It is shown that Thomson's theorem describes the equilibrium energy of a system. If the charge is held constant, this energy is a minimum, but if the potential is held constant the energy is a maximum. The theorem can therefore be used to give upper and lower bounds to the electrostatic energy.
Get full access to this article
View all access options for this article.
References
1.
MahederoB.Rodriguez-IzquierdoG.CivitA., ‘Some comments on Thomson's theorem’, Int. J. Elect. Eng. Educ., 13, pp. 52–55 (Jan. 1976).
2.
ThomsonW. (Lord Kelvin), ‘Theorems with reference to the solution of certain partial differential equations’, Cambridge and Dublin Mathematical Journal, Electrostatics and Magnetism, Article 13 (Feb. 1848).
3.
MaxwellJ. C., Electricity and Magnetism, Vol. 1, Article 100, Clarendon Press, Third Edition (1892).
4.
StrattonJ. A., Electromagnetic Theory, pp. 114–116, McGraw-Hill (1941).
5.
PopovićB. D., Introductory Engineering Electromagnetics, Addison-Wesley, pp. 134–135 (1971).
6.
PanofskyW. K. H.PhillipsM., Classical Electricity and Magnetism, Addison-Wesley, pp. 91–92 (1955).
7.
StrattonJ. A., Electromagnetic Theory, pp. 116–117, McGraw-Hill (1941).
8.
HammondP.PenmanJ., ‘Calculation of inductance and capacitance by means of dual energy principles’, Proc. I.E.E.123, pp. 554–559 (June, 1976).