al conditions in the RLC network shown in Figure 136 are zero. This network is by a sinusoidal current source Jg(t) expressed with the time-domain function of J,(1)=10cos(500f + - 60°) mA e the sinusoidal steady-state expression for the inductor voltage v4(t) in the format v, (1) =V¼m cos(@r +ø.) 4M R3< 2002 33μF Jg(t) R2 L4 V4(t) 1000 470mH Figure 136 Zero-state RLC network oll

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All initial conditions in the RLC network shown in Figure 136 are zero. This network is
driven by a sinusoidal current source Jg(t) expressed with the time-domain function of
J
7 (1)=10cos(5001 +60°) mA
Generate the sinusoidal steady-state expression for the inductor voltage v4(t) in the format
of
v, (1)=V¼M COs (at + $,)
C1
R3
2000
33µF
Jg(t)
R2
L4
V4(t)
1002
470mH
Figure 136
Zero-state RLC network
Transcribed Image Text:All initial conditions in the RLC network shown in Figure 136 are zero. This network is driven by a sinusoidal current source Jg(t) expressed with the time-domain function of J 7 (1)=10cos(5001 +60°) mA Generate the sinusoidal steady-state expression for the inductor voltage v4(t) in the format of v, (1)=V¼M COs (at + $,) C1 R3 2000 33µF Jg(t) R2 L4 V4(t) 1002 470mH Figure 136 Zero-state RLC network
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