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3. Consider the following mass-spring-damper system. Let m= 1 kg, b = 10 Ns/m, and k = 20 N/m. b m F k a) Derive the open-loo

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Answer #1

a)

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\tiny m\ddot x = F - kx - b\dot x

\tiny m\ddot x +kx+ b\dot x= F

Take the Laplace transform.

\tiny (ms^2 +bs+k)X(s)= F (s)

1 X(s) F(s) (ms2 + bs + k) 2

Substitute the given values.

\tiny \frac{X(s)}{F (s)} = \frac{1}{(s^2 +10s+20)}

>> G = tf(1, [1 10 20]) G = 1 s^2 + 10 S + 20 Continuous-time transfer function. >> step (G);

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b)

>> G = tf(1, [1 10 20]); >> C = pid (300,0,0); >> T = feedback (G*C,1) T = 300 S^2 + 10 s + 320 Continuous-time transfer func

Step Response 1.4 1.2 1 0.8 Amplitude 0.6 0.4 0.2 0 0.2 0.4 1 1.2 1.4 0.6 0.8 Time (seconds)

c)

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d)

>> G = tf(1, [1 10 20]); >> C = pid (350, 300,50) C = 1 Kp + Ki * + Kd * S 5 with Kp = 350, Ki 300, Kd = 50 Continuous-time P

Step Response 1 0.9 0.8 0.7 0.6 Amplitude 0.5 0.4 0.3 0.2 0.1 0 0 0.5 1 2 2.5 1.5 Time (seconds)

e)

Performance characteristics of a:

>> G = tf(1, [1 10 20]) G = 1 s^2 + 10 s + 20 Continuous-time transfer function. >> stepinfo (G) ans struct with fields: Rise

Performance characteristics of b:

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Performance characteristics of c:

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Performance characteristics of d:

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****Please upvote.******

The original system(a) is overdamped. It does not have any overshoot.

Adding a proportional controller (b) gives an overshoot to the system and it becomes underdamped.

In (c), the derivative part reduces the overshoot and oscillations in the system by increasing the damping ratio.

Finally, the integral part in (d) removes the overshoot in the system makes it rise up quickly. But this increases the settling time of the system.

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