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MyWikiBiz, Author Your Legacy — Wednesday September 10, 2025
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Here is a table of the two trajectories or ''orbits'' that we get by starting from each of the two permissible initial states and staying within the constraints of the dynamic law <math>d^2 x = (x).\!</math>
 
Here is a table of the two trajectories or ''orbits'' that we get by starting from each of the two permissible initial states and staying within the constraints of the dynamic law <math>d^2 x = (x).\!</math>
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{| cellpadding="8" width="100%"
+
{| align="center" cellpadding="8" style="text-align:center"
| width="10%" | &nbsp;
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| <math>\text{Initial State}\ x \cdot dx</math>
| width="90%" |
+
|-
<p><math>\text{Initial State}\ x \cdot dx</math></p>
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|
<br>
+
<math>\begin{array}{cccc}
<p><math>\begin{array}{cccc}
   
t &  d^0 x &  d^1 x &  d^2 x \\
 
t &  d^0 x &  d^1 x &  d^2 x \\
 +
\\
 
0 &      1 &      1 &      0 \\
 
0 &      1 &      1 &      0 \\
 
1 &      0 &      1 &      1 \\
 
1 &      0 &      1 &      1 \\
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|}
 
|}
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{| align="center" cellpadding="8" width="90%"
+
<br>
|+ <math>\text{Initial State}\ (x) \cdot (dx)</math>
+
 
| align="center" |
+
{| align="center" cellpadding="8" style="text-align:center"
 +
| <math>\text{Initial State}\ (x) \cdot (dx)</math>
 +
|-
 +
|
 
<math>\begin{array}{cccc}
 
<math>\begin{array}{cccc}
 
t &  d^0 x &  d^1 x &  d^2 x \\
 
t &  d^0 x &  d^1 x &  d^2 x \\
 +
\\
 
0 &      0 &      0 &      1 \\
 
0 &      0 &      0 &      1 \\
 
1 &      0 &      1 &      1 \\
 
1 &      0 &      1 &      1 \\
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<pre>
 
<pre>
d d d
  −
0 1 2
  −
x x x
  −
  −
Initial State x dx
  −
  −
1 1 0
  −
0 1 1
  −
1 0 0
  −
1 0 0
  −
1 0 0
  −
" " "
  −
  −
Initial State (x)(dx)
  −
  −
0 0 1
  −
0 1 1
  −
1 0 0
  −
1 0 0
  −
1 0 0
  −
" " "
  −
   
Note that the state x (dx) (d^2.x),
 
Note that the state x (dx) (d^2.x),
 
that is, <x, dx, d^2.x> = <1, 0, 0>,
 
that is, <x, dx, d^2.x> = <1, 0, 0>,
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