22-Mec-A3 System Analysis and Control · December 2017
Question 5 of 6: Lead-Compensator Design for Specified Damping and Natural Frequency
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
Paper format. National Exams, December 2017 — 16-Mec-A3, System Analysis and Control. Three hours, closed book; a Casio or Sharp approved calculator and semi-log graph paper are the only permitted aids. Six questions are printed; any four constitute a complete paper and all questions are of equal value (25 marks each). A table of Laplace transforms is supplied as page 5. All six questions are solved here.
Reference texts. K. Ogata, Modern Control Engineering, 5th ed. (Prentice Hall) — the source of this paper's problem style; N. S. Nise, Control Systems Engineering, 7th ed. (Wiley); R. C. Dorf and R. H. Bishop, Modern Control Systems, 13th ed. (Pearson); G. F. Franklin, J. D. Powell and A. Emami-Naeini, Feedback Control of Dynamic Systems, 8th ed. (Pearson).
Check: conventions used throughout. All transfer functions are written in the Laplace variable s with zero initial conditions unless a question states otherwise. “Unity feedback” means \(H(s)=1\), so the closed-loop transfer function is \(T(s)=G(s)/[1+G(s)]\) and the error signal is \(E(s)=R(s)-C(s)\). Root-locus gains are the gain \(K\) exactly as it appears in the printed \(G(s)\).
Question 5: Lead-Compensator Design for Specified Damping and Natural Frequency (25 marks)
Given. A unity-feedback loop with a first-order (lead or lag) compensator \(G_c(s)=K\dfrac{T_1s+1}{T_2s+1}\) in cascade with the plant \(G_p(s)=\dfrac{10}{s(s+1)}\). Three parameters \(K\), \(T_1\), \(T_2\) are free.
Find. Values of \(K\), \(T_1\) and \(T_2\) such that the dominant closed-loop poles have \(\zeta=0.5\) and \(\omega_n=3\) rad/s.
Figure 5.1 — The compensated unity-feedback system of Question 5, with the designed parameter values annotated.
Approach. Three unknowns against only two specifications leaves one degree of freedom; use it in the standard way — let the compensator zero cancel the plant pole at \(s=-1\), which reduces the loop to a pure second-order system whose two remaining parameters map directly onto \(\zeta\) and \(\omega_n\).
Write the target characteristic polynomial. Dominant poles with \(\zeta=0.5\), \(\omega_n=3\) require
$$s^2+2\zeta\omega_n s+\omega_n^2=s^2+2(0.5)(3)s+3^2=s^2+3s+9=0$$
whose roots are
$$s=-\zeta\omega_n\pm j\omega_n\sqrt{1-\zeta^2}=-1.5\pm j\,3\sqrt{0.75}=-1.5\pm j2.5981$$
Use the spare degree of freedom to cancel the plant pole. Setting the compensator zero at \(s=-1/T_1\) on top of the plant pole at \(s=-1\) means
$$\frac{1}{T_1}=1\;\Longrightarrow\;\boxed{\;T_1=1\ \text{s}\;}$$
The open-loop transfer function then collapses to a second-order form:
$$G(s)=K\,\frac{s+1}{T_2s+1}\cdot\frac{10}{s(s+1)}\cdot\frac{1}{1}=\frac{10K}{s\left(T_2s+1\right)}=\frac{10K/T_2}{s\left(s+1/T_2\right)}$$
Close the loop and match coefficients. With unity feedback the characteristic equation is \(s(s+1/T_2)+10K/T_2=0\), i.e.
$$s^2+\frac{1}{T_2}\,s+\frac{10K}{T_2}=0$$
Comparing term by term with \(s^2+3s+9=0\):
$$\frac{1}{T_2}=2\zeta\omega_n=3\;\Longrightarrow\;\boxed{\;T_2=\frac{1}{3}=0.3333\ \text{s}\;}$$
$$\frac{10K}{T_2}=\omega_n^2=9\;\Longrightarrow\;10K(3)=9\;\Longrightarrow\;\boxed{\;K=0.3\;}$$
Verify the design. Substituting back, the compensated open loop is \(G(s)=3/[s(s+3)]\) and the closed-loop characteristic polynomial is \(s^2+3s+9\), whose roots are \(-1.5\pm j2.5981\). These give
$$\omega_n=\sqrt{1.5^2+2.5981^2}=3.000\ \text{rad/s},\qquad \zeta=\frac{1.5}{3.000}=0.500\ \checkmark$$
Because \(T_1=1\) cancels the plant pole exactly, these are the only two closed-loop poles — so “dominant” is satisfied trivially rather than approximately.
Report the resulting performance. The compensated loop remains type 1, with velocity error constant
$$K_v=\lim_{s\to0}sG(s)=\lim_{s\to0}s\cdot\frac{10K}{s\left(T_2s+1\right)}=10K=3\ \text{s}^{-1}\;\Longrightarrow\;e_{ss,\text{ramp}}=\frac{1}{K_v}=0.333$$
and the standard second-order formulae give
$$M_p=e^{-\pi\zeta/\sqrt{1-\zeta^2}}=e^{-\pi(0.5)/0.8660}=16.3\%,\qquad t_s\approx\frac{4}{\zeta\omega_n}=\frac{4}{1.5}=2.67\ \text{s}$$
Check: the pole-cancellation choice. The problem supplies three unknowns for two specifications, so the solution is not unique — any \((K,T_1,T_2)\) placing a dominant pair at \(-1.5\pm j2.5981\) satisfies the stated requirement, with the third closed-loop pole then sitting somewhere on the negative real axis. Cancelling the plant pole with the compensator zero (\(T_1=1\)) is the standard textbook resolution because it makes the dominant pair exact rather than approximate and yields the clean values above. In hardware, exact cancellation is never achieved; a small residual pole–zero dipole near \(s=-1\) would add a slow, low-amplitude tail to the step response without materially changing \(\zeta\) or \(\omega_n\). This assumption is stated here in accordance with Note 1 of the examination paper.
Quantity
Result
Target characteristic polynomial
\(s^2+3s+9=0\)
Dominant closed-loop poles
\(s=-1.5\pm j2.5981\)
Compensator zero constant
\(T_1=1\) s (cancels the plant pole at \(s=-1\))
Compensator pole constant
\(T_2=1/3=0.3333\) s
Compensator gain
\(K=0.3\)
Compensated open loop
\(G(s)=3/[s(s+3)]\)
Velocity error constant
\(K_v=3\ \text{s}^{-1}\), \(e_{ss}=0.333\) for a unit ramp