he zero-state scaled network shown in Figure 134 is driven by the sinusoidal current purce Jg(t) expressed as J,(1)=V2 sin(21 – 45°).A %3D se phasors and complex immittances to calculate the following: 1) the node voltages Vni and Vn2 as complex numbers in rectangular and polar format, and ) the node voltages Vni(t) and vn2(t) in the time-domain. L2 0.5H Vn1(t) Vn2(t) lll + V2(t) Jg(t) 9mV2(t) C3 1F R1 (9m = 3S)

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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)= 12 sin (21 - 45°) A
Use phasors and complex immittances to calculate the following:
(a)
the node voltages Vnl and Vn2 as complex numbers in rectangular and polar format,
and
(b) the node voltages vn1 (t) and vn2(t) in the time-domain.
L2
0.5H
Vn1(t)
Vn2(t)
+
V2(t)
Jg(t)
9mV2(t)
C3 1F
R1
(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)= 12 sin (21 - 45°) A Use phasors and complex immittances to calculate the following: (a) the node voltages Vnl and Vn2 as complex numbers in rectangular and polar format, and (b) the node voltages vn1 (t) and vn2(t) in the time-domain. L2 0.5H Vn1(t) Vn2(t) + V2(t) Jg(t) 9mV2(t) C3 1F R1 (gm = 3S) Figure 134 Scaled RLC network
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