0 ECE 222 Electric Circuit Analysis II Chapter 5 Duality of Capacitance & Inductance Herbert G....

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1 ECE 222 Electric Circuit Analysis II Chapter 5 Duality of Capacitance & Inductance Herbert G. Mayer, PSU Status 2/3/2016 For use at CCUT Spring 2016

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2 Definition In EE, a dual relationship exists between certain pairs of electric devices and units, e.g. voltage and current Duality manifests itself by ability to interchange dual units in an expression, yielding two dual, valid, different expressions A dual expression is formed by interchanging the two and thus creating a corresponding, dual rule Ultimate reason behind this is the duality of electrical and magnetic phenomena in nature Example: v(t) = L di / dt  i(t) = H dv / dt

Transcript of 0 ECE 222 Electric Circuit Analysis II Chapter 5 Duality of Capacitance & Inductance Herbert G....

Page 1: 0 ECE 222 Electric Circuit Analysis II Chapter 5 Duality of Capacitance & Inductance Herbert G. Mayer, PSU Status 2/3/2016 For use at CCUT Spring 2016.

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ECE 222Electric Circuit Analysis II

Chapter 5Duality of

Capacitance & Inductance

Herbert G. Mayer, PSUStatus 2/3/2016

For use at CCUT Spring 2016

Page 2: 0 ECE 222 Electric Circuit Analysis II Chapter 5 Duality of Capacitance & Inductance Herbert G. Mayer, PSU Status 2/3/2016 For use at CCUT Spring 2016.

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Syllabus Definition Duality Samples Bibliography

Page 3: 0 ECE 222 Electric Circuit Analysis II Chapter 5 Duality of Capacitance & Inductance Herbert G. Mayer, PSU Status 2/3/2016 For use at CCUT Spring 2016.

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Definition In EE, a dual relationship exists between certain

pairs of electric devices and units, e.g. voltage and current

Duality manifests itself by ability to interchange dual units in an expression, yielding two dual, valid, different expressions

A dual expression is formed by interchanging the two and thus creating a corresponding, dual rule

Ultimate reason behind this is the duality of electrical and magnetic phenomena in nature

Example: v(t) = L di / dt i(t) = H dv / dt

Page 4: 0 ECE 222 Electric Circuit Analysis II Chapter 5 Duality of Capacitance & Inductance Herbert G. Mayer, PSU Status 2/3/2016 For use at CCUT Spring 2016.

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Duality Samples

Voltage

Capacitance

Resistance

Parallel

Short Circuit

KCL

Impedance

Thévenin TheoremReactance

CurrentInductanceConductanceSerialOpen CircuitKVLAdmittanceNorton TheoremSusceptance

Page 5: 0 ECE 222 Electric Circuit Analysis II Chapter 5 Duality of Capacitance & Inductance Herbert G. Mayer, PSU Status 2/3/2016 For use at CCUT Spring 2016.

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Duality Samples Resistor & Conductor:

v = i R i = v G

Capacitor & Inductor – differential form:iC = C d vC / dt vL = L d iL / dt

Capacitor & Inductor – integral form:vC(t) = V0 + 1/C iC(t) dt iL(t) = I0 + 1/L vL (t) dt

Voltage Division & Current DivisionvR1 = v * R1 / ( R1 + R2 ) iG1 = i * G1 / ( G1 + G2 )

Inductor Voltage & Capacitor Currentv(t) = L di / dt i(t) = H dv / dt

Page 6: 0 ECE 222 Electric Circuit Analysis II Chapter 5 Duality of Capacitance & Inductance Herbert G. Mayer, PSU Status 2/3/2016 For use at CCUT Spring 2016.

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Duality Samples

Instantaneous change of current is not possible in an inductorInstantaneous change of voltage at the terminals of an inductor is quite possibleInductor current is out of phase with the voltage by + π/2

Instantaneous change of voltage is not possible in a capacitorInstantaneous change of current (displacement current) in a capacitor is quite possibleCapacitor current (displacement current) is out of phase with the voltage by - π/2

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Bibliography1. Wiki on duality:

https://en.wikipedia.org/wiki/Duality_(electrical_circuits)