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0 4 3 0 NO-TRACE-STRING
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.CMD FORMAT  rd=d ct=10 im=i et=3 zt=15 pr=3 mass length time charge
.CMD SET ORIGIN 0
.CMD SET TOL 0.001000000000000
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.CMD DEFINE_FONTSTYLE_NAME fontID=5 name=User^2
.CMD DEFINE_FONTSTYLE_NAME fontID=6 name=User^3
.CMD DEFINE_FONTSTYLE_NAME fontID=7 name=User^4
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.CMD DEFINE_FONTSTYLE_NAME fontID=9 name=User^6
.CMD DEFINE_FONTSTYLE_NAME fontID=10 name=User^7
.CMD DEFINE_FONTSTYLE fontID=0 family=Times^New^Roman points=10 bold=0 italic=0 underline=0
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.CMD UNITS U=1
.TXT 3 1 0 0
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{\rtf1\ansi \deff0
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{\plain {\f0 \fs28 \ul Acceleration in One
 Dimension}{ }{\f0 \fs16 by P. Fraundorf
 Copyright 1992-1995 @newton.umsl.edu: 12
 Oct 1995.}}
}
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{\plain {First, some constants that are 
useful should you decide to change units
 in the calculation...}}
}
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{\plain {speed of light:}}
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{\plain {There are 11 variables of interest,
 at least three of which must be specified
 in order to get the other 8.  Since there
 are 10 different combinations of those 
three initial variables within the input
 kinematic used here, we provide an index
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 results from any one of those 10 setup 
choices.  We initialize the variables to
 arbitrary values in defining them at this
 point...}}
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{\plain {distance traveled}}
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{\plain {constant acceleration}}
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{\plain {Inertial Relativistic (Non-Accelerated
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{\plain {Traveler (Accelerated Observer 
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{\plain {final velocity}}
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{\plain {\f0 \fs28 \ul Inertial Relativistic
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{\plain {A}{ssume here that the time-related
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 initial/final velocities) are specified
 in terms of the inertial relativistic kinematic.
  This time-parameterization follows the
 clocks of an inertial observer, but disagrees
 with accelerated observer clocks for velocities
 near the speed of light.  Some useful functions
 }{\i given }{\i inertial relativistic inputs}{
 are:  }}
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.EQN 10 0 0 0
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{\plain {Newtonian Time:}}
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.EQN 0 13 0 0
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{\plain {Proper Time:}}
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.EQN 0 10 0 0
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Cg a37.375000,40.000000,57
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{\plain {e.g. inertial time needed for 1g
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}
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.EQN 0 6 0 0
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.EQN 0 24 0 0
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.EQN 0 24 0 0
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{\plain {Then...}}
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Cg a38.500000,39.000000,58
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{\plain {e.g. expedition distance after 
20 earth yrs of 1g-burn?}}
}
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.EQN 0 11 0 0
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{\plain {e.g. speed requiring an iyr of 
1g-retroburn to stop?}}
}
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.EQN 1 12 0 0
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C x1,1,0,0
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\b nputs are }{\f0 \fs24 \b \f1 \fs24 \b 
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{\rtf1\ansi \deff0
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{\plain {e.g. 'gees' to do 0 to 0.9c in 
1 week?}}
}
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{\plain {e.g. earthtime for a 1-g space 
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{\plain {e.g. earth time for a 1g retrostop
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{\plain {e.g. retrodeceleration for a 1-ly
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}
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.EQN 0 6 0 0
({0:\Dx}NAME)[(6):1*ly
.EQN 0 27 0 0
(wo)[(6):0*c
.EQN 0 24 0 0
(wf)[(6):.9*c
.TXT 4 -57 0 0
Cg a5.000000,72.000000,10
{\rtf1\ansi \deff0
{\fonttbl
{\f0\fnil Arial;}
{\f1\fnil Symbol;}
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{\plain {Then...}}
}
.EQN 0 13 0 0
(ao)[(6):({0:\g}NAME((wf)[(6))-{0:\g}NAME((wo)[(6)))*((c)^(2))/(({0:\Dx}NAME)[(6))
.EQN 0 27 0 0
({0:\Db}NAME)[(6):(u((wf)[(6))-u((wo)[(6)))/((ao)[(6))
.TXT 5 -41 0 0
Cg a35.875000,38.625000,225
{\rtf1\ansi \deff0
{\fonttbl
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{\f1\fnil Symbol;}
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{\plain {\f0 \fs24 \b Case 7:  I}{\f0 \fs24 
\b nputs are }{\f0 \fs24 \b \f0 \fs24 \b 
 }{\f0 \fs24 \b \f1 \fs24 \b D}{\f0 \fs24 
\b b, }{\f0 \fs24 \b \f0 \fs24 \b  }{\f0 
\fs24 \b \f1 \fs24 \b D}{\f0 \fs24 \b x,
 and ao}{\f0 \fs24 \b :}}
}
.TXT 0 35 0 0
Cg a36.750000,38.000000,57
{\rtf1\ansi \deff0
{\fonttbl
{\f0\fnil Arial;}
{\f1\fnil Symbol;}
}
{\plain {e.g. start speed for a 1g, 1-ly
 burn in 1.5 earth yrs?}}
}
.TXT 2 -34 0 0
Cg a4.500000,73.000000,9
{\rtf1\ansi \deff0
{\fonttbl
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{\plain {Given:}}
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.EQN 0 6 0 0
({0:\Db}NAME)[(7):1.5*iyr
.EQN 0 28 0 0
({0:\Dx}NAME)[(7):1*ly
.EQN 0 24 0 0
(ao)[(7):1*g
.EQN 3 -40 0 0
Y:1-(((({0:\Dx}NAME)[(7))/(c*({0:\Db}NAME)[(7))))^(2)
.EQN 0 25 0 0
Z:((((ao)[(7)*({0:\Db}NAME)[(7)*Y)/(2*c)))^(2)
.TXT 2 -43 0 0
Cg a5.000000,72.000000,10
{\rtf1\ansi \deff0
{\fonttbl
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{\plain {Then...}}
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.TXT 5 0 0 0
Cg a4.125000,72.000000,9
{\rtf1\ansi \deff0
{\fonttbl
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{\plain {and...}}
}
.EQN 0 8 0 0
(wo)[(7):(({0:\Dx}NAME)[(7)-0.5*(ao)[(7)*((({0:\Db}NAME)[(7)))^(2)*Y*\(Y+Z))/(({0:\Db}NAME)[(7)*(1+Z))
.EQN 0 30 0 0
(wf)[(7):(({0:\Dx}NAME)[(7)+0.5*(ao)[(7)*((({0:\Db}NAME)[(7)))^(2)*Y*\(Y+Z))/(({0:\Db}NAME)[(7)*(1+Z))
.TXT 6 -39 0 0
Cg a34.250000,38.625000,193
{\rtf1\ansi \deff0
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{\plain {\f0 \fs24 \b Case 8:  I}{\f0 \fs24 
\b nputs are }{\f0 \fs24 \b \f0 \fs24 \b 
\f1 \fs24 \b D}{\f0 \fs24 \b b, }{\f0 \fs24 
\b \f0 \fs24 \b \f1 \fs24 \b D}{\f0 \fs24 
\b x, and wo}{\f0 \fs24 \b :}}
}
.TXT 0 34 0 0
Cg a38.750000,39.000000,68
{\rtf1\ansi \deff0
{\fonttbl
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{\plain {e.g. accel during a 5 earth-yr 
startup burn to }{\f1 \fs20 a}{-C?}}
}
.TXT 3 -33 0 0
Cg a4.500000,73.000000,9
{\rtf1\ansi \deff0
{\fonttbl
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{\plain {Given:}}
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.EQN 0 6 0 0
({0:\Db}NAME)[(8):5*iyr
.EQN 0 26 0 0
({0:\Dx}NAME)[(8):4*ly
.EQN 0 24 0 0
(wo)[(8):0*c
.TXT 3 -56 0 0
Cg a5.000000,72.000000,10
{\rtf1\ansi \deff0
{\fonttbl
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{\f1\fnil Symbol;}
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{\plain {Then...}}
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.EQN 2 10 0 0
(ao)[(8):2*{0:\g}NAME((wo)[(8))*(({0:\Dx}NAME)[(8)-(wo)[(8)*({0:\Db}NAME)[(8))/(((({0:\Db}NAME)[(8)))^(2)-(((({0:\Dx}NAME)[(8))/(c)))^(2))
.EQN 0 28 0 0
(wf)[(8):(u((wo)[(8))+(ao)[(8)*({0:\Db}NAME)[(8))/(\(1+(((u((wo)[(8))+(ao)[(8)*({0:\Db}NAME)[(8))/(c)))^(2)))
.TXT 10 -39 0 0
Cg a34.750000,38.625000,193
{\rtf1\ansi \deff0
{\fonttbl
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{\plain {\f0 \fs24 \b Case 9:  I}{\f0 \fs24 
\b nputs are }{\f0 \fs24 \b \f0 \fs24 \b 
\f1 \fs24 \b D}{\f0 \fs24 \b b, }{\f0 \fs24 
\b \f0 \fs24 \b \f1 \fs24 \b D}{\f0 \fs24 
\b x, and wf}{\f0 \fs24 \b :}}
}
.TXT 0 35 0 0
Cg a37.500000,39.000000,71
{\rtf1\ansi \deff0
{\fonttbl
{\f0\fnil Arial;}
{\f1\fnil Symbol;}
}
{\plain {e.g. decel for a 5 earth-yr retrostop
 from }{\f1 \fs20 a}{-Centauri?}}
}
.TXT 3 -34 0 0
Cg a4.500000,73.000000,9
{\rtf1\ansi \deff0
{\fonttbl
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{\plain {Given:}}
}
.EQN 0 6 0 0
({0:\Db}NAME)[(9):5*iyr
.EQN 0 26 0 0
({0:\Dx}NAME)[(9):4*ly
.EQN 0 25 0 0
(wf)[(9):0*c
.TXT 4 -57 0 0
Cg a5.000000,72.000000,10
{\rtf1\ansi \deff0
{\fonttbl
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{\plain {Then...}}
}
.EQN 1 10 0 0
(ao)[(9):-2*{0:\g}NAME((wf)[(9))*(({0:\Dx}NAME)[(9)-(wf)[(9)*({0:\Db}NAME)[(9))/(((({0:\Db}NAME)[(9)))^(2)-(((({0:\Dx}NAME)[(9))/(c)))^(2))
.EQN 0 27 0 0
(wo)[(9):(u((wf)[(9))-(ao)[(9)*({0:\Db}NAME)[(9))/(\(1+(((u((wf)[(9))-(ao)[(9)*({0:\Db}NAME)[(9))/(c)))^(2)))
.TXT 14 -38 0 0
C x1,1,0,0
.TXT 8 0 0 0
Cg a51.750000,73.000000,81
{\rtf1\ansi \deff0
{\fonttbl
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{\plain {\ul \f0 \fs28 \b Results Report
 - Relativistic Inertial Inputs}{\f0 \fs28 
\b :}}
}
.TXT 0 48 0 0
Cg a14.500000,71.000000,22
{\rtf1\ansi \deff0
{\fonttbl
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{\plain {\i For Case Number:}}
}
.EQN 0 16 0 0
i:4
.TXT 4 -63 0 0
Cg a66.750000,72.000000,77
{\rtf1\ansi \deff0
{\fonttbl
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{\plain {Variables which are Independent
 of Kinematic or Time-Parameterization are:}}
}
.TXT 3 2 0 0
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{\rtf1\ansi \deff0
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{\plain {Distance:}}
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.EQN 0 8 0 0
({0:\Dx}NAME)[(i)=?ly
.TXT 0 17 0 0
Cg a16.500000,47.000000,25
{\rtf1\ansi \deff0
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{\plain {Constant Acceleration:}}
}
.EQN 0 17 0 0
(ao)[(i)=?g
.TXT 4 -44 0 0
Cg a52.375000,72.000000,78
{\rtf1\ansi \deff0
{\fonttbl
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{\plain {Inertial Relativistic (Non-Accelerated
 Observer)}{ Velocities/Elapsed-Time:}}
}
.EQN 4 0 0 0
(wo)[(i)=?c
.EQN 0 22 0 0
(wf)[(i)=?c
.EQN 0 22 0 0
({0:\Db}NAME)[(i)=?iyr
.TXT 4 -44 0 0
Cg a71.750000,72.000000,79
{\rtf1\ansi \deff0
{\fonttbl
{\f0\fnil Arial;}
{\f1\fnil Symbol;}
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{\plain {Traveler (Accelerated Observer)
 Vector 4-Velocities and Elapsed Proper-Time:}}
}
.EQN 3 0 0 0
(uo)[(i):u((wo)[(i))
.EQN 0 22 0 0
(uf)[(i):u((wf)[(i))
.EQN 0 22 0 0
({0:\D\t}NAME)[(i):{0:D\t}NAME((ao)[(i),(wf)[(i),(wo)[(i),({0:\Dx}NAME)[(i),({0:\Db}NAME)[(i))
.EQN 3 -44 0 0
(uo)[(i)=?rb
.EQN 0 22 0 0
(uf)[(i)=?rb
.EQN 0 22 0 0
({0:\D\t}NAME)[(i)=?tyr
.TXT 3 -44 0 0
Cg a47.625000,72.000000,66
{\rtf1\ansi \deff0
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{\plain {Newtonian (Low-Velocity Approximation)
 Velocities/Elapsed-Time:}}
}
.EQN 3 0 0 0
(vo)[(i):v((wo)[(i))
.EQN 0 22 0 0
(vf)[(i):v((wf)[(i))
.EQN 0 22 0 0
({0:\Dt}NAME)[(i):Dt((ao)[(i),(wf)[(i),(wo)[(i),({0:\Dx}NAME)[(i),({0:\Db}NAME)[(i))
.EQN 3 -44 0 0
(vo)[(i)=?(m)/(sec)
.EQN 0 22 0 0
(vf)[(i)=?(m)/(sec)
.EQN 0 22 0 0
({0:\Dt}NAME)[(i)=?sec
.TXT 5 -45 0 0
Cg a27.875000,73.000000,39
{\rtf1\ansi \deff0
{\fonttbl
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{\plain {\f0 \fs28 Some Graphs of the Result:}}
}
.EQN 4 15 0 0
wT(b):(u((wo)[(i))+(ao)[(i)*b)/(\(1+(((u((wo)[(i))+(ao)[(i)*b)/(c)))^(2)))
.EQN 0 26 0 0
x(b):({0:\g}NAME(wT(b))-{0:\g}NAME((wo)[(i)))*((c)^(2))/((ao)[(i))
.EQN 9 -17 0 0
vT(b):v(wT(b))
.EQN 0 17 0 0
t(b):Dt((ao)[(i),wT(b),(wo)[(i),x(b),b)
.EQN 4 -17 0 0
uT(b):u(wT(b))
.EQN 0 17 0 0
{0:\t}NAME(b):{0:D\t}NAME((ao)[(i),wT(b),(wo)[(i),x(b),b)
.EQN 5 -12 0 0
bInc:(({0:\Db}NAME)[(i))/(100)
.EQN 0 12 0 0
b:0*sec,bInc;({0:\Db}NAME)[(i)
.EQN 4 -41 0 0
&&b,t(b),{0:\t}NAME(b)@&&x(b)
0 0 1 1 0
0 0 1 1 0
0 1 0 0 NO-TRACE-STRING
0 2 1 0 NO-TRACE-STRING
0 3 2 0 NO-TRACE-STRING
0 4 3 0 NO-TRACE-STRING
0 1 4 0 NO-TRACE-STRING
0 2 5 0 NO-TRACE-STRING
0 3 6 0 NO-TRACE-STRING
0 4 0 0 NO-TRACE-STRING
0 1 1 0 NO-TRACE-STRING
0 2 2 0 NO-TRACE-STRING
0 3 3 0 NO-TRACE-STRING
0 4 4 0 NO-TRACE-STRING
0 1 5 0 NO-TRACE-STRING
0 2 6 0 NO-TRACE-STRING
0 3 0 0 NO-TRACE-STRING
0 4 1 0 NO-TRACE-STRING
0 1 23 17
.EQN 0 37 0 0
&&wT(b),vT(b),uT(b)@&&x(b)
0 0 1 1 0
0 0 1 1 0
0 1 0 0 NO-TRACE-STRING
0 2 1 0 NO-TRACE-STRING
0 3 2 0 NO-TRACE-STRING
0 4 3 0 NO-TRACE-STRING
0 1 4 0 NO-TRACE-STRING
0 2 5 0 NO-TRACE-STRING
0 3 6 0 NO-TRACE-STRING
0 4 0 0 NO-TRACE-STRING
0 1 1 0 NO-TRACE-STRING
0 2 2 0 NO-TRACE-STRING
0 3 3 0 NO-TRACE-STRING
0 4 4 0 NO-TRACE-STRING
0 1 5 0 NO-TRACE-STRING
0 2 6 0 NO-TRACE-STRING
0 3 0 0 NO-TRACE-STRING
0 4 1 0 NO-TRACE-STRING
0 1 22 17
.EQN 23 -37 0 0
&&b,t(b),{0:\t}NAME(b)@&&b
0 0 1 1 0
0 0 1 1 0
0 1 0 0 NO-TRACE-STRING
0 2 1 0 NO-TRACE-STRING
0 3 2 0 NO-TRACE-STRING
0 4 3 0 NO-TRACE-STRING
0 1 4 0 NO-TRACE-STRING
0 2 5 0 NO-TRACE-STRING
0 3 6 0 NO-TRACE-STRING
0 4 0 0 NO-TRACE-STRING
0 1 1 0 NO-TRACE-STRING
0 2 2 0 NO-TRACE-STRING
0 3 3 0 NO-TRACE-STRING
0 4 4 0 NO-TRACE-STRING
0 1 5 0 NO-TRACE-STRING
0 2 6 0 NO-TRACE-STRING
0 3 0 0 NO-TRACE-STRING
0 4 1 0 NO-TRACE-STRING
0 1 23 17
.EQN 1 37 0 0
&&wT(b),vT(b),uT(b)@&&b
0 0 1 1 0
0 0 1 1 0
0 1 0 0 NO-TRACE-STRING
0 2 1 0 NO-TRACE-STRING
0 3 2 0 NO-TRACE-STRING
0 4 3 0 NO-TRACE-STRING
0 1 4 0 NO-TRACE-STRING
0 2 5 0 NO-TRACE-STRING
0 3 6 0 NO-TRACE-STRING
0 4 0 0 NO-TRACE-STRING
0 1 1 0 NO-TRACE-STRING
0 2 2 0 NO-TRACE-STRING
0 3 3 0 NO-TRACE-STRING
0 4 4 0 NO-TRACE-STRING
0 1 5 0 NO-TRACE-STRING
0 2 6 0 NO-TRACE-STRING
0 3 0 0 NO-TRACE-STRING
0 4 1 0 NO-TRACE-STRING
0 1 22 17
.TXT 25 -37 0 0
C x1,1,0,0
.TXT 5 1 0 0
Cg a71.500000,72.000000,95
{\rtf1\ansi \deff0
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{\plain {For Cases with i=4,5, a Set of 
Different Kinematic-Dependent Values may
 also Fit the Inputs:}}
}
.TXT 5 3 0 0
Cg a31.750000,69.000000,48
{\rtf1\ansi \deff0
{\fonttbl
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{\plain {We first set up the Alternative
 Value Arrays:}}
}
.EQN 0 39 0 0
k:0,1;9
.EQN 3 -43 0 0
(vo)[(k+10):if(k÷5,(vo)[(k+10),(vo)[(k))
.EQN 0 22 0 0
(vf)[(k+10):if(k÷4,(vf)[(k+10),(vf)[(k))
.EQN 0 21 0 0
({0:\Dt}NAME)[(k+10):if(k<4,({0:\Dt}NAME)[(k),if(k>6,({0:\Dt}NAME)[(k),({0:\Dt}NAME)[(k+10)))
.TXT 5 -39 0 0
Cg a31.500000,71.000000,48
{\rtf1\ansi \deff0
{\fonttbl
{\f0\fnil Arial;}
{\f1\fnil Symbol;}
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{\plain {The Alternative Value Index for
 this Case is:}}
}
.EQN 0 33 0 0
k:i+10
.TXT 0 10 0 0
Cg a17.375000,26.000000,26
{\rtf1\ansi \deff0
{\fonttbl
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{\plain {which has Values for...}}
}
.TXT 3 -46 0 0
Cg a52.375000,72.000000,78
{\rtf1\ansi \deff0
{\fonttbl
{\f0\fnil Arial;}
{\f1\fnil Symbol;}
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{\plain {Inertial Relativistic (Non-Accelerated
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}
.EQN 4 0 0 0
(wo)[(k)=?c
.EQN 0 22 0 0
(wf)[(k)=?c
.EQN 0 22 0 0
({0:\Db}NAME)[(k)=?iyr
.TXT 4 -44 0 0
Cg a71.750000,72.000000,79
{\rtf1\ansi \deff0
{\fonttbl
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{\f1\fnil Symbol;}
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{\plain {Traveler (Accelerated Observer)
 Vector 4-Velocities and Elapsed Proper-Time:}}
}
.EQN 3 0 0 0
(uo)[(k):u((wo)[(k))
.EQN 0 22 0 0
(uf)[(k):u((wf)[(k))
.EQN 0 22 0 0
({0:\D\t}NAME)[(k):{0:D\t}NAME((ao)[(i),(wf)[(k),(wo)[(k),({0:\Dx}NAME)[(i),({0:\Db}NAME)[(k))
.EQN 3 -44 0 0
(uo)[(k)=?rb
.EQN 0 22 0 0
(uf)[(k)=?rb
.EQN 0 22 0 0
({0:\D\t}NAME)[(k)=?tyr
.TXT 3 -44 0 0
Cg a47.625000,72.000000,66
{\rtf1\ansi \deff0
{\fonttbl
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{\f1\fnil Symbol;}
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{\plain {Newtonian (Low-Velocity Approximation)
 Velocities/Elapsed-Time:}}
}
.EQN 3 0 0 0
(vo)[(k):v((wo)[(k))
.EQN 0 22 0 0
(vf)[(k):v((wf)[(k))
.EQN 0 22 0 0
({0:\Dt}NAME)[(k):Dt((ao)[(i),(wf)[(k),(wo)[(k),({0:\Dx}NAME)[(i),({0:\Db}NAME)[(k))
.EQN 3 -44 0 0
(vo)[(k)=?(m)/(sec)
.EQN 0 22 0 0
(vf)[(k)=?(m)/(sec)
.EQN 0 22 0 0
({0:\Dt}NAME)[(k)=?sec
.TXT 4 -45 0 0
Cg a40.500000,73.000000,51
{\rtf1\ansi \deff0
{\fonttbl
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{\f1\fnil Symbol;}
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{\plain {\f0 \fs28 Some Graphs of the Alternate
 Solution:}}
}
.EQN 6 15 0 0
wT(b):(u((wo)[(k))+(ao)[(i)*b)/(\(1+(((u((wo)[(k))+(ao)[(i)*b)/(c)))^(2)))
.EQN 0 26 0 0
x(b):({0:\g}NAME(wT(b))-{0:\g}NAME((wo)[(k)))*((c)^(2))/((ao)[(i))
.EQN 9 -17 0 0
vT(b):v(wT(b))
.EQN 0 17 0 0
t(b):Dt((ao)[(i),wT(b),(wo)[(k),x(b),b)
.EQN 3 -17 0 0
uT(b):u(wT(b))
.EQN 0 17 0 0
{0:\t}NAME(b):{0:D\t}NAME((ao)[(i),wT(b),(wo)[(k),x(b),b)
.EQN 5 -12 0 0
bInc:(({0:\Db}NAME)[(k))/(100)
.EQN 0 12 0 0
b:0*sec,bInc;({0:\Db}NAME)[(k)
.EQN 4 -41 0 0
_n_u_l_l_&_n_u_l_l_&b,t(b),{0:\t}NAME(b)@_n_u_l_l_&_n_u_l_l_&x(b)
0 0 1 1 0
0 0 1 1 0
0 1 0 0 NO-TRACE-STRING
0 2 1 0 NO-TRACE-STRING
0 3 2 0 NO-TRACE-STRING
0 4 3 0 NO-TRACE-STRING
0 1 4 0 NO-TRACE-STRING
0 2 5 0 NO-TRACE-STRING
0 3 6 0 NO-TRACE-STRING
0 4 0 0 NO-TRACE-STRING
0 1 1 0 NO-TRACE-STRING
0 2 2 0 NO-TRACE-STRING
0 3 3 0 NO-TRACE-STRING
0 4 4 0 NO-TRACE-STRING
0 1 5 0 NO-TRACE-STRING
0 2 6 0 NO-TRACE-STRING
0 3 0 0 NO-TRACE-STRING
0 4 1 0 NO-TRACE-STRING
0 1 23 17
.EQN 0 37 0 0
_n_u_l_l_&_n_u_l_l_&wT(b),vT(b),uT(b)@_n_u_l_l_&_n_u_l_l_&x(b)
0 0 1 1 0
0 0 1 1 0
0 1 0 0 NO-TRACE-STRING
0 2 1 0 NO-TRACE-STRING
0 3 2 0 NO-TRACE-STRING
0 4 3 0 NO-TRACE-STRING
0 1 4 0 NO-TRACE-STRING
0 2 5 0 NO-TRACE-STRING
0 3 6 0 NO-TRACE-STRING
0 4 0 0 NO-TRACE-STRING
0 1 1 0 NO-TRACE-STRING
0 2 2 0 NO-TRACE-STRING
0 3 3 0 NO-TRACE-STRING
0 4 4 0 NO-TRACE-STRING
0 1 5 0 NO-TRACE-STRING
0 2 6 0 NO-TRACE-STRING
0 3 0 0 NO-TRACE-STRING
0 4 1 0 NO-TRACE-STRING
0 1 22 17
.EQN 23 -37 0 0
_n_u_l_l_&_n_u_l_l_&b,t(b),{0:\t}NAME(b)@_n_u_l_l_&_n_u_l_l_&b
0 0 1 1 0
0 0 1 1 0
0 1 0 0 NO-TRACE-STRING
0 2 1 0 NO-TRACE-STRING
0 3 2 0 NO-TRACE-STRING
0 4 3 0 NO-TRACE-STRING
0 1 4 0 NO-TRACE-STRING
0 2 5 0 NO-TRACE-STRING
0 3 6 0 NO-TRACE-STRING
0 4 0 0 NO-TRACE-STRING
0 1 1 0 NO-TRACE-STRING
0 2 2 0 NO-TRACE-STRING
0 3 3 0 NO-TRACE-STRING
0 4 4 0 NO-TRACE-STRING
0 1 5 0 NO-TRACE-STRING
0 2 6 0 NO-TRACE-STRING
0 3 0 0 NO-TRACE-STRING
0 4 1 0 NO-TRACE-STRING
0 1 23 17
.EQN 1 37 0 0
_n_u_l_l_&_n_u_l_l_&wT(b),vT(b),uT(b)@_n_u_l_l_&_n_u_l_l_&b
0 0 1 1 0
0 0 1 1 0
0 1 0 0 NO-TRACE-STRING
0 2 1 0 NO-TRACE-STRING
0 3 2 0 NO-TRACE-STRING
0 4 3 0 NO-TRACE-STRING
0 1 4 0 NO-TRACE-STRING
0 2 5 0 NO-TRACE-STRING
0 3 6 0 NO-TRACE-STRING
0 4 0 0 NO-TRACE-STRING
0 1 1 0 NO-TRACE-STRING
0 2 2 0 NO-TRACE-STRING
0 3 3 0 NO-TRACE-STRING
0 4 4 0 NO-TRACE-STRING
0 1 5 0 NO-TRACE-STRING
0 2 6 0 NO-TRACE-STRING
0 3 0 0 NO-TRACE-STRING
0 4 1 0 NO-TRACE-STRING
0 1 22 17