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)
Introductory Circuit Analysis (13th Edition)
13th Edition
ISBN:9780133923605
Author:Robert L. Boylestad
Publisher:Robert L. Boylestad
Chapter1: Introduction
Section: Chapter Questions
Problem 1P: Visit your local library (at school or home) and describe the extent to which it provides literature...
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Question
![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](/v2/_next/image?url=https%3A%2F%2Fcontent.bartleby.com%2Fqna-images%2Fquestion%2F582a1600-15a3-4ab5-9691-4690f1b78015%2F5d0164a6-1e8e-46bf-aaf6-dfaa60127fff%2F01mhgis_processed.png&w=3840&q=75)
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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