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International Journal of Electrical and Computer Engineering (IJECE)
Vol. 10, No. 4, August 2020, pp. 3384~3392
ISSN: 2088-8708, DOI: 10.11591/ijece.v10i4.pp3384-3392  3384
Journal homepage: http://ijece.iaescore.com/index.php/IJECE
A comparison of single phase standalone square waveform solar
inverter topologies: Half bridge and full bridge
Aicha Chemseddine1
, Noureddine Benabadji 2
, Ali Cheknane3
, Salah Eddine Mankour4
1,2
Laboratory of Analysis and Application of Radiation,
University of Science and Technology Mohamed Boudiaf, Algeria
3
Laboratory of Semiconductor and Functional Materials, Amar Tlidji University, Algeria
4
Department of Electrical Engineering, University of Science and Technology Mohamed Boudiaf, Algeria
Article Info ABSTRACT
Article history:
Received Apr 10, 2019
Revised Jan 12, 2020
Accepted Feb 2, 2020
In stand-alone photovoltaic installations the photovoltaic inverter allows
transforming the DC power produced by the photovoltaic modules into an
AC power. Depending on the shape of the AC output voltage generated by
the inverter there exist three main types of stand-alone PV inverters: pure
sine waveform inverters, modulated sine waveform inverters and square
waveform inverters and each type of these inverters is also divided into
different topologies. In this paper we will be interested and study the square
waveform stand-alone inverter topologies which are the half bridge and
the full bridge inverter topologies.
Keywords:
Boost converer
Full bridge inverter
Half bridge inverter
Photovoltaic inverter
Stand-alone installation Copyright © 2020 Institute of Advanced Engineering and Science.
All rights reserved.
Corresponding Author:
Aicha Chemseddine,
Département de Physique,
Laboratoire d’analyse et d’application des rayonnements (LAAR),
Université des Sciences et de la Technologie d’Oran Mohamed Boudiaf,
BP 1505, El M’naouer, 31000 Oran Algérie.
Email: aicha.chemseddine@univ-usto.dz
1. INTRODUCTION
With the revolution and the advance of the use of photovoltaic installations all around the word,
many designs and conceptions of photovoltaic devices have been developed [1-3], especially the conception
and the design of DC-DC and DC-AC converters circuits [4-6]. Because of the low efficiency and the high
cost of solar modules in photovoltaic systems [7], the effiecicy and the cicuits simplicity of the other devices
of photovoltaic system have to be the most higher possible. A Stand-alone photovoltaic installation is an off
grid installation, in which the photovoltaic modules are the only source that generates the electric power to
feed a DC or an AC load [8]. Photovoltaic modules generate a DC electric power thus to feed an AC load in
stand-alone photovoltaic installation a stand-alone photovoltaic inverter has to be used to convert the DC
power produced by the photovoltaic modules into an AC power [9-12].
Depending on the shape of the AC output voltage generated by the inverter there exist three main
types of single phase stand-alone photovoltaic inverters: pure sinewaveform inverters, modulated waveform
inverters and square waveform inverters [13-15] and each type of these inverters is also divided into different
topologies: half bridge and full bridge for the square waveform inverters and multilevel (bridges) for
the modulated waveform and the pure sinewave inverters. Square waveform inverters are designed to feed
loads which have an important inductance [6] as motors because inductive loads allow having relatively pure
sinewave current. Looking for the most efficient and the simplest cicuit design of stand alone single phase
solar inveter to feed AC motors and inductive loads, in this paper we will be interested by the square
waveform single phase inverters doing a comparative study of the efficiency and the simplicity between
the half bridge and full bridge topologies simulating them on ISIS Proteus software.
Int J Elec & Comp Eng ISSN: 2088-8708 
A comparison of single phase standalone square waveform… (Aicha Chemseddine)
3385
2. HALF BRIDGE SQUARE WAVEFORM SOLAR INVERTER CIRCUIT
Figure 1 presents a single phase half bridge square waveform photovoltaicinverter which is
composed of two stages: dc-dc and dc-ac stage. The dc-dc stage is a boost converter which is used to convert
the low voltages produced by the PV modules (12-24V) into V 440 to have an RMS voltage value equal to
220V by the half bridge inverter. The output of the boost converter is connected in parallel with tow
capacitors dividers to get 𝑉𝑜𝑢𝑡 = 𝑉𝑏 2⁄ when :𝑆2 is on and 𝑆3 is off and get 𝑉𝑜𝑢𝑡 = − 𝑉𝑏 2⁄ when 𝑆3 is on and
𝑆2 is off [16-20]. The swiches of this topology would be driven by simple square pulses.
Figure 1. Single phase half bridge square waveform inverter stages
3. FULL BRIDGE SQUARE WAVEFORM SOLARINVERTER CIRCUIT
Figure 2 presents a single phase full bridge square waveform solar inverter which is also composed
of two stages as the half bridge one: a dc-dc and a dc-ac stage. The dc-dc stage is a boost converter which is
used to convert the low voltages produced by the PV modules (12-24V) into a Vdc equal to 220 to have an
RMS voltage value equal to 220V by the full bridge inverter. The output of the boost converter is connected
in parallel with two legs and each leg is composed of two inverting switches connected in series. The output
voltage of the inverter equal to 𝑉𝑏 when𝑆2 and 𝑆5 are on and 𝑆3 and 𝑆4 are off and equal to −𝑉𝑏 when 𝑆3 and
𝑆4 are on and 𝑆2 and 𝑆5 are off [21-25]. The swiches would be driven by simple square pulses.
Figure 2. Single phase half bridge square waveform inverter stages
4. DESIGN OF THE BOOST CONVERTER
Figure 3 shows the basic configuration of a boost converter, its composed of an inductor, a switch:
IGBT or a MOSFET transistor, a diode and a capacitor. In this part of the paper we will presents how to size
and calculate the parameters of each one of its components which depend on the output voltage
and current [26-28].
 ISSN: 2088-8708
Int J Elec & Comp Eng, Vol. 10, No. 4, August 2020 : 3384 - 3392
3386
Figure 3. The boost converter power stage [26].
4.1. Duty cycle
𝐷 = 1 −
𝑉𝐼𝑁
𝑉𝑂𝑈𝑇
× 𝜂 (1)
Where,
𝑉𝐼𝑁: Is the voltage coming from the PV module which is equal to 12V or 24V.
𝑉𝑂𝑈𝑇: Is the desired voltage 220 for the full bridge inverter and 440V for the half bridge one.
𝜂: The inverter efficiency.
4.2. Inductor selection
Equation 2 [26] presents a good estimation for the right inductor:
𝐿 =
𝑉𝐼𝑁 × (𝑉𝑂𝑈𝑇 − 𝑉𝐼𝑁)
Δ𝑙𝑙 × 𝑓𝑆 × 𝑉𝑂𝑈𝑇
(2)
Where,
Δ𝑙𝑙: The estimated inductor ripple current, a good estimation for the inductor ripple current is 20% to 40% of
the output current.
𝑓𝑆: Minimum switching frequency of the converter.
4.3. Inductor ripple current
The inductor ripple current is calculated by the expression [26]:
Δ𝑙𝑙 = (0.2 𝑡𝑜 0.4) × 𝐼 𝑂𝑈𝑇(𝑀𝐴𝑋) (3)
Where,
𝐼 𝑂𝑈𝑇(𝑀𝐴𝑋): The maximum output current.
4.4. Output capacitor selection
Capacitors are used to minimize the ripple on the output voltage. The following equation can be
used to adjust the output capacitor values for a desired output voltage ripple [26]:
𝐶 𝑂𝑈𝑇(𝑀𝐼𝑁) =
𝐼 𝑂𝑈𝑇(𝑀𝐴𝑋) × 𝐷
𝑓𝑆 × Δ𝑉𝑂𝑈𝑇
(4)
5. SIMULATION PROCEDURES
In this part two stand-alone square waveform inverters topologies have been simulated on ISIS
Proteus software: a half and a full bridge inverter. Each one of them has been designed to deliver an output
power equal to 1000 wat and an output voltage equal to 220V with 50HZ of frequency. The PWMs used to
control the circuit switches have been generated and controlled by the PIC 16F877A.
Int J Elec & Comp Eng ISSN: 2088-8708 
A comparison of single phase standalone square waveform… (Aicha Chemseddine)
3387
5.1. The half bridge inverter circuit description
This inverter is composed of two stages: a dc-dc and a dc-ac stage as shown in Figure 4. The dc-dc
stage Figure 5 is a boost converter that converts the panel voltage Vp=24V into Vb=440V. An IGBT
(IRG4PC50S) is used as a switch controlled by the PIC 16F877A and the IR211 driver. The output of
the boost converter is connected in parallel with tow capacitors connected in series and a leg of two IGBTs
(IRG4PC50KD) connected also in seriesto get an output voltage Vo= Vb/2=220V when t=T/2 and
Vo=-Vb/2=-220 when t=T Figure 6. Table 1 presents the boost parameters, they were determined using
the (1-4).
Figure 4. The boost simulated circuit of the half bridge inverter
 ISSN: 2088-8708
Int J Elec & Comp Eng, Vol. 10, No. 4, August 2020 : 3384 - 3392
3388
Figure 5. The haf bridge inverter simulated circuit
HIN
10
LIN
12
VB
6
HO
7
VS
5
LO
1
COM
2
SD
11
VC
3 U10
IR2112
D11(A)
R10
10
D14
1N4007G
D11
1N4007G C12
470nC10
47u
D1
1N4007G
B1
24V
L1
49mH
C1
161u
b
Q5
IRG4PC50KD
Q20
IRG4PC50KD
HIN
10
LIN
12
VB
6
HO
7
VS
5
LO
1
COM
2
SD
11
VC
3 U1
IR2112
C100
10u
C2
470n
D10(A)
D10
1N4007G
R1
33
R20
33
U30
NOT
b
U3
AND
U5
AND
RA0/AN0
2
RA1/AN1
3
RA2/AN2/VREF-/CVREF
4
RA4/T0CKI/C1OUT
6
RA5/AN4/SS/C2OUT
7
RE0/AN5/RD
8
RE1/AN6/WR
9
RE2/AN7/CS
10
OSC1/CLKIN
13
OSC2/CLKOUT
14
RC1/T1OSI/CCP2
16
RC2/CCP1
17
RC3/SCK/SCL
18
RD0/PSP0
19
RD1/PSP1
20
RB7/PGD
40
RB6/PGC
39
RB5
38
RB4
37
RB3/PGM
36
RB2
35
RB1
34
RB0/INT
33
RD7/PSP7
30
RD6/PSP6
29
RD5/PSP5
28
RD4/PSP4
27
RD3/PSP3
22
RD2/PSP2
21
RC7/RX/DT
26
RC6/TX/CK
25
RC5/SDO
24
RC4/SDI/SDA
23
RA3/AN3/VREF+
5
RC0/T1OSO/T1CKI
15
MCLR/Vpp/THV
1
U2
PIC16F877A
+88.8
Volts
d1
d2
U30(D)
R2
194
A
B
C
D
Q1
IRG4PC50S
U10(LIN)
C3
100u
C4
100u
Int J Elec & Comp Eng ISSN: 2088-8708 
A comparison of single phase standalone square waveform… (Aicha Chemseddine)
3389
Figure 6. Theoutput voltageofthe half bridge inverter
Table 1. Boost converter parameters of the half bridge inverter
Parameters Symbol Value
Duty cycle D 0.94
Minimum switching frequency of the converter
Sf 1kHz
Desired inductor ripple current (20% of the output current) Δ𝑙 𝐿 0.454
Desired output voltage ripple (3% of output voltage) Δ𝑉𝑂𝑈𝑇 13.2V
Maximum output current (𝑉𝑂𝑈𝑇 𝑅⁄ ) 𝐼 𝑂𝑈𝑇 2.27A
5.2. The full bridge inverter circuit description
This inverter is also composed of two stages: a dc-dc and a dc-ac as shown in Figure 7 .The dc-dc
stage Figure 8 is a boost converter that converts the panel voltage Vp=24V into Vb=220V. An IGBT
(IRG4PC50S) is used as a switch controlled by the IR211 driver. The output of the boost converter is
connected in parallel with two capacitors in series and two legs, each leg contains two IGBTs
(IRG4PC50KD) in series to give an output voltage Vo=(+Vb/2+Vb/2=+Vb=220V) when t=T/2 and
Vo=(-Vb/2-Vb/2=-Vb=-220V) when t=T. Table 2 presents the Boost converter parameters of the full bridge
inverter.
Figure 7. The boost simulated circuit of the full bridge inverter
HIN
10
LIN
12
VB
6
HO
7
VS
5
LO
1
COM
2
SD
11
VC
3 U10
IR2112
D11(A)
R10
10
D14
1N4007G
D11
1N4007G C12
470nC10
47u
B1
24V
L1
11.7mH
C1
0.6m
b
Volts
+200
U30(D)
U10(LIN)
Q1
IRG4PC50S
D1
1N4007G
 ISSN: 2088-8708
Int J Elec & Comp Eng, Vol. 10, No. 4, August 2020 : 3384 - 3392
3390
Figure 8. The full bridge inverter simulated circuit
Table 2. Boost converter parameters of the full bridge inverter
Parameters Symbol Value
Duty cycle D 0.89
Minimum switching frequency of the converter Sf 1kHz
Desired inductor ripple current (20% of the output current) Δ𝑙 𝐿 0.908
Desired output voltage ripple (3% of output voltage) Δ𝑉𝑂𝑈𝑇 6.6V
Maximum output current (𝑉𝑂𝑈𝑇 𝑅⁄ ) 𝐼 𝑂𝑈𝑇 4.54A
6. SIMULATION RESUTS AND COMPARISON
As presented in Figues 4 and 7, the output voltages of boost converters are different: 220V for
the one used in the full bridge inverter and 440V for that one used in the half bridge inverter that make
theircomponents parameters different using the same switching frequency and the input voltage, the main
differences between the two inverters cited in the points below indicate that the half bridge inverter has less
conduction losses than the full bridge inverter , due to the high output voltage of its boost converter, whereas,
this high voltage could makes a risk on operators and the system, that leads to the use of an important
isolation. Also the half bridge inverter has a simpler circuit design than the full bridge inverter wich reduces
the cost and the time of asemblage
6.1. Desired output voltage ripple
As shown in Figures 9 and 10 the output voltage ripple of the boost converter used in half bridge
inverter is more important than that of full bridge output voltage ripple they are the double because 3% of
220V equal to 6.6 and 3% of 440V equal to 13.2.
HIN
10
LIN
12
VB
6
HO
7
VS
5
LO
1
COM
2
SD
11
VC
3 U10
IR2112
D11(A)
R10
10
D14
1N4007G
D11
1N4007G C12
470nC10
47u
B1
24V
L1
11.7mH
C1
0.6m
b
Q5
IRG4PC50KD
Q20
IRG4PC50KD
HIN
10
LIN
12
VB
6
HO
7
VS
5
LO
1
COM
2
SD
11
VC
3 U1
IR2112
C100
10u
C2
470n
D10(A)
D10
1N4007G
R1
33
R20
33
U30
NOT
Q3
IRG4PC50KD
Q4
IRG4PC50KD
HIN
10
LIN
12
VB
6
HO
7
VS
5
LO
1
COM
2
SD
11
VC
3 U4
IR2112
C3
10u
C4
470n
D2(A)
D2
1N4007G
R3
33
R4
33
U6
NOT
b
U30(D)
U6(D)
R2
49
U10(LIN)
Q1
IRG4PC50S
D1
1N4007G
A
B
C
D
C5
100u
C6
100u
Int J Elec & Comp Eng ISSN: 2088-8708 
A comparison of single phase standalone square waveform… (Aicha Chemseddine)
3391
Figure 9.The boost converter output voltage used in the half bridge inverter
Figure 10.The boost converter output voltage used in the full bridge inverter
6.2. The output voltage in the half bridge inverter
As has been sized, the boost converter of the half bridge inverter has to deliver an output voltage
equal to 440V this high voltage could be a risk on operators and the system which leads to the use of an
important isolation, however,the advantage of this topology voltage is to reduce the current following
the IGBTs into the half and by consequently the conduction losses in the IGBTs with 50% (200% less than
that in the IGBTs of the full bridge inverter).
6.3. Duty cycle and conduction losses
As presented in Tables 1 and 2 the duty cycle of the boost used in the half bridge inverter topology
is higher than that used in the full bridge topology with 5 % (10 % higher than a full bridge inverter) that
enhances the conduction losses in the IGBT with the same amount, because the conduction losses are present
during the period of the duty cycle [15, 19].
6.4. The boost inductor and output capacitor
As shown in Table 1, the boost converter used in the full bridge inverter topology has a higher
capacitor capacitancethan that one used in the half bridge inverter topology but the contrary for the inductor
inductance: the boost converter used in the half bridge inverter has a higher inductor inductance than that one
of the full bridge converter.
6.5. The component number
The full bridge inverter contains more components than the half bridge inverter due to the presence
of one more leg of switches which makes its circuit more complex. Also the production cost of the full bridge
inverter is higher than that of half bridge inverter because of the time and the effort of the assemblage.
6. CONCLUSION
In this paper a comparative study between tow topologies of stand-alone square waveform
photovoltaic inverters has been done, simulating them on ISIS Proteus software. This study shows that
the pefomance and the simplicity of half bridge inverter are higher than those of full bidge inveter wich make
it the best solution in stand alone photovoltaic insallations that feed inductive loads and motors.
 ISSN: 2088-8708
Int J Elec & Comp Eng, Vol. 10, No. 4, August 2020 : 3384 - 3392
3392
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A comparison of single phase standalone square waveform solar inverter topologies: Half bridge and full bridge

  • 1. International Journal of Electrical and Computer Engineering (IJECE) Vol. 10, No. 4, August 2020, pp. 3384~3392 ISSN: 2088-8708, DOI: 10.11591/ijece.v10i4.pp3384-3392  3384 Journal homepage: http://ijece.iaescore.com/index.php/IJECE A comparison of single phase standalone square waveform solar inverter topologies: Half bridge and full bridge Aicha Chemseddine1 , Noureddine Benabadji 2 , Ali Cheknane3 , Salah Eddine Mankour4 1,2 Laboratory of Analysis and Application of Radiation, University of Science and Technology Mohamed Boudiaf, Algeria 3 Laboratory of Semiconductor and Functional Materials, Amar Tlidji University, Algeria 4 Department of Electrical Engineering, University of Science and Technology Mohamed Boudiaf, Algeria Article Info ABSTRACT Article history: Received Apr 10, 2019 Revised Jan 12, 2020 Accepted Feb 2, 2020 In stand-alone photovoltaic installations the photovoltaic inverter allows transforming the DC power produced by the photovoltaic modules into an AC power. Depending on the shape of the AC output voltage generated by the inverter there exist three main types of stand-alone PV inverters: pure sine waveform inverters, modulated sine waveform inverters and square waveform inverters and each type of these inverters is also divided into different topologies. In this paper we will be interested and study the square waveform stand-alone inverter topologies which are the half bridge and the full bridge inverter topologies. Keywords: Boost converer Full bridge inverter Half bridge inverter Photovoltaic inverter Stand-alone installation Copyright © 2020 Institute of Advanced Engineering and Science. All rights reserved. Corresponding Author: Aicha Chemseddine, Département de Physique, Laboratoire d’analyse et d’application des rayonnements (LAAR), Université des Sciences et de la Technologie d’Oran Mohamed Boudiaf, BP 1505, El M’naouer, 31000 Oran Algérie. Email: aicha.chemseddine@univ-usto.dz 1. INTRODUCTION With the revolution and the advance of the use of photovoltaic installations all around the word, many designs and conceptions of photovoltaic devices have been developed [1-3], especially the conception and the design of DC-DC and DC-AC converters circuits [4-6]. Because of the low efficiency and the high cost of solar modules in photovoltaic systems [7], the effiecicy and the cicuits simplicity of the other devices of photovoltaic system have to be the most higher possible. A Stand-alone photovoltaic installation is an off grid installation, in which the photovoltaic modules are the only source that generates the electric power to feed a DC or an AC load [8]. Photovoltaic modules generate a DC electric power thus to feed an AC load in stand-alone photovoltaic installation a stand-alone photovoltaic inverter has to be used to convert the DC power produced by the photovoltaic modules into an AC power [9-12]. Depending on the shape of the AC output voltage generated by the inverter there exist three main types of single phase stand-alone photovoltaic inverters: pure sinewaveform inverters, modulated waveform inverters and square waveform inverters [13-15] and each type of these inverters is also divided into different topologies: half bridge and full bridge for the square waveform inverters and multilevel (bridges) for the modulated waveform and the pure sinewave inverters. Square waveform inverters are designed to feed loads which have an important inductance [6] as motors because inductive loads allow having relatively pure sinewave current. Looking for the most efficient and the simplest cicuit design of stand alone single phase solar inveter to feed AC motors and inductive loads, in this paper we will be interested by the square waveform single phase inverters doing a comparative study of the efficiency and the simplicity between the half bridge and full bridge topologies simulating them on ISIS Proteus software.
  • 2. Int J Elec & Comp Eng ISSN: 2088-8708  A comparison of single phase standalone square waveform… (Aicha Chemseddine) 3385 2. HALF BRIDGE SQUARE WAVEFORM SOLAR INVERTER CIRCUIT Figure 1 presents a single phase half bridge square waveform photovoltaicinverter which is composed of two stages: dc-dc and dc-ac stage. The dc-dc stage is a boost converter which is used to convert the low voltages produced by the PV modules (12-24V) into V 440 to have an RMS voltage value equal to 220V by the half bridge inverter. The output of the boost converter is connected in parallel with tow capacitors dividers to get 𝑉𝑜𝑢𝑡 = 𝑉𝑏 2⁄ when :𝑆2 is on and 𝑆3 is off and get 𝑉𝑜𝑢𝑡 = − 𝑉𝑏 2⁄ when 𝑆3 is on and 𝑆2 is off [16-20]. The swiches of this topology would be driven by simple square pulses. Figure 1. Single phase half bridge square waveform inverter stages 3. FULL BRIDGE SQUARE WAVEFORM SOLARINVERTER CIRCUIT Figure 2 presents a single phase full bridge square waveform solar inverter which is also composed of two stages as the half bridge one: a dc-dc and a dc-ac stage. The dc-dc stage is a boost converter which is used to convert the low voltages produced by the PV modules (12-24V) into a Vdc equal to 220 to have an RMS voltage value equal to 220V by the full bridge inverter. The output of the boost converter is connected in parallel with two legs and each leg is composed of two inverting switches connected in series. The output voltage of the inverter equal to 𝑉𝑏 when𝑆2 and 𝑆5 are on and 𝑆3 and 𝑆4 are off and equal to −𝑉𝑏 when 𝑆3 and 𝑆4 are on and 𝑆2 and 𝑆5 are off [21-25]. The swiches would be driven by simple square pulses. Figure 2. Single phase half bridge square waveform inverter stages 4. DESIGN OF THE BOOST CONVERTER Figure 3 shows the basic configuration of a boost converter, its composed of an inductor, a switch: IGBT or a MOSFET transistor, a diode and a capacitor. In this part of the paper we will presents how to size and calculate the parameters of each one of its components which depend on the output voltage and current [26-28].
  • 3.  ISSN: 2088-8708 Int J Elec & Comp Eng, Vol. 10, No. 4, August 2020 : 3384 - 3392 3386 Figure 3. The boost converter power stage [26]. 4.1. Duty cycle 𝐷 = 1 − 𝑉𝐼𝑁 𝑉𝑂𝑈𝑇 × 𝜂 (1) Where, 𝑉𝐼𝑁: Is the voltage coming from the PV module which is equal to 12V or 24V. 𝑉𝑂𝑈𝑇: Is the desired voltage 220 for the full bridge inverter and 440V for the half bridge one. 𝜂: The inverter efficiency. 4.2. Inductor selection Equation 2 [26] presents a good estimation for the right inductor: 𝐿 = 𝑉𝐼𝑁 × (𝑉𝑂𝑈𝑇 − 𝑉𝐼𝑁) Δ𝑙𝑙 × 𝑓𝑆 × 𝑉𝑂𝑈𝑇 (2) Where, Δ𝑙𝑙: The estimated inductor ripple current, a good estimation for the inductor ripple current is 20% to 40% of the output current. 𝑓𝑆: Minimum switching frequency of the converter. 4.3. Inductor ripple current The inductor ripple current is calculated by the expression [26]: Δ𝑙𝑙 = (0.2 𝑡𝑜 0.4) × 𝐼 𝑂𝑈𝑇(𝑀𝐴𝑋) (3) Where, 𝐼 𝑂𝑈𝑇(𝑀𝐴𝑋): The maximum output current. 4.4. Output capacitor selection Capacitors are used to minimize the ripple on the output voltage. The following equation can be used to adjust the output capacitor values for a desired output voltage ripple [26]: 𝐶 𝑂𝑈𝑇(𝑀𝐼𝑁) = 𝐼 𝑂𝑈𝑇(𝑀𝐴𝑋) × 𝐷 𝑓𝑆 × Δ𝑉𝑂𝑈𝑇 (4) 5. SIMULATION PROCEDURES In this part two stand-alone square waveform inverters topologies have been simulated on ISIS Proteus software: a half and a full bridge inverter. Each one of them has been designed to deliver an output power equal to 1000 wat and an output voltage equal to 220V with 50HZ of frequency. The PWMs used to control the circuit switches have been generated and controlled by the PIC 16F877A.
  • 4. Int J Elec & Comp Eng ISSN: 2088-8708  A comparison of single phase standalone square waveform… (Aicha Chemseddine) 3387 5.1. The half bridge inverter circuit description This inverter is composed of two stages: a dc-dc and a dc-ac stage as shown in Figure 4. The dc-dc stage Figure 5 is a boost converter that converts the panel voltage Vp=24V into Vb=440V. An IGBT (IRG4PC50S) is used as a switch controlled by the PIC 16F877A and the IR211 driver. The output of the boost converter is connected in parallel with tow capacitors connected in series and a leg of two IGBTs (IRG4PC50KD) connected also in seriesto get an output voltage Vo= Vb/2=220V when t=T/2 and Vo=-Vb/2=-220 when t=T Figure 6. Table 1 presents the boost parameters, they were determined using the (1-4). Figure 4. The boost simulated circuit of the half bridge inverter
  • 5.  ISSN: 2088-8708 Int J Elec & Comp Eng, Vol. 10, No. 4, August 2020 : 3384 - 3392 3388 Figure 5. The haf bridge inverter simulated circuit HIN 10 LIN 12 VB 6 HO 7 VS 5 LO 1 COM 2 SD 11 VC 3 U10 IR2112 D11(A) R10 10 D14 1N4007G D11 1N4007G C12 470nC10 47u D1 1N4007G B1 24V L1 49mH C1 161u b Q5 IRG4PC50KD Q20 IRG4PC50KD HIN 10 LIN 12 VB 6 HO 7 VS 5 LO 1 COM 2 SD 11 VC 3 U1 IR2112 C100 10u C2 470n D10(A) D10 1N4007G R1 33 R20 33 U30 NOT b U3 AND U5 AND RA0/AN0 2 RA1/AN1 3 RA2/AN2/VREF-/CVREF 4 RA4/T0CKI/C1OUT 6 RA5/AN4/SS/C2OUT 7 RE0/AN5/RD 8 RE1/AN6/WR 9 RE2/AN7/CS 10 OSC1/CLKIN 13 OSC2/CLKOUT 14 RC1/T1OSI/CCP2 16 RC2/CCP1 17 RC3/SCK/SCL 18 RD0/PSP0 19 RD1/PSP1 20 RB7/PGD 40 RB6/PGC 39 RB5 38 RB4 37 RB3/PGM 36 RB2 35 RB1 34 RB0/INT 33 RD7/PSP7 30 RD6/PSP6 29 RD5/PSP5 28 RD4/PSP4 27 RD3/PSP3 22 RD2/PSP2 21 RC7/RX/DT 26 RC6/TX/CK 25 RC5/SDO 24 RC4/SDI/SDA 23 RA3/AN3/VREF+ 5 RC0/T1OSO/T1CKI 15 MCLR/Vpp/THV 1 U2 PIC16F877A +88.8 Volts d1 d2 U30(D) R2 194 A B C D Q1 IRG4PC50S U10(LIN) C3 100u C4 100u
  • 6. Int J Elec & Comp Eng ISSN: 2088-8708  A comparison of single phase standalone square waveform… (Aicha Chemseddine) 3389 Figure 6. Theoutput voltageofthe half bridge inverter Table 1. Boost converter parameters of the half bridge inverter Parameters Symbol Value Duty cycle D 0.94 Minimum switching frequency of the converter Sf 1kHz Desired inductor ripple current (20% of the output current) Δ𝑙 𝐿 0.454 Desired output voltage ripple (3% of output voltage) Δ𝑉𝑂𝑈𝑇 13.2V Maximum output current (𝑉𝑂𝑈𝑇 𝑅⁄ ) 𝐼 𝑂𝑈𝑇 2.27A 5.2. The full bridge inverter circuit description This inverter is also composed of two stages: a dc-dc and a dc-ac as shown in Figure 7 .The dc-dc stage Figure 8 is a boost converter that converts the panel voltage Vp=24V into Vb=220V. An IGBT (IRG4PC50S) is used as a switch controlled by the IR211 driver. The output of the boost converter is connected in parallel with two capacitors in series and two legs, each leg contains two IGBTs (IRG4PC50KD) in series to give an output voltage Vo=(+Vb/2+Vb/2=+Vb=220V) when t=T/2 and Vo=(-Vb/2-Vb/2=-Vb=-220V) when t=T. Table 2 presents the Boost converter parameters of the full bridge inverter. Figure 7. The boost simulated circuit of the full bridge inverter HIN 10 LIN 12 VB 6 HO 7 VS 5 LO 1 COM 2 SD 11 VC 3 U10 IR2112 D11(A) R10 10 D14 1N4007G D11 1N4007G C12 470nC10 47u B1 24V L1 11.7mH C1 0.6m b Volts +200 U30(D) U10(LIN) Q1 IRG4PC50S D1 1N4007G
  • 7.  ISSN: 2088-8708 Int J Elec & Comp Eng, Vol. 10, No. 4, August 2020 : 3384 - 3392 3390 Figure 8. The full bridge inverter simulated circuit Table 2. Boost converter parameters of the full bridge inverter Parameters Symbol Value Duty cycle D 0.89 Minimum switching frequency of the converter Sf 1kHz Desired inductor ripple current (20% of the output current) Δ𝑙 𝐿 0.908 Desired output voltage ripple (3% of output voltage) Δ𝑉𝑂𝑈𝑇 6.6V Maximum output current (𝑉𝑂𝑈𝑇 𝑅⁄ ) 𝐼 𝑂𝑈𝑇 4.54A 6. SIMULATION RESUTS AND COMPARISON As presented in Figues 4 and 7, the output voltages of boost converters are different: 220V for the one used in the full bridge inverter and 440V for that one used in the half bridge inverter that make theircomponents parameters different using the same switching frequency and the input voltage, the main differences between the two inverters cited in the points below indicate that the half bridge inverter has less conduction losses than the full bridge inverter , due to the high output voltage of its boost converter, whereas, this high voltage could makes a risk on operators and the system, that leads to the use of an important isolation. Also the half bridge inverter has a simpler circuit design than the full bridge inverter wich reduces the cost and the time of asemblage 6.1. Desired output voltage ripple As shown in Figures 9 and 10 the output voltage ripple of the boost converter used in half bridge inverter is more important than that of full bridge output voltage ripple they are the double because 3% of 220V equal to 6.6 and 3% of 440V equal to 13.2. HIN 10 LIN 12 VB 6 HO 7 VS 5 LO 1 COM 2 SD 11 VC 3 U10 IR2112 D11(A) R10 10 D14 1N4007G D11 1N4007G C12 470nC10 47u B1 24V L1 11.7mH C1 0.6m b Q5 IRG4PC50KD Q20 IRG4PC50KD HIN 10 LIN 12 VB 6 HO 7 VS 5 LO 1 COM 2 SD 11 VC 3 U1 IR2112 C100 10u C2 470n D10(A) D10 1N4007G R1 33 R20 33 U30 NOT Q3 IRG4PC50KD Q4 IRG4PC50KD HIN 10 LIN 12 VB 6 HO 7 VS 5 LO 1 COM 2 SD 11 VC 3 U4 IR2112 C3 10u C4 470n D2(A) D2 1N4007G R3 33 R4 33 U6 NOT b U30(D) U6(D) R2 49 U10(LIN) Q1 IRG4PC50S D1 1N4007G A B C D C5 100u C6 100u
  • 8. Int J Elec & Comp Eng ISSN: 2088-8708  A comparison of single phase standalone square waveform… (Aicha Chemseddine) 3391 Figure 9.The boost converter output voltage used in the half bridge inverter Figure 10.The boost converter output voltage used in the full bridge inverter 6.2. The output voltage in the half bridge inverter As has been sized, the boost converter of the half bridge inverter has to deliver an output voltage equal to 440V this high voltage could be a risk on operators and the system which leads to the use of an important isolation, however,the advantage of this topology voltage is to reduce the current following the IGBTs into the half and by consequently the conduction losses in the IGBTs with 50% (200% less than that in the IGBTs of the full bridge inverter). 6.3. Duty cycle and conduction losses As presented in Tables 1 and 2 the duty cycle of the boost used in the half bridge inverter topology is higher than that used in the full bridge topology with 5 % (10 % higher than a full bridge inverter) that enhances the conduction losses in the IGBT with the same amount, because the conduction losses are present during the period of the duty cycle [15, 19]. 6.4. The boost inductor and output capacitor As shown in Table 1, the boost converter used in the full bridge inverter topology has a higher capacitor capacitancethan that one used in the half bridge inverter topology but the contrary for the inductor inductance: the boost converter used in the half bridge inverter has a higher inductor inductance than that one of the full bridge converter. 6.5. The component number The full bridge inverter contains more components than the half bridge inverter due to the presence of one more leg of switches which makes its circuit more complex. Also the production cost of the full bridge inverter is higher than that of half bridge inverter because of the time and the effort of the assemblage. 6. CONCLUSION In this paper a comparative study between tow topologies of stand-alone square waveform photovoltaic inverters has been done, simulating them on ISIS Proteus software. This study shows that the pefomance and the simplicity of half bridge inverter are higher than those of full bidge inveter wich make it the best solution in stand alone photovoltaic insallations that feed inductive loads and motors.
  • 9.  ISSN: 2088-8708 Int J Elec & Comp Eng, Vol. 10, No. 4, August 2020 : 3384 - 3392 3392 REFERENCES [1] A. Mezouari, et al., "A New Photovoltaic Energy Sharing System between Homes in Standalone Areas," Int. J. of Electrical and Computer. Engineering, vol. 8, no. 6, pp. 4855-4862, 2018. [2] H. Fathabadi, “Novel High Efficiency DC/DC Boost Converter for using in Photovoltaic Systems,” Solar Energy, vol. 125, pp. 22-31, 2016. [3] R. Palanisamy, et al., "Simulation of Various DC-DC Converters for Photovoltaic System," Int. J. of Electrical and Computer. Engineering, vol. 9, pp. 917-925, 2019. [4] J. Q. Wang, and J. X. Li, "Design and Experience of Grid-Connecting Photovoltaic Power System," IEEE International Conference on Sustainable Energy Technologies, pp. 607-610, 2008. [5] S. Shanmugasundaram, "Solar Based Z Source Inverter for High Power Application," Bulletin of Electrical Engineering and Informatics, vol. 6, no. 4, pp. 343-347, 2017. [6] Y. P. Siwakoti, and F. Blaabjerg. 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