for the maximum power of the photovoltaic cells at 1000 W/[m.sup.2] is presented in Table 5, where the result obtained for the photovoltaic panel is also presented. This percent slightly varies with the irradiance variation; for example, it varies from 0.38%/[degrees]C at 1000 W/[m.sup.2] to 0.44%/[degrees]C at 400 W/[m.sup.2] for polycrystalline photovoltaic cells. The best behavior is obtained for the multijunction photovoltaic cell.

The fill factor of all the photovoltaic cells considered in this study decreases with the temperature increase, and this dependence for 1000 W/[m.sup.2] is being presented in Figure 10. The behavior of the fill factor function of the temperature is determined by the dependency of the open-circuit voltage, short-circuit current, and the maximum power on the temperature. By analyzing the FF dependency function of the temperature, it is observed that the FF temperature coefficient of the amorphous photovoltaic cell is the smallest and the FF temperature coefficient of the monocrystalline photovoltaic cell is the highest. This situation is the same for all illumination levels taken into consideration.

The FF temperature coefficient in absolute value decreases almost by half for the amorphous photovoltaic cell, while for the monocrystalline silicon, polycrystalline silicon and InGaP/InGaAS/Ge photovoltaic cells, the decrease proportion is much smaller (see the values for [TC.sub.a](FF) from Table 1).

The series resistance and the ideality factor of diode are determined using the five-parameter method. The parameter can be determined with very good accuracy with the five-parameter method, if the maximum power is determined with very good accuracy [38]. The standard uncertainty of the module used to measure the I-V characteristics is 0.016 mV, and the number of I-V points is higher than 1000, to minimize the errors in determining the maximum power.

The dependence of the series resistance for all photovoltaic cells on temperature at 1000 W/[m.sup.2] irradiance is presented in Figure 11(a). The series resistance decreases linearly with the increase in temperature. The series resistance is determined by the semiconductor resistivity and the resistance of the metal conductors. These two components depend on the temperature, first exponentially and then linearly. Figure 11(b) presents the variations of the ideality factor of all four photovoltaic cells with temperature at 1000 W/[m.sup.2] irradiance. A decrease in the ideality factor is observed with the increase in temperature. The ideality factor of diode m decreases due to the decrease of the active layer resistance of the semiconductors or the temperature influence on surface recombination rate mechanism and Shockley-Read-Hall. The results obtained (Figure 11(c)) also indicate that the shunt resistance of all four photovoltaic cells decreases nearly linearly when the temperature of the cells increases. The [R.sub.sh] decreases because the shunt defects, as recombination centers or traps, and manufacturing defects increase with temperature growth. The decrease rate of the shunt resistance differs function of the type of the photovoltaic cells. The linear temperature dependence obtained for the three parameters of the photovoltaic cells is well consistent with ones found in literature [14, 39].

The values of the [TC.sub.n]([I.sub.o]) were determined using (3), and the temperature coefficients [TC.sub.a]([V.sub.oc]) and [TC.sub.n]([I.sub.sc]) are presented in Table 6. This method was verified using the values from reference [13]. The values calculated for the [TC.sub.n]([I.sub.o]) for the three cases reported in [13] are 0.166 [K.sup.-1], 0.166 [K.sup.-1], and 0.155 [K.sup.-1] and using (3) are 0.170 [K.sup.-1], 0.170 [K.sup.-1], and 0.158 [K.sup.-1]. There are some differences due to the approximations made to obtain (3), but it is a very simple and rapid method to find out [TC.sub.n]([I.sub.o]). The error in determining the normalized temperature coefficient of the Io is smaller than 3%.

5. Conclusions

The performance of the four photovoltaic cells, mSi, pSi, aSi, and InGaP/InGaAs/Ge, is analyzed depending upon the temperature and irradiance, by investigating the most important parameters, such as the open-circuit voltage, the short-circuit current, the maximum power, the series resistance, the diode's ideality factor, the reverse saturation current, and the fill factor. The photovoltaic cell temperature was varied from 25[degrees]C to 87[degrees]C, and the irradiance was varied from 400 W/[m.sup.2] to 1000 W/[m.sup.2].

The temperature coefficients and their behavior in function of the irradiance of the enumerated parameters were calculated and compared with related literature results, and a good consistency is obtained. The analysis of the results underlines the fact that the temperature is an important factor which influences the performance of the photovoltaic cells. The maximum power decreases with values between 0.14% and 0.47% if the temperature increases with 1[degrees]C for the photovoltaic cells analyzed.

The analysis shows that the absolute temperature coefficients of the parameters taken into consideration are dependent on the irradiance level. The irradiance has a small influence on the absolute temperature coefficient of the open-circuit voltage, but for the others, such as the absolute temperature coefficients of the short-circuit current and of the maximum power the influence, the irradiance is much higher. The variation of the last two absolute temperature coefficients with irradiance is almost proportional.

The improved models to predict the maximum power, short-circuit current, and the open-circuit voltage function of the temperature and irradiance are developed. A very simple and rapid way to calculate [TC.sub.n]([I.sub.o]) is also described in this paper. The comparative results obtained for the open-circuit voltage, the short-circuit current measured, and the maximum power in different conditions, laboratory and outside, and the values calculated (estimated) with the temperature coefficients found, validate the improved models presented.

Consequently, in order to maximize the power generated by the photovoltaic cells, it is necessary to choose the optimum technology for the respective location, increasing the irradiance, for example, using the concentrated light and assuring a good cooling.

https://doi.org/10.1155/2018/5945602

Conflicts of Interest

The authors declare that they have no conflicts of interest. Acknowledgments

This work was supported by a grant of the Romanian National Authority for Scientific Research and Innovation, CNCS, UEFISCDI, Project no. PN-II-RU-TE-2014-4-1083 and Contract no. 135/1.10.2015.

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Daniel Tudor Cotfas (iD), Petru Adrian Cotfas (iD), and Octavian Mihai Machidon (iD)

Electronics and Computers Department, Transilvania University ofBrasov, Brasov, Romania

Correspondence should be addressed to Daniel Tudor Cotfas; dtcotfas@unitbv.ro

Received 11 September 2017; Revised 19 November 2017; Accepted 22 January 2018; Published 25 March 2018

Academic Editor: Leonardo Sandrolini

Caption: Figure 1: The equivalent circuit for one-diode model.

Caption: Figure 2: The SolarLab system used to characterize the photovoltaic cells.

Caption: Figure 3: The interface of the SolarLab software.

Caption: Figure 4: The I-V characteristics versus temperature at 1000 W/[m.sup.2] irradiance for (a) mSi and (b) InGaP/InGaAs/Ge.

Caption: Figure 5: The open-circuit voltage versus temperature and irradiance for (a) mSi, (b) pSi, (c) aSi, and (d) InGaP/InGaAs/Ge. The lines represent the curve obtained by linear regression.

Caption: Figure 6: The dependency of the absolute temperature coefficient versus irradiance for all photovoltaic cells (a) for the open-circuit voltage and (b) for the maximum power.

Caption: Figure 7: The I-V characteristics at 1000 W/[m.sup.2] and room temperature 21[degrees]C: (a) mSi and pSi; (b) aSi and InGaP/InGaAs/Ge.

Caption: Figure 8: The laboratory experiment.

Caption: Figure 9: The natural sunlight experiment.

Caption: Figure 10: The FF versus temperature at 1000 W/[m.sup.2] irradiance.

Caption: Figure 11: (a) The [R.sub.s] versus temperature at 1000 W/[m.sup.2] irradiance (the values of the aSi [R.sub.s] are divided with 30). (b) The m versus temperature at 1000 W/[m.sup.2] irradiance. (c) The [R.sub.sh] versus temperature at 1000 W/[m.sup.2] irradiance (the values of the aSi [R.sub.sh] are divided with 30 and for multijunction with 40).

Table 1: The absolute temperature coefficients for the important parameters of the photovoltaic cells. PV [I.sub.T] d[V.sub.oc]/dT d[I.sub.sc]/dT (W/[m.sup.2]) (mV [degrees] (mA [degrees] [C.sup.-1]) [C.sup.-1]) mSi 400 -2.36 0.265 600 -2.32 0.375 800 -2.27 0.465 1000 -2.24 0.537 pSi 400 -2.29 0.108 600 -2.27 0.147 800 -2.24 0.191 1000 -2.19 0.215 aSi 400 -8.53 0.00727 600 -8.36 0.0106 800 -8.3 0.0151 1000 -8.09 0.0187 InGaP/InGaAs/Ge 400 -7.46 0.0125 600 -7.21 0.0158 800 -7.05 0.0194 1000 -6.93 0.0253 PV [I.sub.T] d[P.sub.max]/dT dFF/dT (W/[m.sup.2]) (mW [degrees] (% [degrees] [C.sup.-1]) [C.sup.-1]) mSi 400 -0.251 -0.138 600 -0.419 -0.141 800 -0.551 -0.147 1000 -0.691 -0.162 pSi 400 -0.07 -0.122 600 -0.103 -0.130 800 -0.128 -0.139 1000 -0.163 -0.147 aSi 400 -0.0101 -0.026 600 -0.0158 -0.031 800 -0.0208 -0.0411 1000 -0.0268 -0.0487 InGaP/InGaAs/Ge 400 -0.016 -5.49E - 4 600 -0.027 -5.6E - 4 800 -0.032 -5.76E - 4 1000 -0.040 -5.99E - 4 Table 2: Comparison between the temperature coefficients at 1000 W/[m.sup.2]. PV cell Ref. d[V.sub.oc]/dT (d[V.sub.oc]/dT)/ (mV [degrees] [V.sub.oc] [C.sup.-1]) (ppm/[degrees] [C.sup.-1]) mSi TI -2.24 -3835 [16][c.sub.1] -2.19 -- [16][c.sub.2] -2.36 -- [18] -- -3413 pSi TI -2.19 -3725 [18] -- -3675 aSi TI -8.09 -- [29] a -5.8 -- [29] b -5.57 -- InGaP TI -6.93 -- InGa [30] -6.2 -- As/Ge [20] -5.6 -- PV cell Ref. d[I.sub.sc]/dT (d[I.sub.sc]/dT/ (mA [degrees] [I.sub.sc] [C.sup.-1]) (ppm/[degrees] [C.sup.-1]) mSi TI 0.537 138 [16][c.sub.1] 0.326 -- [16][c.sub.2] 0.401 -- [18] -- 130 pSi TI 0.215 870 [18] -- 675 aSi TI 0.0187 -- [29] a 0.007 -- [29] b 0.00788 -- InGaP TI 0.0253 -- InGa [30] 0.005 -- As/Ge [20] 0.0098 -- PV cell Ref. d[P.sub.max]/dT d[P.sub.max]/dT)/ (mW [degrees] [P.sub.max] [C.sup.-1]) (ppm/[degrees] [C.sup.-1]) mSi TI -0.691 -4798 [16][c.sub.1] -- -- [16][c.sub.2] -- -- [18] -- -5035 pSi TI -0.163 -3713 [18] -- -4690 aSi TI -0.0268 -- [29] a -0.0138 -- [29] b -0.0175 -- InGaP TI -0.04 -- InGa [30] -- -- As/Ge [20] -0.055 -- PV cell Ref. dFF/dT (dFF/dT)/FF (% [degrees] (ppm/[degrees] [C.sup.-1]) [C.sup.-1]) mSi TI -0.162 -2189 [16][c.sub.1] -- -- [16][c.sub.2] -- -- [18] -- -1642 pSi TI -0.147 -2046 [18] -- -1732 aSi TI -0.0487 -- [29] a -- -- [29] b -- -- InGaP TI -5.99E - 4 -- InGa [30] -6E - 4 -- As/Ge [20] -6.3E - 4 -- Table 3: The calculated and measured values for [V.sub.oc] and [I.sub.sc]. mSi [V.sub.oc] (V) [I.sub.sc] (A) Calculated 0.59494 0.38664 Measured 0.59483 0.38647 pSi [V.sub.oc] (V) [I.sub.sc] (A) Calculated 0.60593 0.10273 Measured 0.6058 0.102626 aSi [V.sub.oc] (V) [I.sub.sc] (A) Calculated 2.6382 0.008346 Measured 2.6396 0.008351 InGaP/InGaAs/Ge [V.sub.oc] (V) [I.sub.sc] (A) Calculated 2.6863 0.01155 Measured 2.6878 0.01156 Table 4: The calculated and measured values for [V.sub.oc] and [I.sub.sc] of mSi at 30[degrees]C. 900 W/[m.sup.2] [V.sub.oc] (V) [J.sub.sc] (mA) Laboratory Calculated 0.5727 39.138 Measured 0.5719 39.08 Sunlight Calculated 0.5729 39.14 Measured 0.5704 39.04 1000 W/[m.sup.2] [V.sub.oc] (V) [J.sub.sc] (mA) Laboratory Calculated 0.57482 43.487 Measured 0.574 43.422 Sunlight Calculated 0.5748 43.486 Measured 0.5721 43.378 Table 5: The decreasing percent for [P.sub.max] at 1000 W/[m.sup.2]. The mSi pSi aSi InGaP/InGaAs/Ge photovoltaic cell Percent/ TI -0.47% -0.38% -0.18% -0.14% [degrees]C [37] -0.45% -0.39% -0.23% -- Table 6: The normalized temperature coefficient of the [I.sub.o] at 1000 W/[m.sup.2]. The photovoltaic mSi pSi aSi cell (d[I.sub.o]/dT)/ [degrees] 0.164 0.161 0.636 [I.sub.o] [C.sup.-1] The photovoltaic InGaP/InGaAs/Ge cell (d[I.sub.o]/dT)/ [degrees] 0.591 [I.sub.o] [C.sup.-1]

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Title Annotation: | Research Article |
---|---|

Author: | Cotfas, Daniel Tudor; Cotfas, Petru Adrian; Machidon, Octavian Mihai |

Publication: | International Journal of Photoenergy |

Article Type: | Report |

Date: | Jan 1, 2018 |

Words: | 6713 |

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