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GM and PM from Bode plot of 1/[s(0.1s+1)(0.2s+1)]

Short answer

Phase crossover at 7.07 rad/s gives GM = 23.5 dB. Gain crossover near 0.98 rad/s gives PM ≈ 73.4°. Both margins positive; closed-loop system is stable.

Find the Gain Margin and Phase Margin using Bode plots for the following transfer function: G(s) = 1/[s(0.1s+1)(0.2s+1)].

G(s)=1s(1+0.1s)(1+0.2s)G(s)=\frac{1}{s(1+0.1s)(1+0.2s)}

Type-1 system, K=1K=1, corner frequencies ω1=1/0.2=5\omega_1 = 1/0.2 = 5 rad/s and ω2=1/0.1=10\omega_2 = 1/0.1 = 10 rad/s.

Magnitude plot (asymptotic)

Range of ω\omegaSlope
ω<5\omega < 5−20-20 dB/dec (pole at origin)
5<ω<105 < \omega < 10−40-40 dB/dec
ω>10\omega > 10−60-60 dB/dec
  • At ω=0.1\omega=0.1: 20log⁡(1/0.1)=2020\log(1/0.1) = 20 dB; at ω=1\omega=1: 0 dB.
  • At ω=5\omega=5: 20log⁡(1/5)=−1420\log(1/5) = -14 dB.
  • At ω=10\omega=10: −14−40log⁡2=−26-14 - 40\log 2 = -26 dB.
  • At ω=100\omega=100: −26−60=−86-26 - 60 = -86 dB.

Phase plot

ϕ(ω)=−90∘−tan⁡−10.1ω−tan⁡−10.2ω\phi(\omega) = -90^\circ - \tan^{-1}0.1\omega - \tan^{-1}0.2\omega
ω\omega (rad/s)0.11257.071020100
ϕ\phi−91.7∘-91.7^\circ−107∘-107^\circ−123∘-123^\circ−161.6∘-161.6^\circ−180∘-180^\circ−198.4∘-198.4^\circ−229.4∘-229.4^\circ−261.4∘-261.4^\circ
 dB
  20 |\ -20dB/dec
   0 |-\---------------------- w
     |  \ wgc~1
 -14 |   \___ w=5  -40
 -26 |        \__ w=10
     |           \  -60
 deg
 -90 |--__
-180 |-------x---------- wpc=7.07
-270 |            ----___

Phase crossover frequency and gain margin

At ωpc\omega_{pc}, ϕ=−180∘\phi=-180^\circ: tan⁡−10.1ω+tan⁡−10.2ω=90∘⇒0.02ω2=1\tan^{-1}0.1\omega+\tan^{-1}0.2\omega = 90^\circ \Rightarrow 0.02\omega^2 = 1.

ωpc=50=7.07 rad/s∣G(jωpc)∣=17.071+0.51+2=115=0.0667GM=20log⁡10.0667=20log⁡15=23.52 dB\begin{aligned} \omega_{pc} &= \sqrt{50} = 7.07\ \text{rad/s}\\ |G(j\omega_{pc})| &= \frac{1}{7.07\sqrt{1+0.5}\sqrt{1+2}} = \frac{1}{15} = 0.0667\\ GM &= 20\log\frac{1}{0.0667} = 20\log 15 = 23.52\ \text{dB} \end{aligned}

Gain crossover frequency and phase margin

From the asymptotic plot, the magnitude is 0 dB at ω≈1\omega\approx1 rad/s. Solving ∣G(jω)∣=1|G(j\omega)|=1 exactly gives ωgc=0.977\omega_{gc}=0.977 rad/s.

ϕ(ωgc)=−90∘−tan⁡−1(0.0977)−tan⁡−1(0.1954)=−90∘−5.58∘−11.05∘=−106.6∘PM=180∘+ϕ(ωgc)=73.4∘\begin{aligned} \phi(\omega_{gc}) &= -90^\circ - \tan^{-1}(0.0977) - \tan^{-1}(0.1954)\\ &= -90^\circ - 5.58^\circ - 11.05^\circ = -106.6^\circ\\ PM &= 180^\circ + \phi(\omega_{gc}) = 73.4^\circ \end{aligned}

(Using the asymptotic value ωgc=1\omega_{gc}=1: PM=180∘−107.0∘=73∘PM = 180^\circ-107.0^\circ = 73^\circ.)

Answer: GM = 23.5 dB at ωpc=7.07\omega_{pc}=7.07 rad/s; PM ≈ 73.4° at ωgc≈0.98\omega_{gc}\approx0.98 rad/s. Both margins are positive, so the closed-loop system is stable.

✓ Answer checked by Claude Opus 5.5 (high effort)

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