.MCAD 304020000 1 74 102 0
.CMD PLOTFORMAT
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.CMD FORMAT  rd=d ct=10 im=i et=3 zt=15 pr=3 mass length time charge temperature tr=0 vm=0
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.CMD SET PRNPRECISION 4
.CMD PRINT_SETUP 1.200000 1.218750 1.200000 1.200000 0
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.TXT 2 2 63 0 0
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{\rtf\ansi \deff0{\colortbl;\red0\green0\blue128;}{\fonttbl{\f0
\fcharset0\fnil Arial;}}\plain\cf1\fs28 \pard {\fs20 COPYRIGHT MIRON 
KAUFMAN 1995}}
.TXT 4 16 64 0 0
Cg a34.625000,34.625000,32
{\rtf\ansi \deff0{\colortbl;\red0\green0\blue128;}{\fonttbl{\f0
\fcharset0\fnil Arial;}{\f1\fcharset0\fnil Britannic Bold;}}\plain\cf1
\fs28 \pard {\f1\fs36\b Thermal Physics Computer Lab #4\par }}
.TXT 10 -17 71 0 0
Cg a73.000000,73.000000,255
{\rtf\ansi \deff0{\colortbl;\red0\green0\blue128;}{\fonttbl{\f0
\fcharset0\fnil Arial;}}\plain\cf1\fs28 \pard We animate the van der 
Waals isotherms.  We use the equation of state using the scaled 
variables (law of corresponding states) T/T{\dn C}, p/p{\dn C}, v/v{
\dn C}. In terms of the scaled variables the critical isotherm is T = 
1, and the critical point is p = 1 and v = 1.  \par }
.EQN 13 21 82 0 0
{0:v}NAME:.334,.335;5
.EQN 1 -18 68 0 0
{0:T}NAME:({0:FRAME}NAME+1)/(50)
.EQN 6 0 83 0 0
{0:p}NAME({0:v}NAME,{0:T}NAME):8*({0:T}NAME)/(3*{0:v}NAME-1)-(3)/(({0:v}NAME)^(2))
.EQN 4 -2 102 0 0
5&-5&(_n_u_l_l_&_n_u_l_l_)&{0:p}NAME({0:v}NAME,{0:T}NAME)@&0&(_n_u_l_l_&_n_u_l_l_)&{0:v}NAME
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