2. II. PHOTOVOLTAIQUE-ELECTROLYSIS SYSTEM
In this work, we considered that the electrolysis is
connected to the PV system according to the diagram in
“Fig.1”.
Panel (generator) PV Mutsibuchi-180 type, it consists
of 50 elementary photovoltaic cells and can deliver in
standard test conditions 174W of power, a current of
8.3A under optimum voltage of 24V.
The adaptation quadripole is an energy buck
converter already dimensioned and designed to
operate at a frequency of 100 KHz.
An algorithmic unit is developed to pursue the point of
maximum power where we implemented the MPPT
control algorithm known to perturb and observe
(P&O). The result of this program is to generate a
pulse width modulated signal (PWM) with frequency
of 100 KHz and controlling the MOSFET of the
converter. The implemented algorithm allows
adjustment of the duty cycle to pursue the maximum
power point of the PV panel and allows the optimal
operation of the electrolysis.
PEM electrolysis consists of 7 cells connected in
series with a surface of 10cm². The temperature and
the pressure operating electrolysis are T=80°C and
P=101325 Pa.
Figure 1. Schematic of a PV-electrolysis system
A. PV Modeling
A solar cell is generally represented by a current source
connected in parallel with a diode threshold less than 1V, a
series resistor Rs and a parallel resistor Rp “Fig. 2”. The solar
panel is an association Ns cells in series with Np cells in
parallel, the conversion of solar energy into electrical energy
is expressed by a non-linear relationship between the current I
and the voltage V of the PV panel [2].
.
.
1
..
)..(
.exp...
P
pvSpv
s
P
pvS
PSPHPpv
R
IRV
N
N
ATk
IRVq
NIINI
(1)
Where I is the PV generated current, V is PV generated
voltage, IPH is light-generated current (photo-current), Is is
saturated diode current, q is unsigned electron charge, A is an
ideal factor, (varies between 1.2 and 5), k is Boltzmann’s
constant and Tc is the absolute cell temperature.
B. Electrolysis Modeling
1) Water Electrolysis Principle
Electrolysis of water is dissociation of water molecules into
hydrogen and oxygen. A potential is applied across the
electrochemical cell to cause electrochemical reactions at two
electrodes. The scheme shown in "Fig.3" shows the
fundamental principle of electrolysis water.
Figure 2. Equivalent circuit of a solar cell
The main part of the PEM water electrolysis is the
membrane electrode assembly MEA. The perfluorosulfonic
acid polymer such as Nafion has been widely used as a
membrane for electrolysis of water, due to its intrinsic
properties: excellent chemical and mechanical stability and
high proton conductivity [10] [11] [12] [13].
For the anode, the catalysts based on Pt-IrO² alloy are
relatively stable and more practical as an anode electro-
catalyst compared to the platinum, which shows significant
overvoltage and platinum/ruthenium (Pt/Ru) that is not stable
and corrodes under oxygen evolution [14].
For the cathode, platinum offers the best performance and
commonly used for the electrolysis of water [9] [15].
The water introduced at the anode is dissociated into oxygen,
protons and electrons. The reaction at the anode can be
expressed as follows:
H2O (l) ½ O2(g) +2H+
+2e- (2)
Under an electric field, the protons are entrained through the
PEM to the cathode where they combine with electrons
coming from the external circuit to form hydrogen gas:
2H+
+ 2e- H2(g) (3)
Therefore, the overall reaction of this decomposition can be
written as:
H2O (l) H2(g) +1/2O2 (g) (4)
Figure 3.Fundamental principle of electrolysis water.
3. 2) Electrochemical Voltage of a PEM Electrolysis Cell
When the current is applied to the PEM cell, the voltage of
total operation of the electrolytic cell can be represented as the
sum of the Nernst voltage Erev, overvoltage at the cathode ηc
and anode ηa, overvoltage due to the membrane ηm and
interfacial overvoltage ηI “Fig.4”.
E=Erev+ηa-ηc +ηm+ηI (5)
Where the Nernst potential Erev is given empirically by [16]:
)log(
4
3.2)298(109.023.1 22
23
OHrev PP
F
RT
TE (6)
Figure 4. Voltage (V) as a function of current density (A) for a PEM
electrolysis cell operating at 80◦C
The overvoltage’s due to cathode, anode and membrane
resistance is given by: [14]
)
2
(sinh
.
0
1
A
A
I
I
F
TR
(7)
)
2
(sinh
.
0
1
C
C
I
I
F
TR
(8)
(9)
Where IA0 is the anode exchange current [A], Ic0 is the cathode
exchange current [A], LB is the thickness of PEM, σB is
conductivity of the electrolyte.
The interfacial overvoltage ƞI is the production of the
interfacial resistance RI and current I.
ηI=RI.I (10)
3) Modeling of PEM electrolysis cell
“Fig.5” illustrates the electrolysis process which is
represented by an equivalent electrical circuit consisting of a
series of resistors and a back electromotive force.
A separate derivation overvoltage confers resistance
corresponds to anode, cathode and polymer electrolyte
exchange membrane.
2
0
0 )(
4
1
1)2(
.
A
A
A
I
I
FI
TR
R
(11)
Figure 5. The equivalent circuit for the water electrolysis process
2
0
0 )(
4
1
1)2(
.
C
C
C
I
I
FI
TR
R
(12)
.
)(
B
B
m
L
R
(13)
And RI=RI (14)
4) The mass flow
The mass of hydrogen produced at the cathode is
proportional to the amount of current passed through the
electrolyte according to the second Faraday law:
FH
n.F
M
m
.t.I.nc
2
(15)
With:
mH2 = mass of hydrogen formed to the electrode (in kg)
nc = number of cells
M = molar mass of hydrogen (in kg.mole-1)
I = current through the electrolysis (in A)
t = time of electrolysis (sec)
n = number of electrons per mole of product formed
F = Faraday's number (F = 96 485 C/mol)
ŋF = Faraday efficiency is the ratio between the actual value
and the maximum theoretical amount of hydrogen produced in
the electrolysis. The faradic efficiency can be calculated as:
2
5.7509.0
5.96 II
F (16)
.
)( I
L
B
B
m
4. In a PV system, the output power depends on the weather
conditions (rapidly changing), then, it would not be wise to
use directly the quantity of water to be electrolyzed. Our
approach focuses on the flow of water introduced into the
electrolysis taking into account the quickly changing
conditions. In previous work [17], we have shown that the
flow of hydrogen produced can be expressed in the form:
n.F
nM
t
m
m FcH
H
....I
.
2
2
(17)
According to “(4)“ .The amount of hydrogen produced is
given by the following relationship:
.
2
92
OH
H
m
m (18)
We posing
.
.9
.
M
Fn
C
.The amount of hydrogen produced is
given by the following relationship:
F
c
OH
C
nI
m .
.
.
2
(19)
In addition, the electric power P available for ectrolyzing
according to the scheme of "Fig.1" is:
IVP .. (20)
Using “(19)”, “(20)”.
F
c
OH
VC
nP
m .
.
.
.
2
(21)
This relation shows that the water flow is proportional to
the electrical power available. Hence the necessities to control
the water flow to be introduced into the electrolysis.
We have shown that the production of hydrogen is
proportional on one hand to the electrolysis current, and the
other hand to the water flow to be injected into the
electrolysis. Further water flow is proportional to the converter
output power “(17)” “(18)” “(21)”. A control system is
necessary for extracting the maximum photovoltaic power that
will lead undoubtedly to an optimized electrolysis operation
and consequently a maximum hydrogen production.
C. Maximum Power Point Tracking Converter
“Fig.6” shows the flowchart of the type of MPPT control
system developed in this work. This is a technical MPPT
based on P&O algorithm with a variable step size and an
acceleration mechanism [18]. This algorithm is in charge to
find a simple and effective way to improve the accuracy of the
place of maximum power point MPP, and the acceleration of
the system to quickly reach this point. This technique also
adjusts the optimum voltage of the PV panel to the cell voltage
of the electrolysis.
III. EVALUATION OF SIMULATION RESULTS
We simulated the production of hydrogen by a
photovoltaic system using a Buck power converter controlled
by the aforementioned MPPT control and supplying PEM
electrolysis.
The modelization and sizing of PEM electrolysis is made
exactly in a manner to consume all the power produced by the
PV system.
The complete diagram of the PV-electrolysis system is
shown in “Fig.7”.The assembly simulation is conducted in the
Matlab/Simulink. Modeling physical components of PV is
made by the Simscape language and modeling of the digital
part is done by the S-Function CMEX tool using the
programming language C.
Figure 6. Flowchart of the P&O algorithm with a variable step size and an
acceleration mechanism
The solar radiation signal input from the photovoltaic
generator is shown in “Fig.8”. The buck converter equipped
with MPPT control, extracts the maximum power and the
current of photovoltaic module “Fig.9” and “Fig.10” and
transfers them to the electrolysis for:
Control the water mass flow to be injected into the
electrolysis
To produce the maximum amount of hydrogen in the
form of mass flow depending on the sunlight.
5. Figure 7. Modeling of photovoltaic-electrolysis system in Matlab/Simulink
Figure 8. Solar irradiance
Figure 9 . Output power of the PV panel transferred to the electrolysis
The "Fig.11" and "Fig.12" represent the results of
simulations of the water mass flow injected into the
electrolyzer and the mass flow of hydrogen produced during
the different phases of solar radiation. We simulated these two
quantities in a direct coupling of the PV module to the
electrolysis, but also during the coupling of the two systems
by introducing the DC-DC power converter equipped with its
control algorithm (indirect coupling). It appears that:
The water flow follows the variation of the power extracted
from the PV panel following variations illumination. This
proves that the water flow to be introduced into the
electrolysis depends only on the power provided by the
photovoltaic source PV and afterwards of sunlight.
Furthermore by:
The flow of hydrogen produced simultaneously tracks
the water flow; it confirms the importance of
controlling the flow of water injected into the
electrolysis for maximum hydrogen production.
The quantity of water injected into the electrolysis is
most important during the indirect coupling than to
direct coupling with an equal amount of radiation.
Note then, by adopting the process of producing hydrogen
using the PV module, the electrolysis, the DC-DC converter
and controlling the amount of water is obtained a significant
improvement in overall system performance. This
improvement concerns first of maximizing the power supplied
by the PV module, and eventually an increase in the
production of hydrogen through of the water flow control
injected into the electrolysis. This leads to optimum operation
of the electrolysis and therefore a higher production of
hydrogen compared to a direct coupling.
Figure 10. Output current of the PV panel transferred to the electrolysis
6. Figure 11 . Water flow injected into the PEM electrolysis with and without
controlled DC/DC.
Figure 12 . Hydrogen flow produced by the PEM electrolysis with and
without DC/DC controlled
VI. CONCLUSION
In this work, we presented the modeling of various
components of the PV-electrolysis system (PEM electrolysis,
PV, DC/DC buck converter). We have given particular
attention to the electrical modeling of chemical phenomena
that occur in electrolysis for integrated it in an electrical
environment. So we introduced between the PV module and
the electrolysis a DC-DC buck converter type with a digital
control algorithm to prosecute the maximum power (MPPT),
and ensuring the transfer of this power to electrolysis in order
to produce hydrogen.
Simulation results show that the coupling between the
PEM water electrolysis and the PV panel via a DC/DC buck
converter, controlled by an MPPT algorithm and a water flow
controller in the electrolysis, leads to an improvement on
maximization of the power drawn from the PV module on one
hand, and on the other hand maximizing the amount of
hydrogen produced in the electrolysis. This has the effect an
overall improvement in hydrogen production system designed.
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