Duality (electrical circuits)

From KYNNpedia

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 of electricity and magnetism.

Here is a partial list of electrical dualities:

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 display="block">v=iR \iff i=vG \, </math>
  • Capacitor and inductor – differential form <math display="block">i_C=C\frac{d}{dt}v_C \iff v_L=L\frac{d}{dt}i_L</math>
  • Capacitor and inductor – integral form <math display="block">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 — current division

<math display="block">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 display="block">Z_R = R \iff Y_G = G </math> <math display="block">Z_G = {1 \over G } \iff Y_R = { 1 \over R } </math>
  • Capacitor and inductor <math display="block"> Z_C = {1 \over Cs} \iff Y_L = {1 \over Ls} </math> <math display="block"> Z_L = Ls \iff Y_c = Cs</math>

See also

References

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  • Turner, Rufus P, Transistors Theory and Practice, Gernsback Library, Inc, New York, 1954, Chapter 6.