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Bode plot of 512(s+3)/[s(s²+16s+256)]

Short answer

Bode plot yields gain crossover at 24.4 rad/s with phase -137.9°, giving phase margin 42.1°. Phase never reaches -180°, so gain margin is infinite. Closed-loop system is stable.

Draw bode plot for open loop transfer function of closed loop system as G(s) = 512(s+3)/[s(s²+16s+256)]. Also comment on stability.

Time-constant form

G(s)=512(s+3)s(s2+16s+256)=6(1+s3)s(1+s16+s2256)G(s) = \frac{512(s+3)}{s(s^2 + 16s + 256)} = \frac{6\left(1 + \dfrac{s}{3}\right)}{s\left(1 + \dfrac{s}{16} + \dfrac{s^2}{256}\right)}

Quadratic factor: ωn=16\omega_n = 16 rad/s and 2ζωn=162\zeta\omega_n = 16, so ζ=0.5\zeta = 0.5.

Factors and corner frequencies

FactorCorner (rad/s)Slope changePhase
K=6K = 6—20log⁡6=15.5620\log6 = 15.56 dB0°
1/s1/s—−20 dB/dec−90°
(1+s/3)(1 + s/3)3+20 dB/dec+tan⁡−1(ω/3)+\tan^{-1}(\omega/3)
quadratic, ζ = 0.516−40 dB/dec0 to −180°

Magnitude asymptotes

RangeSlopeValue
ω < 3−20 dB/dec35.56 dB at 0.1; 15.56 dB at 1; 6.02 dB at 3
3 < ω < 160 dB/dec6.02 dB
ω > 16−40 dB/dec0 dB at 16×106.02/40=22.616 \times 10^{6.02/40} = 22.6; −25.8 dB at 100

With ζ = 0.5 the resonant correction at ωn\omega_n is −20log⁡(2ζ)=0-20\log(2\zeta) = 0 dB, so the asymptotes are close to the true curve.

Phase

ϕ(ω)=−90∘+tan⁡−1ω3−tan⁡−1ω/161−(ω/16)2\phi(\omega) = -90^\circ + \tan^{-1}\frac{\omega}{3} - \tan^{-1}\frac{\omega/16}{1 - (\omega/16)^2}
ω0.1135101624.450100∞
φ (deg)−88.5−75.2−56.0−50.1−62.4−100.6−137.9−163.8−172.4−180

Bode plot

   40 |*
      |*******
      |      ******
   10 |            **************
      |-------------------------****-----------------
      |                            ****
  -20 |                               ***
      |                                  ***
      |                                    ****
  -50 |                                       ****
      |                                          ****
      |                                             *
  -80 |
      +----------------------------------------------
       0.1        1          10          100        1000
Magnitude asymptotes (dB) vs w (rad/s)
    0 |
      |
      |
  -45 |                  ****
      |              *****  ***
      |        *******        **
  -90 |*********               **
      |                         *
      |                         **
 -135 |                          **
      |                           ***
      |                             ******
 -180 |----------------------------------************
      +----------------------------------------------
       0.1        1          10          100        1000
Phase (deg); -180 line shown

Margins and stability

  • Gain crossover: the exact ∣G∣=1|G| = 1 at ωgc=24.4\omega_{gc} = 24.4 rad/s (asymptotic estimate 22.6 rad/s). There, φ = −137.9°, so
PM=180∘−137.9∘=42.1∘PM = 180^\circ - 137.9^\circ = 42.1^\circ
  • Phase crossover: the phase tends to −180° only as ω → ∞, so it never actually crosses −180°. Hence ωpc=∞\omega_{pc} = \infty and GM = ∞.

Both margins are positive, so the closed-loop system is stable, with PM ≈ 42° (reasonably damped). Check: s3+16s2+768s+1536s^3 + 16s^2 + 768s + 1536 gives 16×768>153616 \times 768 > 1536. ✓

Answer: GM = ∞, PM ≈ 42.1° (at 24.4 rad/s). The system is stable.

✓ Answer checked by Claude Opus 5.5 (high effort)

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