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Phase and gain margins measure, on a Bode plot, the distance of the open loop from critical feedback conditions.
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Formula
Frequency in rad/s; phase in degrees; GM dimensionless or dB = 20 log10(GM)
| Symbol | Meaning | Unit |
|---|---|---|
| Open-loop transfer function at angular frequency ω | dimensionless transfer ratio | |
| Gain-crossover frequency where |L|=1 (0 dB) | rad/s | |
| Phase-crossover frequency where phase is −180° | rad/s | |
| Phase margin at ωgc | ° | |
| Gain factor to the critical magnitude at ωpc | dimensionless or dB |
\mathrm{PM}=180^\circ+\arg L(j\omega_{gc}),\quad \mathrm{GM}=1/|L(j\omega_{pc})|Original schematic by Quanta
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For the usual unity-feedback loop, phase margin at each 0-dB crossing is 180° plus open-loop phase; gain margin is the reciprocal magnitude at a −180° crossing. Positive distance is a robustness indicator in the usual case, but multiple crossings, unstable open-loop poles, delays and nonminimum-phase behavior require careful Nyquist/stability analysis. Margins are local frequency-domain measures, not a replacement for Routh pole counting; they also depend on loop break and model uncertainty. Report consistently unwrapped phase in degrees.
Continuous linear unity-feedback loop; inspect every relevant 0-dB and −180° crossing. With unstable open-loop poles or multiple crossings, use a full Nyquist analysis.
A margin measures the additional phase or gain distance to the critical feedback condition.
Critical loop magnitude
GMdB is gain margin in decibels at phase crossover.
Phase from margin
Applies at gain crossover under the stated convention.
For L(s)=20/((s+1)(s+2)(s+5)), calculate margins given ωgc≈1.286 rad/s with φ≈−99.30° and ωpc=√17 with |L|=10/63.
PM=180°−99.30°=80.70°.
GM=63/10=6.30; GMdB=20log10(6.30)≈15.99 dB.
Check: 10^(15.99/20)≈6.30.
Report linear GM as a dB value or inspect only one crossing.
Report GM as both factor and dB, and inspect all critical cases when multiple crossings exist.
Formula cluster
Bode margins complement pole-count tests with frequency-domain robustness distances.
For L(s)=20/((s+1)(s+2)(s+5)), the 0-dB crossing is ωgc≈1.286 rad/s with phase −99.30°, giving PM≈80.70°. The −180° crossing is ωpc=√17≈4.123 rad/s; |L|=20/126=10/63, so GM=6.30≈15.99 dB. Check: the three pole phases sum to −180° at ωpc.
Assess frequency-domain robustness margins of continuous unity-feedback systems and compare controller settings.
Here is how to work through a typical Bode plot: gain and phase margins (PM = 180° + φ bei |L|=1; GM = 1/|L| bei φ=−180°) task step by step:
Task
For L(s)=20/((s+1)(s+2)(s+5)), calculate margins given ωgc≈1.286 rad/s with φ≈−99.30° and ωpc=√17 with |L|=10/63.
Solution path
PM=180°−99.30°=80.70°.
GM=63/10=6.30; GMdB=20log10(6.30)≈15.99 dB.
Check: 10^(15.99/20)≈6.30.
Find the frequency where open-loop magnitude is one, or 0 dB. Read phase φ there and calculate PM=180°+φ when phase is near −180°. In the example φ≈−99.30°, giving PM≈80.70°. Unwrap phase consistently across frequency. If there are multiple gain crossings, inspect every critical case rather than reporting only a favorable value. Assume a specified open-loop transfer function with consistent unity feedback. With multiple crossings or unstable open-loop poles, simple read-off rules are insufficient; assess Nyquist stability and model assumptions. Application: Assess frequency-domain robustness margins of continuous unity-feedback systems and compare controller settings. The numerical example For L(s)=20/((s+1)(s+2)(s+5)), the 0-dB crossing is ωgc≈1.286 rad/s with phase −99.30°, giving PM≈80.70°. The −180° crossing is ωpc=√17≈4.123 rad/s; |L|=20/126=10/63, so GM=6.30≈15.99 dB. Check: the three pole phases sum to −180° at ωpc anchors the idea in a concrete measurement case.
Find the frequency where open-loop phase reaches −180°, then evaluate |L| there. The factor up to critical magnitude one is GM=1/|L|; in decibels use 20log10(GM). Here |L|=10/63, so GM=6.30 or about 15.99 dB. Do not confuse the linear factor with its decibel value. Assume a specified open-loop transfer function with consistent unity feedback. With multiple crossings or unstable open-loop poles, simple read-off rules are insufficient; assess Nyquist stability and model assumptions. The corresponding units are Frequency in rad/s; phase in degrees; GM dimensionless or dB = 20 log10(GM). For L(s)=20/((s+1)(s+2)(s+5)), the 0-dB crossing is ωgc≈1.286 rad/s with phase −99.30°, giving PM≈80.70°. The −180° crossing is ωpc=√17≈4.123 rad/s; |L|=20/126=10/63, so GM=6.30≈15.99 dB. Check: the three pole phases sum to −180° at ωpc. This checks that the reference quantities are compatible.
For a usual stable open-loop plant with unity feedback, positive PM and GM indicate distance from critical phase and gain. This is a useful robustness indicator for changes in gain or dynamics. It is not a universal stability guarantee when open-loop poles lie in the right half-plane, multiple crossings occur, or delay and uncertainty are unaccounted for. Assume a specified open-loop transfer function with consistent unity feedback. With multiple crossings or unstable open-loop poles, simple read-off rules are insufficient; assess Nyquist stability and model assumptions.
Write the quantity and unit from the variable list next to every value: Frequency in rad/s; phase in degrees; GM dimensionless or dB = 20 log10(GM). Substitute only after converting to a consistent unit system, and state sign or reference direction explicitly. The example For L(s)=20/((s+1)(s+2)(s+5)), the 0-dB crossing is ωgc≈1.286 rad/s with phase −99.30°, giving PM≈80.70°. The −180° crossing is ωpc=√17≈4.123 rad/s; |L|=20/126=10/63, so GM=6.30≈15.99 dB. Check: the three pole phases sum to −180° at ωpc. is a calculation check: result, unit and order of magnitude must fit the described situation. Round after intermediate calculations so small contributions are not lost prematurely. Assume a specified open-loop transfer function with consistent unity feedback. With multiple crossings or unstable open-loop poles, simple read-off rules are insufficient; assess Nyquist stability and model assumptions.
The background states this starting condition: For the usual unity-feedback loop, phase margin at each 0-dB crossing is 180° plus open-loop phase; gain margin. That limits when the result is a valid model prediction. Compare the problem’s boundary conditions with this assumption before substituting values; real components, material properties or loads can introduce additional effects. The cited reference supports the relation used here but does not remove the need to check whether the specific case fits the model. Assume a specified open-loop transfer function with consistent unity feedback. With multiple crossings or unstable open-loop poles, simple read-off rules are insufficient; assess Nyquist stability and model assumptions.
Quanta exam set
Curated exam set for "Bode plot: gain and phase margins":
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Which formula describes Bode plot: gain and phase margins?
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How do you rearrange Bode plot: gain and phase margins for Critical loop magnitude?
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Which common mistake happens with Bode plot: gain and phase margins?
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Create a curated FSRS exam set for PM = 180° + φ bei |L|=1; GM = 1/|L| bei φ=−180°: formula recall, variables, derivation, rearrangement, worked example, common mistakes and exam context.
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