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# 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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