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In [[electrical engineering]], electrical terms are associated into pairs called '''duals'''. A dual of a relationship is formed by interchanging voltage and current in an expression. The dual expression thus produced is of the same form, and the reason that the dual is always a valid statement can be traced to the [[Duality (electricity and magnetism)|duality of electricity and magnetism]].
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Here is a partial list of electrical dualities:
 
* [[voltage]] &mdash; [[Electric current|current]]
* [[Series and parallel circuits|parallel &mdash; serial]] (circuits)
* [[Electrical resistance|resistance]] &mdash; [[Electrical conductance|conductance]]
* [[Electrical impedance|impedance]] &mdash; [[admittance]]
* [[capacitance]] &mdash; [[inductance]]
* [[Reactance (electronics)|reactance]] &mdash; [[susceptance]]
* [[short circuit]] &mdash; [[open circuit]]
* [[Kirchhoff's current law]] &mdash; [[Kirchhoff's voltage law]].
* [[Thévenin's theorem]] &mdash; [[Norton's theorem]]
 
==History==
The use of duality in [[circuit theory]] is due to Alexander Russell who published his ideas in 1904.<ref>Belevitch, V, "Summary of the history of circuit theory", ''Proceedings of the IRE'', '''vol 50''', Iss 5, pp.848-855, May 1962 {{doi|10.1109/JRPROC.1962.288301}}.</ref><ref>Alexander Russell, ''A Treatise on the Theory of Alternating Currents'', volume 1, chapter XXI, Cambridge: University Press 1904 {{OCLC|264936988}}.</ref>
 
== Examples ==
=== Constitutive relations ===
 
* Resistor and conductor (Ohm's law)
 
:: <math>v=iR \iff i=vG \, </math>
 
* Capacitor and inductor &ndash; differential form
 
:: <math>i_C=C\frac{d}{dt}v_C \iff v_L=L\frac{d}{dt}i_L</math>
 
* Capacitor and inductor &ndash; integral form
 
:: <math>v_C(t) = V_0 + {1 \over C}\int_{0}^{t} i_C(\tau) \, d\tau \iff  i_L(t) = I_0 + {1 \over L}\int_{0}^{t} v_L(\tau) \, d\tau </math>
 
=== Voltage division &mdash; current division ===
 
:<math>v_{R_1}=v\frac{R_1}{R_1 + R_2} \iff i_{G_1}=i\frac{G_1}{G_1 + G_2}</math>
 
=== Impedance and admittance ===
 
* Resistor and conductor
 
:: <math>Z_R = R \iff Y_G = G </math>
 
:: <math>Z_G = {1 \over G } \iff Y_R = { 1 \over R } </math>
 
* Capacitor and inductor
 
:: <math> Z_C = {1 \over Cs} \iff  Y_L = {1 \over Ls} </math>
 
:: <math> Z_L = Ls  \iff  Y_c = Cs</math>
 
==See also==
 
*[[Duality (electricity and magnetism)]]
*[[Duality (mechanical engineering)]]
*[[Dual impedance]]
 
==References==
{{reflist}}
* Turner, Rufus P, ''Transistors Theory and Practice'', Gernsback Library, Inc, New York, 1954, Chapter 6.
 
[[Category:Electrical engineering]]
[[Category:Duality theories|Electrical circuits]]

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