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IOSR Journal of Electrical and Electronics Engineering (IOSR-JEEE)
e-ISSN: 2278-1676,p-ISSN: 2320-3331, Volume 10, Issue 4 Ver. I (July – Aug. 2015), PP 10-16
www.iosrjournals.org
DOI: 10.9790/1676-10411016 www.iosrjournals.org 10 | Page
Comparative Study of Monotonic and Non- Monotonic Phase LTI
systems using Improved Analytical PID controller
Monica U. Waikar1
, Nishij G. Kulkarni2
, Dr. Ravindrakumar M. Nagarale3
1
(PG student, M.B.E. Society’s college of engineering, Ambajogai, Maharashtra, India)
2,3
(PG Department, M.B.E. Society’s College of engineering, Ambajogai, Maharashtra, India)
Abstract : A comparative study of monotonic and non monotonic phase LTI systems using analytical design of
PID controller, by means of gain cross over frequency and phase margin specifications, is presented in the
paper. The proposed methodology ensures minimum phase margin inside desired bandwidth giving accurate
performance to step response for closed loop system. Concept of phase margin needs to be redefined when
uncontrolled process presents minimum phase inside bandwidth. For comparative study, bode stability
criterion, nyquist stability criterion and unit step response is used.
Keywords: Improved analytical controller , linear system compensation, monotonic and non-monotonic phase
LTI system.
I. Introduction
A system that maintains a prescribed relationship between the output and the reference input by
comparing them and using the difference as a means of control is called a feedback control system. In case of
feedback control system for monotonically decreasing phase inside bandwidth, phase margin can be defined as
distance between open loop phase at gain crossover frequency and stability limit of−180°. After using bode
stability criterion, if phase margin is positive then closed loop system is stable [1]
In case of classical frequency response it can be considered that phase margin can be defined on gain
cross-over frequency. Whereas this assumption is not valid in general practice, because even for a minimum
phase system with a left half-plane zero located near the dominant- poles, its frequency response will present a
non-monotonic phase.
This abrupt technique shows an improved frequency response design technique for monotonic or non-
monotonic phase (inside the bandwidth) dynamical systems based on gain crossover frequency and phase
margin specifications, which is an expansion of the technique shown by Phillips and Harbor [2], by using this
feature comparative study of monotonic and non-monotonic phase LTI system is possible. To achieve this
feature concept of phase margin can be redefined when the system frequency response shows a non-
monotonically decreasing phase inside the bandwidth. The study of phase margin is necessary due to two
reasons such as it can be considered as good robustness indicator and which allows bode stability criterion for
monotonic and non-monotonic minimum phase systems.
The detailed organization is as follows: section 2 presents problem formulation, some remarks about non-
monotonically decreasing phase can be addressed, for that purpose considered the DC-DC buck regulator.
Section 3 explains detailed study of PID controller design. Section 4 is concerned about simulation and results
where comparative study of monotonic and non-monotonic systems is also explained. Section 5 has conclusion.
II. Problem Formulation
Continuous LTI dynamical system is considered which is given by differential equation,
y(t) + a1 y(t)a0y t = b1u(t) + b0 u t (1)
Here LC low pass filter is to be considered which is commonly used in different type of power
electronics. Hence assume synchronous buck regulator having model no. IRU 3038 used as voltage tracking
application such as DC-DC converter and DDR memory [3]. Buck regulator is taken into considerations which
are combination of power stage given by LC low pass filter and pulse width modulation based controller. The
transfer function of buck converter is output(regulated voltage) to input(PWM input voltage) is,
G s =
VIN
VOSC
1+sRC C
LCS
2 +s RC C+
L
R
+1
(2)
Where ,L is the output inductance, C is the output capacitance, R is the load resistance, RC is the output
capacitor intrinsic resistance,VOSC is the PWM oscillator reference voltage and VIN is the power stage input
voltage. Here assume typical application for buck regulator [3], RC=40ohm, gives transfer function,
G s =
4(1+1.2×10−5s)
3×10−9 s2 +3.6×10−5 s+1
(3)
Comparative Study Of Monotonic And Non-Monotonic Phase Lti Systems Using
DOI: 10.9790/1676-10411016 www.iosrjournals.org 11 | Page
Where the un-damped frequency is approximately 18 Krad/s and the damping ratio is approximately 0.33.
Using this transfer function for buck regulator we can find out bode plot shown in fig.1. Here a valley in phase
curve close to un-damped frequency is to be seen. From this we can conclude that left half-plane zero due to the
output capacitor intrinsic resistance is not located far enough from the poles. Hence this leads to non monotonic
phase compensation because bandwidth is located after zero frequency. Due to this transfer function is in
minimum phase and use of bode plot is not possible. Hence we have to study the improved technique of design
of PID controller[4].
Fig.2 Bode plot for Buck regulator
III. Design Of PID Controller
he PID controller is the most common form of feedback. It was an essential element of early governors
and it became the standard tool when process control emerged in the 1940s. In control system today, more than
95% of the control loops are of PID type, most loops are actually PI control. PID controllers are today found in
all areas where control is used. The controllers come in many different forms[5]. PID control is an important
ingredient of a distributed control system. The controllers are also embedded in many special-purpose control
systems. For improving PID control there are various methods such as empiric method by Ziegler and Nichols
and analytical compensation based on pole-placement and frequency response method[6] [7] due to this
popularity of PID controller is tremendously increased.
Consider equation for PID controller,
K s = KP 1 +
1
T1s
TDs (5)
Where KP is the proportional gain,KI is the integral action time or reset time, and TD is known as the derivative
action time or rate time [1], [3].
Fig.1 Design of PID control of plant
For designing of PID controller one tuning method is used i.e. Ziegler Nichols tuning method. This
process of selecting the controller parameters to meet given performance specifications is known as controller
tuning. Ziegler and Nichols suggested rules for tuning PID controllers based on experimental step responses or
based on the value of that results in marginal stability when only proportional control action is used. Ziegler–
Nichols rules, are useful when mathematical models of plants are not known. However, the resulting system
may exhibit a large maximum overshoot in the step response, which is unacceptable. In such case we need series
of fine tunings until an acceptable result is obtained. In fact, the Ziegler–Nichols tuning rules give an educated
guess for the parameter values and provide a starting point for fine tuning, rather than giving the final settings in
a single shot.[6]-[7]. It should be noted that worst case frequency is exactly the gain crossover frequency i.e., it
defines a monotonic phase system, then the set of (4) becomes the well-known compensating equations shown
by Phillips and Harbor [2].
Comparative Study Of Monotonic And Non-Monotonic Phase Lti Systems Using
DOI: 10.9790/1676-10411016 www.iosrjournals.org 12 | Page
KP =
1
G(jωn ) 1+ ωu TD −
1
ωu TI
(5a)
ωuTD −
1
ωu TI
= tan φ (5b)
φ ≜ −180° + ∅m −< G(jωm ) (5c)
One major drawback of PID controller is that, it has less equations than variables therefore it is very
important to characterize equations having TIand TD values. By rewriting eq (5) in terms of KP and TD gives,
KP =
1
G(jωn ) 1+Ω2 tan φ+
1−Ω−2
ωm TI
2
(6a)
TD =
tan φ
ωm
+
1
ωm
2 TI
(6b)
By using above equations, variations in PI and PD are occurred having a single unique solution each. In
general practice, the PID controller should not be usually used to compensate non-monotonic phase dynamical
systems since these systems, by their own natural behaviour, already present left half-plane zeros in the open-
loop transfer function, yielding a phase-lead effect very similar to the derivative term present in the standard
form in (6). Therefore, the next subsections will present the equations and some comments on the PI and PD
variations.
3.1 PD controller
Assume TI equal to infinity in eq 5(a,b) we obtain,
KP =
1
G(jωn ) 1+Ω2 tan φ2
(7a)
TD =
tan φ
ωm
(7b)
or KD = KPTD =
ωu
−1
G(jωn ) 1+Ω2 cot φ2
(7c)
Now, it should be noted that if monotonicity ratio is larger than KP gain will be smaller and KD gain will be
larger..
3.2 PI controller
Consider TD equal to zero in eq 5(a,b),
KP =
1
G(jωn ) 1+Ω−2 tan φ2
(8a)
TI = −
cot φ
ωm
(8b)
KI =
KP
TI
=
ωu
G(jωn ) 1+Ω2 cot φ2
(8c)
Here, if monotonicity ratio is larger then KP gain will be larger and KI gain will be smaller. In case of non
monotonic phase system as monotonic phase one should lead overvalued KP gain and to an undervalued KD
gain..Due to this reason compensation of non monotonic phase system as monotonic system is avoided in case
of integral action.
IV. Results And Simulation
In this section tools are presented such as fundamental tools and robustness tools which are widely used in
literature.
4.1 Fundamental tools
In fundamental tools consider the factors which are very important for analytical design procedure.
This procedure gives gain crossover frequency and phase margin for stable and minimum phase using transfer
function which can be obtained from bode criterion. Here damping ratio and un-damped frequency is necessary
having transfer function of second order system.
Let us consider negative feedback system into a low-pass behaviour in the open-loop frequency
response, then define four parameters which can be used in frequency response compensation for dynamical LTI
Comparative Study Of Monotonic And Non-Monotonic Phase Lti Systems Using
DOI: 10.9790/1676-10411016 www.iosrjournals.org 13 | Page
systems with non monotonic phase inside bandwidth such as worst case frequency ωm, gain cross over phase
margin ∅u, gain crossover frequency ωu, worst case phase margin ∅m .
The characteristic equation is gain cross over frequency and stability limit of −180° is ωu . For bode
stability criterion if ∅u is positive then system is stable, when system response represents lowest phase inside
bandwidth which is smaller than or equal to the gain crossover frequency ωu whereas worst case phase
margin∅m is distance between open loop phase in worst case frequencyωm, and stability limit of −180°. Solve
equation for frequency domain
K(jωu)G(jωu ∠K jωu G jωu = 1∠ − 180° + ∅u (9a)
With ∅m ≤ ∅u (9b)
If the worst case phase margin ∅ 𝑚 is positive then gain crossover phase margin∅ 𝑢 is positive then system
becomes stable, then 𝜔𝑢 is always larger than or equal to𝜔 𝑚 . Apply bode stability criterion for above equation
it gives,
K(jωu =
1
G(jωu )
(10a)
∠K jωm = −180° + ∅m − ∠G jωm (10b)
With ωm ≤ ωu (10c)
Here to check how system is monotonic then we have to define monotonicity ratio is given by,
Ω ≜
ωu
ωm
(11)
Ω is always greater than or equal to 1. This ratio indicates that if values of is larger then system tends to
non monotonic phase. In next section find the parameters which are useful to shape open loop feedback system
into low pass behaviour inside bandwidth and step response for closed loop system in case of gain cross over
frequency and phase margin.
4.2 Robustness tools
The analytical design procedure includes various characteristics such as stability, performance and robustness.
Above section present stability term now consider factors for designing compensator such as performance and
robustnesss. For future procedure ϰ∞ theory is considered[1]. By using this theory sensitivity function is given
by,
S(jω) ∞ = maxm S(jω) ≤ Ms (12a)
Where
S s = 1 + K s G(s) −1
(12b)
Which is more acceptable as robustness measure [1],[9]. Here Nyquist plot is used where S(jω) ∞ is inverse of
minimum distance from loop transfer function to critical point(-1,0). Therefore if nyquist plot avoids circle
having centre point (-1,0) and radius 1 by MS then it is said that system is robust related to sensitivity function
which are explained in [1],[8],[9]. To obtain better performance of robustness tools consider another
complimentary sensitivity function,
T(jω) ∞ = maxω T(jω) ≤ MT (13a)
where
T s = K s G(s) 1 + K s G(s) −1
(13b)
Here nyquist plot having centre −MT
2
/(MT
2
− 1),0 and radius (MT/MT
2
− 1) is used. If nyquist plot
avoids circle then it is said that system is robust related to complimentary function. For future work use values
given by Skogestad and Postlethwaite as MS =2 and MT=1.25 and Kristiansson and Lennartson suggest
valuesMS =1.7 and MT=1.4 [1],[9]. After comparison we have final conclusion that values suggested by
Skogestad and Postlethwaite are more accurate.
4.3 Comparison of monotonic and non-monotonic system
It describes the results obtained from proposed methodology and buck regulator which is shown in
section 2. The results can be verified by using MATLAB simulink method. In this case it can be found that the
un-damped frequency is near about or equal to 18 krad/s and left half-plane zero frequency is near about or
equal to 83 krad/s[6]. Assume switching frequency of the converter to be equal to 200 kHz (approximately 1250
krad/s), by using reference it is said that gain cross-over frequency is about fifth times the switching
frequency[3]. Therefore the specified gain cross-over frequency is near about 250 krad/s, from this it concludes
Comparative Study Of Monotonic And Non-Monotonic Phase Lti Systems Using
DOI: 10.9790/1676-10411016 www.iosrjournals.org 14 | Page
that system leads to non-monotonic phase where gain-crossover frequency is beyond the left half-plane zero
frequency.
Now the desired phase margin is 40, therefore desired specifications follows the closed loop system
performance having overshoot equal to 25% and a settling time equal to 40 s. In this case the feedback system
must in second order system.
In case of buck regulator non-monotonic phase system is obtained inside desired bandwidth, here PI
controller is superior than PID controller[3]. In this case two parameters for PI controller is studied, first can be
studied by using technique of Phillips and Harbor[2] and another from non-monotonic technique and finally
both results were compared. The values for compensator are shown in Table 1.
Table 1: Comparison of monotonic and non-monotonic compensation
Parameters Monotonic Non-Monotonic
𝐊 𝐏 12.19 14.76
𝐓𝐈[µsec] 5.86 223.05
From Table 1, worst case frequency is 40 krad/s which is close to frequency of buck regulator for non-
monotonic compensation. After comparing values for monotonic and non-monotonic, larger KP and larger TI
(smaller KI) value is found for non monotonic systems. For the monotonic compensation (dashed line) and for
the non-monotonic compensation (solid line), bode plot is presented in fig.3
It should be noticed that from fig.3, bandwidth is same for both compensation, where non-monotonic
system gives larger steady-state error for ramp response and it gives phase margin of at least 40 for all frequency
inside bandwidth whereas monotonic compensation only guarantees the phase margin required for the gain
crossover frequency[4]. It should be remembered that frequencies inside bandwidth only makes control action.
Monotonic compensation does not guarantees the phase margin inside desired bandwidth, since
systems are stable according to Routh–Hurwitz criterion[2],[7]. By using Routh–Hurwitz criterion integral
action time TI is 5.86 microsec and range of gain KP is located in between 0.023 and 2.646. Therefore there is
no real and positive gain able to give the non-monotonically compensated system to instability for the integral
action time equal to 223.05 s
Fig 3. Bode plots for the monotonic compensation (dashed line) and the non-monotonic compensation
(solid line)
From future analysis, monotonic compensation gives two openloop gains which cross the stability limit
of−180°, hence bode plot[1] is not sufficient for analysis. Therefore to check stability limit of both
compensation, we have to use Nyquist plot in frequency response. For the monotonic compensation (dashed
line) and for the non-monotonic compensation (solid line) is presented for Nyquist plot in fig.4
Comparative Study Of Monotonic And Non-Monotonic Phase Lti Systems Using
DOI: 10.9790/1676-10411016 www.iosrjournals.org 15 | Page
Fig 4. Nyquist plots for the monotonic compensation (dashed line) and the non-monotonic compensation
(solid line).
Applying stability criterion for both compensation in Nyquist plot, it should be obtained that monotonic
system is not useful for phase margin as it gives one encirclement around the -1 critical point. Whereas it does
not happened in case of non-monotonic phase systems. Fig.4 also shows that robustness boundaries (lighter
lines) of the sensitivity function (smaller circle) withMS =2 and complementary sensitivity function (larger
circle) withMT= 1.25[1]. From above fig.4 it is seen that monotonic systems are not robust regarding to
complimentary sensitivity function MT whreas non-monotonic system is robust in case of sensitivity
functionMS . Hence for non-monotonic system Nyquist plot gives accurate shape and results.
To find out accurate performance use of Step response is necessary, unit step response for the monotonic
compensation (dashed line) and of the non-monotonic compensation (solid line) is shown in Fig. 4. For unit step
response, monotonic phase system use second order system where non-monotonic phase system use first order
system. The settling time for the non-monotonically compensated system is approximately 40 s and for
monotonically compensated system is approximately 60 s. Whereas overshoot in case of non-monotonic system
is smaller than monotonic system, therefore non-monotonic system completes all robustness properties. From
above analysis, it should be noticed that non-monotonic phase gives accurate performance measure and its
Nyquist plot avoids the circle created by the robustness boundary, which the monotonic compensation does
not[1].
Fig 5. Unit step response of the monotonic compensation (dashed line) and the non-monotonic compensation
(solid line).
V. Conclusion
The comparative study of monotonic and non-monotonic phase LTI systems are presented in paper by
using improved analytical PID controller design using gain cross-over frequency and phase margin
specification. Using this methodology accurate results are obtained. Where minimum phase margin is obtained
inside desired bandwidth for closed loop system. Here non-monotonic phase gives more desirable results than
monotonic phase results for closed loop system. For comparative study Bode stability criterion, Nyquist
criterion and Unit step response are used, whereas nyquist plot are used for stability checking and results
obtained by using MATLAB simulink.
Comparative Study Of Monotonic And Non-Monotonic Phase Lti Systems Using
DOI: 10.9790/1676-10411016 www.iosrjournals.org 16 | Page
References
[1]. S. Skogestad and I. Postlethwaite, Multivariable Feedback Control:Analysis and Design. New York: Wiley, 2005
[2]. C. L. Philips and R. D. Harbor, Feedback Control Systems. Englewood Cliffs, NJ: Prentice-Hall, 1999
[3]. International Rectifier, “Synchronous PWM controller for termination power supply applications,” 2nd Ed., 2002
[4]. Caio F.de Paula and Luís H.C.Ferreira,, An Improved Analytical PID Controller Design for Non-Monotonic Phase LTI Systems ,
IEEE transaction on control system technology, vol.20 No.5, September 2012
[5]. K. J. Åström and T. Hägglund, Advanced PID Control. Research Triangle Park, NC: ISA, 2005.
[6]. J. G. Ziegler and N. B. Nichols, “Process lags in automatic control circuits,” Trans. Amer. Soc. Mechan. Eng., vol. 65, pp. 433–444,
1943.
[7]. K. Ogata, Modern Control Engineering. Englewood Cliffs, NJ: Prentice-Hall, 2009
[8]. K. H. Ang, G. Chong, and Y. Li, “PID control system analysis, design,and technology,” IEEE Trans. Control Syst. Technol., vol.
no. 4, pp.559–576, Jul. 2005.
[9]. B. Kristiansson and B. Lennartson, “Robust and optimal tuning of PIand PID controllers,” IEE Proc.-Control Theory Appl., vol.
149, no. 1,pp. 17–25, 2002
[10]. H. Panagopoulos, K. J. Åström, and T. Hägglund, “Design of PID controllers based on constrained optimisation,” IEE Control
Theory Appl.,vol. 149, no. 1, pp. 32–40, 2002.
[11]. J. R. Mitchell, “Comments on „Bode compensator design‟,” IEEE Trans. Autom. Control, vol. AC-22, no. 5, pp. 869–870, Oct.
1977
[12]. W. R. Wakeland, “Bode compensator design,” IEEE Trans. Autom.Control, vol. AC-21, no. 5, pp. 771–773, Oct. 1976.

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B010411016

  • 1. IOSR Journal of Electrical and Electronics Engineering (IOSR-JEEE) e-ISSN: 2278-1676,p-ISSN: 2320-3331, Volume 10, Issue 4 Ver. I (July – Aug. 2015), PP 10-16 www.iosrjournals.org DOI: 10.9790/1676-10411016 www.iosrjournals.org 10 | Page Comparative Study of Monotonic and Non- Monotonic Phase LTI systems using Improved Analytical PID controller Monica U. Waikar1 , Nishij G. Kulkarni2 , Dr. Ravindrakumar M. Nagarale3 1 (PG student, M.B.E. Society’s college of engineering, Ambajogai, Maharashtra, India) 2,3 (PG Department, M.B.E. Society’s College of engineering, Ambajogai, Maharashtra, India) Abstract : A comparative study of monotonic and non monotonic phase LTI systems using analytical design of PID controller, by means of gain cross over frequency and phase margin specifications, is presented in the paper. The proposed methodology ensures minimum phase margin inside desired bandwidth giving accurate performance to step response for closed loop system. Concept of phase margin needs to be redefined when uncontrolled process presents minimum phase inside bandwidth. For comparative study, bode stability criterion, nyquist stability criterion and unit step response is used. Keywords: Improved analytical controller , linear system compensation, monotonic and non-monotonic phase LTI system. I. Introduction A system that maintains a prescribed relationship between the output and the reference input by comparing them and using the difference as a means of control is called a feedback control system. In case of feedback control system for monotonically decreasing phase inside bandwidth, phase margin can be defined as distance between open loop phase at gain crossover frequency and stability limit of−180°. After using bode stability criterion, if phase margin is positive then closed loop system is stable [1] In case of classical frequency response it can be considered that phase margin can be defined on gain cross-over frequency. Whereas this assumption is not valid in general practice, because even for a minimum phase system with a left half-plane zero located near the dominant- poles, its frequency response will present a non-monotonic phase. This abrupt technique shows an improved frequency response design technique for monotonic or non- monotonic phase (inside the bandwidth) dynamical systems based on gain crossover frequency and phase margin specifications, which is an expansion of the technique shown by Phillips and Harbor [2], by using this feature comparative study of monotonic and non-monotonic phase LTI system is possible. To achieve this feature concept of phase margin can be redefined when the system frequency response shows a non- monotonically decreasing phase inside the bandwidth. The study of phase margin is necessary due to two reasons such as it can be considered as good robustness indicator and which allows bode stability criterion for monotonic and non-monotonic minimum phase systems. The detailed organization is as follows: section 2 presents problem formulation, some remarks about non- monotonically decreasing phase can be addressed, for that purpose considered the DC-DC buck regulator. Section 3 explains detailed study of PID controller design. Section 4 is concerned about simulation and results where comparative study of monotonic and non-monotonic systems is also explained. Section 5 has conclusion. II. Problem Formulation Continuous LTI dynamical system is considered which is given by differential equation, y(t) + a1 y(t)a0y t = b1u(t) + b0 u t (1) Here LC low pass filter is to be considered which is commonly used in different type of power electronics. Hence assume synchronous buck regulator having model no. IRU 3038 used as voltage tracking application such as DC-DC converter and DDR memory [3]. Buck regulator is taken into considerations which are combination of power stage given by LC low pass filter and pulse width modulation based controller. The transfer function of buck converter is output(regulated voltage) to input(PWM input voltage) is, G s = VIN VOSC 1+sRC C LCS 2 +s RC C+ L R +1 (2) Where ,L is the output inductance, C is the output capacitance, R is the load resistance, RC is the output capacitor intrinsic resistance,VOSC is the PWM oscillator reference voltage and VIN is the power stage input voltage. Here assume typical application for buck regulator [3], RC=40ohm, gives transfer function, G s = 4(1+1.2×10−5s) 3×10−9 s2 +3.6×10−5 s+1 (3)
  • 2. Comparative Study Of Monotonic And Non-Monotonic Phase Lti Systems Using DOI: 10.9790/1676-10411016 www.iosrjournals.org 11 | Page Where the un-damped frequency is approximately 18 Krad/s and the damping ratio is approximately 0.33. Using this transfer function for buck regulator we can find out bode plot shown in fig.1. Here a valley in phase curve close to un-damped frequency is to be seen. From this we can conclude that left half-plane zero due to the output capacitor intrinsic resistance is not located far enough from the poles. Hence this leads to non monotonic phase compensation because bandwidth is located after zero frequency. Due to this transfer function is in minimum phase and use of bode plot is not possible. Hence we have to study the improved technique of design of PID controller[4]. Fig.2 Bode plot for Buck regulator III. Design Of PID Controller he PID controller is the most common form of feedback. It was an essential element of early governors and it became the standard tool when process control emerged in the 1940s. In control system today, more than 95% of the control loops are of PID type, most loops are actually PI control. PID controllers are today found in all areas where control is used. The controllers come in many different forms[5]. PID control is an important ingredient of a distributed control system. The controllers are also embedded in many special-purpose control systems. For improving PID control there are various methods such as empiric method by Ziegler and Nichols and analytical compensation based on pole-placement and frequency response method[6] [7] due to this popularity of PID controller is tremendously increased. Consider equation for PID controller, K s = KP 1 + 1 T1s TDs (5) Where KP is the proportional gain,KI is the integral action time or reset time, and TD is known as the derivative action time or rate time [1], [3]. Fig.1 Design of PID control of plant For designing of PID controller one tuning method is used i.e. Ziegler Nichols tuning method. This process of selecting the controller parameters to meet given performance specifications is known as controller tuning. Ziegler and Nichols suggested rules for tuning PID controllers based on experimental step responses or based on the value of that results in marginal stability when only proportional control action is used. Ziegler– Nichols rules, are useful when mathematical models of plants are not known. However, the resulting system may exhibit a large maximum overshoot in the step response, which is unacceptable. In such case we need series of fine tunings until an acceptable result is obtained. In fact, the Ziegler–Nichols tuning rules give an educated guess for the parameter values and provide a starting point for fine tuning, rather than giving the final settings in a single shot.[6]-[7]. It should be noted that worst case frequency is exactly the gain crossover frequency i.e., it defines a monotonic phase system, then the set of (4) becomes the well-known compensating equations shown by Phillips and Harbor [2].
  • 3. Comparative Study Of Monotonic And Non-Monotonic Phase Lti Systems Using DOI: 10.9790/1676-10411016 www.iosrjournals.org 12 | Page KP = 1 G(jωn ) 1+ ωu TD − 1 ωu TI (5a) ωuTD − 1 ωu TI = tan φ (5b) φ ≜ −180° + ∅m −< G(jωm ) (5c) One major drawback of PID controller is that, it has less equations than variables therefore it is very important to characterize equations having TIand TD values. By rewriting eq (5) in terms of KP and TD gives, KP = 1 G(jωn ) 1+Ω2 tan φ+ 1−Ω−2 ωm TI 2 (6a) TD = tan φ ωm + 1 ωm 2 TI (6b) By using above equations, variations in PI and PD are occurred having a single unique solution each. In general practice, the PID controller should not be usually used to compensate non-monotonic phase dynamical systems since these systems, by their own natural behaviour, already present left half-plane zeros in the open- loop transfer function, yielding a phase-lead effect very similar to the derivative term present in the standard form in (6). Therefore, the next subsections will present the equations and some comments on the PI and PD variations. 3.1 PD controller Assume TI equal to infinity in eq 5(a,b) we obtain, KP = 1 G(jωn ) 1+Ω2 tan φ2 (7a) TD = tan φ ωm (7b) or KD = KPTD = ωu −1 G(jωn ) 1+Ω2 cot φ2 (7c) Now, it should be noted that if monotonicity ratio is larger than KP gain will be smaller and KD gain will be larger.. 3.2 PI controller Consider TD equal to zero in eq 5(a,b), KP = 1 G(jωn ) 1+Ω−2 tan φ2 (8a) TI = − cot φ ωm (8b) KI = KP TI = ωu G(jωn ) 1+Ω2 cot φ2 (8c) Here, if monotonicity ratio is larger then KP gain will be larger and KI gain will be smaller. In case of non monotonic phase system as monotonic phase one should lead overvalued KP gain and to an undervalued KD gain..Due to this reason compensation of non monotonic phase system as monotonic system is avoided in case of integral action. IV. Results And Simulation In this section tools are presented such as fundamental tools and robustness tools which are widely used in literature. 4.1 Fundamental tools In fundamental tools consider the factors which are very important for analytical design procedure. This procedure gives gain crossover frequency and phase margin for stable and minimum phase using transfer function which can be obtained from bode criterion. Here damping ratio and un-damped frequency is necessary having transfer function of second order system. Let us consider negative feedback system into a low-pass behaviour in the open-loop frequency response, then define four parameters which can be used in frequency response compensation for dynamical LTI
  • 4. Comparative Study Of Monotonic And Non-Monotonic Phase Lti Systems Using DOI: 10.9790/1676-10411016 www.iosrjournals.org 13 | Page systems with non monotonic phase inside bandwidth such as worst case frequency ωm, gain cross over phase margin ∅u, gain crossover frequency ωu, worst case phase margin ∅m . The characteristic equation is gain cross over frequency and stability limit of −180° is ωu . For bode stability criterion if ∅u is positive then system is stable, when system response represents lowest phase inside bandwidth which is smaller than or equal to the gain crossover frequency ωu whereas worst case phase margin∅m is distance between open loop phase in worst case frequencyωm, and stability limit of −180°. Solve equation for frequency domain K(jωu)G(jωu ∠K jωu G jωu = 1∠ − 180° + ∅u (9a) With ∅m ≤ ∅u (9b) If the worst case phase margin ∅ 𝑚 is positive then gain crossover phase margin∅ 𝑢 is positive then system becomes stable, then 𝜔𝑢 is always larger than or equal to𝜔 𝑚 . Apply bode stability criterion for above equation it gives, K(jωu = 1 G(jωu ) (10a) ∠K jωm = −180° + ∅m − ∠G jωm (10b) With ωm ≤ ωu (10c) Here to check how system is monotonic then we have to define monotonicity ratio is given by, Ω ≜ ωu ωm (11) Ω is always greater than or equal to 1. This ratio indicates that if values of is larger then system tends to non monotonic phase. In next section find the parameters which are useful to shape open loop feedback system into low pass behaviour inside bandwidth and step response for closed loop system in case of gain cross over frequency and phase margin. 4.2 Robustness tools The analytical design procedure includes various characteristics such as stability, performance and robustness. Above section present stability term now consider factors for designing compensator such as performance and robustnesss. For future procedure ϰ∞ theory is considered[1]. By using this theory sensitivity function is given by, S(jω) ∞ = maxm S(jω) ≤ Ms (12a) Where S s = 1 + K s G(s) −1 (12b) Which is more acceptable as robustness measure [1],[9]. Here Nyquist plot is used where S(jω) ∞ is inverse of minimum distance from loop transfer function to critical point(-1,0). Therefore if nyquist plot avoids circle having centre point (-1,0) and radius 1 by MS then it is said that system is robust related to sensitivity function which are explained in [1],[8],[9]. To obtain better performance of robustness tools consider another complimentary sensitivity function, T(jω) ∞ = maxω T(jω) ≤ MT (13a) where T s = K s G(s) 1 + K s G(s) −1 (13b) Here nyquist plot having centre −MT 2 /(MT 2 − 1),0 and radius (MT/MT 2 − 1) is used. If nyquist plot avoids circle then it is said that system is robust related to complimentary function. For future work use values given by Skogestad and Postlethwaite as MS =2 and MT=1.25 and Kristiansson and Lennartson suggest valuesMS =1.7 and MT=1.4 [1],[9]. After comparison we have final conclusion that values suggested by Skogestad and Postlethwaite are more accurate. 4.3 Comparison of monotonic and non-monotonic system It describes the results obtained from proposed methodology and buck regulator which is shown in section 2. The results can be verified by using MATLAB simulink method. In this case it can be found that the un-damped frequency is near about or equal to 18 krad/s and left half-plane zero frequency is near about or equal to 83 krad/s[6]. Assume switching frequency of the converter to be equal to 200 kHz (approximately 1250 krad/s), by using reference it is said that gain cross-over frequency is about fifth times the switching frequency[3]. Therefore the specified gain cross-over frequency is near about 250 krad/s, from this it concludes
  • 5. Comparative Study Of Monotonic And Non-Monotonic Phase Lti Systems Using DOI: 10.9790/1676-10411016 www.iosrjournals.org 14 | Page that system leads to non-monotonic phase where gain-crossover frequency is beyond the left half-plane zero frequency. Now the desired phase margin is 40, therefore desired specifications follows the closed loop system performance having overshoot equal to 25% and a settling time equal to 40 s. In this case the feedback system must in second order system. In case of buck regulator non-monotonic phase system is obtained inside desired bandwidth, here PI controller is superior than PID controller[3]. In this case two parameters for PI controller is studied, first can be studied by using technique of Phillips and Harbor[2] and another from non-monotonic technique and finally both results were compared. The values for compensator are shown in Table 1. Table 1: Comparison of monotonic and non-monotonic compensation Parameters Monotonic Non-Monotonic 𝐊 𝐏 12.19 14.76 𝐓𝐈[µsec] 5.86 223.05 From Table 1, worst case frequency is 40 krad/s which is close to frequency of buck regulator for non- monotonic compensation. After comparing values for monotonic and non-monotonic, larger KP and larger TI (smaller KI) value is found for non monotonic systems. For the monotonic compensation (dashed line) and for the non-monotonic compensation (solid line), bode plot is presented in fig.3 It should be noticed that from fig.3, bandwidth is same for both compensation, where non-monotonic system gives larger steady-state error for ramp response and it gives phase margin of at least 40 for all frequency inside bandwidth whereas monotonic compensation only guarantees the phase margin required for the gain crossover frequency[4]. It should be remembered that frequencies inside bandwidth only makes control action. Monotonic compensation does not guarantees the phase margin inside desired bandwidth, since systems are stable according to Routh–Hurwitz criterion[2],[7]. By using Routh–Hurwitz criterion integral action time TI is 5.86 microsec and range of gain KP is located in between 0.023 and 2.646. Therefore there is no real and positive gain able to give the non-monotonically compensated system to instability for the integral action time equal to 223.05 s Fig 3. Bode plots for the monotonic compensation (dashed line) and the non-monotonic compensation (solid line) From future analysis, monotonic compensation gives two openloop gains which cross the stability limit of−180°, hence bode plot[1] is not sufficient for analysis. Therefore to check stability limit of both compensation, we have to use Nyquist plot in frequency response. For the monotonic compensation (dashed line) and for the non-monotonic compensation (solid line) is presented for Nyquist plot in fig.4
  • 6. Comparative Study Of Monotonic And Non-Monotonic Phase Lti Systems Using DOI: 10.9790/1676-10411016 www.iosrjournals.org 15 | Page Fig 4. Nyquist plots for the monotonic compensation (dashed line) and the non-monotonic compensation (solid line). Applying stability criterion for both compensation in Nyquist plot, it should be obtained that monotonic system is not useful for phase margin as it gives one encirclement around the -1 critical point. Whereas it does not happened in case of non-monotonic phase systems. Fig.4 also shows that robustness boundaries (lighter lines) of the sensitivity function (smaller circle) withMS =2 and complementary sensitivity function (larger circle) withMT= 1.25[1]. From above fig.4 it is seen that monotonic systems are not robust regarding to complimentary sensitivity function MT whreas non-monotonic system is robust in case of sensitivity functionMS . Hence for non-monotonic system Nyquist plot gives accurate shape and results. To find out accurate performance use of Step response is necessary, unit step response for the monotonic compensation (dashed line) and of the non-monotonic compensation (solid line) is shown in Fig. 4. For unit step response, monotonic phase system use second order system where non-monotonic phase system use first order system. The settling time for the non-monotonically compensated system is approximately 40 s and for monotonically compensated system is approximately 60 s. Whereas overshoot in case of non-monotonic system is smaller than monotonic system, therefore non-monotonic system completes all robustness properties. From above analysis, it should be noticed that non-monotonic phase gives accurate performance measure and its Nyquist plot avoids the circle created by the robustness boundary, which the monotonic compensation does not[1]. Fig 5. Unit step response of the monotonic compensation (dashed line) and the non-monotonic compensation (solid line). V. Conclusion The comparative study of monotonic and non-monotonic phase LTI systems are presented in paper by using improved analytical PID controller design using gain cross-over frequency and phase margin specification. Using this methodology accurate results are obtained. Where minimum phase margin is obtained inside desired bandwidth for closed loop system. Here non-monotonic phase gives more desirable results than monotonic phase results for closed loop system. For comparative study Bode stability criterion, Nyquist criterion and Unit step response are used, whereas nyquist plot are used for stability checking and results obtained by using MATLAB simulink.
  • 7. Comparative Study Of Monotonic And Non-Monotonic Phase Lti Systems Using DOI: 10.9790/1676-10411016 www.iosrjournals.org 16 | Page References [1]. S. Skogestad and I. Postlethwaite, Multivariable Feedback Control:Analysis and Design. New York: Wiley, 2005 [2]. C. L. Philips and R. D. Harbor, Feedback Control Systems. Englewood Cliffs, NJ: Prentice-Hall, 1999 [3]. International Rectifier, “Synchronous PWM controller for termination power supply applications,” 2nd Ed., 2002 [4]. Caio F.de Paula and Luís H.C.Ferreira,, An Improved Analytical PID Controller Design for Non-Monotonic Phase LTI Systems , IEEE transaction on control system technology, vol.20 No.5, September 2012 [5]. K. J. Åström and T. Hägglund, Advanced PID Control. Research Triangle Park, NC: ISA, 2005. [6]. J. G. Ziegler and N. B. Nichols, “Process lags in automatic control circuits,” Trans. Amer. Soc. Mechan. Eng., vol. 65, pp. 433–444, 1943. [7]. K. Ogata, Modern Control Engineering. Englewood Cliffs, NJ: Prentice-Hall, 2009 [8]. K. H. Ang, G. Chong, and Y. Li, “PID control system analysis, design,and technology,” IEEE Trans. Control Syst. Technol., vol. no. 4, pp.559–576, Jul. 2005. [9]. B. Kristiansson and B. Lennartson, “Robust and optimal tuning of PIand PID controllers,” IEE Proc.-Control Theory Appl., vol. 149, no. 1,pp. 17–25, 2002 [10]. H. Panagopoulos, K. J. Åström, and T. Hägglund, “Design of PID controllers based on constrained optimisation,” IEE Control Theory Appl.,vol. 149, no. 1, pp. 32–40, 2002. [11]. J. R. Mitchell, “Comments on „Bode compensator design‟,” IEEE Trans. Autom. Control, vol. AC-22, no. 5, pp. 869–870, Oct. 1977 [12]. W. R. Wakeland, “Bode compensator design,” IEEE Trans. Autom.Control, vol. AC-21, no. 5, pp. 771–773, Oct. 1976.