Difference between revisions of "The Wires"
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<center><math>\begin{bmatrix} | <center><math>\begin{bmatrix} | ||
− | Components of \\ | + | Components\ of \\ |
− | same vector \\ | + | same\ vector \\ |
− | in new system | + | in\ new\ system |
− | \end{bmatrix} | + | \end{bmatrix} |
− | + | =\begin{bmatrix} | |
Passive \\ | Passive \\ | ||
transformation \\ | transformation \\ | ||
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\end{bmatrix}\cdot | \end{bmatrix}\cdot | ||
\begin{bmatrix} | \begin{bmatrix} | ||
− | Components of \\ | + | Components\ of \\ |
− | vector in \\ | + | vector\ in \\ |
− | original system | + | original\ system |
\end{bmatrix}</math></center> | \end{bmatrix}</math></center> | ||
Revision as of 16:23, 1 May 2017
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
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.