In electrical and
mechanical Engineering, a transient response or natural response is the reaction of a system to a change from
equilibrium (steady state). Over an infinitely long time of being unperturbed, the system again returns to a
steady state a either its original state or some new state.
In an electrical system, a simple example of
transient response would be the output of a DC power supply when it is turned on. The output voltage is initially
0 V, and sometime after being switched on, settles into some new voltage level. During the transition from 0 V to
some new DC voltage level, the output voltage follows some variation of the three waveforms illustrated below. An
underdamped supply would allow the output voltage to swing higher than the final voltage (a potentially
destructive scenario). Overdamping would cause the output voltage to take an excessively long time to reach the
final value. A critically damped system allows the voltage to ramp up as quickly as theoretically possible without
ever overshooting the final steady state voltage level. Choosing appropriate values of resistance, inductance, and
capacitance allows the response to be tailored to the specific need.
In a mechanical system, a simple
example is a mass/spring/damper system. The transient response is the position of the mass as the system returns
to equilibrium after an initial force or a non zero initial condition. Think of jumping on the bumper of a car and
observing who the car moves when you get off. An over damped system results in it being difficult to even get the
car rocking. Under damped results in the car bouncing up and down many cycles after you get off. Critically damped
results in a smooth return to the neutral position.
|f(t) = A1*es1t + A2*es2t
||Over Damped - Roots of the characteristic equation are real and
|f(t) B1e-at cos ( w t ) + B2e-at
sin ( w t )
||Under Damped - Roots of the characteristic equation are complex.
|f(t) = D1te-at + D2e-at
||Critically Damped - Roots of the characteristic equation are equal