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Two series connected capacitors Cland C2 have been ci EVci(t) discharged at t-0 through a resistor R. If C1 has an initial v1(0") voltage Vland C2 has an initial voltage V2 with the same R VR(t) orientation, then the voltage across the resistor can be C2 Vc2(t) determined by the following formula: V2(0") VR(1)- (V1(0*))e ad v VR(1)- (V1(0*) – V2(0*))e te1+c2)R V VR(1)- (V1(0*) + v2(0*))e VR(1)- (V2(0*))e d v VR(t)- (V1(0*) – v2(0*))e V VR(1)-(V1(0*) + v2(0*))etec2)K V VR(1)- (V1(0*))e¯ (as2 V

Two series connected capacitors Cland C2 have been ci EVci(t) discharged at t-0 through a resistor R. If C1 has an initial v1(0") voltage Vland C2 has an initial voltage V2 with the same R VR(t) orientation, then the voltage across the resistor can be C2 Vc2(t) determined by the following formula: V2(0") VR(1)- (V1(0*))e ad v VR(1)- (V1(0*) – V2(0*))e te1+c2)R V VR(1)- (V1(0*) + v2(0*))e VR(1)- (V2(0*))e d v VR(t)- (V1(0*) – v2(0*))e V VR(1)-(V1(0*) + v2(0*))etec2)K V VR(1)- (V1(0*))e¯ (as2 V

Introductory Circuit Analysis (13th Edition)
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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Two series connected capacitors Cland C2 have been ci EVci(t) discharged at t-0 through a resistor R. If C1 has an initial v1(0") voltage Vland C2 has an initial voltage V2 with the same R VR(t) orientation, then the voltage across the resistor can be C2 v2(0") Vc2(t) determined by the following formula: VR(1)= (V1(0*))e d VR(1)- (V1(0*) – v2(0*))e¯te1+c2}R V VR(1)- (V1(0*) + V2(0*))e & Va(1)- (V2(0*))e d v "R(t)- (V1(0*) – v2(0*))e &* (1-C2, V VR(1)- (V1(0*) + v2(0*))e¯1+62)k V V'R(1)= (V1(0*))e¯ (as V
Transcribed Image Text:Two series connected capacitors Cland C2 have been ci EVci(t) discharged at t-0 through a resistor R. If C1 has an initial v1(0") voltage Vland C2 has an initial voltage V2 with the same R VR(t) orientation, then the voltage across the resistor can be C2 v2(0") Vc2(t) determined by the following formula: VR(1)= (V1(0*))e d VR(1)- (V1(0*) – v2(0*))e¯te1+c2}R V VR(1)- (V1(0*) + V2(0*))e & Va(1)- (V2(0*))e d v "R(t)- (V1(0*) – v2(0*))e &* (1-C2, V VR(1)- (V1(0*) + v2(0*))e¯1+62)k V V'R(1)= (V1(0*))e¯ (as V
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