The zero-state scaled network shown in Figure 131 is driven by the sinusoidal voltage source Eg(t) expressed as E, (1)= 2 cos (21 +45°)V Use phasors and complex immittances to calculate the following: (a) the mesh currents Iml and Im2 as complex numbers in rectangular and polar format, and (b) the mesh currents imi(t) and im2(t) in the time-domain.

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The zero-state scaled network shown in Figure 131 is driven by the sinusoidal voltage
source Eg(t) expressed as
E (1) = /2 cos (2t + 45°)V
Use phasors and complex immittances to calculate the following:
(a)
the mesh currents Iml and Im2 as complex numbers in rectangular and polar format,
and
(b) the mesh currents im1 (t) and im2(t) in the time-domain.
i,(t)
R1
L3
lell
1H
Eg(t) +
Imi1 (t)
C2
İm1(t)
İm2(t)▼
0.5F
(rm = 0.50)
%3D
Figure 131
Scaled RLC network
Transcribed Image Text:The zero-state scaled network shown in Figure 131 is driven by the sinusoidal voltage source Eg(t) expressed as E (1) = /2 cos (2t + 45°)V Use phasors and complex immittances to calculate the following: (a) the mesh currents Iml and Im2 as complex numbers in rectangular and polar format, and (b) the mesh currents im1 (t) and im2(t) in the time-domain. i,(t) R1 L3 lell 1H Eg(t) + Imi1 (t) C2 İm1(t) İm2(t)▼ 0.5F (rm = 0.50) %3D Figure 131 Scaled RLC network
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