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• After being familiar with the mathematical characteristics of sinusoids, we are ready to apply a sinusoidal forcing function to a simple circuit and obtain the forced response.

• Then we write the differential equation that applies to the given circuit.

• The complete solution is posed of two parts, the complementary solution (which we call the natural response) and the particular integral (or forced response).

• The only interested response in our study is the “steady-state” response or the forced response.

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