0 ECE 222 Electric Circuit Analysis II Chapter 5 Duality of Capacitance & Inductance Herbert G....
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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.](https://reader036.fdocuments.us/reader036/viewer/2022082723/5a4d1b597f8b9ab0599aa575/html5/thumbnails/1.jpg)
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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.](https://reader036.fdocuments.us/reader036/viewer/2022082723/5a4d1b597f8b9ab0599aa575/html5/thumbnails/2.jpg)
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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.](https://reader036.fdocuments.us/reader036/viewer/2022082723/5a4d1b597f8b9ab0599aa575/html5/thumbnails/3.jpg)
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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.](https://reader036.fdocuments.us/reader036/viewer/2022082723/5a4d1b597f8b9ab0599aa575/html5/thumbnails/4.jpg)
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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.](https://reader036.fdocuments.us/reader036/viewer/2022082723/5a4d1b597f8b9ab0599aa575/html5/thumbnails/5.jpg)
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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.](https://reader036.fdocuments.us/reader036/viewer/2022082723/5a4d1b597f8b9ab0599aa575/html5/thumbnails/6.jpg)
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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
![Page 7: 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.](https://reader036.fdocuments.us/reader036/viewer/2022082723/5a4d1b597f8b9ab0599aa575/html5/thumbnails/7.jpg)
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Bibliography1. Wiki on duality:
https://en.wikipedia.org/wiki/Duality_(electrical_circuits)