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Means OF Partial Fractions

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Process Control Systems 3B

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Warning: TT: undefined function: 32 Warning: TT: undefined function: 32

MEANS OF PARTIAL FRACTIONS,

Inverting yields for the response

no (t) = (1 -4e 3t +3e )u (Table B. 1, APPENDIX B)

Note that as time approaches infinity, no Because no = nin for steady-state operation, the

coefficient of the v = nin term in Equation (4) [Text book] must be unity. This fact is

substantiated by Equation (4) [Text book], which describes the steady-state behaviour of

this system.

(b) Response of this system when all initial conditions

are zero, and u is a step function of constant value

u, and nin = 0.

u For Nin(s) = O and — the transformed equation is:

s

u (6)

AGAIN THIS EQUATION IS OBTAINED BY MEANS OF PARTIAL

FRACTIONS

Inverting yields for the response:

no (t) — (Table B. 1, APPENDIX B)

For steady-state operation, no = -5u. As is verified by Equation (4), the coefficient of the u term is -5.

The steady-state behaviour does not depend on the values of and T2, but the transient 1 behaviour does. For example, if =and — , the transformed equation becomes 15 2

(7)

n For Nin (s) =

s

and U(s) = 0, the preceding becomes:

n (8)

Inverting yields for the response:

-12t n

For Nin (s) = 0

u and U(s) — S

Equation (7) becomes:

u (9)

Inverting yields for the response:

-12t u

NOTE: See different partial fraction techniques, paragraph 3.

Example 6

Ref. RAVEN example 5, page 188.

See question in text book.

Solution

Response ofthe system to a unit step change in the input x. From the open-loop system, Fig. (5) [Text book], the equation relating the output y to the input x is:

K 1

x [K = I and (given)]

1+tD 1+51)

i. Y + 5Dy = x

thus

5

Transforming each term yields for the Laplace transform

sY(s) - y(0) + =

For y(0) = O (initial conditions are zero)

(1)

and

(unit step change in the input x)

5

s

then Equation (1) becomes

(partial-fraction expansion)

Inverting yields for the response

(Table B l , APPENDIX B)

This result shows that the time constant is 5 and the steady-state gain is 1.

-o,2t

i.

i. x

Therefore the equation relating the output y to the input x is:

x (1)

To decrease the time constant by a factor of 10, then 1 + KIK2 =10. To maintain the same steady-state gain of l ,

Hence

From the relationship 1 +KlK2 =1 +10K2 = 10, it follows that K2 0,9.

Response ofthis system to a unit step change in the input x. Substitute the values of Kl and K2 into Equation (1), the resulting input-output equation is: 1 x 1 + o,5D

or Dy + 2y = 2x

Transforming each term yields for the Laplace transform: sY(s) - y(0) + 2Y(s) = 2X(s)

For y(0) = 0 (initial conditions are zero)

2X(s) (2)

1 and X(s) = (unit step change), then Equation (2) becomes s

2 1 1

(partial-fraction expansion)

Inverting yields for the response -t/0,

This result shows that the time constant — 0,5 has been reduced by a factor of 10 and the steady-

state gain remains 1.

The partial-fraction expansion constants are:

— 214 -

Thus

3 4 1

Inverting yields for the response:

c(t) = 3e-t - 4e 2t + e

The derivative is:

t 8e-2t - 3 e

Substitution oft = 0+ into the preceding expressions shows that c(0+) 0 and c' (0+) -2.

These values may also be verified by application of the initial-value theorem.

c(0+) = S = 00

c l (0+) = limsL[c l = s[sC(s) —

Note that the initial value c l (0) = 0 at time t = 0- is different from the value c l (0+) at time t = 0+. Thus, this problem could not be solved by classical methods.

Example 9

Example 12

For the second-order system shown in Fig. 3, of which the transfer function is given by:

9 s 2

+3s+

Determine the following transient response characteristics for a unit-step input:

  1. peak time tp;

  2. the percentage overshoot (PO), and

  3. rise time tr.

  4. the settling time, ts

Solution

1. Peak time tp

Figure 3.

The closed-loop transfer ftmction, T(s), is given by ( See Chapter 2, paragraph 2.12).

The denominator of the closed-loop transfer function does not have real roots.

Thus s 2 + 3s + 18 = s 2 + 2Cons - Fon

2

9

therefore (1)

From equation (1), the undamped natural frequency (on) and the damping ratio (C), can be

determined.

on = 4,24 rad/s c = 0,

The damped natural frequency (Od), is then:

4,24 1 -0,354 2

= 3,965 rad/ s

The peak time is then:

tP

3,

= 0,792 sec

2. Percentage overshoot

PO = exp x 100%

Thus

c(t) (2)

The steady-state value is thus 0,5.

Suppose ti is the time taken for the response to reach 10 % of the steady-state value.

(See Fig.3).

Thus

10

c(tl )

10

= 0,05 units

Now, equation (2) becomes:

0 05 — — 2

Therefore ti = 0, 113 sec

Suppose t2 is the time taken for the response to reach 90 % of the steady-state value, 1.

(Again: See Fig. 3).

Thus

90

100

2

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Means OF Partial Fractions

Course: Process Control Systems 3B

22 Documents
Students shared 22 documents in this course
Was this document helpful?
MEANS OF PARTIAL FRACTIONS,
Inverting yields for the response
no (t) = (1 -4e 3t +3e )u (Table B. 1, APPENDIX B)
Note that as time approaches infinity, no Because no = nin for steady-state operation, the
coefficient of the v = nin term in Equation (4.1) [Text book] must be unity. This fact is
substantiated by Equation (4.12) [Text book], which describes the steady-state behaviour of
this system.
(b) Response of this system when all initial conditions
are zero, and u is a step function of constant value
u, and nin = 0.
u
For Nin(s) = O and the transformed equation is:
s
u (6)
AGAIN THIS EQUATION IS OBTAINED BY MEANS OF PARTIAL
FRACTIONS
Inverting yields for the response:
no (t) (Table B. 1, APPENDIX B)
For steady-state operation, no = -5u. As is verified by Equation
(4.12), the coefficient of the u
term is -5.