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Improved design of advanced controller for a step up converter used in photovoltaic system

  • Nadia Ben Si Ali EMAIL logo , Nadia Benalia and Nora Zerzouri
Published/Copyright: May 30, 2023
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Abstract

The expanding need for electricity has stimulated research and development of novel supply sources for energy production, conversion, and storage. Many studies are being done to increase the effectiveness of conversion systems as renewable energy is integrated into power networks on a larger scale. The global challenge is to minimize manufacturing costs and increase the use of sustainable resources. In this sense, photovoltaics is viewed as a particularly promising source due to the low cost of implementation and the wide range of applications it could be used for. This research focuses on the analysis, modeling, and simulation of a smart controller for a step-up converter that uses an artificial neural network (ANN) as a maximum power point tracking (MPPT) technique to provide maximum power. The proposed ANN-based algorithm is performed in Matlab/Simulink software, and its effectiveness has been demonstrated under varying climatic conditions.

1 Introduction

Interest in renewable energy sources has risen as a result of depleting energy supplies, rising environmental degradation, and global warming. The sun is the renewable energy source that is used the most frequently.

The solution is to use renewable energies which offer the possibility of producing electricity that meets ecological requirements, such as photovoltaic energy, but unfortunately this issue encounters economic constraints, high cost and low yield. The maximum power pursuit problem is among the problems of photovoltaic systems. This observation is confirmed by the large number of works concerning this problem encountered in the literature. Different maximum power point tracking MPPT methods have been used in the literature in order to achieve optimal performance. The most popular algorithm is perturb and observe (P&O) (Ben Si Ali, Zerzouri, and Benalia 2019; Derdar et al. 2021). The incremental conductance (INC) (Gupta, Chauhan, and Pachauri 2016; Manisha and Kumar 2021). The open-circuit voltage (OCV) (Tey and Mekhilef 2014), fuzzy logic method (Tey and Mekhilef 2014), genetic algorithm (Putri, Wibowo, and Rifa’i 2015). and MPPT algorithms based on neural networks in (Abdulrazzaq and Ali 2018; Hadji, Gaubert, and Krim 2018). Intelligence techniques play an important role in performance analysis, prediction, and control of renewable energy systems.

The main objective of this work is to investigate the performance of a solar system that uses an ANN MPPT technique for power maximization. The behavior and performance of PV panels utilizing this algorithm are assessed for climatic condition variations. The article is structured as follows: Section 1 describes the proposed system; Sections 2 and 3 present modeling and simulation of the PV system and step up converter, respectively; and Section 4 presents the proposed ANN-Based MPPT Algorithm, as well as its MATLAB/Simulink Simulation results and discussion. Section 6 conclusion.

2 System description

The system consists of photovoltaic PV panel connected to a load through a step-up DC-DC converter that uses an artificial neural network (ANN) as a maximum power point tracking (MPPT) algorithm to generate maximum power. The structure of the overall conversion chain is presented in Figure 1.

Figure 1: 
Structure of the overall converting chain.
Figure 1:

Structure of the overall converting chain.

3 Electrical equivalent circuit model of PV panel

A single solar cell can be modeled by using a current source, a diode, and two resistors (Rai et al. 2011; Salmi et al. 2012). This model is known as a single diode model. A PV array is a group of several PV cells which are electrically connected in series and parallel circuits to generate the required current and voltage (Figure 2).

Figure 2: 
Photovoltaic system.
Figure 2:

Photovoltaic system.

Light induced current basically depends on irradiance and temperature.

(1) I p h = I s c + k i ( T T r e f ) ( G 1000 )

The short-circuit current I sc is defined by:

I s c = I s = I p h

The module-reverse saturation current I rs and I 0 which varies with cell temperature are given by:

(2) I r s = I s c / [ exp ( q V o c N s k n T ) 1 ]

(3) I o = I r s [ T T r ] 3 exp [ q E g n k ( 1 T 1 T r ) ]

The current voltage characteristics will be:

(4) I = I p h I s ( e q ( V + I R s ) n K T 1 ) V + I R s R s h

Nomenclature

G

solar irradiance

T

cell p-n junction temperature

R sh

equivalent shunt resistance

R s

equivalent series resistance

I

output current

V

output voltage

I ph

photo generated electric current

I sc

short circuit current

I d

current at diode D

K

Boltzman’s constant

q

electron charge

I s

diode reverse bias saturation current

n

diode ideality factor

N s

number of series cells

E g

band gap energy of the semi-conductor.

Table 1 includes a datasheet and a list of the parameters for the PV panel Soltech 1STH-215-P used in Matlab Simulink. The first simulation is done for environmental condition variation for PV panels with two series modules and two parallel strings. The effect of application of different levels of irradiance as well as temperature on voltage-current (V–I) and voltage-power (V–P) is shown in Figure 3. The irradiance level and photo-generated current are directly related, therefore an increase in irradiation results in a larger photo-generated current. Additionally, because the photo generated current and short circuit current are particularly related, irradiance is directly proportional to both of them. It is clear that the variation in temperature mainly affects the open circuit voltage V oc. It decreases with temperature rise.

Table 1:

Electrical characteristics of 1Soltech 1STH-215-P module.

Open circuit voltage (V oc) 36.3 V
Short-circuit current (I sc) 7.84 A
Voltage at MPP (V mp) 29 V
Current at MPP (I mp) 7.35
Maximum power (P m ) 213.15 w
N s 96
Voltage/temp. Coefficient VK −0.38 %/°C
Current/temp. Coefficient I K 0.065 %/°C
Figure 3: 
PV characteristics for climatic condition variation. (a) I–V curves, (b) P–V curves.
Figure 3:

PV characteristics for climatic condition variation. (a) I–V curves, (b) P–V curves.

In standard test condition STC conditions (G = 1000 w/m2, T = 25 °C) this panel generates a maximum power of 852.6 w corresponding to PV voltage of 58 V and a current of 15.68 A.

3.1 Step up converter design and control

Maximum Power Point Tracking (MPPT) is a technique used in photovoltaic (PV) systems to optimize the energy output of solar panels. PV systems rely on converting sunlight into electrical energy, and the amount of energy produced depends on various factors such as the angle of incidence of the sunlight, irradiation and temperature. The MPPT technology maximizes the power output of solar panels by continuously tracking and adjusting the operating point of the PV system to extract the maximum power available from the panels at any given time. Usually, in order to extract at all times, the maximum power available at the terminals of the photovoltaic module and transfer it to the load, an adaptation stage DC-DC converter is used. The proposed model incorporates a PV array and a step-up converter, which is used as an interface device connecting the PV panel to the load (Nema et al. 2010; Ram, Babu, and Rajasekar 2017).

The Step up DC-DC chopper is a power converter with a dc output voltage higher than its dc input voltage. It contains two semiconductors (diode, switch) and at least one energy storage element. The output capacity is added to reduce output voltage ripple (Figure 4). Relationship between input and output voltage and current are given by equation (5).

(5) V o u t V i n = I i n I o u t = 1 1 D

Figure 4: 
Step up converter.
Figure 4:

Step up converter.

The operation of the step-up boost converter can be divided into two modes, Mode 1 and Mode 2. Mode 1 begins when the transistor IGBT is switched on at time t = 0. The input current rises and flows through the inductor L and the transistor IGBT. Mode 2 begins when the transistor IGBT is switched off. The input current, in this case, flows through L, C, load, and diode D. The inductor current falls until the next cycle. The energy stored in inductor L flows through the load.

3.2 Component calculations

The design of the step up converter parameters is done according to equations in Table 2.

Table 2:

Design of the step up converter.

Duty cycle Load resistance Inductor Capacitor Output current
D = 1 V i n V o u t R L o a d = V o u t I o u t L = V o u t . D f s . I C = I o u t . D f s . V I o u t = P max V o u t

I and V are admissible current and voltage ripple respectively.

4 Conventional methods used for MPP tracking

4.1 Perturb and observe P&O technique

The Perturb and Observe (P&O) algorithm is regarded as the most popular because of its ease of use and effectiveness. The basic idea behind this technique is illustrated in Figure 5, where each iteration involves perturbing (increasing or decreasing) the array terminal voltage and observing the impact on the PV output power, then comparing it with the previous iteration’s value. If the power is increased, the perturbation will continue in its current direction; otherwise, it will reverse. The operating point begins to oscillate around the maximum power point (MPP) after it is achieved. This technique presents some limitations, such as an increase in power losses as a result of the steady state condition oscillation around the MPP, particularly in the case of big steps (Ram, Babu, and Rajasekar 2017). The (P&O) algorithm is sluggish during a quick change of atmospheric conditions. The flow chart in Figure 5 recapitulates the P&O algorithm.

Figure 5: 
Flowchart of P&O algorithm.
Figure 5:

Flowchart of P&O algorithm.

4.2 Incremental conductance (INC) technique

As shown in Figure 6, the incremental conductance approach INC is based on tracking the MPP based on the slope of the solar panel’s output power. In this technique, the incremental conductance (ΔIV) and the instantaneous conductance (I/V) are compared. The terminal voltage of the PV array decreases if the slope of the P–V curve (ΔPV) is negative, indicating that the operating point is to the right of the MPP. If the slope is positive, the operating point is to the left of the MPP and the terminal voltage of the PV array is raised; if the slope is zero, the MPP is attained and the instantaneous and incremental conductances are equal (Chellal, Guimaraes, and Leite 2021).

Figure 6: 
Incremental conductance algorithm flowchart.
Figure 6:

Incremental conductance algorithm flowchart.

The first simulations were done for the perturb and observe P&O and incremental INC algorithms. Results have been established for T = 25 °C and variable irradiations to analyze the behavior of each technique (Figure 7). Figures 8 13 show voltage and current of the PV panel and the load, PV power, and the duty cycle.

Figure 7: 
Radiation pattern.
Figure 7:

Radiation pattern.

Figure 8: 
Load and PV voltages and currents for the P&O algorithm.
Figure 8:

Load and PV voltages and currents for the P&O algorithm.

Figure 9: 
PV power for the P&O algorithm.
Figure 9:

PV power for the P&O algorithm.

Figure 10: 
Duty cycle for the P&O technique.
Figure 10:

Duty cycle for the P&O technique.

Figure 11: 
Load and PV voltages and currents for the for the INC technique.
Figure 11:

Load and PV voltages and currents for the for the INC technique.

Figure 12: 
PV power for the INC technique.
Figure 12:

PV power for the INC technique.

Figure 13: 
Duty cycle for INC technique.
Figure 13:

Duty cycle for INC technique.

At standard test conditions, STC The PV system performances using P&O and INC MPPT algorithms are shown. It is clear that for constant irradiation G = 1000 w/m2, P&O finds MPP quickly but oscillates at MPP. As shown in Figure 12, INC finds MPP after a time delay. But the oscillations at constant irradiation are less as compared to P&O. Duty cycle dynamics of both algorithms for variable climatic conditions show that for P&O, D is perturbed continuously and results in greater oscillation at MPP with better tracking performances for instantaneous variation or quick slope of irradiance. While for INC, D presents less oscillation at MPP and more time to reach steady state. Thus, in order to overcome these limitations of conventional MPPT techniques, an efficient MPPT algorithm is needed. For this reason, a neural network MPPT algorithm is proposed.

5 Basic structure of neural network

The neural network technology is composed of a huge number of interconnected processors known as neurons. Each neuron has an important number of weighted connections for signal processing. As a result, it may be able to handle the challenging task of data processing and interpretation. Basically, the architecture consists of three types of neuron layers: the input layer, the hidden layer, and the output layer. A simple neuron model is shown in Figure 14. There are different activation functions that can be used (Khanam and Foo 2018). A mathematical model of the output of a neuron k can be written as:

V k = i = 1 n x i w k j + b

y k = f ( V k )

Figure 14: 
Basic structure of neuron.
Figure 14:

Basic structure of neuron.

The output neuron is obtained by summing each of the input signals after they have been multiplied by the connection weights. The proposed ANN in this study is a feed-forward neural network. The input layers represent the irradiance and temperature. The output layer is the voltage Vmpp corresponding to the maximum power generated by the panel. A duty cycle signal is then applied for adjusting PV voltage through the boost converter. The ANN Adaptive Neural Network for MPPT is shown in Figure 15.

Figure 15: 
ANN adaptive neural network for MPPT.
Figure 15:

ANN adaptive neural network for MPPT.

Figure 16 shows the topology that has been suggested and simulated in Matlab/Simulink. The NN algorithm provides the gate signal for the DC-DC converter. The algorithm uses the solar PV module’s temperature and irradiance to calculate the appropriate voltage to optimize for generating a referenced duty cycle for the dc-dc step up converter.

Figure 16: 
ANN MPPT based structure.
Figure 16:

ANN MPPT based structure.

6 Training data for learning (inputs and targets)

The ANN of MPPT is obtained from the PV model parameters presented in Section 2. The tansig is an activation function for the input layer. The purelin is the activation function for the output layer. A Mean Square Error criterion is used in training the network for determination of error. The Levenberg-Marquardt (LM)optimization technique is a network learning function (Trainlm) that amends weight and bias values (Khabou, Souissi, and Aitouche 2020; Motahhir, El Hammoumi, and El Ghzizal 2020). When required performances are achieved, the trained ANN becomes ready to track the MPP. The difference in voltage generated by the PV panel and the voltage generated by a trained artificial neural network is fed into the PI controller, whose output is compared to a high frequency signal to generate duty cycle. The flowchart, showing the training process is presented in Figure 17. Inputs and target variables obtained by the training process are presented in Figure 18. Some of the data are presented in Table 3. Neural network training is done using nntraintool (Figure 19).

Figure 17: 
Training process flowchart.
Figure 17:

Training process flowchart.

Figure 18: 
Data of the training process: Inputs (a) temperature T, (b) radiation G, (c) target Vmpp.
Figure 18:

Data of the training process: Inputs (a) temperature T, (b) radiation G, (c) target Vmpp.

Table 3:

A sample of some ANN training data.

Figure 19: 
Feed-forward neural network.
Figure 19:

Feed-forward neural network.

The command gensim (net) is used to develop a SIMULINK block for neural networks. The global Simulink model consists of two layers, as shown in Figure 20. The structures of layer 1 and layer 2 are shown in Figure 21.

Figure 20: 
Simulink model of neural network input layers.
Figure 20:

Simulink model of neural network input layers.

Figure 21: 
Structure of layer.
Figure 21:

Structure of layer.

The success of the ANN was measured using mean square error (MSE) and regression coefficient (Bataineh 2018; Khanaki, Radzi, and Marhaban 2013). Figure 22 shows validation performance graph obtained for the optimal value of the objective function of the network where training data, testing data and validation data are very close to each other. Best validation value is MSE = 1.802e−10 obtained at epoch 1000.

Figure 22: 
Validation performance graph.
Figure 22:

Validation performance graph.

Regression plot a graph for each of training, validation and test cases and average of the three make a plot graph mention as all. It is observed from Figure 23 that all the samples are aligned on the same line which represent a high accuracy of the acquisition of data and the validity of them.

Figure 23: 
Regression graph of the network.
Figure 23:

Regression graph of the network.

The Simulink model shown in Figure 24 is the block diagram of the PV array connected to a resistive load through a dc/dc step up converter with artificial neuron network MPPT controller. It is used to simulate dynamic behavior and power generated using this algorithm with irradiation and temperature variation patterns. The three methods were tested and compared under different scenarios. Figure 25 shows generated power and Figure 26 shows input and output voltages and currents. Variations in solar irradiance and temperature are applied to check and evaluate the robustness of the proposed controller.

Figure 24: 
Matlab/simulink model of pv panel with ANN Algorithm.
Figure 24:

Matlab/simulink model of pv panel with ANN Algorithm.

Figure 25: 
PV power with ANN algorithm.
Figure 25:

PV power with ANN algorithm.

Figure 26: 
Load and PV voltages and currents for the ANN algorithm.
Figure 26:

Load and PV voltages and currents for the ANN algorithm.

Figures 27 30 show simulation results of P&O, INC and ANN algorithm for maximum power point tracking for atmospheric condition variation. It is clear that all of NN, P&O, and INC track MPP with varying degrees of efficiency and accuracy. the NN algorithm has a fast response it takes less time to reach MPP, with high efficiency and less oscillation compared with traditional methods.

Figure 27: 
Irradiance variation.
Figure 27:

Irradiance variation.

Figure 28: 
PV power obtained applying P&O, INC and ANN algorithm for irradiation variation.
Figure 28:

PV power obtained applying P&O, INC and ANN algorithm for irradiation variation.

Figure 29: 
Temperature variation.
Figure 29:

Temperature variation.

Figure 30: 
PV power obtained applying P&O, INC and ANN algorithm for temperature variation.
Figure 30:

PV power obtained applying P&O, INC and ANN algorithm for temperature variation.

7 Conclusions

The present research investigates how artificial neural networks (ANN) may be used to improve MPPT accuracy and smoothness in solar power systems. The efficiency of solar manufacturing processes under fast and slow-changing atmospheric scenarios is proven through a comparison study of maximum power point tracking approaches. The behavior of a PV system is studied using conventional methods such as perturb and observe, incremental conductance, and the intelligently proposed ANN technique. Before using the ANN-suggested method, data collection must be done by selecting the network structure, then training it, and finally testing the network. Based on the simulation findings, it can be shown that all approaches are stable at MPP, although P&O and INC overshoot when the irradiance varies quickly. The findings show that applying the ANN algorithm allows tracking of the MPP faster and with reduced fluctuations, which enhances efficiency, improves robustness, and minimizes power losses.


Corresponding author: Nadia Ben Si Ali, Electrical Engineering Department, Badji Mokhtar Annaba University, Annaba, Algeria, E-mail:

  1. Author contributions: All the authors have accepted responsibility for the entire content of this submitted manuscript and approved submission.

  2. Research funding: No funding.

  3. Conflict of interest statement: The authors declare no conflicts of interest regarding this article.

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Received: 2022-07-24
Accepted: 2023-05-14
Published Online: 2023-05-30

© 2024 the author(s), published by De Gruyter, Berlin/Boston

This work is licensed under the Creative Commons Attribution 4.0 International License.

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