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Ramakrishnan Sumathi Int. Journal of Engineering Research and Applications www.ijera.com
ISSN: 2248-9622, Vol. 6, Issue 3, (Part -2) March 2016, pp.19- 23
www.ijera.com 19|P a g e
A PID Controller with Anti-Windup Mechanism for Firminga
Carbon Steel
Ramakrishnan Sumathi
Department of Electrical and Electronics Engineering Pavai College of Technology, Namakkal-637018, Tamil
Nadu, India
ABSTRACT
In this Paper, a classical PID controller with anti-windup technique is employed for controlling the
microstructure development during hot working process. The strength of any material is dependent on the grain
size of that material [4], [9]. The strength of the material is increased when its grain size is reduced. In this
paper, the standard Arrehenious equation of 0.3% carbon steel is utilized to obtain an optimal deformation path
such that the grain size of the product should be 26m. The 0.3% carbon steel improves in the machinability
by heat treatment [8]. It must also be noted that this steel is especially adaptable for machining or forging and
where surface hardness is desirable. The plant model is developed with grain size. The effect of process control
parameters such as strain, strain rate, and temperature on important microstructural features can be
systematically formulated and then solved as an optimal control problem. These approaches are applied to
obtain the desired grain size of 26m from an initial grain size of 180m. The simulation is done on various
grain sizes using the controller by MATLAB simulink toolbox. From the response it is found that the PID
controller with anti-windup provides better performance. Resulting tabulated performance indices showed a
considerable improvement in settling time besides reducing steady state error.
Keywords– Carbon steel, strain, strain rate, temperature, PID Controller, anti-windup.
I. INTRODUCTION
The development of optimal design and
control methods for manufacturing processes is
needed for effectively reducing part cost,
improving part delivery schedules, and producing
specified part quality on a repeatable basis.
Existing design methods are generally ad hoc and
lack adequate capabilities for finding effective
process parameters such as deformation rate, die
and work piece temperature, and tooling system
configuration. This situation presents major
challenges to process engineers who are faced with
smaller lot sizes, higher yield requirements, and
superior quality standards. Therefore, it is
important to develop new systematic
methodologies for process design and control based
upon scientific principles, which sufficiently
consider the behavior of work piece material and
the mechanics of the manufacturing process. A new
strategy for systematically calculating near optimal
control parameters for control of microstructure
during hot deformation processes has been
developed based on optimal control theory [1].This
approach treats the deforming material as a
dynamical system explained below.
II. STATIC AND DYNAMIC MODEL
The static model of 0.3% carbon steel [3]
is,
𝑑 = 22600 𝜀−0.27
𝑒−0.27 𝑄/𝑅𝑇
(1)
Where,
d = grain size
ε = strain
ε = strain rate
Q =
Activation energy for dynamic recrystallization
= 267KJmol−1
R = Gas constant = 8.314 x 10−3
KJK−1
mol−1
T = Billet temprature
The dynamic model of 0.3% carbon steel is
obtained by using the Arrehenius equation for
changes in temperature during hot extrusion is
given below.
𝜕𝑇
𝜕𝑡
= 𝑇 =
𝜂
𝜌𝐶𝑝
𝜎𝜀 (2)
Where,
Η = Fraction of work which transforms into heat
= 0.95
𝜎 =
𝑠𝑖𝑛𝑕−1
[(𝜀/𝐴)
1
𝑛 𝑒
𝑄
𝑛𝑅𝑇 ]
0.0115 𝑥 10−3
𝑛 = −0.97 + 3.787/𝜀0.368
𝑙𝑛⁡(𝐴) = 13.92 + 9.023/𝜀0.502
𝑄 = 125 + 133.3/𝜀0.393
RESEARCH ARTICLE OPEN ACCESS
Ramakrishnan Sumathi Int. Journal of Engineering Research and Applications www.ijera.com
ISSN: 2248-9622, Vol. 6, Issue 3, (Part -2) March 2016, pp.19- 23
www.ijera.com 20|P a g e
𝜌 = 𝐷𝑒𝑛𝑠𝑖𝑡𝑦 = 7.8 𝑔𝑚/𝑐𝑚3
𝐶𝑝 = 𝑆𝑝𝑒𝑐𝑖𝑓𝑖𝑐 𝑕𝑒𝑎𝑡 = 496 𝐽/𝐾𝑔𝐾
The dynamic equation for grain size can be
obtained by differentiating the equation (1) with
respect to temperature and then multiplied by
change in temperature T, which follows that,
𝜕𝑑
𝜕𝑡
=
−0.27 𝑑𝑄𝜂 𝑠𝑖𝑛𝑕−1 𝜀
𝐴
1
𝑛
𝑒
𝑄
𝑛𝑅𝑇 𝜀
𝑅𝑇2 𝜌𝐶𝑝 𝑥 0.0115 𝑥 10−3
(3)
III. OPEN LOOP MODEL
It is proposed to optimize the grain size of
26m from the initial grain size of 180m. The
Matlab/Simulink simulation model for open loop
system is obtained from the equation (3). The
steady state operating ranges for the control
parameters temperature, strain, strain rate and the
grain size are considered as,
𝑇 = 1200𝐾 𝑡𝑜 1300𝐾
𝜀 = 0.5 𝑡𝑜 1
𝜀 = 0 𝑡𝑜 1
𝑑 = 180𝜇𝑚 𝑡𝑜 26𝜇𝑚
IV. PID CONTROLLER WITH ANTI-
WINDUP
PID controllers are used extensively in the
industry as an all-in-all controller, mostly because
it is an intuitive control algorithm. A theoretical
PID controller [6] is
𝑢 𝑡 = 𝐾𝑝 [𝑒 𝑡 +
1
𝑇𝑖
𝑒 𝜏
𝑡
0
𝑑𝜏 + 𝑇𝑑
𝑑𝑒(𝑡)
𝑑𝑡
]
Where,
u(t) = the input signal to the plant model
e(t) = the error signal is defined as e(t) = r(t) – y(t)
r(t) = the reference input signal.
y(t) = plant output
Kp, Ti and Td are the proportional gain,
integral time and derivative time respectively. The
coefficients Kp, Ti, Td and P, I, D are related by:
P = Kp ; I = Kp/Ti ; D = KpTd
The controller has three parts:
The proportional term (P) gives a system
control input proportional with the error. Using
only P control gives a stationary error in all cases
except when the system control input is zero and
the system process value equals the desired value.
The proportional term is providing an overall
control action proportional to the error signal
through the all-pass gain factor.
The integral term (I) gives an addition
from the sum of the previous errors to the system
control input. The summing of the error will
continue until the system process value equals the
desired value and these results in no stationary
error when the reference is table. Theintegral term
is reducing steady-state errors through low-
frequency compensation by an integrator.
The derivative term (D) gives an addition
from the rate of change in the error to the system
control input. A rapid change in the error will give
an addition to the system control input. This
improves the response to a sudden change in the
system state or reference value. The derivative term
is improving transient response through high-
frequency compensation by a differentiator.
The derivative term can improve the
stability of the closed loop system but the
drawback of derivative action is that an ideal
derivative controller has very high gain for high
frequency signals. The derivative action has to be
filtered in order to make the controller proper and
to filter the measurement noise; in addition, the
derivative action is often applied directly to the
process variable instead of to the control error in
order to avoid the so-called derivative kick when a
step signal is applied to the set-point. The
derivative filter has to be taken into consideration
in the overall design of the controller [13]. To
avoid this problem, a first order low pass filter is
placed on the derivative term and its pole is tuned.
Since it attenuates high frequency noise, the
chattering due to the noise does not occur. The low
pass filter to be incorporated into the derivative
term is,
𝐺 𝑚𝑑 𝑠 =
𝑇𝑑 𝑠
𝑇 𝑑
𝑁
𝑠 + 1
(4)
Where, Td and N denote derivative time
constant and filter coefficients respectively. In the
commercial PID controllers, the value of N should
be in the range 2 < N < 100 to meet the desired
performance.
It has been recognized for many years that
actuator saturations, which are present in most
control systems, can cause undesirable effects such
as excessive overshoots, long settling times [2], and
in some cases instability. These phenomena were
initially observed for systems controlled by
conventional PID control but will be present in any
dynamical controller with relatively slow or
unstable states [5].
The problem arises when an actuator
saturates and results in a mismatch between the
controller output and the system input. A change in
the controller output does not affect the system.
The integrator in the PID controller, for example, is
an unstable state, and saturations can cause the
integrator to drift to undesirable values as the
integrator will continue to integrate a tracking error
and produce even larger control signals. In other
words, the integrator windupcan lock the system in
saturation. Control techniques designed to reduce
Ramakrishnan Sumathi Int. Journal of Engineering Research and Applications www.ijera.com
ISSN: 2248-9622, Vol. 6, Issue 3, (Part -2) March 2016, pp.19- 23
www.ijera.com 21|P a g e
the effects from integrator windup are known as
anti-windup[6]. The integral windup may occur in
connection with large setpoint changes or by large
disturbances or by equipment malfunctions.
Windup can also happen when selectors are used to
the fact that several controllers are driving one
actuator. In cascade control, windup may occur in
the primary controller when the secondary
controller is switched to manual mode, if it uses its
local setpoint, or if its control signal saturates.
The impact of this integrator windup is to
be minimized to obtain a faster rise time with less
overshoot. Hence, anti-windup schemes are
necessary to minimize performance degradation.
For continuous time-controlled systems, there
exists a large repertoire of so-called anti-windup
techniques to compensate the potential
performance degradation due to saturating
actuators [7], [8], [10].
This is achieved by placing a saturation
block at the output of the PID controller. It has an
extra feedback path around the integrator. The
signal e(t) is the difference between the nominal
controller output v(t) and the saturated controller
output u(t). The signal e(t) is fed to the input of the
integrator through gain 1/Tt. The extra feedback
loop reduces the input to the integrator in
proportion to the saturation error [11]. The time
constant Ttdetermines the speed with which the
integral term is reset. It is chosen as Tt< Ti, where
Ti is an integral time of the controller [12]. The
signal e(t) is zero when there is no saturation.
Under this condition, it will not have any effect on
the integrator. When the actuator saturates, the
signal e(t) is different from zero and it will try to
drive the integrator output to a value such that the
signal v(t) is close to the saturation limit.
By nesting PID controller using anti-
windup mechanism with the carbon steel
optimization system, full control and robust
requirements are achieved. The controller
parameters are all squared up using trial and error
method. After several trial and error runs, the
nominal values of the PID controller parameters are
set as,
𝐾𝑝 = 5
𝐾𝑖 = 2
𝐾𝑑 = 1.25
𝑇𝑑 =
𝐾𝑑
𝐾𝑝
= 0.25
𝑇𝑖 =
𝐾𝑝
𝐾𝑖
= 2.5
Since Tt< Ti, let𝑇𝑡 = 2.5 and N = 100 to
provide the desired response. The derivative filter
time constant is calculated as,
𝜏𝑓 =
𝑇𝑑
𝑁
=
0.25
100
= 0.0025
The closed loop control system with a
negative unity feedback is shown in Figure 1. Here,
the PID controller with a derivative filter and the
anti-windup mechanism is implemented for
strengthening the carbon steel.
Figure.1Block Diagram to Optimize Grain Size by
PID Controller with anti-windup
The PID controller with anti-windup
implemented in optimization of grain size is shown
in Figure 2.
Figure.2PID Controller with anti-windup
V. SIMULATION AND ERROR
CALCULATION
On the above analyzing, the simulations
are carried out for the grain size optimization in
Matlab-simulink using the solver ODE45 to
examine the performance of the proposed control
system
The process control parameters strain,
strain rate and temperature are optimized for a
required grain size of 26μm from an initial grain
size of 180μm and its corresponding trajectories are
shown in Figure 3. The time taken is in seconds.
The performances such as settling time,
integral square error (ISE) and integral absolute
error (IAE) values are obtained in PID controller
with anti-windup technique which is tabulated in
Table 1.
Ramakrishnan Sumathi Int. Journal of Engineering Research and Applications www.ijera.com
ISSN: 2248-9622, Vol. 6, Issue 3, (Part -2) March 2016, pp.19- 23
www.ijera.com 22|P a g e
Figure.3Response for Grain Size of 26μm
TABLE 1 Performance analysis
Set point Settling Time
(sec)
ISE IAE
26μm 0.035 274.4 2.521
30μm 0.037 282.8 2.542
35μm 0.041 285.5 2.584
VI. CONCLUSION
The dynamic model for 0.3% carbon steel
for microstructure control is developed. The steady
state value for strain, strain rate and temperature to
obtain grain size from 180m to 26m are selected
as 1, 1 and 1100 respectively. The dynamic model
is simulated by PID controller with anti-windup to
optimize grain size from 180m to 26m.
Simulation time of 10 seconds is considered and
the optimization is done. The settling time, integral
square error and integral absolute error are also
calculated. It is observed that the settling time is
less and also the ISE and IAE are less.
From these results, PID controller with
anti-windup seems to be better choice for
optimization of process control parameters.
REFERENCES
[1]. D.E. Kirk: Optimal Control Theory: An
Introduction, Prentice-Hall Inc.,
Englewood Cliffs, NJ, 1970, pp. 29-46
and pp. 184-309.
[2]. Huang Chun-Qing, Peng Xia-Fu & Wang
Jun-Ping 2008, „Robust nonlinear PID
controllers for anti-windup design of
robot manipulators with an uncertain
Jacobian matrix‟, ActaAutomaticaSinica,
vol. 34, no. 9, pp. 1113-1121.
[3]. James C Malaset.al.,”Optimization of
microstructure development during hot
working using control
theory,”Metullurgical and Materials
Transactions A, Vol 28 A, pp.1921-1930,
Sep 1997.
[4]. L.W. Ma, X. Wu and K.
Xia,”Microstructure and property of a
medium carbon steel processed by equal
channel angular pressing”, materials
forum volume 32 –2008, Edited by
J.M. Cairney, S.P. Ringer and R.
Wuhrer© Institute of Materials
Engineering Australasia Ltd.
[5]. Doyle, J, Smith, R &Enns, D 1987,
„Control of plants with input saturation
nonlinearities‟, American Control
Conference, Minneapolis, USA, pp. 1034 –
1039.
[6]. YoubinPeng, DamirVrancic& Raymond
Hanus 1996, „Anti-windup, bumpless, and
conditioned transfer techniques for PID
controllers‟, IEEE on Control Systems,
vol. 16, no. 4, pp. 48-57.
[7]. Georg Alexander Kiener, Daniel Lehmann
& Karl Henrik Johansson 2014, „Actuator
saturation and anti-windup compensation
in event-triggered control‟, Discrete Event
Dynamics System, vol. 24, no. 2, pp. 173-
197.
[8]. AnirbanGhoshal&Vinod John 2010,
„Anti-windup schemes for proportional
integral and proportional resonant
controller‟, National Power Electronic
Conference, pp. 1-6.
[9]. Monika HRADILOVÁa,b, Frank
MONTHEILLET, Anna
FRACZKIEWICZ, Christophe
DESRAYAUD and Pavel LEJČEK,
“Microstructure development of ca-
doped mg–zn alloy during hot
deformation “, 23. – 25. 5. 2012,
Brno, Czech Republic, EU.
[10]. Xin-lan Li, Jong-Gyu Park &Hwi-Beom
Shin 2011, „Comparison and evaluation of
anti-windup PI controllers‟, Journal of
Power Electronics, vol. 11, no. 1, pp. 45-
50.
[11]. SrikanthMandarapu, SreedharLolla&
Suresh Kumar, MV 2013, „Digital PI
controller using anti-wind-up mechanism
for a speed controlled electric drive
system‟, International Journal of
Innovative Technology and Exploring
Engineering, vol. 3, no. 1, pp. 239-242.
[12]. StaffanHaugwitz, Maria Karlsson,
StephaneVelut& Per Hagander 2005,
„Anti-windup in mid-ranging control‟,
Proceedings of the 44th IEEE Conference
on Decision and Control, and the
European Control Conference, pp. 12-15.
[13]. Antonio Visioli, “Research Trends for PID
Controllers”, ActaPolytechnica, Vol. 52,
No. 5, pp: 144-150, 2012.
Ramakrishnan Sumathi Int. Journal of Engineering Research and Applications www.ijera.com
ISSN: 2248-9622, Vol. 6, Issue 3, (Part -2) March 2016, pp.19- 23
www.ijera.com 23|P a g e
AUTHOR PROFILE
Dr. R.Sumathi received the U.G degree in
Electrical and Electronics Engineering from
Madras University, Tamilnadu, in 1998 and P.G
degree in Process Control and Instrumentation
from Annamalai University, Tamilnadu in 2004.
She received her Ph.D degree in Electrical
Engineering from Anna University, Chennai,
Tamilnadu in 2015.

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A PID Controller with Anti-Windup Mechanism for Firminga Carbon Steel

  • 1. Ramakrishnan Sumathi Int. Journal of Engineering Research and Applications www.ijera.com ISSN: 2248-9622, Vol. 6, Issue 3, (Part -2) March 2016, pp.19- 23 www.ijera.com 19|P a g e A PID Controller with Anti-Windup Mechanism for Firminga Carbon Steel Ramakrishnan Sumathi Department of Electrical and Electronics Engineering Pavai College of Technology, Namakkal-637018, Tamil Nadu, India ABSTRACT In this Paper, a classical PID controller with anti-windup technique is employed for controlling the microstructure development during hot working process. The strength of any material is dependent on the grain size of that material [4], [9]. The strength of the material is increased when its grain size is reduced. In this paper, the standard Arrehenious equation of 0.3% carbon steel is utilized to obtain an optimal deformation path such that the grain size of the product should be 26m. The 0.3% carbon steel improves in the machinability by heat treatment [8]. It must also be noted that this steel is especially adaptable for machining or forging and where surface hardness is desirable. The plant model is developed with grain size. The effect of process control parameters such as strain, strain rate, and temperature on important microstructural features can be systematically formulated and then solved as an optimal control problem. These approaches are applied to obtain the desired grain size of 26m from an initial grain size of 180m. The simulation is done on various grain sizes using the controller by MATLAB simulink toolbox. From the response it is found that the PID controller with anti-windup provides better performance. Resulting tabulated performance indices showed a considerable improvement in settling time besides reducing steady state error. Keywords– Carbon steel, strain, strain rate, temperature, PID Controller, anti-windup. I. INTRODUCTION The development of optimal design and control methods for manufacturing processes is needed for effectively reducing part cost, improving part delivery schedules, and producing specified part quality on a repeatable basis. Existing design methods are generally ad hoc and lack adequate capabilities for finding effective process parameters such as deformation rate, die and work piece temperature, and tooling system configuration. This situation presents major challenges to process engineers who are faced with smaller lot sizes, higher yield requirements, and superior quality standards. Therefore, it is important to develop new systematic methodologies for process design and control based upon scientific principles, which sufficiently consider the behavior of work piece material and the mechanics of the manufacturing process. A new strategy for systematically calculating near optimal control parameters for control of microstructure during hot deformation processes has been developed based on optimal control theory [1].This approach treats the deforming material as a dynamical system explained below. II. STATIC AND DYNAMIC MODEL The static model of 0.3% carbon steel [3] is, 𝑑 = 22600 𝜀−0.27 𝑒−0.27 𝑄/𝑅𝑇 (1) Where, d = grain size ε = strain ε = strain rate Q = Activation energy for dynamic recrystallization = 267KJmol−1 R = Gas constant = 8.314 x 10−3 KJK−1 mol−1 T = Billet temprature The dynamic model of 0.3% carbon steel is obtained by using the Arrehenius equation for changes in temperature during hot extrusion is given below. 𝜕𝑇 𝜕𝑡 = 𝑇 = 𝜂 𝜌𝐶𝑝 𝜎𝜀 (2) Where, Η = Fraction of work which transforms into heat = 0.95 𝜎 = 𝑠𝑖𝑛𝑕−1 [(𝜀/𝐴) 1 𝑛 𝑒 𝑄 𝑛𝑅𝑇 ] 0.0115 𝑥 10−3 𝑛 = −0.97 + 3.787/𝜀0.368 𝑙𝑛⁡(𝐴) = 13.92 + 9.023/𝜀0.502 𝑄 = 125 + 133.3/𝜀0.393 RESEARCH ARTICLE OPEN ACCESS
  • 2. Ramakrishnan Sumathi Int. Journal of Engineering Research and Applications www.ijera.com ISSN: 2248-9622, Vol. 6, Issue 3, (Part -2) March 2016, pp.19- 23 www.ijera.com 20|P a g e 𝜌 = 𝐷𝑒𝑛𝑠𝑖𝑡𝑦 = 7.8 𝑔𝑚/𝑐𝑚3 𝐶𝑝 = 𝑆𝑝𝑒𝑐𝑖𝑓𝑖𝑐 𝑕𝑒𝑎𝑡 = 496 𝐽/𝐾𝑔𝐾 The dynamic equation for grain size can be obtained by differentiating the equation (1) with respect to temperature and then multiplied by change in temperature T, which follows that, 𝜕𝑑 𝜕𝑡 = −0.27 𝑑𝑄𝜂 𝑠𝑖𝑛𝑕−1 𝜀 𝐴 1 𝑛 𝑒 𝑄 𝑛𝑅𝑇 𝜀 𝑅𝑇2 𝜌𝐶𝑝 𝑥 0.0115 𝑥 10−3 (3) III. OPEN LOOP MODEL It is proposed to optimize the grain size of 26m from the initial grain size of 180m. The Matlab/Simulink simulation model for open loop system is obtained from the equation (3). The steady state operating ranges for the control parameters temperature, strain, strain rate and the grain size are considered as, 𝑇 = 1200𝐾 𝑡𝑜 1300𝐾 𝜀 = 0.5 𝑡𝑜 1 𝜀 = 0 𝑡𝑜 1 𝑑 = 180𝜇𝑚 𝑡𝑜 26𝜇𝑚 IV. PID CONTROLLER WITH ANTI- WINDUP PID controllers are used extensively in the industry as an all-in-all controller, mostly because it is an intuitive control algorithm. A theoretical PID controller [6] is 𝑢 𝑡 = 𝐾𝑝 [𝑒 𝑡 + 1 𝑇𝑖 𝑒 𝜏 𝑡 0 𝑑𝜏 + 𝑇𝑑 𝑑𝑒(𝑡) 𝑑𝑡 ] Where, u(t) = the input signal to the plant model e(t) = the error signal is defined as e(t) = r(t) – y(t) r(t) = the reference input signal. y(t) = plant output Kp, Ti and Td are the proportional gain, integral time and derivative time respectively. The coefficients Kp, Ti, Td and P, I, D are related by: P = Kp ; I = Kp/Ti ; D = KpTd The controller has three parts: The proportional term (P) gives a system control input proportional with the error. Using only P control gives a stationary error in all cases except when the system control input is zero and the system process value equals the desired value. The proportional term is providing an overall control action proportional to the error signal through the all-pass gain factor. The integral term (I) gives an addition from the sum of the previous errors to the system control input. The summing of the error will continue until the system process value equals the desired value and these results in no stationary error when the reference is table. Theintegral term is reducing steady-state errors through low- frequency compensation by an integrator. The derivative term (D) gives an addition from the rate of change in the error to the system control input. A rapid change in the error will give an addition to the system control input. This improves the response to a sudden change in the system state or reference value. The derivative term is improving transient response through high- frequency compensation by a differentiator. The derivative term can improve the stability of the closed loop system but the drawback of derivative action is that an ideal derivative controller has very high gain for high frequency signals. The derivative action has to be filtered in order to make the controller proper and to filter the measurement noise; in addition, the derivative action is often applied directly to the process variable instead of to the control error in order to avoid the so-called derivative kick when a step signal is applied to the set-point. The derivative filter has to be taken into consideration in the overall design of the controller [13]. To avoid this problem, a first order low pass filter is placed on the derivative term and its pole is tuned. Since it attenuates high frequency noise, the chattering due to the noise does not occur. The low pass filter to be incorporated into the derivative term is, 𝐺 𝑚𝑑 𝑠 = 𝑇𝑑 𝑠 𝑇 𝑑 𝑁 𝑠 + 1 (4) Where, Td and N denote derivative time constant and filter coefficients respectively. In the commercial PID controllers, the value of N should be in the range 2 < N < 100 to meet the desired performance. It has been recognized for many years that actuator saturations, which are present in most control systems, can cause undesirable effects such as excessive overshoots, long settling times [2], and in some cases instability. These phenomena were initially observed for systems controlled by conventional PID control but will be present in any dynamical controller with relatively slow or unstable states [5]. The problem arises when an actuator saturates and results in a mismatch between the controller output and the system input. A change in the controller output does not affect the system. The integrator in the PID controller, for example, is an unstable state, and saturations can cause the integrator to drift to undesirable values as the integrator will continue to integrate a tracking error and produce even larger control signals. In other words, the integrator windupcan lock the system in saturation. Control techniques designed to reduce
  • 3. Ramakrishnan Sumathi Int. Journal of Engineering Research and Applications www.ijera.com ISSN: 2248-9622, Vol. 6, Issue 3, (Part -2) March 2016, pp.19- 23 www.ijera.com 21|P a g e the effects from integrator windup are known as anti-windup[6]. The integral windup may occur in connection with large setpoint changes or by large disturbances or by equipment malfunctions. Windup can also happen when selectors are used to the fact that several controllers are driving one actuator. In cascade control, windup may occur in the primary controller when the secondary controller is switched to manual mode, if it uses its local setpoint, or if its control signal saturates. The impact of this integrator windup is to be minimized to obtain a faster rise time with less overshoot. Hence, anti-windup schemes are necessary to minimize performance degradation. For continuous time-controlled systems, there exists a large repertoire of so-called anti-windup techniques to compensate the potential performance degradation due to saturating actuators [7], [8], [10]. This is achieved by placing a saturation block at the output of the PID controller. It has an extra feedback path around the integrator. The signal e(t) is the difference between the nominal controller output v(t) and the saturated controller output u(t). The signal e(t) is fed to the input of the integrator through gain 1/Tt. The extra feedback loop reduces the input to the integrator in proportion to the saturation error [11]. The time constant Ttdetermines the speed with which the integral term is reset. It is chosen as Tt< Ti, where Ti is an integral time of the controller [12]. The signal e(t) is zero when there is no saturation. Under this condition, it will not have any effect on the integrator. When the actuator saturates, the signal e(t) is different from zero and it will try to drive the integrator output to a value such that the signal v(t) is close to the saturation limit. By nesting PID controller using anti- windup mechanism with the carbon steel optimization system, full control and robust requirements are achieved. The controller parameters are all squared up using trial and error method. After several trial and error runs, the nominal values of the PID controller parameters are set as, 𝐾𝑝 = 5 𝐾𝑖 = 2 𝐾𝑑 = 1.25 𝑇𝑑 = 𝐾𝑑 𝐾𝑝 = 0.25 𝑇𝑖 = 𝐾𝑝 𝐾𝑖 = 2.5 Since Tt< Ti, let𝑇𝑡 = 2.5 and N = 100 to provide the desired response. The derivative filter time constant is calculated as, 𝜏𝑓 = 𝑇𝑑 𝑁 = 0.25 100 = 0.0025 The closed loop control system with a negative unity feedback is shown in Figure 1. Here, the PID controller with a derivative filter and the anti-windup mechanism is implemented for strengthening the carbon steel. Figure.1Block Diagram to Optimize Grain Size by PID Controller with anti-windup The PID controller with anti-windup implemented in optimization of grain size is shown in Figure 2. Figure.2PID Controller with anti-windup V. SIMULATION AND ERROR CALCULATION On the above analyzing, the simulations are carried out for the grain size optimization in Matlab-simulink using the solver ODE45 to examine the performance of the proposed control system The process control parameters strain, strain rate and temperature are optimized for a required grain size of 26μm from an initial grain size of 180μm and its corresponding trajectories are shown in Figure 3. The time taken is in seconds. The performances such as settling time, integral square error (ISE) and integral absolute error (IAE) values are obtained in PID controller with anti-windup technique which is tabulated in Table 1.
  • 4. Ramakrishnan Sumathi Int. Journal of Engineering Research and Applications www.ijera.com ISSN: 2248-9622, Vol. 6, Issue 3, (Part -2) March 2016, pp.19- 23 www.ijera.com 22|P a g e Figure.3Response for Grain Size of 26μm TABLE 1 Performance analysis Set point Settling Time (sec) ISE IAE 26μm 0.035 274.4 2.521 30μm 0.037 282.8 2.542 35μm 0.041 285.5 2.584 VI. CONCLUSION The dynamic model for 0.3% carbon steel for microstructure control is developed. The steady state value for strain, strain rate and temperature to obtain grain size from 180m to 26m are selected as 1, 1 and 1100 respectively. The dynamic model is simulated by PID controller with anti-windup to optimize grain size from 180m to 26m. Simulation time of 10 seconds is considered and the optimization is done. The settling time, integral square error and integral absolute error are also calculated. It is observed that the settling time is less and also the ISE and IAE are less. From these results, PID controller with anti-windup seems to be better choice for optimization of process control parameters. REFERENCES [1]. D.E. Kirk: Optimal Control Theory: An Introduction, Prentice-Hall Inc., Englewood Cliffs, NJ, 1970, pp. 29-46 and pp. 184-309. [2]. Huang Chun-Qing, Peng Xia-Fu & Wang Jun-Ping 2008, „Robust nonlinear PID controllers for anti-windup design of robot manipulators with an uncertain Jacobian matrix‟, ActaAutomaticaSinica, vol. 34, no. 9, pp. 1113-1121. [3]. James C Malaset.al.,”Optimization of microstructure development during hot working using control theory,”Metullurgical and Materials Transactions A, Vol 28 A, pp.1921-1930, Sep 1997. [4]. L.W. Ma, X. Wu and K. Xia,”Microstructure and property of a medium carbon steel processed by equal channel angular pressing”, materials forum volume 32 –2008, Edited by J.M. Cairney, S.P. Ringer and R. Wuhrer© Institute of Materials Engineering Australasia Ltd. [5]. Doyle, J, Smith, R &Enns, D 1987, „Control of plants with input saturation nonlinearities‟, American Control Conference, Minneapolis, USA, pp. 1034 – 1039. [6]. YoubinPeng, DamirVrancic& Raymond Hanus 1996, „Anti-windup, bumpless, and conditioned transfer techniques for PID controllers‟, IEEE on Control Systems, vol. 16, no. 4, pp. 48-57. [7]. Georg Alexander Kiener, Daniel Lehmann & Karl Henrik Johansson 2014, „Actuator saturation and anti-windup compensation in event-triggered control‟, Discrete Event Dynamics System, vol. 24, no. 2, pp. 173- 197. [8]. AnirbanGhoshal&Vinod John 2010, „Anti-windup schemes for proportional integral and proportional resonant controller‟, National Power Electronic Conference, pp. 1-6. [9]. Monika HRADILOVÁa,b, Frank MONTHEILLET, Anna FRACZKIEWICZ, Christophe DESRAYAUD and Pavel LEJČEK, “Microstructure development of ca- doped mg–zn alloy during hot deformation “, 23. – 25. 5. 2012, Brno, Czech Republic, EU. [10]. Xin-lan Li, Jong-Gyu Park &Hwi-Beom Shin 2011, „Comparison and evaluation of anti-windup PI controllers‟, Journal of Power Electronics, vol. 11, no. 1, pp. 45- 50. [11]. SrikanthMandarapu, SreedharLolla& Suresh Kumar, MV 2013, „Digital PI controller using anti-wind-up mechanism for a speed controlled electric drive system‟, International Journal of Innovative Technology and Exploring Engineering, vol. 3, no. 1, pp. 239-242. [12]. StaffanHaugwitz, Maria Karlsson, StephaneVelut& Per Hagander 2005, „Anti-windup in mid-ranging control‟, Proceedings of the 44th IEEE Conference on Decision and Control, and the European Control Conference, pp. 12-15. [13]. Antonio Visioli, “Research Trends for PID Controllers”, ActaPolytechnica, Vol. 52, No. 5, pp: 144-150, 2012.
  • 5. Ramakrishnan Sumathi Int. Journal of Engineering Research and Applications www.ijera.com ISSN: 2248-9622, Vol. 6, Issue 3, (Part -2) March 2016, pp.19- 23 www.ijera.com 23|P a g e AUTHOR PROFILE Dr. R.Sumathi received the U.G degree in Electrical and Electronics Engineering from Madras University, Tamilnadu, in 1998 and P.G degree in Process Control and Instrumentation from Annamalai University, Tamilnadu in 2004. She received her Ph.D degree in Electrical Engineering from Anna University, Chennai, Tamilnadu in 2015.