LC circuits

An LC circuit is simply a closed loop with only two elements, a capacitor and an inductor. We will show that the LC circuits have resonant properties - they respond to certain frequencies. Therefore they can serve as the basis for any device that needs to tune to a specific frequency such as a radio. In an LC loop the charge oscillates back and forth through the capacitor with a given frequency just as a mass on a spring oscillates. To demonstrate this equivalence, we list several equations for both a mechanical spring and for an LC circuit.

 

mechanical spring

LC circuit

velocity:     wpe5.gif (999 bytes) current:     wpe7.gif (1031 bytes)
kinetic energy:     wpe6.gif (1046 bytes) inductor's energy:     wpe8.gif (1023 bytes)
potential energy:     wpe9.gif (1037 bytes) capacitor's energy:     wpe2.gif (1235 bytes)
Eq. of motion:     wpe5.gif (1172 bytes) Kirchoff's law:     
frequency:      wpe4.gif (1161 bytes) frequency:     wpe3.gif (1186 bytes)

The parameters that determine the motion of a spring are the mass m, spring constant k, the position x, and the velocity v which is the rate of change of x. The parameters that determine the behavior of an LC circuit are L, C, Q and I which is the rate of change of Q. Thus there is a one-to-one correspondence since the equations of motion are identical given the substitutions:

The characteristic frequency of and LC circuit is the frequency at which large amplitudes are built up when a driving force comes in at that frequency. A child on a swing will be sensitive to a pushing force which comes regularly with the natural frequency of the swing. A force that comes at a different frequency will not build up a large amplitude as it will often be pushing against the child's motion. We call this the resonant frequency.


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