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{\rtf\ansi \deff0{\colortbl;\red0\green0\blue128;}{\fonttbl{\f0
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RECTANGULAR LOOPS}
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{\rtf\ansi \deff0{\colortbl;\red0\green0\blue128;}{\fonttbl{\f0
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{\rtf\ansi \deff0{\colortbl;\red0\green0\blue128;}{\fonttbl{\f0
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rectangular wire loop       LRECT()\par Impedance magnitude of 
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.TXT 3 -36 5 0 0
Cg a15.250000,15.250000,15
{\rtf\ansi \deff0{\colortbl;\red0\green0\blue128;}{\fonttbl{\f0
\fcharset0\fnil Courier;}}\plain\cf1\fs20 \pard Variables used:}
.TXT 4 2 7 0 0
Cg a30.250000,30.250000,89
{\rtf\ansi \deff0{\colortbl;\red0\green0\blue128;}{\fonttbl{\f0
\fcharset0\fnil Courier;}}\plain\cf1\fs20 \pard d   Diameter of wire 
(in.)\par \par x   Length of wire loop (in.)\par \par y   Breadth of 
wire loop (in.)}
.TXT 24 -2 8 0 0
Cg a28.250000,28.250000,28
{\rtf\ansi \deff0{\colortbl;\red0\green0\blue128;}{\fonttbl{\f0
\fcharset0\fnil Courier;}}\plain\cf1\fs20 \pard Inductance of wire 
loop (H):}
.EQN 4 9 9 0 0
{0:LRECT}NAME({0:d}NAME,{0:x}NAME,{0:y}NAME):10.16*(10)^(-9)*({0:x}NAME*{0:ln}NAME((2*{0:y}NAME)/({0:d}NAME))+{0:y}NAME*{0:ln}NAME((2*{0:x}NAME)/({0:d}NAME)))
.TXT 8 -7 10 0 0
Cg a37.250000,37.250000,65
{\rtf\ansi \deff0{\colortbl;\red0\green0\blue128;}{\fonttbl{\f0
\fcharset0\fnil Courier;}}\plain\cf1\fs20 \pard A loop of 24-gauge 
wire 1 in.\\253 has\par about 100 nH of inductance.}
.TXT 6 0 11 0 0
Cg a44.250000,44.250000,126
{\rtf\ansi \deff0{\colortbl;\red0\green0\blue128;}{\fonttbl{\f0
\fcharset0\fnil Courier;}}\plain\cf1\fs20 \pard Changing the wire 
diameter from AWG 30 \par to AWG 10 makes little difference.  The log 
function is very insensitive to wire size.}
.TXT 7 0 16131 0 0
Cg a49.250000,49.250000,90
{\rtf\ansi \deff0{\colortbl;\red0\green0\blue128;}{\fonttbl{\f0
\fcharset0\fnil Courier;}}\plain\cf1\fs20 \pard If your loop consists 
of different-sized\par conductors, use the diameter of the smallest one.}
.TXT 6 0 16135 0 0
Cg a51.500000,51.500000,51
{\rtf\ansi \deff0{\colortbl;\red0\green0\blue128;}{\fonttbl{\f0
\fcharset0\fnil Courier;}{\f1\fcharset2\fnil Symbol;}}\plain\cf1\fs20 
\pard Impedance magnitude of inductor at frequency f ({\f1 W}):}
.TXT 4 0 16133 0 0
Cg a20.250000,20.250000,42
{\rtf\ansi \deff0{\colortbl;\red0\green0\blue128;}{\fonttbl{\f0
\fcharset0\fnil Courier;}}\plain\cf1\fs20 \pard l     Inductance (H)
\par \par f     Frequency (Hz)}
.EQN 2 30 16137 0 0
{0:XLF}NAME({0:l}NAME,{0:f}NAME):2*{0:\p}NAME*{0:f}NAME*{0:l}NAME
.TXT 7 -30 16138 0 0
Cg a32.250000,32.250000,57
{\rtf\ansi \deff0{\colortbl;\red0\green0\blue128;}{\fonttbl{\f0
\fcharset0\fnil Courier;}{\f1\fcharset2\fnil Symbol;}}\plain\cf1\fs20 
\pard The impedance, at 100 MHz, of a \par 100-nH inductor is 62 {\f1 W}.}
.TXT 8 -2 18 0 0
Cg a59.500000,59.500000,59
{\rtf\ansi \deff0{\colortbl;\red0\green0\blue128;}{\fonttbl{\f0
\fcharset0\fnil Courier;}{\f1\fcharset2\fnil Symbol;}}\plain\cf1\fs20 
\pard Impedance magnitude of inductor as seen by rising edge ({\f1 W}):}
.TXT 4 2 19 0 0
Cg a27.250000,27.250000,51
{\rtf\ansi \deff0{\colortbl;\red0\green0\blue128;}{\fonttbl{\f0
\fcharset0\fnil Courier;}}\plain\cf1\fs20 \pard l      Inductance (H)
\par \par tr     10-90% rise time (s)\par }
.EQN 10 23 20 0 0
{0:XLT}NAME({0:l}NAME,{0:tr}NAME):({0:\p}NAME*{0:l}NAME)/({0:tr}NAME)
.TXT 8 -23 21 0 0
Cg a45.250000,45.250000,75
{\rtf\ansi \deff0{\colortbl;\red0\green0\blue128;}{\fonttbl{\f0
\fcharset0\fnil Courier;}{\f1\fcharset2\fnil Symbol;}}\plain\cf1\fs20 
\pard The impedance, as seen by a 5-ns rising edge,\par of a 100-nH 
inductor is 62 {\f1 W}.}