The zero-state scaled network shown in Figure 134 is driven by the sinusoidal current source Jg(t) expressed as J,(1) =VZsin(2r-45°).4 Use phasors and complex immittances to calculate the following: (a) the node voltages Val and Va2 as complex mumbers in rectangular and polar format, and (b) the node voltages val(t) and vn2(t) in the time-domain. L2 0.5H Vai(t) Vnz(t) + v-(t) J(t) g-V2(t) C3 1F R, 10 (gm = 3S) Figure 134 Scaled RLC network

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The zero-state scaled network shown in Figure 134 is driven by the sinusoidal current
source Jg(t) expressed as
J,(1) =VZsin(2r-45°).4
Use phasors and complex immittances to calculate the following:
(a) the node voltages Val and Va2 as complex mumbers in rectangular and polar format,
and
(b) the node voltages val(t) and vn2(t) in the time-domain.
L2 0.5H
lll
+ v(t)
Vai(t)
Vaa(t)
J(t)
9-V2(t)
C3 1F
R,
(gm = 3S)
Figure 134
Scaled RLC network
Transcribed Image Text:The zero-state scaled network shown in Figure 134 is driven by the sinusoidal current source Jg(t) expressed as J,(1) =VZsin(2r-45°).4 Use phasors and complex immittances to calculate the following: (a) the node voltages Val and Va2 as complex mumbers in rectangular and polar format, and (b) the node voltages val(t) and vn2(t) in the time-domain. L2 0.5H lll + v(t) Vai(t) Vaa(t) J(t) 9-V2(t) C3 1F R, (gm = 3S) Figure 134 Scaled RLC network
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