Any linear sinusoidal driven combination of capacitors, inductors, resistors has a steady state solution of the form

which can be found using a complex impedance Z defined by

where I and V are also treated as complex quantities. The current I is given in terms of the electromotive force
by


and the phase shift by

For circuit elements in series,

and in parallel,

For capacitors,

where
is the angular frequency, Q is the charge, and C is the capacitance. Taking the derivative on each side gives

so

For inductors,

where L is the inductance. Integrating both sides gives

so

For resistors, the impedance is simply equal to the resistance R,


(1)
which can be found using a complex impedance Z defined by

(2)
where I and V are also treated as complex quantities. The current I is given in terms of the electromotive force


(3)

(4)
and the phase shift by

(5)
For circuit elements in series,

(6)
and in parallel,

(7)
For capacitors,

(8)
where


(9)
so

(10)
For inductors,

(11)
where L is the inductance. Integrating both sides gives

(12)
so

(13)
For resistors, the impedance is simply equal to the resistance R,

(14)
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