171022-2002
Fishn sparky:
This post will mean very little to you, it is useful information, but possibly not to your students.
If you consider a series circuit of a capacitor, inductor, and resistance, then the differential equation for this is
L d(dq)/dt + R dq/dt + q/C = 0
that is the sum of the voltages around a closed loop is 0.
If R is small, then the result is a damped sine wave assuming an initial charge of energy at time t = 0.
If R = 0, then there is no damping and a continuous sine wave exists.
The frequency of this oscillation is called the resonant frequency.
What is occurring here is an exchange of stored energy back and forth between the inductor and capacitor.
Suppose you change the circuit to a resistor, capacitor, and inductor in parallel, and apply an excitation sine wave at the resonant frequency, then the power source only sees the resistance as a load because the capacitor and inductor are exchanging energy back and forth between each other.
Next suppose the L and C are not at resonance, then some of the energy associated with the L and C is being exchanged with the excitation voltage source.
More later.
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