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oftheastepresponseofthesystem. T ofasystemprovidesaqualitativedefinitionofthefilteringcapabilitiesofthesystem,andprovidesalsoaqualitativemeasureoftherisetime ω G / 2 ,thatis3dblessthanthestaticgain G .Thebandwidth √ :thefrequencywherethemoduleoffunction 3.B

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0.0. 4.3 1

Bandwidth

The time behavior of the module Bode diagram of a feedback system G0(s) is usually similar to that of a second-order system, due to the presence of two dominant complex conjugates poles:

Amplitude

Mmax

G0

G0/ 2

The frequency parameters that characterize this frequency response are:

1. Resonance frequency ωR: the frequency where the module of function G0(jω) is maximum;

2. Resonance peak MR: the ratio between the maximum module Mmax of function G0(jω) and the static gain G0 = G0(0): MR = Mmax/G0; 3. Bandwidth ωf: the frequency where the module of function G0(jω) is

equal to G0/√

2, that is 3 db less than the static gain G0.

The bandwidth ωf of a system provides a qualitative definition of the filtering capabilities of the system, and provides also a qualitative measure of the rise time Ts of the a step response of the system.

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4.3. BANDWIDTH 4.3 2

The qualitative relation between bandwidth ωf and rise time Ts is:

Ts ∝ 1 ωf

that is, the rise time Ts is proportional to the inverse of bandwidth ωf.

For first-order systems the relation is evident: the rise time Ts is proportional to time constant τ while bandwidth ωf = τ1 is inversely proportional to τ . It can be shown that relation Ts ∝ 1/ωf holds also for high order systems.

In feedback systems with high loop gain, i.e. H(s)G(s) ≫ 1, the bandwidth ωf 0 of feedback system G0(s) can be easily obtained (in an approximate way) from the module Bode diagram of function H(s)G(s).

- - -



6 G(s)

H(s)

r(t) e(t) c(t)

G0(s) = G(s) 1 + H(s)G(s)

Let us suppose, for example, that H(s) = 1. In this case, it follows that:

G0(jω) = G(jω)

1 + G(jω) ≃

1 if |G(jω)| ≫ 1 G(jω) if |G(jω)| ≪ 1

If G(jω) ≃ G0 ≫ 1 when ω < ωf, the frequency response of function G0(jω) remains almost constant, equal to 1, for all the frequencies ω that belong ro the bandwidth: ω < ωf.

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4.3. BANDWIDTH 4.3 3

Amplitude Bode diagrams of functions , G(s) and G0(s):

G0

1

The bandwidth of the feedback system (from 0 to ωf 0) is greater than that of the open loop system (from 0 to ωf).

The bandwidth ωf 0 of a feedback system can be easily obtained from the Nyquist diagram:

−2 −1.5 −1 −0.5 0 0.5 1 1.5 2

−1.5

−1

−0.5 0 0.5 1 1.5

0.47 0.56

0.68 0.82

1 1.2 1.5 2.2

0.15 0.18 0.22 0.27 0.33 0.39 0.47 0.56 0.68 1

Nyquist diagram

0 10 20 30 40 50 60

0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8

risposta nel tempo

secondi

In the figure are shown the Nyquist diagrams of the following two systems:

G1(s) = 10

s(s + 1)2(s + 10), G2(s) = 2

s(s + 1)2(s + 10)

Next to the Nyquist diagrams are shown the time behaviors of the step response of the corresponding feedback systems. In both cases the rise time (Ts1 ≃ 1.7 and Ts2 ≃ 7 s) is “inversely proportional” to the bandwidth of the two feedback systems (ωf 01 ≃ 0.68 and ωf 02 ≃ 0.19).

Riferimenti

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