1996 - 2016
BSEE - KB3UON
RF Cafe began life in 1996 as "RF Tools" in an AOL screen name web space totaling 2 MB. Its primary purpose was to provide me with ready access to commonly needed formulas and reference material while performing my work as an RF system and circuit design engineer. The Internet was still largely an unknown entity at the time and not much was available in the form of WYSIWYG ...
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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 unique.|
|f(t) B1e-at cos (ω t) + B2e-at sin (ω 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 and real.|