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From this, it is easy to show that the correlation function of the current is given by RI (τ ) = nAq2 E[Vx (t)Vx (t + τ )] L (23) where we have dropped the subscript k for convenience. Assuming that electron collisions occur according to a Poisson law with intensity given by Ͱ (2) and that the average variance of the velocity of an electron is given by kBT/m, where kB is Boltzmann’s constant and m is the mass of an electron (from the equipartition theorem for electrons), it can be shown that RI (τ ) = kT −α|τ | αe R (24) where R is the resistance of the rod.

Kotz, Continuous Univariate Distributions, Vol. 1, Boston: Houghton-Mifflin, 1970. 16. N. L. Johnson and S. Kotz, Continuous Univariate Distributions, Vol. 2, Boston: Houghton-Mifflin, 1970. 17. J. L. Doob, Stochastic Processes, New York: Wiley, 1953. 18. E. Wong and B. Hajek, Stochastic Processes in Engineering Systems, New York: Springer-Verlag, 1985. GEOFFREY C. ORSAK Southern Methodist University NOISE, CIRCUIT. See CIRCUIT NOISE. htm ● HOME ● ABOUT US ● // CONTACT US ● HELP Wiley Encyclopedia of Electrical and Electronics Engineering Telephone Interference Standard Article Toshio Ishizaki1, Makoto Sakakura1, Toru Yamada1, Koichi Ogawa1 1Matsushita Electric Industrial Co.

And Commun. Japan, Part 1, 80 (8): 39– 49, 1997. TOSHIO ISHIZAKI MAKOTO SAKAKURA TORU YAMADA KOICHI OGAWA Figure 13. Current distribution on the wire grid (5). Matsushita Electric Industrial Co. htm ● HOME ● ABOUT US // ● CONTACT US ● HELP Wiley Encyclopedia of Electrical and Electronics Engineering Whistlers Standard Article Vikas S. Sonwalkar1 1University of Alaska Fairbanks, Fairbanks, AK Copyright © 1999 by John Wiley & Sons, Inc. All rights reserved. htm Abstract The sections in this article are The Whistler Phenomenon Wave Propagation in a Cold Magnetoplasma Propagation Through the Ionosphere Propagation Through the Magnetosphere Whistler–Lightning Correlations Effects of Whistlers on the Geospace Environment Concluding Remarks | | | Copyright © 1999-2008 All Rights Reserved.

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