The zero-state scaled network shown in Figure 134 is driven by the sinusoidal currentsource Jg(t) expressed asJ,(1)= 12 sin (21 - 45°) AUse 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.L20.5HVn1(t)Vn2(t)+V2(t)Jg(t)9mV2(t)C3 1FR1(gm = 3S)Figure 134Scaled RLC network

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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)

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)

Power System Analysis and Design (MindTap Course List)

6th Edition

ISBN:9781305632134

Author:J. Duncan Glover, Thomas Overbye, Mulukutla S. Sarma

Publisher:J. Duncan Glover, Thomas Overbye, Mulukutla S. Sarma

Chapter6: Power Flows

Section: Chapter Questions

Problem 6.61P

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