L p c z c p l qrsqrtr2z l22 intqr0a yn

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Unformatted text preview: e9re given th—t M a M z F ‡e st—rt with t—™kson SFIHH in t—™ksonX ” 0  : ~x n ~x I  ¡~ HA d xH C I s ~ H ¡ M @~ HA daH rH M @ ¨M @~ A a R x j~ ~ Hj xx R S j~ ~ Hj xx V s s HA z ¡ M @~ ” ~x CI z ¡ M @~ HA daH ” ~x a RI  j~ ~ Hj R xx j~ ~ Hj xx   a   a I M M H dH d'H I p p a R  R ' H H H C @z L=PA H C @z C L=PA 'H H a a M M I HHI HH p p aP H C @z L=PA  d P H H C @z C L=PA  d   H ! !     Mp Mp L L a C @z L=PA z  a C @z C L=PA z C  aP   P P P 0 3 top bottom 2 2 0 =0 2 =0 2 =0 0 0 M0 p =0 2 H dH d'H 0 2 =0 0 2 2 2 2 =0 0 2 p 2 2   z  aP a C @z L=PA a C @z C L=PA where the integr—l w—s ev—lu—ted using the w—ple ™omm—nd 2 2 2 2 2   !  L   P  C z C P  L  Q:=r/sqrt(r^2+(z-L/2)^2); int(Q,r=0..a); ~ yn the —xis of the ™ylinderD H lies only in the z Edire™tionX ¨M a M Hz a @z P @ 4 0 p a2 5     L=P z C L=P @ L @ L p @z z P  C @z z C P      C @z L=PA a C...
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This note was uploaded on 12/08/2011 for the course PHYSICS 505 taught by Professor Liu during the Winter '08 term at University of Michigan.

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