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Direct Current and Transient Analysis 133


and s 1 and s 2 are referred as the complex frequencies given by

sw 12 , ^202

R.2.110 As mentioned, the natural response of a parallel RLC circuit results in one of the
following three cases:
a. Overdamped
b. Critical damped
c. Underdamped
Observe that the elements defi ne the specifi c case.
R.2.111 Let us analyze each case, starting with the overdamped parallel confi guration that
occurs for the following condition:

^22 w 0 

and since
sw 12 , ^2  02

then

^2 ww^022 ^20 ^0

Note that both s 1 and s 2 are real, distinct, and negative. Then the solution of the
differential equation of R.2.109 is of the form

vt Ae Ae
()st s t
1212


where A 1 and A 2 are constants that can be evaluated from the network initial
conditions.
R.2.112 The critical-damped parallel case occurs for the following condition:

^2 w 02  0

Therefore both s 1 and s 2 are equal to −α, and α is real and negative. The solution
of the differential equation of R.2.109 is then of the form

vt Ae Ate
()tt
12


where A 1 and A 2 are constants that can be evaluated from the network initial
conditions.
R.2.113 The underdamped parallel case occurs for the following condition:




(^22) w  0
Then s 1 and s 2 become complex conjugate frequencies, and the response of the
differential equation of R.2.109 is of the following form:
vt e A wt A wt
t
()[ cos(dd) sin( )]

(^12)

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