Fig 8.2: Expected Result of Various Damping Parameters
Red: Underdamped | Yellow: Critically Damped | Green: Overdamped
To observe the three classes of damping most commonly encountered in engineering, and how to design for or predict particular behavior in circuits.
Much like in the capacitor and inductor introductory lab, the circuits in this lab have a transient response. The voltage and current across the components are time variant, and dependent on the nature of the particular circuit to which they are connected. To build on the principles of Lab 7, these circuits will have a non-first-order response. The following circuits illustrate cases in which the complex responses are a result of the combined effects of both the capacitor and inductor influencing each other.
Resistors have a simple "Real" resistance, but capacitors and inductors have a frequency dependent "Complex" resistance, in time-varying circuits, the term impedance is used as an umbrella term for the resistance of all components. Used in this context, the word Real refers to the Real numbers, and Complex, the Complex numbers.
Just as in the last lab, we will simulate a step response (switch turning on and off) with a signal of an appropriate frequency to allow settling and steady-state between cycles. The step response allows for the demonstration of the natural response. The natural response is different than a forced response, one where there is a continuous AC signal driving the circuit.
There are several properties which are relative each other at a given frequency, and are considered characteristic of a given circuit:
As mentioned above, the resonant frequency occurs when the total impedance is at a minimum. Since capacitor impedance, and inductor impedance act in opposite directions, when they are of equal magnitude, the resulting vector will be zero. This serves as the basis for calculating the resistance for a critically damped circuit in which ζ=1, implying that α = ωo. The procedure will first calculate the frequency at which the impedance of the capacitor and inductor is identical and opposite, and then the resistance which will cause this frequency in the circuit.
If α = ωo Then:
1/sqrt(LC) = R/(2L) for a series circuit
or
1/(2RL) for a parallel circuit.
Solving for R will give the Real resistance (due to resistors only) to critically damp the circuit. A similar calculation can be used to find any parameter missing given the remaining two. Additionally, for any desired damping ratio, you can solve for a set of parameters that will behave as desired.
In all, you will have 4 oscilloscope images.
(1) Underdamped
(2) Near Critically Damped
(3) Critically Damped
(4) Overdamped
(order listed may not reflect results order)
Include: