SlideShare a Scribd company logo
ECE4510/5510: Feedback Control Systems. 5–1
STABILITY ANALYSIS
5.1: Bounded-input bounded-output (BIBO) stability
I A system may be “stable,” “neutrally or marginally stable,” or
“unstable.” This can be illustrated using cones:
Stable Neutral Unstable
• The cone in the “stable” configuration can be perturbed by nudging
it from any direction, and its position will not change much.
• The cone in the “neutral” configuration can be nudged in the axial
direction without changing its position much, but if it is nudged in
the radial direction, it will roll and its position will change a lot. (The
“stability” of a neutral system depends on the input.)
• The cone in the “unstable” position can be nudged from any
direction, and its position will change a lot.
I We want stability because we don’t want a small input (e.g., possibly
disturbance, or a small change in the reference input) to cause the
output to grow without bound (seem to become “uncontrolled”).
I In system analysis, there are many ways to mathematically define
and evaluate whether a system is stable.
Lecture notes prepared by and copyright c 1998–2013, Gregory L. Plett and M. Scott Trimboli
ECE4510/ECE5510, STABILITY ANALYSIS 5–2
I For LTI systems, all are basically the same, and equivalent to
“bounded-input bounded-output” or BIBO stability.
I If the system’s input is bounded by some positive constant K1
|u(t)| < K1 ∀t
then BIBO stability guarantees that the output will also be bounded by
some (possibly different) positive constant K2
|y(t)| < K2 ∀t.
I In the time domain,
y(t) =
∞
−∞
h(τ)u(t − τ) dτ
|y(t)| =
∞
−∞
h(τ)u(t − τ) dτ
≤
∞
−∞
|h(τ)| |u(t − τ)| dτ
≤ K1
∞
−∞
|h(τ)| dτ.
I So, |y(t)| < ∞ iff
∞
−∞
|h(τ)| dτ < ∞. This is one test for BIBO
stability.
y(t)u(t) C Stable? Note: (h(t) = 1(t)).
I Integrating the absolute value of a function can be very tricky.
Sometimes it’s easier to integrate a simpler function that gives an
upper bound instead.
I Consider h(t) = exp(−t) sin(2πt)1(t). Is this system BIBO stable?
Lecture notes prepared by and copyright c 1998–2013, Gregory L. Plett and M. Scott Trimboli
ECE4510/ECE5510, STABILITY ANALYSIS 5–3
I The blue line in the figure is h(t);
and the green dotted line is |h(t)|.
I To determine stability, we need to
integrate to find the area under the
green dotted line—if this area is
finite, then the system is stable.
h(t)
|h(t)|
exp(−t)
I Finding the exact answer for this integral is hard. But, the integral
under the green dotted line is less than the integral under the red line.
I So, if the integral under the red line is finite, the system is stable.
∞
0
e−t
dt = −e−t ∞
0
= 1.
I So, we have determined that the system is BIBO stable, and we
didn’t need to integrate a very challenging piecewise function.
I We can also evaluate BIBO stability in the Laplace domain:
H(s) =
Y(s)
R(s)
=
K m
1 (s − zi)
n
1(s − pi)
m ≤ n.
(assume poles unique)
h(t) =
n
i=1
kiepi t
1(t)
∞
−∞
|h(τ)| dτ < ∞ iff R(pi) < 0 ∀ i.
(If poles are not distinct, h(t) will have terms
k
(m − 1)!
tm−1
epi t
for an mth order root.
Lecture notes prepared by and copyright c 1998–2013, Gregory L. Plett and M. Scott Trimboli
ECE4510/ECE5510, STABILITY ANALYSIS 5–4
∞
−∞
|h(τ)| dτ < ∞ iff R(pi) < 0;
Same condition.)
I Laplace-domain condition for stability: All poles in the transfer
function must be in the open left hand plane. (i.e., none on jω axis.)
EXAMPLE: T(s) =
2
s2 + 3s + 2
. Is T(s) stable?
T (s) =
2
(s + 1)(s + 2)
,
I Roots at s = −1, s = −2. Stable!
EXAMPLE: T(s) =
10s + 24
s3 + 2s2 − 11s − 12
. Is T (s) stable?
T (s) =
10(s + 2.4)
(s + 1)(s − 3)(s + 4)
,
I Roots at s = −1, s = +3, s = −4. Unstable!
EXAMPLE: T(s) =
s
s2 + 1
. Is T (s) stable?
T(s) =
s
(s − j)(s + j)
,
I Roots at s = ± j. MARGINALLY stable.
I Use input = sin(t).
Y(s) =
s
s2 + 1
1
s2 + 1
=
s
(s2 + 1)2
y(t) =
1
2
t sin(t) . . . unbounded.
I MARGINALLY stable = unstable (bounded impulse response, but
unbounded output for some inputs.)
Lecture notes prepared by and copyright c 1998–2013, Gregory L. Plett and M. Scott Trimboli
ECE4510/ECE5510, STABILITY ANALYSIS 5–5
5.2: Routh–Hurwitz stability (cases 0 and 1)
I Factoring high-degree polynomials to find roots is tedious and
numerically not well conditioned.
I Want other stability tests, and also MARGINS of stability.
(1) Routh test
(2) Root locus
(3) Nyquist test
(4) Bode stability margins



Can you tell this is
an important topic?
I In 1868, Maxwell found conditions on the coefficients of a transfer
function polynomial of 2nd and 3rd order to guarantee stability.
I It became the subject of the 1877 Adams Prize to determine
conditions for stability for higher-order polynomials.
I Routh won this prize, and the method is still useful.
Routh test “case 0”
I Consider the denominator a(s).
2nd order:
a(s) = s2
+ a1s + a0 = (s − p1)(s − p2) = s2
− (p1 + p2)s + p1 p2.
3rd order:
a(s) = s3
+ a2s2
+ a1s + a0
= (s − p1)(s − p2)(s − p3)
= s2
− (p1 + p2)s + p1 p2 s − p3
Lecture notes prepared by and copyright c 1998–2013, Gregory L. Plett and M. Scott Trimboli
ECE4510/ECE5510, STABILITY ANALYSIS 5–6
= s3
− (p1 + p2 + p3)s2
+ (p1 p2 + p1 p3 + p2 p3)s − p1 p2 p3.
TREND: Stability « none of the coefficients ai can be ≤ 0.
Does this trend continue?
an−1 = (−1)× sum of all roots.
an−2 = sum of products of roots taken two at a time.
an−3 = (−1)× sum of products of roots taken three at a time.
...
a0 = (−1)n
× product of all roots.
I Conclusions:
1. If any coefficient ai = 0, not all roots in LHP.
2. If any coefficient ai < 0, at least one root in RHP.
TEST: If any coefficient ai ≤ 0, system is unstable.
EXAMPLE: a(s) = s2
+ 0s + 1.
I From conclusion (1), not all roots in LHP.
I Roots at s = ± j.
I “Marginally” stable.
EXAMPLE: a(s) = s3
+ 2s2
− 11s − 12.
I From conclusion (2), at least one root is in RHP.
I Roots at s = −1, s = −4, s = +3.
I Unstable.
EXAMPLE: a(s) = s3
+ s2
+ 2s + 8.
Lecture notes prepared by and copyright c 1998–2013, Gregory L. Plett and M. Scott Trimboli
ECE4510/ECE5510, STABILITY ANALYSIS 5–7
I We don’t know yet if this system is stable or not.
I Roots at s = −2, s =
1
2
±
j
√
15
2
. Unstable, but how do we find out
without factoring?
Routh test “case 1”
I Once we have determined that ai > 0 ∀ i, we need to run the full
Routh test (“case 0” doesn’t really count).
I Very mechanical, not intuitive. Proof difficult.
I Start with characteristic polynomial (denominator of closed-loop
transfer function), a(s) = sn
+ an−1sn−1
+ · · · + a1s + a0.
I Form “Routh array”.
• First two rows are coefficients directly copied from a(s);
• Remaining rows are calculated as shown.
sn
an an−2 an−4 · · ·
sn−1
an−1 an−3 an−5 · · ·
sn−2
b1 b2 · · ·
sn−3
c1 c2 · · ·
...
s1
j1
s0
k1
b1 =
−1
an−1
an an−2
an−1 an−3
b2 =
−1
an−1
an an−4
an−1 an−5
· · ·
c1 =
−1
b1
an−1 an−3
b1 b2
c2 =
−1
b1
an−1 an−5
b1 b3
· · ·
TEST: Number of unstable roots = number of sign changes in left column.
Lecture notes prepared by and copyright c 1998–2013, Gregory L. Plett and M. Scott Trimboli
ECE4510/ECE5510, STABILITY ANALYSIS 5–8
EXAMPLE: a(s) = s3
+ s2
+ 2s + 8.
s3
1 2
s2
1 8
s1
−6
s0
8 b1 =
−1
1
1 2
1 8
= −(8 − 2) = −6
c1 =
−1
−6
1 8
−6 0
=
1
6
(0 + 6 × 8) = 8
I Two sign changes (1 → −6, −6 → 8) Two roots in RHP.
EXAMPLE: a(s) = s2
+ a1s + a0.
s2
1 a0
s1
a1
s0
a0
b1 =
−1
a1
1 a0
a1 0
=
−1
a1
(0 − a0a1) = a0
I Stable iff a1 > 0, a0 > 0.
EXAMPLE: a(s) = s3
+ a2s2
+ a1s + a0.
s3
1 a1
s2
a2 a0
s1
a1 −
a0
a2
s0
a0
b1 =
−1
a2
1 a1
a2 a0
=
−1
a2
(a0 − a1a2)
= a1 −
a0
a2
c1 =
−1
b1
a2 a0
b1 0
=
−1
b1
(−a0b1) = a0.
I Stable iff a2 > 0, a0 > 0, a1 >
a0
a2
.
Lecture notes prepared by and copyright c 1998–2013, Gregory L. Plett and M. Scott Trimboli
ECE4510/ECE5510, STABILITY ANALYSIS 5–9
5.3: Routh–Hurwitz stability (cases 2 and 3)
Routh test “case 2”
I In the process of filling in the Routh array, we sometimes find an
element in first column = 0.
I This leads to a divide by zero computation in a subsequent step,
which has an indeterminate result.
I Solution: Replace the zero in the left column with ± as → 0. (Will
get same result for + and − .)
EXAMPLE: a(s) = s5
+ 2s4
+ 2s3
+ 4s2
+ 11s + 10.
s5
1 2 11
s4
2 4 10
s3
0 6
new s3
6
s2 −12
10
s1
6
s0
10
If > 0, two sign changes.
If < 0, two sign changes.
« Two poles in RHP.
b1 =
−1
2
1 2
2 4
=
−1
2
(4 − 4) = 0
b2 =
−1
2
1 11
2 10
=
−1
2
(10 − 22) = 6
c1 =
−1 2 4
6
=
−1
(12 − 4 ) ≈
−12
c2 =
−1 2 10
0
=
−1
(0 − 10 ) = 10
d1 =
12
6
−12
10
=
12
(10 +
72
) ≈ 6
e1 =
−1
6
−12
10
6 0
=
−1
6
(0 − 60) = 10
Lecture notes prepared by and copyright c 1998–2013, Gregory L. Plett and M. Scott Trimboli
ECE4510/ECE5510, STABILITY ANALYSIS 5–10
Routh test “case 3”
I Sometimes an entire row in Routh array = 0.
I This means that polynomial factors such that one factor has
conjugate-MIRROR-roots, which can be configured as shown in the
figure:
I(s)
R(s)
I(s)
R(s)
I(s)
R(s)
I In any case, system is unstable. But how many RHP roots?
I Complete Routh array by making polynomial a1(s) from last non-zero
row in array. Poly has every second order of s only!!
• We do this in a reverse fashion from how we entered a(s) into the
array in the first place.
I It turns out that a1(s) is a factor of the original a(s). It is missing some
orders of s, so IS NOT STABLE (by “case 0”.)
I We want to see if it has roots in the RHP or only on the jω-axis.
I Replace zero row with coefficients from
da1(s)
ds
and continue.
Lecture notes prepared by and copyright c 1998–2013, Gregory L. Plett and M. Scott Trimboli
ECE4510/ECE5510, STABILITY ANALYSIS 5–11
EXAMPLE: a(s) = s4
+ s3
+ 3s2
+ 2s + 2.
s4
1 3 2
s3
1 2 0
s2
1 2
s1
0
new s1
2
s0
2
No sign changes in Routh
array. So, no RHP roots.
Roots of a1(s) at s = ± j
√
2.
Marginally stable.
b1 =
−1
1
1 3
1 2
= 1
b2 =
−1
1
1 2
1 0
= 2
c1 =
−1
1
1 2
1 2
= 0
a1(s) = s2
+ 2
da1(s)
ds
= 2s
d1 =
−1
2
1 2
2 0
= 2
EXAMPLE: a(s) = s4
+ 4 (Hard).
s4
1 0 4
s3
0 0
new s3
4 0
s2
0 4
new s2
4
s1 −16
s0
4
Two sign changes. Therefore
2 RHP poles. Other two
poles are mirrors in LHP.
a1(s) = s4
+ 4;
da1(s)
ds
= 4s3
.
b1 =
−1
4
1 0
4 0
= 0
b2 =
−1
4
1 4
4 0
= 4
c1 =
−1 4 0
4
=
−16
d1 =
16
4
−16
0
= 4
Lecture notes prepared by and copyright c 1998–2013, Gregory L. Plett and M. Scott Trimboli
ECE4510/ECE5510, STABILITY ANALYSIS 5–12
5.4: Routh test as a design tool
I Consider the system:
R(s) Y(s)K
s + 1
s(s − 1)(s + 6)
T(s) =
Y(s)
R(s)
=
K s+1
s(s−1)(s+6)
1 + K s+1
s(s−1)(s+6)
=
K(s + 1)
s(s − 1)(s + 6) + K(s + 1)
I We might be interested in knowing for what values of K the system is
stable.
I Compute the denominator of the transfer function:
a(s) = s(s − 1)(s + 6) + K(s + 1)
= s3
+ 5s2
+ (K − 6)s + K.
I Perform the Routh test
s3
1 K − 6
s2
5 K
s1 4K − 30
5
s0
K
b1 =
−1
5
1 K − 6
5 K
=
−1
5
(K − 5(K − 6))
= (4K − 30)/5.
c1 =
−1
b1
5 K
b1 0
=
−1
b1
(−b1K) = K
I For stability of the closed-loop system, K > 0, and K > 30/4.
I Step response for different values of K.
Lecture notes prepared by and copyright c 1998–2013, Gregory L. Plett and M. Scott Trimboli
ECE4510/ECE5510, STABILITY ANALYSIS 5–13
0 2 4 6 8 10 12
−0.5
0
0.5
1
1.5
2
2.5
K=7.5
K=13
K=25
Amplitude
Time (sec.)
EXAMPLE:
R(s) Y(s)K 1 +
1
TI s
1
(s + 1)(s + 2)
T (s) =
Y(s)
R(s)
=
K TI s+K
TI s(s+1)(s+2)
1 + K TI s+K
TI s(s+1)(s+2)
=
K TI s + K
TI s(s + 1)(s + 2) + K TI s + K
.
I a(s) = TI s3
+ 3TI s2
+ TI (2 + K)s + K.
s3
TI TI (2 + K)
s2
3TI K
s1
TI (K + 2) −
K
3
s0
K
b1 =
−1
3TI
TI TI (2 + K)
3TI K
= TI (K + 2) −
K
3
c1 =
−1
b1
3TI K
b1 0
=
−1
b1
(−b1K) = K
Lecture notes prepared by and copyright c 1998–2013, Gregory L. Plett and M. Scott Trimboli
ECE4510/ECE5510, STABILITY ANALYSIS 5–14
I For stability of the closed-loop system, K > 0 and TI > 0 and
TI >
K
3(K + 2)
.
I Alternately, K < 0 and TI < 0 and TI <
K
3(K + 2)
for −2 < K < 0, (or
instead TI >
K
3(K + 2)
for K < −2 but this is a contradiction since the
quotient is positive and TI is negative by assumption).
0 2 4 6 8 10 12
0
0.5
1
1.5
Time (seconds)
K = 3, TI = 0.5
K = 1, TI = 0.25
K = 1, TI = ∞
Amplitude
Lecture notes prepared by and copyright c 1998–2013, Gregory L. Plett and M. Scott Trimboli
ECE4510/ECE5510, STABILITY ANALYSIS 5–15
5.5: Advanced applications of the Routh test
I Note that the Routh test is not specifically a controls recipe.
• It is a geometric algorithm.
• It counts the number of roots of a polynomial that have R(si) ≥ 0.
Modification #1
I Suppose we want to ensure a settling-time specification (or some
form of robust stability), so we want R(si) ≤ −σ for all poles.
I Routh test doesn’t apply directly; but, perform a change of variables:
• Let p = s + σ. Then, si < −σ corresponds to pi < 0.
I So, we can perform a Routh test on a(p) instead of a(s).
EXAMPLE: Let T (s) =
K
s2 + 4s + K
. For what values of K are all poles to
the left of s = −1?
I Note, σ = 1, and we let p = s + 1 or s = p − 1.
T (p) =
K
(p − 1)2 + 4(p − 1) + K
=
K
p2 − 2p + 1 + 4p − 4 + K
=
K
p2 + 2p + K − 3
.
I So, a(p) = p2
+ 2p + (K − 3). Form the Routh array:
p2
1 (K − 3)
p1
2
p0
(K − 3)
I If K > 3, the real part of all poles of
T(s) are less than −1. −5 −4 −3 −2 −1 0 1
−2
−1.5
−1
−0.5
0
0.5
1
1.5
2
Real axis
Imaginaryaxis
Root locus
K = 3
Lecture notes prepared by and copyright c 1998–2013, Gregory L. Plett and M. Scott Trimboli
ECE4510/ECE5510, STABILITY ANALYSIS 5–16
Modification #2
I When working with digital control systems, the complex frequency
domain is represented by “z” instead of “s”, and a system is stable if
all poles of T (z) have magnitude strictly less than 1.
I The stability region is the unit circle in
the z-plane.
I The Routh test does not apply directly.
I But, we can perform the change of variables (where α > 0)
z =
1 + αs
1 − αs
or s =
1
α
z − 1
z + 1
,
which is known as the bilinear transformation.
I We can show that this transformation maps the inside of the unit
circle in the z-plane to the left-half s-plane.
I Let z = rejθ
. We have stability if z < 1. So, we want to show that r < 1
produces R(s) < 0.
I Substituting into the change of variables
s =
1
α
rejθ
− 1
rejθ + 1
=
1
α
rejθ
− 1
rejθ + 1
re− jθ
+ 1
re− jθ + 1
=
1
α





r2
− 1 +
j2r sin θ
rejθ
− re− jθ
r2 + 1 + rejθ
+ re− jθ
2r cos θ





.
I Note that:
Lecture notes prepared by and copyright c 1998–2013, Gregory L. Plett and M. Scott Trimboli
ECE4510/ECE5510, STABILITY ANALYSIS 5–17
• When r = 1, s is purely imaginary (translating the unit circle into
the jω axis)
• When r < 1, the real part of s is less than zero (translating the
inside of the unit disc into the left-half s-plane)
• When r > 1, the real part of s is greater than zero (translating the
outside of the unit disc into the right-half s-plane).
EXAMPLE: Let T (z) =
K
z + (K − 0.5)
.
I We can see from inspection (for this simple example) that
−0.5 < K < 1.5 will result in a pole location that is between z = −1
and z = +1.
I But, let’s perform the bilinear transformation and the Routh test.
Choose α = 1.
T (s) = T (z)|z=1+s
1−s
=
K
1+s
1−s
+ (K − 0.5)
=
K(1 − s)
1 + s + (K − 0.5)(1 − s)
=
K(1 − s)
(1.5 − K)s + (K + 0.5)
.
I Form the (trivial) Routh array:
s1
(1.5 − K)
s0
(K + 0.5)
I So, we have stability when K < 1.5 and
when K > −0.5, as expected.
Lecture notes prepared by and copyright c 1998–2013, Gregory L. Plett and M. Scott Trimboli
ECE4510/ECE5510, STABILITY ANALYSIS 5–18
5.6: Internal stability
I BIBO stability requires that the output be bounded for every possible
bounded input.
I However, a system may be input-output stable and still have
unbounded internal signals.
I The issue is internal stability.
I Consider the following diagram:
R(s)
E(s) U(s)
W(s)
Y(s)D(s) G(s)
I We can find the following four transfer functions:
Y(s)
R(s)
=
D(s)G(s)
1 + D(s)G(s)
Y(s)
W(s)
=
G(s)
1 + D(s)G(s)
.
U(s)
R(s)
=
D(s)
1 + D(s)G(s)
U(s)
W(s)
=
1
1 + D(s)G(s)
.
I For internal stability, all four of these transfer functions must be stable.
EXAMPLE: Let G(s) =
1
s − 1
and D(s) =
s − 1
s + 1
.
I Then,
Y(s)
R(s)
=
D(s)G(s)
1 + D(s)G(s)
=
s−1
(s−1)(s+1)
1 + s−1
(s−1)(s+1)
Lecture notes prepared by and copyright c 1998–2013, Gregory L. Plett and M. Scott Trimboli
ECE4510/ECE5510, STABILITY ANALYSIS 5–19
=
s − 1
(s − 1)(s + 1) + (s − 1)
=
1
s + 1 + 1
=
1
s + 2
.
I This system passes the test for BIBO stability.
I However,
Y(s)
W(s)
=
G(s)
1 + D(s)G(s)
=
1
s−1
1 + s−1
(s−1)(s+1)
=
s + 1
(s − 1)(s + 1) + (s − 1)
=
s + 1
(s − 1)(s + 2)
,
which is unstable.
I Therefore, this system is not internally stable.
I In this case, any (even very tiny) amount of disturbance will cause the
output y(t) to grow without bound. The feedback will not help.
I This brings up the point that it is important to avoid “bad”
cancellations of pole-zero pairs!
I We cannot stabilize a system by canceling an unstable pole with a
compensator zero.
• We will see the same idea again from a different perspective when
we look at root-locus design.
Lecture notes prepared by and copyright c 1998–2013, Gregory L. Plett and M. Scott Trimboli

More Related Content

PDF
Ece4510 notes06
PPT
Inverse laplace transforms
PDF
Laplace transform
PDF
Jif 315 lesson 1 Laplace and fourier transform
PPTX
160280102011 c1 aem
PPTX
Laplace transformation
PPTX
Laplace transform
PPT
Damped force vibrating Model Laplace Transforms
Ece4510 notes06
Inverse laplace transforms
Laplace transform
Jif 315 lesson 1 Laplace and fourier transform
160280102011 c1 aem
Laplace transformation
Laplace transform
Damped force vibrating Model Laplace Transforms

What's hot (20)

PPT
Laplace transform
PPS
M1 unit viii-jntuworld
PPTX
EM3 mini project Laplace Transform
PDF
Inverse laplace
PPTX
Properties of laplace transform
PPTX
Laplace transformation
PDF
Inverse Laplace Transform
PDF
Laplace Transforms
PPTX
Laplace transform and its application
PDF
Using Laplace Transforms to Solve Differential Equations
PPTX
Chapter 2 laplace transform
PPT
Laplace transform
PPTX
Laplace transformation
PPTX
Laplace transform
PPTX
Laplace transform and its application
PPT
Laplace transforms
PPTX
Chapter 2 Laplace Transform
PPT
Laplace
PDF
Application of Convolution Theorem
PPTX
Laplace Transformation & Its Application
Laplace transform
M1 unit viii-jntuworld
EM3 mini project Laplace Transform
Inverse laplace
Properties of laplace transform
Laplace transformation
Inverse Laplace Transform
Laplace Transforms
Laplace transform and its application
Using Laplace Transforms to Solve Differential Equations
Chapter 2 laplace transform
Laplace transform
Laplace transformation
Laplace transform
Laplace transform and its application
Laplace transforms
Chapter 2 Laplace Transform
Laplace
Application of Convolution Theorem
Laplace Transformation & Its Application
Ad

Similar to Ece4510 notes05 (20)

PDF
BEC 26 control-systems_unit-IV
PPTX
Classical control 2(2)
PPTX
Classical control 2(1)
PPTX
Classical control 2
PPTX
Classical control 2(3)
PDF
Control Systems ..(K-Wiki_Stability).pdf
PPT
Stabiltiy & R-H Ccriterion
PDF
Control and Instrumentation.pdf.pdf
PDF
chapter 6 control system engineering.pdf
PPTX
lecture_21-22_routh_hurwitz_stability_criterion.pptx
PDF
PDF
A novel two-polynomial criteria for higher-order systems stability boundaries...
PDF
PPTX
lecture6-stabilty_Routh-Hurwitz criterion.pptx
PPT
K11038 Mayur control ppt
PDF
Stability criteria and Analysis_Control Systems Engineering_MEB 4101.pdf
PDF
Lecture7bewekwkewoenw weeojwnewnejwenw.pdf
PPTX
LECTURE 4. Stability criteria and Analysis_Control Systems Engineering_MEB 41...
PPTX
Stability of control systems in time-domain
PPT
Control chap5
BEC 26 control-systems_unit-IV
Classical control 2(2)
Classical control 2(1)
Classical control 2
Classical control 2(3)
Control Systems ..(K-Wiki_Stability).pdf
Stabiltiy & R-H Ccriterion
Control and Instrumentation.pdf.pdf
chapter 6 control system engineering.pdf
lecture_21-22_routh_hurwitz_stability_criterion.pptx
A novel two-polynomial criteria for higher-order systems stability boundaries...
lecture6-stabilty_Routh-Hurwitz criterion.pptx
K11038 Mayur control ppt
Stability criteria and Analysis_Control Systems Engineering_MEB 4101.pdf
Lecture7bewekwkewoenw weeojwnewnejwenw.pdf
LECTURE 4. Stability criteria and Analysis_Control Systems Engineering_MEB 41...
Stability of control systems in time-domain
Control chap5
Ad

More from K. M. Shahrear Hyder (13)

PPTX
Feasibility study of pvc pipe manufacturing plant
PDF
Ece4510 notes10
PDF
Ece4510 notes09
PDF
Ece4510 notes08
PDF
Ece4510 notes07
PDF
Ece4510 notes04
PDF
Ece4510 notes03
PDF
Ece4510 notes02
PDF
Ece4510 notes01
PDF
Ece4510 notes00
PPT
Generator hyder
PDF
Presentation on art203 for electrical engineers
PPTX
Hydro electric power plant
Feasibility study of pvc pipe manufacturing plant
Ece4510 notes10
Ece4510 notes09
Ece4510 notes08
Ece4510 notes07
Ece4510 notes04
Ece4510 notes03
Ece4510 notes02
Ece4510 notes01
Ece4510 notes00
Generator hyder
Presentation on art203 for electrical engineers
Hydro electric power plant

Recently uploaded (20)

PPTX
bas. eng. economics group 4 presentation 1.pptx
PDF
Evaluating the Democratization of the Turkish Armed Forces from a Normative P...
PPT
Mechanical Engineering MATERIALS Selection
PPTX
Geodesy 1.pptx...............................................
DOCX
ASol_English-Language-Literature-Set-1-27-02-2023-converted.docx
PPTX
Infosys Presentation by1.Riyan Bagwan 2.Samadhan Naiknavare 3.Gaurav Shinde 4...
PDF
Embodied AI: Ushering in the Next Era of Intelligent Systems
PPTX
Sustainable Sites - Green Building Construction
PPTX
MET 305 2019 SCHEME MODULE 2 COMPLETE.pptx
PPTX
CH1 Production IntroductoryConcepts.pptx
PPTX
web development for engineering and engineering
PDF
July 2025 - Top 10 Read Articles in International Journal of Software Enginee...
PDF
Digital Logic Computer Design lecture notes
PDF
Mohammad Mahdi Farshadian CV - Prospective PhD Student 2026
PPTX
additive manufacturing of ss316l using mig welding
PPTX
Engineering Ethics, Safety and Environment [Autosaved] (1).pptx
PDF
Well-logging-methods_new................
PPTX
CARTOGRAPHY AND GEOINFORMATION VISUALIZATION chapter1 NPTE (2).pptx
PPTX
Welding lecture in detail for understanding
PDF
keyrequirementskkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkk
bas. eng. economics group 4 presentation 1.pptx
Evaluating the Democratization of the Turkish Armed Forces from a Normative P...
Mechanical Engineering MATERIALS Selection
Geodesy 1.pptx...............................................
ASol_English-Language-Literature-Set-1-27-02-2023-converted.docx
Infosys Presentation by1.Riyan Bagwan 2.Samadhan Naiknavare 3.Gaurav Shinde 4...
Embodied AI: Ushering in the Next Era of Intelligent Systems
Sustainable Sites - Green Building Construction
MET 305 2019 SCHEME MODULE 2 COMPLETE.pptx
CH1 Production IntroductoryConcepts.pptx
web development for engineering and engineering
July 2025 - Top 10 Read Articles in International Journal of Software Enginee...
Digital Logic Computer Design lecture notes
Mohammad Mahdi Farshadian CV - Prospective PhD Student 2026
additive manufacturing of ss316l using mig welding
Engineering Ethics, Safety and Environment [Autosaved] (1).pptx
Well-logging-methods_new................
CARTOGRAPHY AND GEOINFORMATION VISUALIZATION chapter1 NPTE (2).pptx
Welding lecture in detail for understanding
keyrequirementskkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkk

Ece4510 notes05

  • 1. ECE4510/5510: Feedback Control Systems. 5–1 STABILITY ANALYSIS 5.1: Bounded-input bounded-output (BIBO) stability I A system may be “stable,” “neutrally or marginally stable,” or “unstable.” This can be illustrated using cones: Stable Neutral Unstable • The cone in the “stable” configuration can be perturbed by nudging it from any direction, and its position will not change much. • The cone in the “neutral” configuration can be nudged in the axial direction without changing its position much, but if it is nudged in the radial direction, it will roll and its position will change a lot. (The “stability” of a neutral system depends on the input.) • The cone in the “unstable” position can be nudged from any direction, and its position will change a lot. I We want stability because we don’t want a small input (e.g., possibly disturbance, or a small change in the reference input) to cause the output to grow without bound (seem to become “uncontrolled”). I In system analysis, there are many ways to mathematically define and evaluate whether a system is stable. Lecture notes prepared by and copyright c 1998–2013, Gregory L. Plett and M. Scott Trimboli
  • 2. ECE4510/ECE5510, STABILITY ANALYSIS 5–2 I For LTI systems, all are basically the same, and equivalent to “bounded-input bounded-output” or BIBO stability. I If the system’s input is bounded by some positive constant K1 |u(t)| < K1 ∀t then BIBO stability guarantees that the output will also be bounded by some (possibly different) positive constant K2 |y(t)| < K2 ∀t. I In the time domain, y(t) = ∞ −∞ h(τ)u(t − τ) dτ |y(t)| = ∞ −∞ h(τ)u(t − τ) dτ ≤ ∞ −∞ |h(τ)| |u(t − τ)| dτ ≤ K1 ∞ −∞ |h(τ)| dτ. I So, |y(t)| < ∞ iff ∞ −∞ |h(τ)| dτ < ∞. This is one test for BIBO stability. y(t)u(t) C Stable? Note: (h(t) = 1(t)). I Integrating the absolute value of a function can be very tricky. Sometimes it’s easier to integrate a simpler function that gives an upper bound instead. I Consider h(t) = exp(−t) sin(2πt)1(t). Is this system BIBO stable? Lecture notes prepared by and copyright c 1998–2013, Gregory L. Plett and M. Scott Trimboli
  • 3. ECE4510/ECE5510, STABILITY ANALYSIS 5–3 I The blue line in the figure is h(t); and the green dotted line is |h(t)|. I To determine stability, we need to integrate to find the area under the green dotted line—if this area is finite, then the system is stable. h(t) |h(t)| exp(−t) I Finding the exact answer for this integral is hard. But, the integral under the green dotted line is less than the integral under the red line. I So, if the integral under the red line is finite, the system is stable. ∞ 0 e−t dt = −e−t ∞ 0 = 1. I So, we have determined that the system is BIBO stable, and we didn’t need to integrate a very challenging piecewise function. I We can also evaluate BIBO stability in the Laplace domain: H(s) = Y(s) R(s) = K m 1 (s − zi) n 1(s − pi) m ≤ n. (assume poles unique) h(t) = n i=1 kiepi t 1(t) ∞ −∞ |h(τ)| dτ < ∞ iff R(pi) < 0 ∀ i. (If poles are not distinct, h(t) will have terms k (m − 1)! tm−1 epi t for an mth order root. Lecture notes prepared by and copyright c 1998–2013, Gregory L. Plett and M. Scott Trimboli
  • 4. ECE4510/ECE5510, STABILITY ANALYSIS 5–4 ∞ −∞ |h(τ)| dτ < ∞ iff R(pi) < 0; Same condition.) I Laplace-domain condition for stability: All poles in the transfer function must be in the open left hand plane. (i.e., none on jω axis.) EXAMPLE: T(s) = 2 s2 + 3s + 2 . Is T(s) stable? T (s) = 2 (s + 1)(s + 2) , I Roots at s = −1, s = −2. Stable! EXAMPLE: T(s) = 10s + 24 s3 + 2s2 − 11s − 12 . Is T (s) stable? T (s) = 10(s + 2.4) (s + 1)(s − 3)(s + 4) , I Roots at s = −1, s = +3, s = −4. Unstable! EXAMPLE: T(s) = s s2 + 1 . Is T (s) stable? T(s) = s (s − j)(s + j) , I Roots at s = ± j. MARGINALLY stable. I Use input = sin(t). Y(s) = s s2 + 1 1 s2 + 1 = s (s2 + 1)2 y(t) = 1 2 t sin(t) . . . unbounded. I MARGINALLY stable = unstable (bounded impulse response, but unbounded output for some inputs.) Lecture notes prepared by and copyright c 1998–2013, Gregory L. Plett and M. Scott Trimboli
  • 5. ECE4510/ECE5510, STABILITY ANALYSIS 5–5 5.2: Routh–Hurwitz stability (cases 0 and 1) I Factoring high-degree polynomials to find roots is tedious and numerically not well conditioned. I Want other stability tests, and also MARGINS of stability. (1) Routh test (2) Root locus (3) Nyquist test (4) Bode stability margins    Can you tell this is an important topic? I In 1868, Maxwell found conditions on the coefficients of a transfer function polynomial of 2nd and 3rd order to guarantee stability. I It became the subject of the 1877 Adams Prize to determine conditions for stability for higher-order polynomials. I Routh won this prize, and the method is still useful. Routh test “case 0” I Consider the denominator a(s). 2nd order: a(s) = s2 + a1s + a0 = (s − p1)(s − p2) = s2 − (p1 + p2)s + p1 p2. 3rd order: a(s) = s3 + a2s2 + a1s + a0 = (s − p1)(s − p2)(s − p3) = s2 − (p1 + p2)s + p1 p2 s − p3 Lecture notes prepared by and copyright c 1998–2013, Gregory L. Plett and M. Scott Trimboli
  • 6. ECE4510/ECE5510, STABILITY ANALYSIS 5–6 = s3 − (p1 + p2 + p3)s2 + (p1 p2 + p1 p3 + p2 p3)s − p1 p2 p3. TREND: Stability « none of the coefficients ai can be ≤ 0. Does this trend continue? an−1 = (−1)× sum of all roots. an−2 = sum of products of roots taken two at a time. an−3 = (−1)× sum of products of roots taken three at a time. ... a0 = (−1)n × product of all roots. I Conclusions: 1. If any coefficient ai = 0, not all roots in LHP. 2. If any coefficient ai < 0, at least one root in RHP. TEST: If any coefficient ai ≤ 0, system is unstable. EXAMPLE: a(s) = s2 + 0s + 1. I From conclusion (1), not all roots in LHP. I Roots at s = ± j. I “Marginally” stable. EXAMPLE: a(s) = s3 + 2s2 − 11s − 12. I From conclusion (2), at least one root is in RHP. I Roots at s = −1, s = −4, s = +3. I Unstable. EXAMPLE: a(s) = s3 + s2 + 2s + 8. Lecture notes prepared by and copyright c 1998–2013, Gregory L. Plett and M. Scott Trimboli
  • 7. ECE4510/ECE5510, STABILITY ANALYSIS 5–7 I We don’t know yet if this system is stable or not. I Roots at s = −2, s = 1 2 ± j √ 15 2 . Unstable, but how do we find out without factoring? Routh test “case 1” I Once we have determined that ai > 0 ∀ i, we need to run the full Routh test (“case 0” doesn’t really count). I Very mechanical, not intuitive. Proof difficult. I Start with characteristic polynomial (denominator of closed-loop transfer function), a(s) = sn + an−1sn−1 + · · · + a1s + a0. I Form “Routh array”. • First two rows are coefficients directly copied from a(s); • Remaining rows are calculated as shown. sn an an−2 an−4 · · · sn−1 an−1 an−3 an−5 · · · sn−2 b1 b2 · · · sn−3 c1 c2 · · · ... s1 j1 s0 k1 b1 = −1 an−1 an an−2 an−1 an−3 b2 = −1 an−1 an an−4 an−1 an−5 · · · c1 = −1 b1 an−1 an−3 b1 b2 c2 = −1 b1 an−1 an−5 b1 b3 · · · TEST: Number of unstable roots = number of sign changes in left column. Lecture notes prepared by and copyright c 1998–2013, Gregory L. Plett and M. Scott Trimboli
  • 8. ECE4510/ECE5510, STABILITY ANALYSIS 5–8 EXAMPLE: a(s) = s3 + s2 + 2s + 8. s3 1 2 s2 1 8 s1 −6 s0 8 b1 = −1 1 1 2 1 8 = −(8 − 2) = −6 c1 = −1 −6 1 8 −6 0 = 1 6 (0 + 6 × 8) = 8 I Two sign changes (1 → −6, −6 → 8) Two roots in RHP. EXAMPLE: a(s) = s2 + a1s + a0. s2 1 a0 s1 a1 s0 a0 b1 = −1 a1 1 a0 a1 0 = −1 a1 (0 − a0a1) = a0 I Stable iff a1 > 0, a0 > 0. EXAMPLE: a(s) = s3 + a2s2 + a1s + a0. s3 1 a1 s2 a2 a0 s1 a1 − a0 a2 s0 a0 b1 = −1 a2 1 a1 a2 a0 = −1 a2 (a0 − a1a2) = a1 − a0 a2 c1 = −1 b1 a2 a0 b1 0 = −1 b1 (−a0b1) = a0. I Stable iff a2 > 0, a0 > 0, a1 > a0 a2 . Lecture notes prepared by and copyright c 1998–2013, Gregory L. Plett and M. Scott Trimboli
  • 9. ECE4510/ECE5510, STABILITY ANALYSIS 5–9 5.3: Routh–Hurwitz stability (cases 2 and 3) Routh test “case 2” I In the process of filling in the Routh array, we sometimes find an element in first column = 0. I This leads to a divide by zero computation in a subsequent step, which has an indeterminate result. I Solution: Replace the zero in the left column with ± as → 0. (Will get same result for + and − .) EXAMPLE: a(s) = s5 + 2s4 + 2s3 + 4s2 + 11s + 10. s5 1 2 11 s4 2 4 10 s3 0 6 new s3 6 s2 −12 10 s1 6 s0 10 If > 0, two sign changes. If < 0, two sign changes. « Two poles in RHP. b1 = −1 2 1 2 2 4 = −1 2 (4 − 4) = 0 b2 = −1 2 1 11 2 10 = −1 2 (10 − 22) = 6 c1 = −1 2 4 6 = −1 (12 − 4 ) ≈ −12 c2 = −1 2 10 0 = −1 (0 − 10 ) = 10 d1 = 12 6 −12 10 = 12 (10 + 72 ) ≈ 6 e1 = −1 6 −12 10 6 0 = −1 6 (0 − 60) = 10 Lecture notes prepared by and copyright c 1998–2013, Gregory L. Plett and M. Scott Trimboli
  • 10. ECE4510/ECE5510, STABILITY ANALYSIS 5–10 Routh test “case 3” I Sometimes an entire row in Routh array = 0. I This means that polynomial factors such that one factor has conjugate-MIRROR-roots, which can be configured as shown in the figure: I(s) R(s) I(s) R(s) I(s) R(s) I In any case, system is unstable. But how many RHP roots? I Complete Routh array by making polynomial a1(s) from last non-zero row in array. Poly has every second order of s only!! • We do this in a reverse fashion from how we entered a(s) into the array in the first place. I It turns out that a1(s) is a factor of the original a(s). It is missing some orders of s, so IS NOT STABLE (by “case 0”.) I We want to see if it has roots in the RHP or only on the jω-axis. I Replace zero row with coefficients from da1(s) ds and continue. Lecture notes prepared by and copyright c 1998–2013, Gregory L. Plett and M. Scott Trimboli
  • 11. ECE4510/ECE5510, STABILITY ANALYSIS 5–11 EXAMPLE: a(s) = s4 + s3 + 3s2 + 2s + 2. s4 1 3 2 s3 1 2 0 s2 1 2 s1 0 new s1 2 s0 2 No sign changes in Routh array. So, no RHP roots. Roots of a1(s) at s = ± j √ 2. Marginally stable. b1 = −1 1 1 3 1 2 = 1 b2 = −1 1 1 2 1 0 = 2 c1 = −1 1 1 2 1 2 = 0 a1(s) = s2 + 2 da1(s) ds = 2s d1 = −1 2 1 2 2 0 = 2 EXAMPLE: a(s) = s4 + 4 (Hard). s4 1 0 4 s3 0 0 new s3 4 0 s2 0 4 new s2 4 s1 −16 s0 4 Two sign changes. Therefore 2 RHP poles. Other two poles are mirrors in LHP. a1(s) = s4 + 4; da1(s) ds = 4s3 . b1 = −1 4 1 0 4 0 = 0 b2 = −1 4 1 4 4 0 = 4 c1 = −1 4 0 4 = −16 d1 = 16 4 −16 0 = 4 Lecture notes prepared by and copyright c 1998–2013, Gregory L. Plett and M. Scott Trimboli
  • 12. ECE4510/ECE5510, STABILITY ANALYSIS 5–12 5.4: Routh test as a design tool I Consider the system: R(s) Y(s)K s + 1 s(s − 1)(s + 6) T(s) = Y(s) R(s) = K s+1 s(s−1)(s+6) 1 + K s+1 s(s−1)(s+6) = K(s + 1) s(s − 1)(s + 6) + K(s + 1) I We might be interested in knowing for what values of K the system is stable. I Compute the denominator of the transfer function: a(s) = s(s − 1)(s + 6) + K(s + 1) = s3 + 5s2 + (K − 6)s + K. I Perform the Routh test s3 1 K − 6 s2 5 K s1 4K − 30 5 s0 K b1 = −1 5 1 K − 6 5 K = −1 5 (K − 5(K − 6)) = (4K − 30)/5. c1 = −1 b1 5 K b1 0 = −1 b1 (−b1K) = K I For stability of the closed-loop system, K > 0, and K > 30/4. I Step response for different values of K. Lecture notes prepared by and copyright c 1998–2013, Gregory L. Plett and M. Scott Trimboli
  • 13. ECE4510/ECE5510, STABILITY ANALYSIS 5–13 0 2 4 6 8 10 12 −0.5 0 0.5 1 1.5 2 2.5 K=7.5 K=13 K=25 Amplitude Time (sec.) EXAMPLE: R(s) Y(s)K 1 + 1 TI s 1 (s + 1)(s + 2) T (s) = Y(s) R(s) = K TI s+K TI s(s+1)(s+2) 1 + K TI s+K TI s(s+1)(s+2) = K TI s + K TI s(s + 1)(s + 2) + K TI s + K . I a(s) = TI s3 + 3TI s2 + TI (2 + K)s + K. s3 TI TI (2 + K) s2 3TI K s1 TI (K + 2) − K 3 s0 K b1 = −1 3TI TI TI (2 + K) 3TI K = TI (K + 2) − K 3 c1 = −1 b1 3TI K b1 0 = −1 b1 (−b1K) = K Lecture notes prepared by and copyright c 1998–2013, Gregory L. Plett and M. Scott Trimboli
  • 14. ECE4510/ECE5510, STABILITY ANALYSIS 5–14 I For stability of the closed-loop system, K > 0 and TI > 0 and TI > K 3(K + 2) . I Alternately, K < 0 and TI < 0 and TI < K 3(K + 2) for −2 < K < 0, (or instead TI > K 3(K + 2) for K < −2 but this is a contradiction since the quotient is positive and TI is negative by assumption). 0 2 4 6 8 10 12 0 0.5 1 1.5 Time (seconds) K = 3, TI = 0.5 K = 1, TI = 0.25 K = 1, TI = ∞ Amplitude Lecture notes prepared by and copyright c 1998–2013, Gregory L. Plett and M. Scott Trimboli
  • 15. ECE4510/ECE5510, STABILITY ANALYSIS 5–15 5.5: Advanced applications of the Routh test I Note that the Routh test is not specifically a controls recipe. • It is a geometric algorithm. • It counts the number of roots of a polynomial that have R(si) ≥ 0. Modification #1 I Suppose we want to ensure a settling-time specification (or some form of robust stability), so we want R(si) ≤ −σ for all poles. I Routh test doesn’t apply directly; but, perform a change of variables: • Let p = s + σ. Then, si < −σ corresponds to pi < 0. I So, we can perform a Routh test on a(p) instead of a(s). EXAMPLE: Let T (s) = K s2 + 4s + K . For what values of K are all poles to the left of s = −1? I Note, σ = 1, and we let p = s + 1 or s = p − 1. T (p) = K (p − 1)2 + 4(p − 1) + K = K p2 − 2p + 1 + 4p − 4 + K = K p2 + 2p + K − 3 . I So, a(p) = p2 + 2p + (K − 3). Form the Routh array: p2 1 (K − 3) p1 2 p0 (K − 3) I If K > 3, the real part of all poles of T(s) are less than −1. −5 −4 −3 −2 −1 0 1 −2 −1.5 −1 −0.5 0 0.5 1 1.5 2 Real axis Imaginaryaxis Root locus K = 3 Lecture notes prepared by and copyright c 1998–2013, Gregory L. Plett and M. Scott Trimboli
  • 16. ECE4510/ECE5510, STABILITY ANALYSIS 5–16 Modification #2 I When working with digital control systems, the complex frequency domain is represented by “z” instead of “s”, and a system is stable if all poles of T (z) have magnitude strictly less than 1. I The stability region is the unit circle in the z-plane. I The Routh test does not apply directly. I But, we can perform the change of variables (where α > 0) z = 1 + αs 1 − αs or s = 1 α z − 1 z + 1 , which is known as the bilinear transformation. I We can show that this transformation maps the inside of the unit circle in the z-plane to the left-half s-plane. I Let z = rejθ . We have stability if z < 1. So, we want to show that r < 1 produces R(s) < 0. I Substituting into the change of variables s = 1 α rejθ − 1 rejθ + 1 = 1 α rejθ − 1 rejθ + 1 re− jθ + 1 re− jθ + 1 = 1 α      r2 − 1 + j2r sin θ rejθ − re− jθ r2 + 1 + rejθ + re− jθ 2r cos θ      . I Note that: Lecture notes prepared by and copyright c 1998–2013, Gregory L. Plett and M. Scott Trimboli
  • 17. ECE4510/ECE5510, STABILITY ANALYSIS 5–17 • When r = 1, s is purely imaginary (translating the unit circle into the jω axis) • When r < 1, the real part of s is less than zero (translating the inside of the unit disc into the left-half s-plane) • When r > 1, the real part of s is greater than zero (translating the outside of the unit disc into the right-half s-plane). EXAMPLE: Let T (z) = K z + (K − 0.5) . I We can see from inspection (for this simple example) that −0.5 < K < 1.5 will result in a pole location that is between z = −1 and z = +1. I But, let’s perform the bilinear transformation and the Routh test. Choose α = 1. T (s) = T (z)|z=1+s 1−s = K 1+s 1−s + (K − 0.5) = K(1 − s) 1 + s + (K − 0.5)(1 − s) = K(1 − s) (1.5 − K)s + (K + 0.5) . I Form the (trivial) Routh array: s1 (1.5 − K) s0 (K + 0.5) I So, we have stability when K < 1.5 and when K > −0.5, as expected. Lecture notes prepared by and copyright c 1998–2013, Gregory L. Plett and M. Scott Trimboli
  • 18. ECE4510/ECE5510, STABILITY ANALYSIS 5–18 5.6: Internal stability I BIBO stability requires that the output be bounded for every possible bounded input. I However, a system may be input-output stable and still have unbounded internal signals. I The issue is internal stability. I Consider the following diagram: R(s) E(s) U(s) W(s) Y(s)D(s) G(s) I We can find the following four transfer functions: Y(s) R(s) = D(s)G(s) 1 + D(s)G(s) Y(s) W(s) = G(s) 1 + D(s)G(s) . U(s) R(s) = D(s) 1 + D(s)G(s) U(s) W(s) = 1 1 + D(s)G(s) . I For internal stability, all four of these transfer functions must be stable. EXAMPLE: Let G(s) = 1 s − 1 and D(s) = s − 1 s + 1 . I Then, Y(s) R(s) = D(s)G(s) 1 + D(s)G(s) = s−1 (s−1)(s+1) 1 + s−1 (s−1)(s+1) Lecture notes prepared by and copyright c 1998–2013, Gregory L. Plett and M. Scott Trimboli
  • 19. ECE4510/ECE5510, STABILITY ANALYSIS 5–19 = s − 1 (s − 1)(s + 1) + (s − 1) = 1 s + 1 + 1 = 1 s + 2 . I This system passes the test for BIBO stability. I However, Y(s) W(s) = G(s) 1 + D(s)G(s) = 1 s−1 1 + s−1 (s−1)(s+1) = s + 1 (s − 1)(s + 1) + (s − 1) = s + 1 (s − 1)(s + 2) , which is unstable. I Therefore, this system is not internally stable. I In this case, any (even very tiny) amount of disturbance will cause the output y(t) to grow without bound. The feedback will not help. I This brings up the point that it is important to avoid “bad” cancellations of pole-zero pairs! I We cannot stabilize a system by canceling an unstable pole with a compensator zero. • We will see the same idea again from a different perspective when we look at root-locus design. Lecture notes prepared by and copyright c 1998–2013, Gregory L. Plett and M. Scott Trimboli