The Wires: Difference between revisions
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<center><math>\underline{\textbf{Navigation}}</math> | |||
[[Points_of_Intersection|<math>\vartriangleleft </math>]] | |||
[[VanWasshenova_Thesis#Determining_wire-theta_correspondence|<math>\triangle </math>]] | |||
[[Right_Hand_Wall|<math>\vartriangleright </math>]] | |||
</center> | |||
We can parametrize the equations for the wires and wire midpoints to express the equation in vector form. In the y'-x' plane the general equation follows the relationship: | We can parametrize the equations for the wires and wire midpoints to express the equation in vector form. In the y'-x' plane the general equation follows the relationship: | ||
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<center><math>x' = y\ sin\ 6^{\circ}+x_0</math></center> | <center><math>x' = y\ sin\ 6^{\circ}+x_0</math></center> | ||
<center><math>y' = y\ cos\ 6^{\circ}</math></center> | <center><math>y' = y\ cos\ 6^{\circ}</math></center> | ||
The parameterization has reduced two equations with two variables, to two equations which depend on one variable. Working in the y-x plane, we will undergo a positive rotation, | The parameterization has reduced two equations with two variables, to two equations which depend on one variable. Working in the y-x plane, we will undergo a positive rotation, | ||
) | <center><math>R(\theta_{yx})=\begin{bmatrix} | ||
cos\ 6^{\circ} &-sin\ 6^{\circ} & 0 \\ | |||
sin\ 6^{\circ} & cos\ 6^{\circ} &0 \\ | |||
0 &0 & 1 | |||
\end{bmatrix}</math></center> | |||
<center><math>\begin{bmatrix} | |||
same vector | Components\ of \\ | ||
in new system | same\ vector \\ | ||
in\ new\ system | |||
\end{bmatrix} | |||
transformation | =\begin{bmatrix} | ||
Passive \\ | |||
transformation \\ | |||
matrix | matrix | ||
\end{bmatrix}\cdot | |||
\begin{bmatrix} | |||
Components\ of \\ | |||
vector\ in \\ | |||
original\ system | |||
\end{bmatrix}</math></center> | |||
<center><math> | |||
\begin{bmatrix} | |||
x'' \\ | |||
y'' \\ | |||
y'' | |||
z'' | z'' | ||
\end{bmatrix}= | |||
\begin{bmatrix} | |||
sin 6\ | cos\ 6^{\circ} &-sin\ 6^{\circ} & 0 \\ | ||
0 0 1 | sin\ 6^{\circ} & cos\ 6^{\circ} &0 \\ | ||
0 &0 & 1 | |||
\end{bmatrix}\cdot | |||
y' | \begin{bmatrix} | ||
x' \\ | |||
y' \\ | |||
z' | z' | ||
\end{bmatrix}</math></center> | |||
<center><math> | |||
y' | \begin{bmatrix} | ||
z' | x'' \\ | ||
y'' \\ | |||
z'' | |||
\end{bmatrix}= | |||
\begin{bmatrix} | |||
cos\ 6^{\circ} &-sin\ 6^{\circ} & 0 \\ | |||
sin\ 6^{\circ} & cos\ 6^{\circ} &0 \\ | |||
0 &0 & 1 | |||
\end{bmatrix}\cdot | |||
\begin{bmatrix} | |||
y'\ sin\ 6^{\circ}+x_0 \\ | |||
y'\ cos\ 6^{\circ} \\ | |||
0 | |||
\end{bmatrix}</math></center> | |||
<center><math> | |||
\begin{bmatrix} | |||
x'' \\ | |||
y'' | y'' \\ | ||
z'' | z'' | ||
\end{bmatrix}= | |||
\begin{bmatrix} | |||
-y'\ cos\ 6^{\circ}sin\ 6^{\circ}+x_0\ cos\ 6^{\circ} +y'\ cos\ 6^{\circ}sin\ 6^{\circ}\\ | |||
y'\ cos^2 6^{\circ}+x_0\sin\ 6^{\circ}+y sin^2 6^{\circ} \\ | |||
0 | |||
\end{bmatrix}</math></center> | |||
<center><math> | |||
y | \begin{bmatrix} | ||
x'' \\ | |||
y'' \\ | |||
z'' | |||
\end{bmatrix}= | |||
\begin{bmatrix} | |||
x_0\ cos\ 6^{\circ}\\ | |||
y'\ +x_0\sin\ 6^{\circ} \\ | |||
0 | 0 | ||
\end{bmatrix}</math></center> | |||
This relationship shows us that x'' is a constant in this frame while y'' can have any value, which is the horizontal line with respect to the y axis as expected. | |||
---- | |||
<center><math>\underline{\textbf{Navigation}}</math> | |||
[[Points_of_Intersection|<math>\vartriangleleft </math>]] | |||
[[VanWasshenova_Thesis#Determining_wire-theta_correspondence|<math>\triangle </math>]] | |||
[[Right_Hand_Wall|<math>\vartriangleright </math>]] | |||
</center> | |||
Latest revision as of 20:32, 15 May 2018
[math]\displaystyle{ \vartriangleleft }[/math] [math]\displaystyle{ \triangle }[/math] [math]\displaystyle{ \vartriangleright }[/math]
We can parametrize the equations for the wires and wire midpoints to express the equation in vector form. In the y'-x' plane the general equation follows the relationship:
where [math]\displaystyle{ x_0 }[/math] is the point where the line crosses the x axis.
In this form we can easily see that the components of x and y , in the y'-x' plane are
The parameterization has reduced two equations with two variables, to two equations which depend on one variable. Working in the y-x plane, we will undergo a positive rotation,
This relationship shows us that x is a constant in this frame while y can have any value, which is the horizontal line with respect to the y axis as expected.
[math]\displaystyle{ \vartriangleleft }[/math] [math]\displaystyle{ \triangle }[/math] [math]\displaystyle{ \vartriangleright }[/math]