1. Introduction
Recently, Excessive use of conventional sources causes environmental concerns. These reasons promote using alternative, renewable and sustainable, energy sources [
1] (Vafaeipour et al., 2014).
In Morocco, many farmers started using clean energy assisted by subsidy programs launched by government to supply their sustainable irrigated agricultural systems [
2] (Moumen, 2014). Meanwhile, R&D actions still needed to improve systems performance and their reliability for large extension in developing countries.
Several researchers have developed strategies to optimize electrical and hydraulic performances. For better PV panels performance, many authors were focused on improving PV panel conversion of PVWPS. In fact, MPPT (Maximum Power Point Tracking) technologies using a diversity of algorithms that allows systems benefiting from maximum of PV power generated [
3,
4,
5,
6] (Akihiro et al. (2009), Khan et al. (2012), Sefriti and Boumhidi, (2015) and Essam et al. (2017)).
Moreover, numerous research studies have been conducted to improve energy efficiency systems. For instance, one approach suggested in [
7] (Almeida et al., 2018) involved selecting a pump based on its efficiency across the entire spectrum of operational frequencies. This method led to a decrease in the power threshold necessary to begin pumping, enabling longer pumping durations. Another innovations related to pumps design, detailed in [
8] (Hamidat et al. (2003)) involved an investigation into the performance of Photovoltaic Water Pumping Systems (PVWPS), employing centrifugal and positive displacement pumps. In their study, they integrated a multistage centrifugal pump with an alternating current (AC) motor and a three-phase inverter. Additionally, a second pump was linked to a DC-DC converter, controlling a Brushless Direct Current (BLDC) motor. Their findings demonstrated that the positive displacement pump attained an efficiency rate of 45%, while the centrifugal pump lagged behind, registering a mere 14% efficiency. In a separate study, Hamidat and Benyoucef (2008) [
9] undertook a comparison of PVWPS performance involving centrifugal and positive displacement pumps. They employed simulations in a range of locations, each distinguished by varying atmospheric conditions, including the Saharan climate and summer rainfall. By assessing the electrical and hydraulic components of both centrifugal and positive displacement pumps, they noted that the positive displacement pump outperformed in terms of efficiency, reduced energy losses, and higher water volume displacement.
Furthermore, Protogeropoulos and Pearce (2000) [
10], along with Kashyap et al. (2013) [
11], emphasized the necessity for further enhancements in standalone Photovoltaic Water Pumping Systems (PVWPS). These improvements are required to effectively meet the water requirements of small-scale drip irrigation systems while effectively managing the changes in surrounding pressure caused by the fluctuations in daily insolation. Presently, a notable number of photovoltaic pumping facilities incorporate two or more pumps linked in parallel. This arrangement serves as a suitable solution for accommodating fluctuating water flow requirements, minimizing the impact of climatic and sunlight fluctuations. Utilizing multiple parallel pumps may additionally enhance facility efficiency and extend daily operational periods [
12] (Harkani et al., 2019). Similarly, the authors in [
13] (Zhounian et al.,(2020)) introduced an optimization model for parallel pump systems with the objective of decreasing power consumption and enhancing reliability by addressing off-design operational issues of pumps. The approach employs the particle swarm optimization method to solve the optimization problem. In [
14] the authors (Koor et al., (2016)) developed an algorithm designed to predict the steady operation of variable speed pumps (VSPs) functioning in parallel, with the primary goal of maintaining their operation in close proximity to the optimal efficiency point (BEP) provided by the pump manufacturer. Utilizing optimization software allows for the determination of the optimal combined efficiency when pumps operate in parallel. In cases where pumps are identical and have matching discharges, the best combined efficiency is achieved, consistent with various studies. Conversely, for non-identical pumps, the optimal combined efficiency is attained when varying water discharges are taken into account. Additionally, the optimization software can assist in estimating the ideal number of pumps to be operational for optimal performance.
Additionally, divers’ investigations have been extended to predict the hourly flow rate and to maximize the discharge of the daily water volume of PVWPS using mathematical model [
15,
16] (Katan et al., (1996), Zahab et al., (2017)). The author in [
15] (Katan et al., (1996)) developed a mathematical model that predict output water flow rate according to electrical operating energy. Based on experimental results, the obtained volume of pumped water was found inversely proportional to the total head. Another methods are employed to characterize pump’s behavior through various parameters like rotation speed, flow rate, and power inputs. These parameters are used to calculate the head output corresponding to the irradiance intensity [
17,
18,
19] (Jafar., (2000), de Blas., (2002), Ahonen et al., (2010)). The expressions of these parameters are represented as affinity laws, which are employed for the optimal management of PVWPS [
20,
21] (Kalaiselvan, et al., (2108), and Zhang et al., (2016)). All of these publications have engaged with traditional analytical methods, with a specific focus on utilizing the polynomial model.
All previously mentioned research predicts PVWPS outputs based on irradiances. Notably, a simple and accurate model was developed using experimental findings. Moreover, when examining the PV pumping system’s performance, it becomes evident that the electrical power is directly impacted by the PV panels’ output power. This output power follows a growth model curve. This distribution shape also influences hydraulic power. To effectively capture this growth pattern, considering models like exponential or power models becomes pertinent.
3. Modeling of PVWPS
In order to assess the connection between solar irradiance and the hydraulic efficiency of our photovoltaic pumping setup, we employed both power and exponential growth models. We selected these models due to their capacity to capture rapid growth trends. Exponential and Power models are characterized by these two equations 3 and 4, respectively:
Where: y is the desired output at a given time, a is the initial value of y (when x=0), b is the base of the exponential, often called the growth factor, and x is the independent variable.
Where: y, a, b and x are the desired output at a given time, proportionality coefficient, the exponent of the power, and the independent variable, respectively.
The fitting of the generated models was assessed using the Root Mean Square Error (RMSE) method (eq. 5). Additionally, the Mean Absolute Error (MAE) (eq. 6) and the correlation coefficient (R²) were employed to demonstrate how well the model curves fit.
Where Mi and Ci are measured and calculated values, respectively and N is the number of measurements.
4. Results and Discussions
4.1. Results of Experimental Study
Standalone DC PVWPS performance was evaluated using a multi pumps approach. The system was monitored from 08:00 am to 06:00 pm showing its behavior. Taking into consideration irradiance and hydraulic power induced, three behaviors were obtained, the behavior of morning, mid-day and afternoon (
Table 1)
Table 1.
Daily performance of PVWPS according to irradiance change and portion of switched on pump (experimental test results).
Table 1.
Daily performance of PVWPS according to irradiance change and portion of switched on pump (experimental test results).
Time |
Irradiance (W/m²) |
Number of operating Pumps |
Mean Pressure (bar) (CV%) |
Mean Flowrate (L/min) (CV%) |
Mean Hydraulic Power (CV%)
|
Mean Hydraulic Yield% (CV%)
|
08. am |
178 |
1 |
01.18 (16) |
02.46 (08) |
04.65 (24) |
30 (19) |
197 |
2 |
00.45 (20) |
03.28 (11) |
02.41 (28) |
13 (31) |
213 |
3 |
00.26 (19) |
03.61 (10) |
01.51 (27) |
07 (26) |
09. am |
331 |
1 |
01.24 (17) |
02.43 (09) |
04.74 (24) |
33 (18) |
350 |
2 |
00.71 (20) |
02.91 (10) |
03.44 (28) |
14 (23) |
368 |
3 |
00.45 (22) |
03.29 (12) |
02.39 (32) |
07 (32) |
10. am |
515 |
1 |
02.63 (27) |
03.19 (14) |
02.51 (37) |
06 (28) |
530 |
2 |
00.93 (37) |
02.70 (19) |
04.00 (56) |
13 (38) |
544 |
3 |
00.60 (32) |
03.08 (17) |
02.96 (45) |
06 (40) |
11. am |
662 |
2 |
00.84 (37) |
02.83 (19) |
03.39 (55) |
12 (42) |
679 |
3 |
00.65 (35) |
03.03 (20) |
03.11 (47) |
07 (38) |
12. pm |
749 |
2 |
00.76 (24) |
02.91 (13) |
03.39 (32) |
12 (31) |
758 |
3 |
00.72 (26) |
02.93 (15) |
03.38 (36) |
06 (38) |
01. pm |
777 |
3 |
00.78 (31) |
02.87 (17) |
3.55 (41) |
34 (38) |
02. pm |
754 |
2 |
01.12 (33) |
02.61 (18) |
04.25 (46) |
13 (37) |
748 |
3 |
00.95 (28) |
02.74 (16) |
03.90 (40) |
06 (38) |
03. pm |
670 |
2 |
01.08 (32) |
02.64 (18) |
04.16 (45) |
12 (38) |
508 |
3 |
00.94 (27) |
02.71 (15) |
03.96 (37) |
06 (36) |
04. pm |
534 |
1 |
01.97 (29) |
02.69 (16) |
03.97 (40) |
12 (35) |
517 |
2 |
01.00 (29) |
02.67 (16) |
04.08 (40) |
09 (37) |
500 |
3 |
00.45 (38) |
03.30 (22) |
02.36 (53) |
06 (39) |
05. pm |
344 |
1 |
00.80 (53) |
03.01 (31) |
03.16 (73) |
24 (48) |
326 |
2 |
00.59 (32) |
03.11 (19) |
02.89 (44) |
10 (38) |
312 |
3 |
00.36 (30) |
03.45 (19) |
01.95 (38) |
06 (38) |
06. pm |
37 |
1 |
00.62 (28) |
03.06 (16) |
03.03 (38) |
25 (35) |
34 |
2 |
00.20 (25) |
03.74 (13) |
01.16 (35) |
09 (47) |
42 |
3 |
00.04 (34) |
04.05 (19) |
00.29 (46) |
02 (55) |
Table 1 presents the system’s response to different levels of irradiance. In the morning hours (8:00 am, 9:00 am, 10:00 am), three distinct flow patterns are described, each associated with a specific number of active pumps required to adjust the system’s operating point. This adjustment is essential for optimizing system performance. In essence, achieving better performance depends on adapting the number of active pumps to match the actual irradiance levels. When the pressure requirements are met, an improved performance is linked to a specific count of engaged pumps.
However, at 11:00 am, 12:00 pm, 2:00 pm and 3:00 pm, the increase of pressure was observed as irradiance were important. Consequently, an increase of hydraulic power was obtained. At 11:00 am, 12:00 pm, 2:00 pm and 3:00 pm, there is no need to operate with one small pump, since using the two pumps meet maximum pressure (1.12 bar). The results obtained showed efficiency arranged from 6% to 13%. According to mid-day (1:00 pm) with high irradiance (777 W/m2), the system showed interesting performance (Around 34%). Indeed, the abundant irradiance at 777 W/m² enabled the system to run with the maximum number of pumps without causing any decline in pump efficiency, as previously demonstrated during the morning incident irradiance. One system behavior using three pumps was obtained, since use of a single small pump increases pressure and risks damaging the system.
At the afternoon, the system performance showed a behavior similar to the morning. This can be attributed to the insufficient incident irradiance in the range of 38-516 W/m². The findings reveal an efficiency range between 2% and 25%. When the pump is not operating under low levels of sunlight, adjustments in flow and pressure become necessary to optimize pump efficiency, aligning with the hydraulic equivalence model of the connected pumps. The system’s performance is noticeably influenced by the presence of low incident irradiance at 38 W/m², subsequently affecting pump efficiencies.
As per the pumping system’s response for each configuration of the number of active pumps,
Table 1 demonstrates a significant variance in terms of efficiency. This table provides a summary of the independent system’s behavior throughout the day. Under low irradiance conditions, the system operates in normal mode (with all pumps active), resulting in lower yields. However, activating the pumps shifts the system’s operating point to an optimal position, compelling it to perform more efficiently (yielding higher results).
In contrast, during periods of high irradiance, the system operates in normal mode, maintaining consistent performance. It is worth noting that changes in irradiance negatively impact the system’s efficiency. This observed variability in efficiency is attributed to the standalone system’s behavior, as it lacks capacitors to regulate and stabilize the instantaneous relationship between flow and pressure, which is influenced by fluctuations in solar irradiance.
Hydraulic performance of the PVWPS was tested by three cases: The first case using one equivalent pump (30W), the second using two equivalent pumps (2*30W) and the last using three equivalent pumps (3*30W).
At low irradiance, first case results (
Figure 4a–c) showed that the equivalent pump (30W) operated efficiently in low irradiance. In normal condition, results showed that the system could not operate efficiently (7%). But when we changed three pumps (90W) with one equivalent pump (30W), the efficiency of the system was reached (30%), with an average daily pumped water obtained was about 164 (L/h). This case (Use of one equivalent pump) allowed the system to operate 5 hours per day since, at high irradiance, use of a single equivalent pump increases pressure and risks damaging the system. (
Figure 4a/ Case 2) showed that the system perform using two pumps (60W) with irradiance increasing. Consequently, the daily pumped water was increased and reached a maximum of 349 (L/h) (
Figure 4c/ Case 2). Operating time of the system using two equivalent pumps (60W) was 5 hours (From 10:00 am 03:00 pm excluding 01:00 pm). At low irradiance the system showed a worse efficiency using three equivalent pumps (90W). Except a significant increase in yield (46%) was obtained at 01:00 pm when irradiance was at its maximum (777 W/m²) (
Figure 4a/ Case 3). This case (use of three equivalent pumps (90W)) allowed the system to operate 1 hour. At high irradiance,the daily pumped water was about 516(L/h) (
Figure 4c/ Case 3).
Figure 4.
PVWPS behavior using: One equivalent Pump (Case 1); Two equivalent Pumps (Case 2); Three equivalent Pumps (Case 3): a). Hydraulic Efficiency (HE-G); (b). Flowrate (Q-G); (c). Pumped Volume (VP-G).
Figure 4.
PVWPS behavior using: One equivalent Pump (Case 1); Two equivalent Pumps (Case 2); Three equivalent Pumps (Case 3): a). Hydraulic Efficiency (HE-G); (b). Flowrate (Q-G); (c). Pumped Volume (VP-G).
4.2. Modeling of PVWP System Using Experimental Data
PVWPS model
Simulations of the standalone PVWPS’s performance are conducted on an hourly basis. Growth curves were generated through the application of two non-linear models—the exponential model and the power model—utilizing two distinct software platforms: Python and R. These models were evaluated based on the coefficient of determination R²(
Table 2)
Table 2.
Coefficients values of the generated models linking all parameters with time.
Table 2.
Coefficients values of the generated models linking all parameters with time.
Increasing Irradiance Trend |
|
Model |
Software Tools |
a |
b |
R² |
Irradiance Vs Time |
Exponential |
Python |
62,093 |
0,202 |
0,86 |
Exponential |
R |
62,092 |
0,202 |
0,86 |
Power |
Python |
2,874 |
2,219 |
0,9 |
Power |
R |
2,874 |
2,22 |
0,9 |
Electrical Power Vs Time |
Exponential |
Python |
5,185 |
0,203 |
0,88 |
Exponential |
R |
5,185 |
0,203 |
0,88 |
Power |
Python |
0,262 |
2,188 |
0,88 |
Power |
R |
0,262 |
2,188 |
0,88 |
Hydraulic Power Vs Time |
Exponential |
Python |
0,293 |
0,358 |
0,82 |
Exponential |
R |
0,293 |
0,358 |
0,82 |
Power |
Python |
0,001 |
3,917 |
0,62 |
Power |
R |
0,001 |
3,917 |
0,62 |
Decreasing Irradiance Trend |
|
Model |
Software Tools |
a |
b |
R² |
Irradiance Vs Time |
Exponential |
Python |
22539,772 |
-0,251 |
0,82 |
Exponential |
R |
22539,772 |
-0,251 |
0,82 |
Power |
Python |
10939913,381 |
-3,679 |
0,78 |
Power |
R |
3378000 |
-3,245 |
0,77 |
Electrical Power Vs Time |
Exponential |
Python |
1328,821 |
-0,218 |
0,85 |
Exponential |
R |
1328,793 |
-0,218 |
0,84 |
Power |
Python |
295836,902 |
-3,209 |
0,81 |
Power |
R |
298100 |
-3,21 |
0,81 |
Hydraulic Power Vs Time |
Exponential |
Python |
8165,452 |
-0,423 |
0,95 |
Exponential |
R |
8165,454 |
-0,423 |
0,95 |
Power |
Python |
243140608,495 |
-6,158 |
0,95 |
Power |
R |
12560000 |
-5,038 |
0,92 |
After an analysis of the generated models, it was observed that their outcomes exhibited a high degree of similarity. Nevertheless, the exponential model emerged as the top choice due to its superior performance according to the evaluation metrics R² (
Figure 5).
Figure 5.
a/ Fitting Curves of two models of Irradiance versus Time, b/ . Fitting Curves of two models of EP versus Time, c/ Fitting Curves of two models of HP versus Time.
Figure 5.
a/ Fitting Curves of two models of Irradiance versus Time, b/ . Fitting Curves of two models of EP versus Time, c/ Fitting Curves of two models of HP versus Time.
Based on the fitting curves, the results have demonstrated comparable behavior between the two models, with a minor distinction observed primarily in relation to the exponential model (
Table 3). The analytical model’s validation involved utilizing RMSE and MAE methods. The outcomes of the error assessments concerning irradiance, electrical power, and hydraulic power are consolidated in
Table 3.
From the exponential models presented herein, the derivations of transfer functions become feasible, establishing interrelationships among various parameters such as hydraulic power versus electrical power, and electrical power concerning irradiance. The mathematical representation of these transfer functions is as follows:
Electrical Power & Irradiance
Hydraulic Power & Electrical Power
Where: EP, G, HP, t are Electrical Power, Irradiance, Hydraulic Power and time, respectively.
Table 3.
Validation Model using RMSE and MAE Methods.
Table 3.
Validation Model using RMSE and MAE Methods.
Increasing Irradiance Trend |
|
Time |
Real Data |
PP Exponential Model |
Power Model |
|
|
Irradiance Vs Time |
08:00 |
196 |
313 |
290 |
Exponential Model |
09:00 |
350 |
382 |
377 |
RMSE |
79,09 |
10:00 |
530 |
468 |
476 |
MAE |
73,83 |
11:00 |
671 |
573 |
588 |
Power Model |
12:00 |
754 |
701 |
713 |
RMSE |
66,68 |
01:00 |
777 |
858 |
852 |
MAE |
62,33 |
Electrical Power Vs Time |
08:00 |
20,38 |
26,31 |
24,79 |
Exponential Model |
09:00 |
32,85 |
32,23 |
32,08 |
RMSE |
05,97 |
10:00 |
50,90 |
39,48 |
40,39 |
MAE |
04,30 |
11:00 |
41,72 |
48,36 |
49,76 |
Power Model |
12:00 |
59,84 |
59,25 |
60,19 |
RMSE |
05,92 |
01:00 |
72,71 |
72,59 |
71,71 |
MAE |
04,25 |
Hydraulic Power Vs Time |
08:00 |
04,84 |
05,14 |
03,45 |
Exponential Model |
09:00 |
05,01 |
07,35 |
05,47 |
RMSE |
04,00 |
10:00 |
16,69 |
10,51 |
08,26 |
MAE |
3,15 |
11:00 |
15,75 |
15,04 |
12,00 |
Power Model |
12:00 |
14,81 |
21,51 |
16,87 |
RMSE |
5,75 |
01:00 |
33,43 |
30,77 |
23,08 |
MAE |
4,41 |
Decreasing Irradiance Trend |
|
Time |
Real Data |
PP Exponential Model |
Power Model |
|
|
Irradiance Vs Time |
01:00 |
777 |
863 |
873 |
Exponential Model |
02:00 |
751 |
671 |
664 |
RMSE |
111,05 |
03:00 |
589 |
522 |
515 |
MAE |
93,83 |
04:00 |
517 |
406 |
406 |
Power Model |
05:00 |
327 |
316 |
325 |
RMSE |
119,49 |
06:00 |
38 |
2446 |
264 |
MAE |
99,33 |
Electrical Power Vs Time |
01:00 |
72,71 |
78,10 |
78,78 |
Exponential Model |
02:00 |
62,85 |
62,81 |
62,11 |
RMSE |
07,94 |
03:00 |
63,42 |
50,50 |
49,77 |
MAE |
06,29 |
04:00 |
46,40 |
40,61 |
40,46 |
Power Model |
05:00 |
31,37 |
32,66 |
33,31 |
RMSE |
08,98 |
06:00 |
13,18 |
26,26 |
27,73 |
MAE |
07,24 |
Hydraulic Power Vs Time |
01:00 |
33,43 |
33,40 |
33,59 |
Exponential Model |
02:00 |
19,49 |
21,88 |
21,28 |
RMSE |
02,33 |
03:00 |
18,95 |
14,33 |
13,92 |
MAE |
01,77 |
04:00 |
08,84 |
09,39 |
09,35 |
Power Model |
05:00 |
04,02 |
06,15 |
06,44 |
RMSE |
02,47 |
06:00 |
03,15 |
04,03 |
04,53 |
MAE |
01,88 |