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Feedback Control: Stabilizing Unstable Systems with Pole Placement, Exams of Signals and Systems

Methods for stabilizing unstable systems using feedback control. It covers the use of a cascade controller and a feedback controller, as well as the importance of negative feedback for system stabilization. The document also discusses the application of these techniques to various types of systems, including mechanical actuators and transfer functions. Students of electrical engineering and computer science (eecs) may find this document useful for understanding the concepts of feedback control and pole placement in systems engineering.

Typology: Exams

Pre 2010

Uploaded on 09/02/2009

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Download Feedback Control: Stabilizing Unstable Systems with Pole Placement and more Exams Signals and Systems in PDF only on Docsity! EECS 216 FEEDBACK CONTROL Given: Fixed LTI system with impulse response h(t) = e2tu(t) (unstable!) Goal: Somehow connect a controller to the system to make system stable. Open Use cascade controller (compensator) C(s) in series with given system Loop: H(s)=L{e2tu(t)}= 1s−2=→ C(s)= 1H(s)=s–2→ c(t) ∗ x(t)=dxdt − 2x(t). But: This is a BAD idea: Roundoff error→won’t cancel pole {2} exactly! Closed Use a feedback controller G(s) = K (constant gain) in feedback loop: Loop: x(t) → ⊕ → |h(t)| → • → y(t) equivalent to Y (s)X(s) = H(s) 1−G(s)H(s) . տ |g(t)| ւ (feedback connection) Then: HCLOSED LOOP (s)=HCL(s)= Y (s) X(s)= H(s) 1−KH(s)=[ 1 s−2 ]/[1 − K 1s−2 ] = 1s−2−K . Pole: K+2<0 if K<–2. In fact, K=–102→ hCLOSED LOOP (t)=hCL(t)=e −100tu(t)! Note: We need K<0→negative feedback to stabilize an unstable system. Given: Mechanical actuator has a very slow step response s(t)=(1–e−t)u(t). Goal: Use feedback to speed up step response so output tracks input rapidly. Have: S(s)=1s– 1 s+1= 1 s(s+1) → H(s)= 1s+1 → HCL(s)=[ 1s+1 ]/[1–K 1s+1 ]= 1s+1−K Then: Using K=–99→ HCL(s)= 1s+100 → SCL(s)= 1s(s+100)=0.01s – 0.01s+100 And: sCL(t)=.01u(t)–.01e −100tu(t). Much faster! Also need amplify ×100. Given: h(t)=cos(t)u(t)→H(s)= s s2+1 → HCL(s)=[ ss2+1 ]/[1−K ss2+1 ]= ss2−Ks+1 . Poles: K2 ± √ (K2 ) 2 − 1. Need K < 0 (negative feedback again) to stabilize. |K| < 2 : Poles: K2 ± j √ 1 − (K2 )2 both lie on the unit circle at e±j cos −1(K/2). |K| > 2 : Poles: K2 ± √ (K2 ) 2 − 1 both lie on the real axis (their midpoint is K2 ). K=–2: Double pole at –1→ HCL(s)= s(s+1)2 → hCL(t)=(1–t)e−tu(t) (try s−1s2 ) Note: H(s)=N(s)D(s) → HCL(s)= N(s)/D(s) 1−KN(s)/D(s)= N(s) D(s)−KN(s)=polynomial ratio. So: Zeros unchanged; Poles move from roots of D(s)=0 to D(s)–KN(s)=0 Problem: What choices of poles? Need:plot of roots of D(s)–KN(s)=0 as K varies Solution: This is called a root locus. Learn about it in EECS 460. Above example: EX: K decreases from 0 to −∞: Poles move along unit circle from ±j to -1; coalesce at –1; split apart; move in opposite directions along real axis. One pole becomes “fast,” other becomes “slow.” Fastest for both=–1.
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