stability is the most important system specification
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* STABILITYISTHEMOSTIMPORTANTSYSTEM
SPECIFICATION. IFASYSTEMISUNSTABLE,
TRANSIENTRESPONSEANDSTEADY-STATEERRORS
AREMOOTPOINTS.* ANUNSTABLESYSTEMCANNOTBEDESIGNEDFOR
ASPECIFICTRANSIENTRESPONSEORSTEADY-STATE
ERRORREQUIREMENT.
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TOTALRESPONSEOFASYSTEM
is the sum of the forced and natural responses, or
C(t) = cforced (t)+ cnatural(t)
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STABILITYFORLINEAR, TIME-INVARIANTSYSTEMS.
Using the natural response:
1. A system is stable if the natural response approaches zero
as time approaches infinity.
2. A system is unstable if the natural response approaches
infinity as time approaches infinity.
3. Asystem is marginally stable if the natural response
neither decays nor grows but remains constant or
oscillates.
Using the total response (BIBO):
1. A system is stable if every bounded input yields a bounded
output.
2. A system is unstable if any bounded input yields an
unbounded output.
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SECOND-ORDER SYSTEMS
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OVERDAMPED RESPONSE
* has a pole at the origin that comes from the unit step input and two
real poles that come from the system* The input pole at the origin generates the constant forced response; each of
the two system poles on the real axis generates an exponential
natural response whose exponential frequency is equal tothe ole location.
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UNDERDAMPED RESPONSE
This function has a pole at the origin that comes from the unit step input and two complex poles that comefrom the system.
the poles that generate the natural response are at s= -1 j(sq2)
the real part of the pole matches the exponential decay frequency of the sinusoids amplitude, while the
imaginary part of the pole matches the frequency of the sinusoidal oscillation
The time constant of the exponential decay is equal to the reciprocal
of the real part of the system pole. The value of the imaginary part
is the actual frequency of the sinusoid, as depicted in Figure 4.8.
* This sinusoidal frequency is given the name damped frequency of
oscillation, vd. Finally, the steady-state response (unit step)
was generated by the input pole located at the origin
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UNDAMPED RESPONSE
*has a pole at the origin that comes from the unit step inputand two imaginary poles that come from the system.
The input pole at the origin generates the constant forced
response, and the two system poles on the imaginary axis at
j3 generate a sinusoidal natural response whose frequency
is equal to the location of the imaginary poles.
c(t) = K1 + k4 cos(3t )
Note that the absence of a real part in the pole pair
corresponds to an exponential that does not decay.
Mathematically, the exponential is e -0t =1.
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CRITICALLY DAMPED RESPONSE
* This function has a pole at the origin that comes from the unit step input and two
multiple real poles that come from the system.The input pole at the origin generates the constant forced response, and the two
poles on the real axis at 3 generate a natural response consisting of an
exponential and an exponential multiplied by time, where the exponential
frequency is equal to the location of the real poles
* Critically damped responses are the fastest possible without the overshoot that
is characteristic of the underdamped response.
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Natural Frequency, Wn - The natural frequency of a
second-order system is the frequency of oscillation of the
system without damping.
- For example, the frequency of oscillation of a series RLC
circuit with the resistance shorted would be the natural
frequency.
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DAMPING RATIO,
Aviable definition for this quantity is one that compares the
exponential decay
frequency of the envelope to the natural frequency.
the ratio is constant regardless of the time scale of the response
the reciprocal, which is proportional to the ratio of the natural periodto the exponential time constant, remains the same regardless of the
time base.
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