In general q can be expresses as q zl r2 2 now z we

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Unformatted text preview: le locations of the second dipole. 0B' !"! "#$!%&'()$!*&+",-$!./0"#!,1!023$4,1)$5!"#,"!"#$!+&,4!%$$%!/#$1!,1!67!/,*$!0% c) Since Pr = 1 |Ir |2 R, we have 01)04$1"!&1!"#$!,1"$11,8! 2 |Ir | = !" q 8 /73 2 ⇥ 1.703 ⇥ 10 $# 9 =$>%" ? 9 ;8@<: ;< ⇡ 4.32 ⇥ 10 9 @: d) Thevenin equivalent circuit is shown in the below figure. %" 5 A. :8;BC ;< : ! A&+"% %D !& !" %& ! E(0"$!"#$!3&/$(!01"&!"#$!+&,4!,%!$&F!"#$1!$G3($%%! $& $8! |VT |2 Recalling Pr = 8Re{ZT } , we can write | VT | = q Pr 8Re{ZT } = p 1.703 ⇥ 10 8 '$# F!/#$($!'!0%!"#$!20%2,")#! ⇥ 8 ⇥ C (D (&am...
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This note was uploaded on 02/03/2014 for the course ECE 350 taught by Professor Kudeki during the Spring '11 term at University of Illinois, Urbana Champaign.

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