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Assign. #10 - Gene and Linda Voiland School of Chemical ...

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BE 440/ChE 441<br />

Unified Systems Bioengineering II/<br />

Process Control<br />

Fall, 2009<br />

Washington State University<br />

Voil<strong>and</strong> <strong>School</strong> <strong>of</strong> <strong>Chemical</strong> Engineering <strong>and</strong><br />

Bioengineering<br />

Richard L. Zollars<br />

Homework <strong>Assign</strong>ment <strong>#10</strong><br />

Due: October 2, 2009<br />

You are working with a system described by the following transfer function<br />

G(<br />

s)<br />

<br />

K <br />

a<br />

s 1<br />

<br />

s 1<br />

s 1<br />

1 2<br />

<br />

where K = 1, τ 1 = 4 <strong>and</strong> τ 2 = 1. This system will be subjected to a unit step change at t = 0.<br />

Enter this transfer function in to Simulink <strong>and</strong> plot the response <strong>of</strong> the system for the<br />

following values <strong>of</strong> τ a : -4, -1, 1, 4, 8 <strong>and</strong> 16. (Plot the values out to t = 20). Using a partial<br />

fraction expansion determine equation representing the time domain response <strong>of</strong> this system<br />

for three values <strong>of</strong> τ a : τ a = -4, 1, <strong>and</strong> 8. In the time domain equation, what has changed in the<br />

equation for the various values <strong>of</strong> τ a ?<br />

SOLUTION<br />

The Simulink file used to generate the data for this problem is shown below<br />

Clock<br />

time<br />

To Workspace1<br />

Step<br />

-4s+1<br />

4s 2+5s+1<br />

Transfer Fcn<br />

Out<br />

To Workspace<br />

The plot <strong>of</strong> the results is shown on the following page. Substituting -4 for τ a into the transfer<br />

function <strong>and</strong> using a unit step function for the input gives the following expression for the<br />

output (Y(s))


3<br />

<strong>Assign</strong>ement <strong>#10</strong><br />

2.5<br />

2<br />

Taua = -4<br />

Taua = -1<br />

Taua = 1<br />

Taua = 4<br />

Taua = 8<br />

Taua = 16<br />

1.5<br />

Output<br />

1<br />

0.5<br />

0<br />

-0.5<br />

0 2 4 6 8 10 12 14 16 18 20<br />

Time<br />

Y ( s)<br />

<br />

s<br />

<br />

4 s 1<br />

4<br />

s 1s<br />

1<br />

<br />

1 <br />

<br />

s <br />

4 <br />

1 <br />

s s s<br />

1<br />

4 <br />

The form for a partial fraction expansion is<br />

Y ( s)<br />

<br />

1 <br />

<br />

s <br />

4 <br />

<br />

1 <br />

s s s<br />

1<br />

4 <br />

A<br />

s<br />

B<br />

<br />

1 <br />

s <br />

4 <br />

<br />

C<br />

s 1<br />

<br />

<br />

Multiply both sides by s <strong>and</strong> let s = 0 to get A = 1. Multiply both sides by (s + ¼) then let<br />

s = -1/4 to get B = -8/3. Finally multiply both sides by (s + 1) then let s = -1 to get C = 5/3.<br />

So for τ a = -4.0 the time domain response (y(t)) is<br />

t<br />

8 <br />

4<br />

( t)<br />

1 e<br />

y<br />

3<br />

5<br />

e<br />

3<br />

t


For τ a = 1 the LaPlace domain expression is<br />

Y ( s)<br />

<br />

s<br />

s<br />

1<br />

4<br />

s 1s<br />

1<br />

<br />

1<br />

<br />

4s<br />

s <br />

<br />

1 <br />

<br />

4 <br />

<br />

A B<br />

<br />

s 1 <br />

s <br />

4 <br />

Multiply by s <strong>and</strong> let s = 0 to get A = 1. Multiply by (s + ¼) <strong>and</strong> let s = -1/4 to get B = -1.<br />

This gives a time domain response <strong>of</strong><br />

y(<br />

t)<br />

1 e<br />

t<br />

<br />

4<br />

For τ a = 4 the LaPlace domain expression is<br />

Y ( s)<br />

<br />

s<br />

8s<br />

1<br />

4<br />

s 1s<br />

1<br />

<br />

<br />

8s<br />

1<br />

1 <br />

4s<br />

s s<br />

1<br />

4 <br />

<br />

<br />

A B<br />

<br />

s 1 <br />

s <br />

4 <br />

<br />

C<br />

s 1<br />

<br />

<br />

Multiply by s <strong>and</strong> let s = 0 to get A = 1. Multiply by (s + ¼) <strong>and</strong> let s = -1/4 to get B = 4/3.<br />

Multiply by (s + 1) <strong>and</strong> let s = -1 to get C = -7/3. This gives a time domain response <strong>of</strong><br />

t<br />

4 <br />

4<br />

( ) 1 <br />

y t<br />

e<br />

3<br />

<br />

7<br />

e<br />

3<br />

t<br />

There are two time dependent portions <strong>of</strong> all <strong>of</strong> the solutions; e -t/4 <strong>and</strong> e -t . Since the time<br />

constant for the first <strong>of</strong> these is 4 it is the slower <strong>of</strong> the two solutions. For τ a = -4 the<br />

coefficient on this slower term is larger in magnitude than the coefficient on the faster term.<br />

In addition the coefficient on the slower term is negative while that on the faster term is<br />

positive. Thus at small times, when both solutions influence the final result, the system<br />

response first goes in the wrong direction (lower for a positive step change). For τ a = 8 the<br />

situation is reversed with the coefficient on the slower solution being positive <strong>and</strong> small in<br />

magnitude. Thus at short times the faster solution plays a major role resulting in an<br />

overshoot. As the faster solution decays away the system response approaches the new<br />

steady-state from the side opposite the initial state. For τ a = 1 we get a cancellation between<br />

a term in the numerator <strong>and</strong> the denominator. As a result there is only one time dependent<br />

solution, he slower <strong>of</strong> the two responses in the other two cases. Thus the system response is<br />

a monotonic increase to the new steady-state.

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