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Bulletin of Electrical Engineering and Informatics
Vol. 9, No. 3, June 2020, pp. 1291~1298
ISSN: 2302-9285, DOI: 10.11591/eei.v9i3.1780  1291
Journal homepage: http://beei.org
Comparison analysis of chattering in smooth sliding mode
controlled DC-DC buck converter using constant plus
proportional reaching law and proposed reaching laws
K. B. Siddesh1
, B. Banakara2
, R. Shivarudraswamy3
1
Department of Electronics and Communication Engineering, SJMIT, VT University, Belagavi
2
Department of Electrical & Electronics Engineering, UBDTCE, VT University, Belagavi
3
Department of Electrical & Electronics Engineering, MIT, Karnataka
Article Info ABSTRACT
Article history:
Received Sep 7, 2019
Revised Dec 28, 2019
Accepted Feb 20, 2020
This paper presents a comparative analysis of chattering in sliding mode
controlled DC-DC buck converter for chattering suppression using constant
plus proportional reaching law and proposed reaching laws. A smooth SMC
is used for chattering suppression in buck converter. The different switching
functions are used in proposed reaching laws and constant plus proportional
reaching law applied to SMC buck converter, the tan hyperbolic reaching
law, sigmoid reaching law and constant plus proportional rate reaching law.
The proposed method tan hyperbolic gives less switching loss among
the reaching laws and stable output voltage. Inturn, performance of the buck
converter increases, tanhyperbolic reaching law is more sensitive to matched,
mismatched disturbance and parameter uncertainties. Loading conditions
are also applied to the buck converter to measure the disturbances
and parametric variations. The results are verified by MATLAB/Simulink.
Keywords:
Chattering
Reaching law
Sigmoid reaching law
Sliding mode control
Tan hyperbolic reaching law
This is an open access article under the CC BY-SA license.
Corresponding Author:
K. B. Siddesh,
Department of Electronics and Communication Engg,
SJMIT, VTU Belagavi. 577501.
Email: kondapur.b@gmail.com
1. INTRODUCTION
DC-DC converters are operated at very high switching frequencies, and this allows the use of small
inductive and capacitive components which increases the dynamic behavior and alleviate the size
of the converter. The DC-DC converter working with a sliding mode controller based reaching
law. Even though many parameters influence the operating points of the converters.1) Line and load
variation. 2) Electromagnetic interferences (EMI). 3) Chattering. The SMC is derived from VSCS (variable
structure control systems) and applied to many non linear applications, using reaching laws, the objective
structure of a system is changed intentionally during the time concerning the present structure control law.
The traditional reaching laws are explained [1]. The applications and survey given in [2], the variable
structure applied with reaching laws, it can minimize the chattering in the systems but not removed from
the system. The design and analysis of DC-DC converter done using adaptive SMC, here not mentioned
the chattering of converter [3]. Using fixed-frequency modulation for quasi sliding mode control (QSMC)
has been done through experimental and simulation verifications [4]. Analysis of new improved reaching law
with chattering reduction in SMC based on many applications [5]. In this work comparative study of sliding
mode control (SMC) with PID controller, derivative sliding surface with three different reaching laws,
namely, constant rate, exponential and power rate reaching law to control a two-link robotic manipulator [6].
 ISSN: 2302-9285
Bulletin of Electr Eng & Inf, Vol. 9, No. 3, June 2020 : 1291 – 1298
1292
An improved traditional SMC in positive invariant ones, the sliding surfaces enters by the variables, it will
not move away from the sliding line [7]. In this work presents a new methods based on a novel reaching law
to overcome slow convergence rate and reduce the chattering in sliding mode control of permanent magnet
synchronous motors (PMSM). The constant reaching law converges slowly. Although the power reaching
law converges fast during large error [8].
This work proposes a novel continuous reaching law for chattering-less sliding mode control by
using two hyperbolic functions with like changing rate and contradictory amplitude characteristics.
The earliest function is an inverse hyperbolic sine function, which can guarantee the quick convergence as
the first value of the sliding mode variable is far away from the equilibrium. When the sliding mode variable
is approaching to zero, the second hyperbolic tangent function can ensure the sliding mode variable be
infinitely close to zero slightly than cross the zero [9]. In this work, the sigmoid variable rate reaching law
applied to the systems and its analysis with conventional reaching law, sigmoid reaching law is dynamic
and superior to traditional reaching law [10]. In this work comparison between sigmoid and exponential
reaching law applied DC-DC buck converter, chattering was minimized [11]. This work gives chattering
minimization with SMC based reaching laws [12]. This work presents chattering alleviation using modified
power rate reaching law for robotics, here varying the exponential term of power rate reaching law to
minimize he chattering [13]. This work presents saturation function instead of signum function, so that it
covers the entire sliding mode portion and chattering reduces [14]. This work presents an improved reaching
law in SMC for chattering minimization, as compare to previous works [15]. This reaching law is an adaptive
but it implemented to second-order nonlinear function [16]. This work presents new power exponential
rate reaching law for second-order system to reduce the chattering in the system and control gains
automatically adjusts the switching function [17]. In this work discrete sliding mode control and classical
SMC with relative degree1 and relative degree2 for DC-DC buck converter discussed, no chattering issues
in this work [18]. In this work reaching law based SMC for DC-DC buck converter has been done. Here d+
and d- method implemented, chattering is alleviated, but not measured and traditional reaching law
implemented [19]. In this work newly exponential term added to the power reaching law. It implemented to
PMSM system to achieve better performance, fast convergence and reduces the chattering in the PMSM [20].
All the above [14-17] new reaching law in their differential equations, these law are reduces
the chattering to a certain extent and adapts the smooth variation of switching function. All these
new reaching laws reduces the amplitude of the chattering in the system. The problems in the previous
work [11, 18-20]. Sliding mode portion not covered, Chattering existence, more switching loss, more time to
reach the steady state, ripple in the output voltage, less response to external disturbances and uncertainty
of the systems. As many researchers are discussed about the new modified reaching laws, chattering
mitigation and their consequences on the converter. As in this work considered a buck converter,
this converter applied to many applications such as renewable energy sources, laptops, electronics industries,
electronic gadgets, etc., using a sliding mode controller achieving a constant output voltage. But more
switching loss occur due to chattering in system, in turn, high speed switching frequency operation in
the switching devices. To the above mentioned problem to alleviate the chattering, a proposed tan hyperbolic
reaching law, sigmoid reaching law and constant plus proportional pace reaching law are examined
and applied to buck converter [21-23].
2. GENERAL IMPLEMENTATION OF SMOOTH SLIDING MODE CONTROL FOR BUCK
CONVERTER USING REACHING LAW
The converter output voltage and its derivative both are selected as state variables for buck
converter. Figure 1 shows the structure of SMC for buck converter [5].
Figure 1. A Circuit diagram of SMC for buck converter
Bulletin of Electr Eng & Inf ISSN: 2302-9285 
Comparison analysis of chattering in smooth sliding mode controlled DC-DC… (K. B. Siddesh)
1293
The mathematical equation,
1
1
buck 2 2
3
3
X = Vref -βVo
X
βVo βVo -βViU
X = X = X = + dt
RLC LC
X
X = X1dt
 
   
   

   
 
 
  
 
[5]
X = AX + BU + D (1)
X1 is the error, X2 is the derivative of the error and X3 is the integral error. The sliding surface is given by;
1 1 2 2 3 3
S = α X + α X + α X (2)
The derivative of the sliding surface and this equation equated with proposed reaching laws.
1 1 2 2 3 3
S = α X + α X + α X = 0 [5] (3)
where α1 α2 & α3 represent the sliding coefficients.
2.1. Implementation of smooth sliding mode control for buck converter with constant plus proportional
pace reaching law (traditional reaching law)
Constant plus proportional pace reaching law (traditional reaching law) it is given by [1]
S = -Qsgn(S) - kS (4)
where Q and k are constants [1]. Equating the (3) and (4) (implementation of SMC with buck converter),
1 1 2 2 3 3
S=-Qsgn(S)-kS=α X +α X +α X (5)
 
βic UVinβ βV0
β
-Qsgn(S)-kS = α1 - ic + α2 - α2 + α2 + α3 Vref -βVo
2 LC LC
C RC
 
 
 
 
(6)
Simulation modelling eqution:
where Ueq=d; d=Vc/Vramp; Vramp=β Vin
 
LC α1icβ βic βVo
Ueq= Qsgn(S)+kS- +α2 +α2 +α3 Vref-βVo
2
α2Vinβ C LC
RC
 
 
 
 
LC α1icβ βic βVo
Vc= Qsgn(S)+kS- +α2 +α2 +α3 Vref-βVo
2
α2 C LC
RC
 
 
 
(7)
2.2. Implementation of smooth sliding mode control for buck converter with proposed method 1:
Sigmoid reaching law
The proposed sigmoid reaching law is given by [10, 24, 25].
-αX+θ -1
sig(X,α,θ) = (1+e ) (8)
if 1, 0
X
1 e
sig(X) 2sig(X,1, 0) 1
X
1 e
if 2, 0
X X
e e
tanh(X) sig(2X)
X X
e e
   


  


   


 


 ISSN: 2302-9285
Bulletin of Electr Eng & Inf, Vol. 9, No. 3, June 2020 : 1291 – 1298
1294
n
X Xi , 0, K 0
i 1
   


 
S sig X sgn S(X) K1S(X)
   (9)
Equating the (3) and (9) (implementation of SMC with buck converter),
Simulation modeling equations:
   
ic UVin V0
sig X sgn S(X) K1S(X) 1 ic 2 2 2 3 Vref Vo
2
C LC LC
RC
   
              
 
 
 
(10)
   
LC 1ic ic Vo
Ueq sig X sgn S(X) K1S(X) 2 2 3 Vref Vo
2
2Vin C LC
RC
   
           
 
 
 
 
(11)
where Ueq=d; d=Vc/Vramp; Vramp=β Vin where β is a feedback factor.
   
LC 1ic ic Vo
Vc sig X sgn S(X) K1S(X) 2 2 3 Vref Vo
2
2 C LC
RC
   
           

 
 
 
(12)
2.3. Implementation of smooth sliding mode control for buck converter with proposed method 2:
Tan hyperbolic reaching law
Proposed a novel continuoustan hyperbolic reaching law is given by [9].
A proposed method 2 reaching law is given by;
α λ
S = - m1* s tanh(s) - m2 s tanh(s) (13)
m1>0, m2>0,α >0, λ>0
The hyperbolic function range from (-1, +1),
x x
e e
tanh(s) x x
e e


 
 [9].
This hyperbolic reaching laws gives smooth switching function by
α
-m1* s tanh(s)
,where α
is a switching gain.
λ
-m2 s tanh(s)
where λ is a linear gain for controlling the chattering in the sliding surface.
By selecting propoer lear gain chatterin will be limited.
Simulation modeling equations
α
-m1* s tanh(s)
Equating the (3) and (13) (Implementation of SMC with buck converter)
1 2
1 2 1 1 2 2 3 3
K K
-m * s tanh(s)-m s tanh(s)=S=α X +α X +α X
 
1 2
1 2 1 2 2 2 3
K K βic UVinβ βV0
β
-m * s tanh(s) - m s tanh(s) = α - ic + α - α + α + α Vref-βVo
2 LC LC
C RC
 
 
 
 
(14)
where Ueq=d; d=Vc/Vramp; Vramp=β Vin
 
LC α1icβ βic βVo
α λ
Ueq = -m1* s tanh(s) - m2 s tanh(s) - + α2 + α2 + α3 Vref -βVo
2
α2Vinβ C LC
RC
 
 
 
 
LC α1icβ βic βVo
α λ
Vc = -m1* s tanh(s) - m2 s tanh(s) - + α2 + α2 + α3 Vref - βVo
2
α2 C LC
RC
 
 
 
(15)
Bulletin of Electr Eng & Inf ISSN: 2302-9285 
Comparison analysis of chattering in smooth sliding mode controlled DC-DC… (K. B. Siddesh)
1295
3. RESULTS AND DISCUSSION
Table 1 specification of sliding mode control buck converter with reaching laws. Figure 2 shows
that proposed method 1 gives the ripple in the output voltage is 2mV, ouput voltage is 12.065V, whereas
the proposed method 2 tan hyperbolic reaching law gives no ripple in the output voltage and it provides
the output voltage of 12.01V. This is due to chattering exists in the sigmoid reaching law. Constant plus
proportional pace reaching law not yet reached steady state because more chattering exist in the sliding
manifold as shown in the Figure 2 and output voltage is 11.97V. (Simulation results of this
Figure 2 from modelling (7), (12), (15)).
Figure 3 shows that the proposed method 2 has s overshoot voltage of 1.5V, ripple in the output
voltage (2mV) and output voltage of 12.025V. Whereas the proposed method 1 gives no overshoot,
no ripple in the output voltage and an output voltage is 12.02V.Constant plus proportional pace reaching law
has taken more time to reach the steady state and output voltage is 11.97V. The more chattering occurs in
the proposed method 2. It is observed that proposed method 2 is more sensitive for load component
variations. (Simulation results of this Figure 3 from modelling (7), (12), (15)).
Table 1. Gives the specifications of the of sliding mode control buck converter with reaching laws
Sl.No. Parameter Symbol Value
1 Input voltage Vi 24Volts
2 Capacitance C 220μF
3 Inductance L 69μH
4 Switching Frequency fs 250KHz
6 load resistance RL(max) 10 Ohm
7 Desired Output voltage Vod 12V
8 Reference voltage Vref 12V
9 Inductance LL 1mH
10 Capacitance CL 1microF
11 Feedback factor β 0.98
12 Sliding coefficients, α1, α2, α3 3,25,200
13 Duty cycle α 0.5
14 Efficiency of the Converter η 0.91
15 .λ α,K1,K2 0.5,1,0.95
Figure 2. Shows the output voltage v/s time in secs of buck converter,
Proposed method 1 (sigmoid reaching law), Proposed method 2 (tan hyperbolic reaching law),
and Constant plus proportional pace reaching law (R-Load)
Figure 3. Shows the output voltage v/s time in secs of buck converter,
Proposed method 1 (tanhyperbolic reaching law), Proposed method 2 (sigmoid reaching law),
and Constant plus proportional pace reaching law (R-L Load)
0 0.001 0.002 0.003 0.004 0.005 0.006 0.007 0.008 0.009 0.01
11.85
11.9
11.95
12
12.05
Time in Secs
Output
Voltage
Constnt plus proportional rate reaching law
Proposed method 1
Proposed method 2
0 0.001 0.002 0.003 0.004 0.005 0.006 0.007 0.008 0.009 0.01
11.9
12
12.1
Time in Secs
Output
Voltage
Constant plus proportional rate reaching law
Proposed method 2
Proposed method 1
 ISSN: 2302-9285
Bulletin of Electr Eng & Inf, Vol. 9, No. 3, June 2020 : 1291 – 1298
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Figure 4 shows that the proposed method 1 gives a deviated from the desired output voltage
is 0.38V, whereas the proposed method 2 has 0.28V, deviated from the desired output voltage respectively.
The output voltage of proposed method 1 is 12.32V and output voltage of proposed method 2 is 12.36V.
Constant plus proportional pace reaching law reaches the steady state at 6msecs and output voltage
is 12.01V, but not stable in output voltage. Proposed method 1 has a more sensitive to change in load
components and exhibits the change in output voltage. (Simulation results of this Figure 4 from
modelling (7), (12), (15))
Figure 5 shows that proposed method 1 has deviated the output voltage 0.43V, whereas
the proposed method 2 has 0.29V.The output voltage of proposed method 1 is 12.44V and the output voltage
of proposed method 2 is 12.29V. Constant plus proportional pace reaching law reaches the steady state at
6msecs and output voltage is 11.99V, but not stable in output voltage. In R-L-C load, the proposed method 2
has less deviated from the desired output voltage and more stable. Proposed method 1 has more deviated
from the output voltage.
Figure 4. Shows output voltage v/s time in secs of buck converter,
Proposed method 1 (sigmoid reaching law), Proposed method 2 (tanhyperbolic reaching law),
and constant plus proportional rate reaching law (R-C Load)
Figure 5. Shows output voltage v/s time in secs of Buck converter,
Proposed method 1 (sigmoid reaching law), Proposed method 2 (tan hyperbolic reaching law),
and Constant plus proportional rate reaching law (R-L-C Load)
Figure 6 shows the derivative of error and error. The chattering has occurred on nearby the origin
of both methods. Whereas the constant plus proportional pace reaching law is far away from the origin, due
to chattering in the sliding manifold. Proposed method 1 is just away from the origin when compared to
proposed method 2 and constant plus proportional reaching law. This is due to sign switching function gives
discontinuous in the sliding mode, proposed method 2 gives a smoother switching function and avoid
the discontinuity in the sliding mode, whereas the proposed method 1 gives less discontinuity in the sliding
mode. Hence proposed method 2 exhibits superior continuous approximation than other methods.
The chattering of proposed method 1 is 0.156, the proposed method 2 chattering is 0.143 and constant plus
proportional pace reaching law chattering is 0.5. In turn, switching loss is more in constant plus proportional
pace reaching law than proposed method 2. Results are tabulated in Table 2. (Simulation results of this
Figure 6 and Table 2 are obtained from modellin (7), (12), (15)).
0 0.001 0.002 0.003 0.004 0.005 0.006 0.007 0.008 0.009 0.01
11
11.5
12
12.5
Output
Voltage
Time inSecs
Constant plus proportional rater reaching law
Proiposed method 1
Proposed method 2
0 0.001 0.002 0.003 0.004 0.005 0.006 0.007 0.008 0.009 0.01
11
11.5
12
12.5
Output
Voltage
Time inSecs
Constant plus proportional rater reaching law
Proiposed method 1
Proposed method 2
Bulletin of Electr Eng & Inf ISSN: 2302-9285 
Comparison analysis of chattering in smooth sliding mode controlled DC-DC… (K. B. Siddesh)
1297
Figure 6. Shows derivative of error v/s error of buck converter,
Proposed method 1 (sigmoid reaching law), Proposed method 2 (tan hyperbolic reaching law),
and Constant plus proportional rate reaching law (chattering)
Table 2. Comparison of proposed method 1, proposed method 2 and constant plus proportional
pace reaching law (buck converter)
Parameters
A proposed method1
sigmoid reaching law
A proposed method2 tan
hyperbolicreaching law
Constant plus proportional
pace reaching law
Chattering amplitude from x and y-axis 0. 156 0.143 0.5
Output Voltage(R load) 12.065V 12.01V 11.97V
Output Voltage(R-L load) 12.025V 12.012V 11.97V
Output Voltage(R-C load) 12.32V 12.36V 12.01V
Output Voltage(R-L-C load) 12.44V 12.29V 11.99V
Switching loss 0.31W 0.29W 0.55W
4. CONCLUSION
The proposed method 2 (tan hyperbolic reaching law) gives constant output voltage, reaches
steady state with fast convergence time and it mitigates chattering, it covers the entire sliding mode portion
of the phase plane trajectory as compared to method 1 (sigmoid reaching law). The different loading
is applied to converter, among these two methods the tan hyperbolic reaching law gives better controlling
the output voltage and fewer ripples in the output voltage than the sigmoid reaching law and constant plus
proportional pace reaching law. Tanhyperbolic reaching law gives less chattering and takes less time to reach
a steady-state. In turn, less switching loss in the buck converter.
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-5
0
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Ic(Dervative
of
error)
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BIOGRAPHIES OF AUTHORS
K. B. Siddesh is a Research Scholar at VTU, Karnataka, India, and currently working as
an Associate Professor in the Department of Electronics and Communication Engineering at
SJMIT, Chitradurga, India. His area of interest includes Power Electronics & Drives, Insulation
Coordination and Power Quality Issues. He has 21 Years of Teaching Experience.
Dr. B. Basavaraja is currently working as a Professor in the Department of Electrical
and Electronics Engineering at the University of BDT Engineering College (Constituent College
of Visvesvaraya Technological University) Davanagere, Karnataka, India. He has 26 Years
of Teaching Experience, 13 Years of Research & Developments and 15 Years of Administration.
His area of interest includes Power Electronics and Drives, Insulation Coordination and Power
Quality Issues. He has published several papers in various International and National Journals
R. Shivarudraswamy is currently working as an Assoc. Professor in EEE Department, Manipal
Institute of Technology, Manipal. His areas of interest are Insulation Coordination and Power
Quality Issues. He has 21 Years of Teaching Experience.

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Comparison analysis of chattering in smooth sliding mode controlled DC-DC buck converter using constant plus proportional reaching law and proposed reaching laws

  • 1. Bulletin of Electrical Engineering and Informatics Vol. 9, No. 3, June 2020, pp. 1291~1298 ISSN: 2302-9285, DOI: 10.11591/eei.v9i3.1780  1291 Journal homepage: http://beei.org Comparison analysis of chattering in smooth sliding mode controlled DC-DC buck converter using constant plus proportional reaching law and proposed reaching laws K. B. Siddesh1 , B. Banakara2 , R. Shivarudraswamy3 1 Department of Electronics and Communication Engineering, SJMIT, VT University, Belagavi 2 Department of Electrical & Electronics Engineering, UBDTCE, VT University, Belagavi 3 Department of Electrical & Electronics Engineering, MIT, Karnataka Article Info ABSTRACT Article history: Received Sep 7, 2019 Revised Dec 28, 2019 Accepted Feb 20, 2020 This paper presents a comparative analysis of chattering in sliding mode controlled DC-DC buck converter for chattering suppression using constant plus proportional reaching law and proposed reaching laws. A smooth SMC is used for chattering suppression in buck converter. The different switching functions are used in proposed reaching laws and constant plus proportional reaching law applied to SMC buck converter, the tan hyperbolic reaching law, sigmoid reaching law and constant plus proportional rate reaching law. The proposed method tan hyperbolic gives less switching loss among the reaching laws and stable output voltage. Inturn, performance of the buck converter increases, tanhyperbolic reaching law is more sensitive to matched, mismatched disturbance and parameter uncertainties. Loading conditions are also applied to the buck converter to measure the disturbances and parametric variations. The results are verified by MATLAB/Simulink. Keywords: Chattering Reaching law Sigmoid reaching law Sliding mode control Tan hyperbolic reaching law This is an open access article under the CC BY-SA license. Corresponding Author: K. B. Siddesh, Department of Electronics and Communication Engg, SJMIT, VTU Belagavi. 577501. Email: kondapur.b@gmail.com 1. INTRODUCTION DC-DC converters are operated at very high switching frequencies, and this allows the use of small inductive and capacitive components which increases the dynamic behavior and alleviate the size of the converter. The DC-DC converter working with a sliding mode controller based reaching law. Even though many parameters influence the operating points of the converters.1) Line and load variation. 2) Electromagnetic interferences (EMI). 3) Chattering. The SMC is derived from VSCS (variable structure control systems) and applied to many non linear applications, using reaching laws, the objective structure of a system is changed intentionally during the time concerning the present structure control law. The traditional reaching laws are explained [1]. The applications and survey given in [2], the variable structure applied with reaching laws, it can minimize the chattering in the systems but not removed from the system. The design and analysis of DC-DC converter done using adaptive SMC, here not mentioned the chattering of converter [3]. Using fixed-frequency modulation for quasi sliding mode control (QSMC) has been done through experimental and simulation verifications [4]. Analysis of new improved reaching law with chattering reduction in SMC based on many applications [5]. In this work comparative study of sliding mode control (SMC) with PID controller, derivative sliding surface with three different reaching laws, namely, constant rate, exponential and power rate reaching law to control a two-link robotic manipulator [6].
  • 2.  ISSN: 2302-9285 Bulletin of Electr Eng & Inf, Vol. 9, No. 3, June 2020 : 1291 – 1298 1292 An improved traditional SMC in positive invariant ones, the sliding surfaces enters by the variables, it will not move away from the sliding line [7]. In this work presents a new methods based on a novel reaching law to overcome slow convergence rate and reduce the chattering in sliding mode control of permanent magnet synchronous motors (PMSM). The constant reaching law converges slowly. Although the power reaching law converges fast during large error [8]. This work proposes a novel continuous reaching law for chattering-less sliding mode control by using two hyperbolic functions with like changing rate and contradictory amplitude characteristics. The earliest function is an inverse hyperbolic sine function, which can guarantee the quick convergence as the first value of the sliding mode variable is far away from the equilibrium. When the sliding mode variable is approaching to zero, the second hyperbolic tangent function can ensure the sliding mode variable be infinitely close to zero slightly than cross the zero [9]. In this work, the sigmoid variable rate reaching law applied to the systems and its analysis with conventional reaching law, sigmoid reaching law is dynamic and superior to traditional reaching law [10]. In this work comparison between sigmoid and exponential reaching law applied DC-DC buck converter, chattering was minimized [11]. This work gives chattering minimization with SMC based reaching laws [12]. This work presents chattering alleviation using modified power rate reaching law for robotics, here varying the exponential term of power rate reaching law to minimize he chattering [13]. This work presents saturation function instead of signum function, so that it covers the entire sliding mode portion and chattering reduces [14]. This work presents an improved reaching law in SMC for chattering minimization, as compare to previous works [15]. This reaching law is an adaptive but it implemented to second-order nonlinear function [16]. This work presents new power exponential rate reaching law for second-order system to reduce the chattering in the system and control gains automatically adjusts the switching function [17]. In this work discrete sliding mode control and classical SMC with relative degree1 and relative degree2 for DC-DC buck converter discussed, no chattering issues in this work [18]. In this work reaching law based SMC for DC-DC buck converter has been done. Here d+ and d- method implemented, chattering is alleviated, but not measured and traditional reaching law implemented [19]. In this work newly exponential term added to the power reaching law. It implemented to PMSM system to achieve better performance, fast convergence and reduces the chattering in the PMSM [20]. All the above [14-17] new reaching law in their differential equations, these law are reduces the chattering to a certain extent and adapts the smooth variation of switching function. All these new reaching laws reduces the amplitude of the chattering in the system. The problems in the previous work [11, 18-20]. Sliding mode portion not covered, Chattering existence, more switching loss, more time to reach the steady state, ripple in the output voltage, less response to external disturbances and uncertainty of the systems. As many researchers are discussed about the new modified reaching laws, chattering mitigation and their consequences on the converter. As in this work considered a buck converter, this converter applied to many applications such as renewable energy sources, laptops, electronics industries, electronic gadgets, etc., using a sliding mode controller achieving a constant output voltage. But more switching loss occur due to chattering in system, in turn, high speed switching frequency operation in the switching devices. To the above mentioned problem to alleviate the chattering, a proposed tan hyperbolic reaching law, sigmoid reaching law and constant plus proportional pace reaching law are examined and applied to buck converter [21-23]. 2. GENERAL IMPLEMENTATION OF SMOOTH SLIDING MODE CONTROL FOR BUCK CONVERTER USING REACHING LAW The converter output voltage and its derivative both are selected as state variables for buck converter. Figure 1 shows the structure of SMC for buck converter [5]. Figure 1. A Circuit diagram of SMC for buck converter
  • 3. Bulletin of Electr Eng & Inf ISSN: 2302-9285  Comparison analysis of chattering in smooth sliding mode controlled DC-DC… (K. B. Siddesh) 1293 The mathematical equation, 1 1 buck 2 2 3 3 X = Vref -βVo X βVo βVo -βViU X = X = X = + dt RLC LC X X = X1dt                         [5] X = AX + BU + D (1) X1 is the error, X2 is the derivative of the error and X3 is the integral error. The sliding surface is given by; 1 1 2 2 3 3 S = α X + α X + α X (2) The derivative of the sliding surface and this equation equated with proposed reaching laws. 1 1 2 2 3 3 S = α X + α X + α X = 0 [5] (3) where α1 α2 & α3 represent the sliding coefficients. 2.1. Implementation of smooth sliding mode control for buck converter with constant plus proportional pace reaching law (traditional reaching law) Constant plus proportional pace reaching law (traditional reaching law) it is given by [1] S = -Qsgn(S) - kS (4) where Q and k are constants [1]. Equating the (3) and (4) (implementation of SMC with buck converter), 1 1 2 2 3 3 S=-Qsgn(S)-kS=α X +α X +α X (5)   βic UVinβ βV0 β -Qsgn(S)-kS = α1 - ic + α2 - α2 + α2 + α3 Vref -βVo 2 LC LC C RC         (6) Simulation modelling eqution: where Ueq=d; d=Vc/Vramp; Vramp=β Vin   LC α1icβ βic βVo Ueq= Qsgn(S)+kS- +α2 +α2 +α3 Vref-βVo 2 α2Vinβ C LC RC         LC α1icβ βic βVo Vc= Qsgn(S)+kS- +α2 +α2 +α3 Vref-βVo 2 α2 C LC RC       (7) 2.2. Implementation of smooth sliding mode control for buck converter with proposed method 1: Sigmoid reaching law The proposed sigmoid reaching law is given by [10, 24, 25]. -αX+θ -1 sig(X,α,θ) = (1+e ) (8) if 1, 0 X 1 e sig(X) 2sig(X,1, 0) 1 X 1 e if 2, 0 X X e e tanh(X) sig(2X) X X e e                     
  • 4.  ISSN: 2302-9285 Bulletin of Electr Eng & Inf, Vol. 9, No. 3, June 2020 : 1291 – 1298 1294 n X Xi , 0, K 0 i 1         S sig X sgn S(X) K1S(X)    (9) Equating the (3) and (9) (implementation of SMC with buck converter), Simulation modeling equations:     ic UVin V0 sig X sgn S(X) K1S(X) 1 ic 2 2 2 3 Vref Vo 2 C LC LC RC                          (10)     LC 1ic ic Vo Ueq sig X sgn S(X) K1S(X) 2 2 3 Vref Vo 2 2Vin C LC RC                         (11) where Ueq=d; d=Vc/Vramp; Vramp=β Vin where β is a feedback factor.     LC 1ic ic Vo Vc sig X sgn S(X) K1S(X) 2 2 3 Vref Vo 2 2 C LC RC                        (12) 2.3. Implementation of smooth sliding mode control for buck converter with proposed method 2: Tan hyperbolic reaching law Proposed a novel continuoustan hyperbolic reaching law is given by [9]. A proposed method 2 reaching law is given by; α λ S = - m1* s tanh(s) - m2 s tanh(s) (13) m1>0, m2>0,α >0, λ>0 The hyperbolic function range from (-1, +1), x x e e tanh(s) x x e e      [9]. This hyperbolic reaching laws gives smooth switching function by α -m1* s tanh(s) ,where α is a switching gain. λ -m2 s tanh(s) where λ is a linear gain for controlling the chattering in the sliding surface. By selecting propoer lear gain chatterin will be limited. Simulation modeling equations α -m1* s tanh(s) Equating the (3) and (13) (Implementation of SMC with buck converter) 1 2 1 2 1 1 2 2 3 3 K K -m * s tanh(s)-m s tanh(s)=S=α X +α X +α X   1 2 1 2 1 2 2 2 3 K K βic UVinβ βV0 β -m * s tanh(s) - m s tanh(s) = α - ic + α - α + α + α Vref-βVo 2 LC LC C RC         (14) where Ueq=d; d=Vc/Vramp; Vramp=β Vin   LC α1icβ βic βVo α λ Ueq = -m1* s tanh(s) - m2 s tanh(s) - + α2 + α2 + α3 Vref -βVo 2 α2Vinβ C LC RC         LC α1icβ βic βVo α λ Vc = -m1* s tanh(s) - m2 s tanh(s) - + α2 + α2 + α3 Vref - βVo 2 α2 C LC RC       (15)
  • 5. Bulletin of Electr Eng & Inf ISSN: 2302-9285  Comparison analysis of chattering in smooth sliding mode controlled DC-DC… (K. B. Siddesh) 1295 3. RESULTS AND DISCUSSION Table 1 specification of sliding mode control buck converter with reaching laws. Figure 2 shows that proposed method 1 gives the ripple in the output voltage is 2mV, ouput voltage is 12.065V, whereas the proposed method 2 tan hyperbolic reaching law gives no ripple in the output voltage and it provides the output voltage of 12.01V. This is due to chattering exists in the sigmoid reaching law. Constant plus proportional pace reaching law not yet reached steady state because more chattering exist in the sliding manifold as shown in the Figure 2 and output voltage is 11.97V. (Simulation results of this Figure 2 from modelling (7), (12), (15)). Figure 3 shows that the proposed method 2 has s overshoot voltage of 1.5V, ripple in the output voltage (2mV) and output voltage of 12.025V. Whereas the proposed method 1 gives no overshoot, no ripple in the output voltage and an output voltage is 12.02V.Constant plus proportional pace reaching law has taken more time to reach the steady state and output voltage is 11.97V. The more chattering occurs in the proposed method 2. It is observed that proposed method 2 is more sensitive for load component variations. (Simulation results of this Figure 3 from modelling (7), (12), (15)). Table 1. Gives the specifications of the of sliding mode control buck converter with reaching laws Sl.No. Parameter Symbol Value 1 Input voltage Vi 24Volts 2 Capacitance C 220μF 3 Inductance L 69μH 4 Switching Frequency fs 250KHz 6 load resistance RL(max) 10 Ohm 7 Desired Output voltage Vod 12V 8 Reference voltage Vref 12V 9 Inductance LL 1mH 10 Capacitance CL 1microF 11 Feedback factor β 0.98 12 Sliding coefficients, α1, α2, α3 3,25,200 13 Duty cycle α 0.5 14 Efficiency of the Converter η 0.91 15 .λ α,K1,K2 0.5,1,0.95 Figure 2. Shows the output voltage v/s time in secs of buck converter, Proposed method 1 (sigmoid reaching law), Proposed method 2 (tan hyperbolic reaching law), and Constant plus proportional pace reaching law (R-Load) Figure 3. Shows the output voltage v/s time in secs of buck converter, Proposed method 1 (tanhyperbolic reaching law), Proposed method 2 (sigmoid reaching law), and Constant plus proportional pace reaching law (R-L Load) 0 0.001 0.002 0.003 0.004 0.005 0.006 0.007 0.008 0.009 0.01 11.85 11.9 11.95 12 12.05 Time in Secs Output Voltage Constnt plus proportional rate reaching law Proposed method 1 Proposed method 2 0 0.001 0.002 0.003 0.004 0.005 0.006 0.007 0.008 0.009 0.01 11.9 12 12.1 Time in Secs Output Voltage Constant plus proportional rate reaching law Proposed method 2 Proposed method 1
  • 6.  ISSN: 2302-9285 Bulletin of Electr Eng & Inf, Vol. 9, No. 3, June 2020 : 1291 – 1298 1296 Figure 4 shows that the proposed method 1 gives a deviated from the desired output voltage is 0.38V, whereas the proposed method 2 has 0.28V, deviated from the desired output voltage respectively. The output voltage of proposed method 1 is 12.32V and output voltage of proposed method 2 is 12.36V. Constant plus proportional pace reaching law reaches the steady state at 6msecs and output voltage is 12.01V, but not stable in output voltage. Proposed method 1 has a more sensitive to change in load components and exhibits the change in output voltage. (Simulation results of this Figure 4 from modelling (7), (12), (15)) Figure 5 shows that proposed method 1 has deviated the output voltage 0.43V, whereas the proposed method 2 has 0.29V.The output voltage of proposed method 1 is 12.44V and the output voltage of proposed method 2 is 12.29V. Constant plus proportional pace reaching law reaches the steady state at 6msecs and output voltage is 11.99V, but not stable in output voltage. In R-L-C load, the proposed method 2 has less deviated from the desired output voltage and more stable. Proposed method 1 has more deviated from the output voltage. Figure 4. Shows output voltage v/s time in secs of buck converter, Proposed method 1 (sigmoid reaching law), Proposed method 2 (tanhyperbolic reaching law), and constant plus proportional rate reaching law (R-C Load) Figure 5. Shows output voltage v/s time in secs of Buck converter, Proposed method 1 (sigmoid reaching law), Proposed method 2 (tan hyperbolic reaching law), and Constant plus proportional rate reaching law (R-L-C Load) Figure 6 shows the derivative of error and error. The chattering has occurred on nearby the origin of both methods. Whereas the constant plus proportional pace reaching law is far away from the origin, due to chattering in the sliding manifold. Proposed method 1 is just away from the origin when compared to proposed method 2 and constant plus proportional reaching law. This is due to sign switching function gives discontinuous in the sliding mode, proposed method 2 gives a smoother switching function and avoid the discontinuity in the sliding mode, whereas the proposed method 1 gives less discontinuity in the sliding mode. Hence proposed method 2 exhibits superior continuous approximation than other methods. The chattering of proposed method 1 is 0.156, the proposed method 2 chattering is 0.143 and constant plus proportional pace reaching law chattering is 0.5. In turn, switching loss is more in constant plus proportional pace reaching law than proposed method 2. Results are tabulated in Table 2. (Simulation results of this Figure 6 and Table 2 are obtained from modellin (7), (12), (15)). 0 0.001 0.002 0.003 0.004 0.005 0.006 0.007 0.008 0.009 0.01 11 11.5 12 12.5 Output Voltage Time inSecs Constant plus proportional rater reaching law Proiposed method 1 Proposed method 2 0 0.001 0.002 0.003 0.004 0.005 0.006 0.007 0.008 0.009 0.01 11 11.5 12 12.5 Output Voltage Time inSecs Constant plus proportional rater reaching law Proiposed method 1 Proposed method 2
  • 7. Bulletin of Electr Eng & Inf ISSN: 2302-9285  Comparison analysis of chattering in smooth sliding mode controlled DC-DC… (K. B. Siddesh) 1297 Figure 6. Shows derivative of error v/s error of buck converter, Proposed method 1 (sigmoid reaching law), Proposed method 2 (tan hyperbolic reaching law), and Constant plus proportional rate reaching law (chattering) Table 2. Comparison of proposed method 1, proposed method 2 and constant plus proportional pace reaching law (buck converter) Parameters A proposed method1 sigmoid reaching law A proposed method2 tan hyperbolicreaching law Constant plus proportional pace reaching law Chattering amplitude from x and y-axis 0. 156 0.143 0.5 Output Voltage(R load) 12.065V 12.01V 11.97V Output Voltage(R-L load) 12.025V 12.012V 11.97V Output Voltage(R-C load) 12.32V 12.36V 12.01V Output Voltage(R-L-C load) 12.44V 12.29V 11.99V Switching loss 0.31W 0.29W 0.55W 4. CONCLUSION The proposed method 2 (tan hyperbolic reaching law) gives constant output voltage, reaches steady state with fast convergence time and it mitigates chattering, it covers the entire sliding mode portion of the phase plane trajectory as compared to method 1 (sigmoid reaching law). The different loading is applied to converter, among these two methods the tan hyperbolic reaching law gives better controlling the output voltage and fewer ripples in the output voltage than the sigmoid reaching law and constant plus proportional pace reaching law. Tanhyperbolic reaching law gives less chattering and takes less time to reach a steady-state. In turn, less switching loss in the buck converter. REFERENCES [1] W. Gao and J. C. Hung, “Variable structure control of nonlinear systems: A new approach,” IEEE Transactions on Industrial Electronics, vol. 40, no.1, pp. 45-55, 1993. [2] J. Y. Hung, W. Gao, and J. C. Hung, “Variable structure control: A survey,” IEEE Transactions on Industrial Electronics, vol. 40, no.1, pp. 2-22, 1993 [3] Y. He and F. L. Luo, “Design and analysis of adaptive sliding-mode-like controller for DC-DC converter,” IEE Proceedings-Electric Power Applications, vol. 153, no. 3, pp. 401-410, 2006. [4] S-C. Tan, Y. M. Lai, C. K. Tse, and M. K. H. Cheung, “A fixed-frequency pulse width modulation based quasi-sliding-mode controller for buck converter,” IEEE Transactions on Power Electronics, vol. 20, no. 6, pp-1379-1392, 2005. [5] S. Kasera, A. Kumar, and L. B. Prasad, “Analysis of chattering free improved sliding mode control,” International Conference on Innovations in Information, Embedded and Communication Systems (ICIIECS), pp. 1-6, 2017. [6] Pranav, J. Kumar, V. Kumar, and K. P. S. Rana, “Efficient reaching law for SMC with PID surface applied to a manipulator,” Second International Innovative Applications of Computational Intelligence on Power, Energy and Controls with their Impact on Humanity (CIPECH), pp. 51-56, 2016. [7] P. Zhang and Q. Wu,”Double power reaching law for sliding mode control with unidirectional auxiliary surfaces,” Chinese Control Conference (CCC), pp. 3798-3803, 2017. [8] Q. Hu, L. Liu, and H. Yang, “A sliding mode speed controller based on novel reaching law of permanent magnet synchronous motor system,” Chinese Automation Congress (CAC), pp. 954-958, 2017. [9] L. Tao, Q. Chen, Y. Nan, and C. Wu, “Double hyperbolic reaching law with chattering-free and fast convergence,” IEEE Access, vol. 6, pp. 27717-27725, 2018. [10] Y-L. Liu, C-C. Gao, and X. Liang, “Variable structure control for affine systems based on sigmoid variable rate reaching law,” 8th World Congress on Intelligent Control and Automation, pp. 4623-4627, 2010. [11] G. S. Rajanna and H. N. Nagaraj, “Comparison between sigmoid variable reaching law and exponential reaching law for sliding mode controlled DC-DC Buck converter,” International Conference on Power, Energy and Control (ICPEC), pp. 316-319, 2013. -2 0 2 4 6 8 10 12 -20 -15 -10 -5 0 Error(Vref-Beta*Vo) Ic(Dervative of error) Constant plus proportional rate reaching law Proposed method 2 Proposed method 1 Chattering Chattering
  • 8.  ISSN: 2302-9285 Bulletin of Electr Eng & Inf, Vol. 9, No. 3, June 2020 : 1291 – 1298 1298 [12] Y. M. Alsmadi, V. Utkin, M. A. Haj-ahmed, and L. Xu, “Sliding mode control of power converters: DC/DC converters,” International Journal of Control, vol. 91, no. 11 SI, pp. 2472-2493, 2017. [13] K. B. Devika and S. Thomas, “Improved sliding mode controller performance through power rate exponential reaching law,” Second International Conference on Electrical, Computer and Communication Technologies. (ICECCT), pp. 1-7, 2017. [14] H. Ye, M. Li, and W. Luo, “A novel reaching law of sliding mode control design and analysis,” Chinese Automation Congress (CAC), pp. 1803-1807, 2017. [15] Y. Li and L. liu, “The research of the sliding mode control method based on improved double reaching law,” Chinese Control and Decision Conference (CCDC), pp. 672-675, 2018. [16] H. Han, X. Wu, and J. Qiao, “Design of robust sliding mode control with adaptive reaching law,” IEEE Transactions on Systems, Man, and Cybernetics: Systems, pp. 1-10, 2018. [17] H. Ma, Y. Li, and Z. Xiong, “Discrete-time sliding-mode control with enhanced power reaching law,” IEEE Transactions On Industrial Electronics, vol. 66, no. 6, pp. 4629-4638, 2018. [18] J. Samantaray and S. Chakrabarty, “Digital implementation of sliding mode controllers with DC-DC buck converter system,” 15th International Workshop on Variable Structure Systems (VSS), pp. 255-260, 2018. [19] Y. Hey, W. Xu, and Y. Cheng, “A novel scheme for sliding-mode control of DC-DC buck converter with a constant frequency based on the averaging mode,” Journal of Power Electronics, vol. 10, no. 1, pp. 1-8, 2010. [20] J. Leng and C. Ma, “Sliding mode control for PMSM based on a novel hybrid reaching law,” 37th Chinese Control Conference (CCC), pp. 3006-3011, 2018. [21] Y. Han, Y. Cheng, and G. Xu, “Trajectory tracking control of AGV based on sliding mode control with the improved reaching law,” IEEE Access, vol. 7, pp. 20748-20755, 2019. [22] A. Wang and S. Wei, “Sliding mode control for permanent magnet synchronous motor drive based on an improved exponential reaching law,” IEEE Access, vol. 7, pp. 146866-146875, 2019. [23] Y. Wang, Y. Feng, X. Zhang, J. Liang and X. Cheng, “New reaching law control for permanent magnet synchronous motor with extended disturbance observer,” IEEE Access, vol. 7, pp. 186296-186307, 2019. [24] H. Ma and Y. Li, “Multi-power reaching law based discrete-time sliding-mode control,” IEEE Access, vol. 7, pp. 49822-49829, 2019. [25] L. Ren, S. Xie, Y. Zhang, J. Peng, and L. Zhang, “Chattering analysis for discrete sliding Mode control of distributed control system,” Journal of Systems engineering and Electronics, vol. 27, no. 5, pp 1096-1107, 2016. BIOGRAPHIES OF AUTHORS K. B. Siddesh is a Research Scholar at VTU, Karnataka, India, and currently working as an Associate Professor in the Department of Electronics and Communication Engineering at SJMIT, Chitradurga, India. His area of interest includes Power Electronics & Drives, Insulation Coordination and Power Quality Issues. He has 21 Years of Teaching Experience. Dr. B. Basavaraja is currently working as a Professor in the Department of Electrical and Electronics Engineering at the University of BDT Engineering College (Constituent College of Visvesvaraya Technological University) Davanagere, Karnataka, India. He has 26 Years of Teaching Experience, 13 Years of Research & Developments and 15 Years of Administration. His area of interest includes Power Electronics and Drives, Insulation Coordination and Power Quality Issues. He has published several papers in various International and National Journals R. Shivarudraswamy is currently working as an Assoc. Professor in EEE Department, Manipal Institute of Technology, Manipal. His areas of interest are Insulation Coordination and Power Quality Issues. He has 21 Years of Teaching Experience.