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Bode plot of 48(1+s)/[s²(1+3s)(1+0.5s)(2+0.2s)]

Short answer

From the Bode plot of G(s)=24(1+s)/[s²(1+3s)(1+0.5s)(1+0.1s)], phase remains below −180° at all finite frequencies, so no phase crossover exists. Gain crossover ωgc≈2.34 rad/s gives PM≈−77.6°. Gain margin is negative (effectively −∞ dB); the closed-loop system is unstable.

Draw the bode plot for transfer function G(s) = 48(1+s)/[s²(1+3s)(1+0.5s)(2+0.2s)]; from the graph determine (i) Phase crossover frequency (ii) Gain crossover frequency (iii) P.M (iv) G.M (v) Stability of the system.

Step 1: Time-constant form

G(s)=48(1+s)s2(1+3s)(1+0.5s)(2+0.2s)=24(1+s)s2(1+3s)(1+0.5s)(1+0.1s)G(s)=\frac{48(1+s)}{s^2(1+3s)(1+0.5s)(2+0.2s)} = \frac{24(1+s)}{s^2(1+3s)(1+0.5s)(1+0.1s)}
  • K=24K=24, type-2 (double pole at origin): initial slope −40-40 dB/dec.
  • Corner frequencies: pole 1/3=0.3331/3=0.333, zero 11, pole 1/0.5=21/0.5=2, pole 1/0.1=101/0.1=10 rad/s.

Step 2: Asymptotic magnitude plot

RangeFactor addedNet slope
ω<0.333\omega<0.33324/s224/s^2−40-40 dB/dec
0.3330.333–11pole 1/(1+3s)1/(1+3s)−60-60 dB/dec
11–22zero (1+s)(1+s)−40-40 dB/dec
22–1010pole 1/(1+0.5s)1/(1+0.5s)−60-60 dB/dec
>10>10pole 1/(1+0.1s)1/(1+0.1s)−80-80 dB/dec
ω=0.1: 20log⁡(24/0.01)=67.6 dBω=0.333: 67.6−40log⁡(3.33)=46.7 dBω=1: 46.7−60log⁡3=18.1 dBω=2: 18.1−40log⁡2=6.0 dBω=10: 6.0−60log⁡5=−35.9 dB\begin{aligned} \omega=0.1:&\ 20\log(24/0.01) = 67.6\ \text{dB}\\ \omega=0.333:&\ 67.6-40\log(3.33)=46.7\ \text{dB}\\ \omega=1:&\ 46.7-60\log 3 = 18.1\ \text{dB}\\ \omega=2:&\ 18.1-40\log 2 = 6.0\ \text{dB}\\ \omega=10:&\ 6.0-60\log 5 = -35.9\ \text{dB} \end{aligned}

Step 3: Phase plot

ϕ(ω)=−180∘+tan⁡−1ω−tan⁡−13ω−tan⁡−10.5ω−tan⁡−10.1ω\phi(\omega) = -180^\circ + \tan^{-1}\omega - \tan^{-1}3\omega - \tan^{-1}0.5\omega - \tan^{-1}0.1\omega
ω\omega0.10.20.512410
ϕ\phi−194∘-194^\circ−207∘-207^\circ−227∘-227^\circ−239∘-239^\circ−253∘-253^\circ−275∘-275^\circ−307∘-307^\circ
 dB  67 |\ -40
     46 | \__ -60
     18 |     \__ -40
      6 |        \__ -60
      0 |-----------x-------- w
                 wgc~2.5
deg -180|------------------- w
        |\___
        |    \____ (always
        |         \__ below -180)

(i) Phase crossover frequency

tan⁡−13ω>tan⁡−1ω\tan^{-1}3\omega > \tan^{-1}\omega for every ω>0\omega>0, so the phase is always below −180∘-180^\circ; it equals −180∘-180^\circ only in the limit ω→0\omega\to0. The phase curve never crosses −180∘-180^\circ at a finite non-zero frequency, so ωpc\omega_{pc} does not exist (it is at ω=0\omega=0).

(ii) Gain crossover frequency

From the asymptotic plot, the slope is −60-60 dB/dec after ω=2\omega=2 (6 dB): 6.0−60log⁡(ω/2)=0⇒ωgc=2.526.0 - 60\log(\omega/2)=0 \Rightarrow \omega_{gc}=2.52 rad/s. The exact value from ∣G(jω)∣=1|G(j\omega)|=1 is ωgc=2.34\omega_{gc}=2.34 rad/s.

(iii) Phase margin

ϕ(2.34)=−180∘+66.8∘−81.9∘−49.4∘−13.1∘=−257.6∘PM=180∘+(−257.6∘)=−77.6∘\begin{aligned} \phi(2.34) &= -180^\circ + 66.8^\circ - 81.9^\circ - 49.4^\circ - 13.1^\circ = -257.6^\circ\\ PM &= 180^\circ + (-257.6^\circ) = -77.6^\circ \end{aligned}

(iv) Gain margin

The phase crossover is effectively at ω=0\omega=0, where the magnitude is infinite, so GM is negative (−∞ dB). Since the phase stays below −180∘-180^\circ at every frequency, no reduction in gain can make the system stable.

(v) Stability

PM is negative and GM is negative, so the closed-loop system is unstable. Check: the characteristic equation 0.3s5+3.7s4+7.2s3+2s2+48s+48=00.3s^5+3.7s^4+7.2s^3+2s^2+48s+48=0 has roots 0.995±j1.940.995\pm j1.94 in the right half plane.

Answer: ωpc\omega_{pc} – none (phase always below −180°); ωgc≈2.34\omega_{gc}\approx2.34 rad/s (2.5 rad/s asymptotic); PM ≈ −77.6°; GM negative; closed loop unstable.

✓ Answer checked by Claude Opus 5.5 (high effort)

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