capacitors and inductorscarmenere.ucsd.edu/.../4to5capacitor-inductor.pdfcapacitor behaves as open...

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129 MAE140 Linear Circuits 129 Capacitors and inductors 1. New circuit elements that are able to store energy Dynamic elements, i.e., change with time 2. Allow to design circuits that perform integration and differentiation Make possible signal processing operations in modern communication and audio equipment

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Page 1: Capacitors and inductorscarmenere.ucsd.edu/.../4to5capacitor-inductor.pdfCapacitor behaves as open circuit under dc excitations Power p C (t) =C/2 dv C 2/dt. 131 MAE140 Linear Circuits

129MAE140 Linear Circuits

129

Capacitors and inductors

1. New circuit elements that are able to store energyDynamic elements, i.e., change with time

2. Allow to design circuits that perform integration anddifferentiationMake possible signal processing operations in modern

communication and audio equipment

Page 2: Capacitors and inductorscarmenere.ucsd.edu/.../4to5capacitor-inductor.pdfCapacitor behaves as open circuit under dc excitations Power p C (t) =C/2 dv C 2/dt. 131 MAE140 Linear Circuits

130MAE140 Linear Circuits

130

Capacitors

Defining relationship for the capacitorq(t)=CvC(t)

C is capacitance, unit is farad (F), range 10-12 - 10-3

i-v relationshipiC(t) = dq/dt =CdvC/dt

If vC is constant then iC=0. Capacitor behaves asopen circuit under dc excitations

Power pC(t) =C/2 dvC

2/dt

Page 3: Capacitors and inductorscarmenere.ucsd.edu/.../4to5capacitor-inductor.pdfCapacitor behaves as open circuit under dc excitations Power p C (t) =C/2 dv C 2/dt. 131 MAE140 Linear Circuits

131MAE140 Linear Circuits

131

Inductors

Defining relationship for the inductorλ(t)=LiL(t), λ(t) is flux linkage

L is inductance, unit is henry (H), range 10-6 - 10-3

i-v relationshipvL(t) = dλ /dt =LdiL/dt

If iL is constant then vL=0. Inductor behaves as shortcircuit under dc excitations

Power pL(t) =L/2 diL

2/dt