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International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 07 Issue: 03 | Mar 2020 www.irjet.net p-ISSN: 2395-0072
© 2020, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 5516
CLOSED LOOP CONTROL OF NON ISOLATED POSITIVE OUTPUT BUCK
BOOST DC-DC CONVERTER
Rohini L.T1, Roshan Akthar G2, Pravin A3
1,2,3Student, Department of Electrical and Electronics Engineering, Rajalakshmi Engineering College,
Tamilnadu, India
---------------------------------------------------------------------***----------------------------------------------------------------------
Abstract –The closed loop control of a transformerless DC
to DC Buck Boost converter with positive output has been
achieved using Genetic Algorithm based PI controller for
which the tuning of controller parameters is done using
Integrated Time Absolute Error (ITAE).Though a widevariety
of converter topologies have been proposed earlier, their
applications are restricted due to limited voltage gain,
topological complexity, cost, volume and losses .Compared
with the traditional converters, the transformerless
converter’s voltage gain is high with non-inverted output.
Simulation, state space modelling, derivation of transfer
function and closed loop control will be performed to validate
the effectiveness of the transformerless DC to DC converter.
Key Words: DC to DC converter, PI controller, Genetic
algorithm, Closed loop control, Non isolated converter,
Transformerless converter, Positive output
1.INTRODUCTION
DC to DC converters are electronic circuits used for
converting voltage of DC supply from one level to another,
which may be higher or lower. They are used in a wide
variety of applications such as discharge lamp ballasts for
automobile headlamps, fuel-cell energy conversionsystems,
solar-cell energy conversion systems, and battery backup
systems for uninterruptible power supplies. Though a wide
variety of converter topologies have been proposed earlier,
their applications are restricted due to limited voltage gain,
topological complexity, cost, volume and losses .Compared
with the traditional converters, the transformerless
converter’s voltage gain is high with non-inverted output.
1.1 Literature Survey
In 1998, A.J. Forsyth and S.V.Mollov has clearly explained
the averaging and linearisation techniques used for state
space modelling andderivationoftransferfunctionofDC–DC
Converters. DC-DC Converters can beprovidedwithisolation
using transformersandreductionofswitchinglosseswiththe
help of resonant techniques or soft switching. The three
control methods namely Single loop control, Input voltage
feed forward control , and current mode control are
described with simulation block diagrams. The single loop
control produces control signal with the help of error signal
obtained by comparing output voltage with the reference
signal . Input voltage feed forward control directlysensesthe
voltage disturbances and provides the necessary correction.
The current mode control is based on feedback of inductor
current. These methods can be used for conventional DC-DC
converters and other similar complex systems like the
proposed model. Out of the three control methods, the
current mode control gives a better performance
comparatively in the case of source voltage disturbancesand
load transients. This article greatly aided in the case of
simulation, state space modelling and derivation of transfer
function to design a controller for the proposed model.
In 2008, Boris Axelrod, Yefim Berkovich have proposed
hybrid converters with few simple structures formed by
either two capacitors and two or threediodes/twoinductors
and two or three diodes with high step up/ step down
conversion voltage ratio. For high volage conversion ratio ,
extreme duty cycle is necessary which in turn affects
efficiency. Transformers are not used since it increases the
cost , losses and the volume. Cascade and quadratic
converters has their own disadvantages. Thus, simple
switching structures are defined which can be inserted in
classical buck, boost, buck-boost, cuk, sepic and zeta
converters. These new hybrid converters reduces weight,
size, cost , conduction losses and gives a better efficiency.
In 2009, Lung-Sheng Yang has proposed non isolated DC-
DC converters with high voltage gain without high duty cycle
which is limited due to the effect of power semiconductor
switches, diodes, inductors and capacitors. The converter
structure used is simple and the proposed DC-DC converters
uses the switched inductor technique, where two inductors
with same level of inductance are charged in parallel during
the switch-on period and are discharged in series during the
switch-off period, to get high step-up voltage gain without
high duty ratio.
In 2011, K.I.HwuandW.C.Tuhaveproposedthreetypesof
converters in order to achieve high voltage conversionratios
by pumping the energy stored in inductors and capacitors
with the input voltage into output during off mode. These
three converters have been addressed on the basis of circuit
connection and control strategy. They are suitable for
industrial applications as they providegood steady stateand
transient performances .Voltage stress are also reduced
comapared to traditional buck boost converters.
In 2011,Wuhua Li has summarised the converter
topologies for high step up, low cost and high efficiencyDCto
DC conversion as it is required for photovoltaic grid
connected power system due to shortage of fossil fuel and
modern world being energy saving conscious. It has been
concluded that non isolated high step up converters can be
preferred due to its low cost and improved efficiency.
Increasing voltage gain, reducing stressacrosstheswitchare
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 07 Issue: 03 | Mar 2020 www.irjet.net p-ISSN: 2395-0072
© 2020, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 5517
some of the challenges faced by non isolated high step up
converters . Thesechallengeswillbeovercomeinthisproject.
1.2 Summary of Literature Survey
• Based on literature survey, a new transformerlessDCto
DC Buck Boost converter with positive output is to be
proposed.
• High voltage gain with required duty cycle , high
efficiency , less switching losses are to be achieved by facing
and overcoming the difficulties as stated by many
researches.
• Controller design andrealisationoftheconvertergreatly
depends on state space modelling and derivation of transfer
function.
1.3 Objectives
The main objectives are the following:
• To achieve high voltage gain with required duty cycle using
low cost, low weight, positive output Buck Boost converter
• Better efficiency compared to traditional converters
• Low conduction losses and switching losses compared to
traditional converters
2. CIRCUIT DIAGRAM
An additional switched network is added to the traditional
buck-boost converter in which the two power switches are
controlled synchronously. In the continuous conduction
mode, the inductors are energisedandcapacitors(i.e.charge
pump capacitor and output capacitor) are discharged when
the power switches are turned on. When they are turnedoff,
inductors are deenergised while the capacitors are charged.
2.1 Modes of operation
• On mode
• Off mode
2.1.1 On mode
In on mode i.e. during turn on period, the switches S1 and S2
are turned on.. The diodes D1 and D2 are reverse biased
during this period and does not conduct as their anodes are
at negative voltage compared to their cathodes.
The inductor L1 gets energised by thesupplyvoltageand the
current through the inductor increases from Imin to Imax
due to which diode D1 is reverse biased. L2 gets energised
by supply voltage and the charge pump capacitor C1 and the
current through the inductor increases from Imin to I max
due to which diode D2 is reverse biased. During this period,
the charge pump capacitor C1 getsdischargedenergisingthe
inductor L2 while output capacitor C0 gets discharged and
supplies the output voltage.
2.1.2 Off mode
In off mode i.e. during turn off period, the switchesS1and S2
are turned off. The diodes are forward biased during this
period and it conducts as their anodes are atpositivevoltage
compared to their cathodes. The inductors L1 and L2 get
deenergised. The current through the inductors L1 and L2
decreases from Imin and Imax due to which the diodes D1
and D0 are forward biased. The stored energy in the
inductors L1 charges the charge pump capacitor C1 via the
diode D1 whereas the stored energy in the inductor L2 is
released into the charge pump capacitor C1 , the output
capacitor C0 and the resistive load R via the diodes D1 and
D0. The switching operation of both the power
semiconductor switches are synchronised i.e. they are
turned on and off at the same time.
2.2 CALCULATION OF CONVERTER PARAMETERS
The converter parameters are calculated as follows:
Vin = 18 V, fS = 20KHz, R = 30 Ohm, D = 0.6
∆IL1 = 20% to 40% of IL1
Assume,
∆IL1 = 30% of IL1
IL1 =
Substituting the known values, we get,
IL1 = 0.995 A
∆IL1 = 30% of 0.995 = 0.299 A
L1 ≥
Substituting the known values, we get,
L1 ≥ 1.81Mh
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 07 Issue: 03 | Mar 2020 www.irjet.net p-ISSN: 2395-0072
© 2020, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 5518
∆IL2 = 20% to 40% of IL2
Assume,
∆IL2 = 30% of IL2
IL2 =
Substituting the known values, we get, IL2 = 3.38 A
∆IL2 = 30% of 0.995 = 1.01 A
L2 ≥
Substituting the known values, we get,
L2 ≥ 1.34mH
∆VC1 = 1% to 5% of VC1
Assume,
∆VC1 = 1% of VC1
VC1 =
Substituting the known values, we get,
VC1 = 27 V
∆VC1 = 1% of 27 = 0.27 V
C1 ≥
Here, V0 = VC0 = = 40.5 V
Substituting the known values, we get,
C1 ≥ 375µF
∆VC0= 1% of 40.5= 0.405 V
C0 ≥
Substituting the known values, we get,
C0 ≥ 100µF
3 OPEN LOOP SIMULATIONS
3.1 Without disturbance
Table 3.1 Simulation results without disturbance
PULSE WIDTH(%
OF PERIOD)
OUTPUT
VOLTAGE(V0)
(Theoretical)
OUTPUT
VOLTAGE(V0)
(Practical)
10 0.22 0.141
20 1.125 1.958
30 3.33 6.093
40 8.08 13.33
50 18 25.84
60 40.5 47.57
70 97.72 84.70
80 288 128.40
90 1458 131.80
3.2 With disturbance
Table 3.2 Simulation results with disturbance
PULSE WIDTH(%
OF PERIOD)
OUTPUT
VOLTAGE(V0)
(Theoretical)
OUTPUT
VOLTAGE(V0)
(Practical)
10 0.22 0.141
20 1.125 1.958
30 3.33 6.093
40 8.08 13.33
50 18 25.84
60 40.5 47.57
70 97.72 84.70
80 288 128.40
90 1458 131.80
3.1 Open loop simulation without
disturbance
3.2 Open loop simulation with disturbance
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 07 Issue: 03 | Mar 2020 www.irjet.net p-ISSN: 2395-0072
© 2020, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 5519
4. STATE SPACE MODELLING
IL1 ,IL2 , VC1 , VC1 are the state variables and Vin is the input
variable.
4.1 On mode
By applying Kirchoff’s voltage law and current law,
…………………….…....…. (1)
…………..………..… (2)
.......................................... (3)
………………………..... (4)
x’(t) = A1x(t) +B1u(t)
= +
y(t) = C1x(t) +D1u(t)
=
4.2 Off mode
By applying Kirchoff’s voltage law and current law,
…………….…………….…(5)
…………..….……….(6)
.......................................(7)
…..……………...……....(8)
x’(t) = A2x(t) +B2u(t)
= +
y(t) = C2x(t) +D2u(t)
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 07 Issue: 03 | Mar 2020 www.irjet.net p-ISSN: 2395-0072
© 2020, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 5520
=
5. DERIVATION OF TRANSFER FUNCTION
Input voltage=18 V, L1=1.81mH, L2=1.34mH,
C1=375 microFarad, C2=100 microFarad, R=30ohm,
d=0.6
A1 =
B1 =
C1 =
D1 =
A2 =
B2 =
C2 =
D2 =
A= A1d+A2(1-d)
A =
B= B1d+B2(1-d)
B =
C= C1d+C2(1-d)
C =
D= D1d+D2(1-d)
D =
Transfer function = C*[sI-A]^-1*B+D
The transfer function has been derived using matlab.
5.1 MATLAB program
A=[0 0 -220.996 0;0 0 149.252 -298.508;1066.668 -533.334
0 0;0 4000 0 333.331];
B=[331.494;447.762;0;0];
C=[0 0 0 1];
D=0;
sys=ss(A,B,C,D);
tf(sys)
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 07 Issue: 03 | Mar 2020 www.irjet.net p-ISSN: 2395-0072
© 2020, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 5521
5.2 Output
1.791e06 s^2 + 2.111e11
------------------------------------------------------
s^4 – 333.3s^3 + 1.35e06 s^2 – 5.204e07 s + 2.815e11
Continuous-time transfer function.
6.TUNINGOFPICONTROLLERPARAMETERSUSING
GENETIC ALGORITHM
Genetic Algorithm based PI controller is used forclosedloop
control of the proposed DC to DC converter for which the
tuning of controller parameters is done using Integrated
Time Absolute Error (ITAE).The stability analysis is done
using bode plot. The simulation of the closed loop control of
the proposed converter is used to obtain the desired output
and satisfactory performance.
6.1 MATLAB program
function [J] = pi_optim(x)
s = tf('s');
plant = (2667*s^2 + 4.268e07)/(s^4 + 0.668*s^3 +
8.667e04*s^2 + 5.077e04*s + 6.827e08);
Kp = x(1)
Ki = x(2)
cont = Kp + Ki/s ;
step(feedback(plant*cont,1));
dt = 0.01;
t = 0:dt:1;
e = 1 - step(feedback(plant*cont,1),t);
J = sum(t'.*abs(e)*dt);
6.2 Output
After 117 iterations, KP = 0.8838 and KI = 0.00008
7. STABILITY ANALYSIS
7.1 MATLAB program
syms s;
G=tf([1.76e06 2.111e11],[1 -333.3 1.35e06 -5.204e07
2.815e11]);
K=tf([0.8838 0.00008],[1 0]);
L=feedback(K*G,1);
pole(L)
bode(L),grid
8. CLOSED LOOP SIMULATION
By simulating the above model, the desired output is
obtained.
9. CONCLUSION
The simulation, state space modelling and derivation of
transfer function has been used to validate the effectiveness
of the proposed positiveoutputDC-DCBuck Boostconverter.
The state space modelling has been used to derivetheclosed
loop transfer function using MATLAB. The PI controller
parameters has been tuned by using Genetic Algorithm ( i.e.
Integrated Time Absolute Error function) in MATLAB. The
stability analysis and closed loop simulation has been used
to obtain satisfactory performance from the proposed
positive output DC-DC Buck Boost converter. This proposed
model will overcome the disadvantages of traditional
converters and is suitable for industrial applications.
REFERENCES
[1] K.I. Hwu W.C. Tu , “Voltage-boosting converters with
hybrid energy pumping “,Department of Electrical
Engineering, National Taipei University of Technology,
1, Sec. 3, Chung-Hsiao E. Rd., 2011
7.1 Bode plot ( closed loop – stable)
8.1 Closed loop simulation
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 07 Issue: 03 | Mar 2020 www.irjet.net p-ISSN: 2395-0072
© 2020, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 5522
[2] Wuhua Li, Member, IEEE, and Xiangning He, Fellow,
IEEEM, “Review of Nonisolated High-Step-Up DC/DC
Converters in Photovoltaic Grid-Connected
Applications” Mill Valley, CA: University Science, 1989.
[3] Lung-Sheng Yang, Tsorng-Juu Liang, Member, IEEE, and
Jiann-Fuh Chen,Member,IEEE,“TransformerlessDC–DC
Converters With High Step-Up Voltage Gain” , 2009
[4] F.L. Luo and H. Ye , “Positive output cascade boost
converters “ , 2004

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Exploring_Network_Security_with_JA3_by_Rakesh Seal.pptx
 

IRJET - Closed Loop Control of Non Isolated Positive Output Buck Boost DC-DC Converter

  • 1. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 07 Issue: 03 | Mar 2020 www.irjet.net p-ISSN: 2395-0072 © 2020, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 5516 CLOSED LOOP CONTROL OF NON ISOLATED POSITIVE OUTPUT BUCK BOOST DC-DC CONVERTER Rohini L.T1, Roshan Akthar G2, Pravin A3 1,2,3Student, Department of Electrical and Electronics Engineering, Rajalakshmi Engineering College, Tamilnadu, India ---------------------------------------------------------------------***---------------------------------------------------------------------- Abstract –The closed loop control of a transformerless DC to DC Buck Boost converter with positive output has been achieved using Genetic Algorithm based PI controller for which the tuning of controller parameters is done using Integrated Time Absolute Error (ITAE).Though a widevariety of converter topologies have been proposed earlier, their applications are restricted due to limited voltage gain, topological complexity, cost, volume and losses .Compared with the traditional converters, the transformerless converter’s voltage gain is high with non-inverted output. Simulation, state space modelling, derivation of transfer function and closed loop control will be performed to validate the effectiveness of the transformerless DC to DC converter. Key Words: DC to DC converter, PI controller, Genetic algorithm, Closed loop control, Non isolated converter, Transformerless converter, Positive output 1.INTRODUCTION DC to DC converters are electronic circuits used for converting voltage of DC supply from one level to another, which may be higher or lower. They are used in a wide variety of applications such as discharge lamp ballasts for automobile headlamps, fuel-cell energy conversionsystems, solar-cell energy conversion systems, and battery backup systems for uninterruptible power supplies. Though a wide variety of converter topologies have been proposed earlier, their applications are restricted due to limited voltage gain, topological complexity, cost, volume and losses .Compared with the traditional converters, the transformerless converter’s voltage gain is high with non-inverted output. 1.1 Literature Survey In 1998, A.J. Forsyth and S.V.Mollov has clearly explained the averaging and linearisation techniques used for state space modelling andderivationoftransferfunctionofDC–DC Converters. DC-DC Converters can beprovidedwithisolation using transformersandreductionofswitchinglosseswiththe help of resonant techniques or soft switching. The three control methods namely Single loop control, Input voltage feed forward control , and current mode control are described with simulation block diagrams. The single loop control produces control signal with the help of error signal obtained by comparing output voltage with the reference signal . Input voltage feed forward control directlysensesthe voltage disturbances and provides the necessary correction. The current mode control is based on feedback of inductor current. These methods can be used for conventional DC-DC converters and other similar complex systems like the proposed model. Out of the three control methods, the current mode control gives a better performance comparatively in the case of source voltage disturbancesand load transients. This article greatly aided in the case of simulation, state space modelling and derivation of transfer function to design a controller for the proposed model. In 2008, Boris Axelrod, Yefim Berkovich have proposed hybrid converters with few simple structures formed by either two capacitors and two or threediodes/twoinductors and two or three diodes with high step up/ step down conversion voltage ratio. For high volage conversion ratio , extreme duty cycle is necessary which in turn affects efficiency. Transformers are not used since it increases the cost , losses and the volume. Cascade and quadratic converters has their own disadvantages. Thus, simple switching structures are defined which can be inserted in classical buck, boost, buck-boost, cuk, sepic and zeta converters. These new hybrid converters reduces weight, size, cost , conduction losses and gives a better efficiency. In 2009, Lung-Sheng Yang has proposed non isolated DC- DC converters with high voltage gain without high duty cycle which is limited due to the effect of power semiconductor switches, diodes, inductors and capacitors. The converter structure used is simple and the proposed DC-DC converters uses the switched inductor technique, where two inductors with same level of inductance are charged in parallel during the switch-on period and are discharged in series during the switch-off period, to get high step-up voltage gain without high duty ratio. In 2011, K.I.HwuandW.C.Tuhaveproposedthreetypesof converters in order to achieve high voltage conversionratios by pumping the energy stored in inductors and capacitors with the input voltage into output during off mode. These three converters have been addressed on the basis of circuit connection and control strategy. They are suitable for industrial applications as they providegood steady stateand transient performances .Voltage stress are also reduced comapared to traditional buck boost converters. In 2011,Wuhua Li has summarised the converter topologies for high step up, low cost and high efficiencyDCto DC conversion as it is required for photovoltaic grid connected power system due to shortage of fossil fuel and modern world being energy saving conscious. It has been concluded that non isolated high step up converters can be preferred due to its low cost and improved efficiency. Increasing voltage gain, reducing stressacrosstheswitchare
  • 2. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 07 Issue: 03 | Mar 2020 www.irjet.net p-ISSN: 2395-0072 © 2020, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 5517 some of the challenges faced by non isolated high step up converters . Thesechallengeswillbeovercomeinthisproject. 1.2 Summary of Literature Survey • Based on literature survey, a new transformerlessDCto DC Buck Boost converter with positive output is to be proposed. • High voltage gain with required duty cycle , high efficiency , less switching losses are to be achieved by facing and overcoming the difficulties as stated by many researches. • Controller design andrealisationoftheconvertergreatly depends on state space modelling and derivation of transfer function. 1.3 Objectives The main objectives are the following: • To achieve high voltage gain with required duty cycle using low cost, low weight, positive output Buck Boost converter • Better efficiency compared to traditional converters • Low conduction losses and switching losses compared to traditional converters 2. CIRCUIT DIAGRAM An additional switched network is added to the traditional buck-boost converter in which the two power switches are controlled synchronously. In the continuous conduction mode, the inductors are energisedandcapacitors(i.e.charge pump capacitor and output capacitor) are discharged when the power switches are turned on. When they are turnedoff, inductors are deenergised while the capacitors are charged. 2.1 Modes of operation • On mode • Off mode 2.1.1 On mode In on mode i.e. during turn on period, the switches S1 and S2 are turned on.. The diodes D1 and D2 are reverse biased during this period and does not conduct as their anodes are at negative voltage compared to their cathodes. The inductor L1 gets energised by thesupplyvoltageand the current through the inductor increases from Imin to Imax due to which diode D1 is reverse biased. L2 gets energised by supply voltage and the charge pump capacitor C1 and the current through the inductor increases from Imin to I max due to which diode D2 is reverse biased. During this period, the charge pump capacitor C1 getsdischargedenergisingthe inductor L2 while output capacitor C0 gets discharged and supplies the output voltage. 2.1.2 Off mode In off mode i.e. during turn off period, the switchesS1and S2 are turned off. The diodes are forward biased during this period and it conducts as their anodes are atpositivevoltage compared to their cathodes. The inductors L1 and L2 get deenergised. The current through the inductors L1 and L2 decreases from Imin and Imax due to which the diodes D1 and D0 are forward biased. The stored energy in the inductors L1 charges the charge pump capacitor C1 via the diode D1 whereas the stored energy in the inductor L2 is released into the charge pump capacitor C1 , the output capacitor C0 and the resistive load R via the diodes D1 and D0. The switching operation of both the power semiconductor switches are synchronised i.e. they are turned on and off at the same time. 2.2 CALCULATION OF CONVERTER PARAMETERS The converter parameters are calculated as follows: Vin = 18 V, fS = 20KHz, R = 30 Ohm, D = 0.6 ∆IL1 = 20% to 40% of IL1 Assume, ∆IL1 = 30% of IL1 IL1 = Substituting the known values, we get, IL1 = 0.995 A ∆IL1 = 30% of 0.995 = 0.299 A L1 ≥ Substituting the known values, we get, L1 ≥ 1.81Mh
  • 3. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 07 Issue: 03 | Mar 2020 www.irjet.net p-ISSN: 2395-0072 © 2020, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 5518 ∆IL2 = 20% to 40% of IL2 Assume, ∆IL2 = 30% of IL2 IL2 = Substituting the known values, we get, IL2 = 3.38 A ∆IL2 = 30% of 0.995 = 1.01 A L2 ≥ Substituting the known values, we get, L2 ≥ 1.34mH ∆VC1 = 1% to 5% of VC1 Assume, ∆VC1 = 1% of VC1 VC1 = Substituting the known values, we get, VC1 = 27 V ∆VC1 = 1% of 27 = 0.27 V C1 ≥ Here, V0 = VC0 = = 40.5 V Substituting the known values, we get, C1 ≥ 375µF ∆VC0= 1% of 40.5= 0.405 V C0 ≥ Substituting the known values, we get, C0 ≥ 100µF 3 OPEN LOOP SIMULATIONS 3.1 Without disturbance Table 3.1 Simulation results without disturbance PULSE WIDTH(% OF PERIOD) OUTPUT VOLTAGE(V0) (Theoretical) OUTPUT VOLTAGE(V0) (Practical) 10 0.22 0.141 20 1.125 1.958 30 3.33 6.093 40 8.08 13.33 50 18 25.84 60 40.5 47.57 70 97.72 84.70 80 288 128.40 90 1458 131.80 3.2 With disturbance Table 3.2 Simulation results with disturbance PULSE WIDTH(% OF PERIOD) OUTPUT VOLTAGE(V0) (Theoretical) OUTPUT VOLTAGE(V0) (Practical) 10 0.22 0.141 20 1.125 1.958 30 3.33 6.093 40 8.08 13.33 50 18 25.84 60 40.5 47.57 70 97.72 84.70 80 288 128.40 90 1458 131.80 3.1 Open loop simulation without disturbance 3.2 Open loop simulation with disturbance
  • 4. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 07 Issue: 03 | Mar 2020 www.irjet.net p-ISSN: 2395-0072 © 2020, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 5519 4. STATE SPACE MODELLING IL1 ,IL2 , VC1 , VC1 are the state variables and Vin is the input variable. 4.1 On mode By applying Kirchoff’s voltage law and current law, …………………….…....…. (1) …………..………..… (2) .......................................... (3) ………………………..... (4) x’(t) = A1x(t) +B1u(t) = + y(t) = C1x(t) +D1u(t) = 4.2 Off mode By applying Kirchoff’s voltage law and current law, …………….…………….…(5) …………..….……….(6) .......................................(7) …..……………...……....(8) x’(t) = A2x(t) +B2u(t) = + y(t) = C2x(t) +D2u(t)
  • 5. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 07 Issue: 03 | Mar 2020 www.irjet.net p-ISSN: 2395-0072 © 2020, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 5520 = 5. DERIVATION OF TRANSFER FUNCTION Input voltage=18 V, L1=1.81mH, L2=1.34mH, C1=375 microFarad, C2=100 microFarad, R=30ohm, d=0.6 A1 = B1 = C1 = D1 = A2 = B2 = C2 = D2 = A= A1d+A2(1-d) A = B= B1d+B2(1-d) B = C= C1d+C2(1-d) C = D= D1d+D2(1-d) D = Transfer function = C*[sI-A]^-1*B+D The transfer function has been derived using matlab. 5.1 MATLAB program A=[0 0 -220.996 0;0 0 149.252 -298.508;1066.668 -533.334 0 0;0 4000 0 333.331]; B=[331.494;447.762;0;0]; C=[0 0 0 1]; D=0; sys=ss(A,B,C,D); tf(sys)
  • 6. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 07 Issue: 03 | Mar 2020 www.irjet.net p-ISSN: 2395-0072 © 2020, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 5521 5.2 Output 1.791e06 s^2 + 2.111e11 ------------------------------------------------------ s^4 – 333.3s^3 + 1.35e06 s^2 – 5.204e07 s + 2.815e11 Continuous-time transfer function. 6.TUNINGOFPICONTROLLERPARAMETERSUSING GENETIC ALGORITHM Genetic Algorithm based PI controller is used forclosedloop control of the proposed DC to DC converter for which the tuning of controller parameters is done using Integrated Time Absolute Error (ITAE).The stability analysis is done using bode plot. The simulation of the closed loop control of the proposed converter is used to obtain the desired output and satisfactory performance. 6.1 MATLAB program function [J] = pi_optim(x) s = tf('s'); plant = (2667*s^2 + 4.268e07)/(s^4 + 0.668*s^3 + 8.667e04*s^2 + 5.077e04*s + 6.827e08); Kp = x(1) Ki = x(2) cont = Kp + Ki/s ; step(feedback(plant*cont,1)); dt = 0.01; t = 0:dt:1; e = 1 - step(feedback(plant*cont,1),t); J = sum(t'.*abs(e)*dt); 6.2 Output After 117 iterations, KP = 0.8838 and KI = 0.00008 7. STABILITY ANALYSIS 7.1 MATLAB program syms s; G=tf([1.76e06 2.111e11],[1 -333.3 1.35e06 -5.204e07 2.815e11]); K=tf([0.8838 0.00008],[1 0]); L=feedback(K*G,1); pole(L) bode(L),grid 8. CLOSED LOOP SIMULATION By simulating the above model, the desired output is obtained. 9. CONCLUSION The simulation, state space modelling and derivation of transfer function has been used to validate the effectiveness of the proposed positiveoutputDC-DCBuck Boostconverter. The state space modelling has been used to derivetheclosed loop transfer function using MATLAB. The PI controller parameters has been tuned by using Genetic Algorithm ( i.e. Integrated Time Absolute Error function) in MATLAB. The stability analysis and closed loop simulation has been used to obtain satisfactory performance from the proposed positive output DC-DC Buck Boost converter. This proposed model will overcome the disadvantages of traditional converters and is suitable for industrial applications. REFERENCES [1] K.I. Hwu W.C. Tu , “Voltage-boosting converters with hybrid energy pumping “,Department of Electrical Engineering, National Taipei University of Technology, 1, Sec. 3, Chung-Hsiao E. Rd., 2011 7.1 Bode plot ( closed loop – stable) 8.1 Closed loop simulation
  • 7. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 07 Issue: 03 | Mar 2020 www.irjet.net p-ISSN: 2395-0072 © 2020, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 5522 [2] Wuhua Li, Member, IEEE, and Xiangning He, Fellow, IEEEM, “Review of Nonisolated High-Step-Up DC/DC Converters in Photovoltaic Grid-Connected Applications” Mill Valley, CA: University Science, 1989. [3] Lung-Sheng Yang, Tsorng-Juu Liang, Member, IEEE, and Jiann-Fuh Chen,Member,IEEE,“TransformerlessDC–DC Converters With High Step-Up Voltage Gain” , 2009 [4] F.L. Luo and H. Ye , “Positive output cascade boost converters “ , 2004