Two-Dimensional Rotations |
The 2D analogy given in the explanation of Euler angles is a standard way of explaining three-dimensional rotations. But sometimes it is hard to see how the actual rotation matrix is obtained, and most authors don't dwell on it. The purpose of this page is to explain this in more detail.
Suppose the coordinates, (x,y), of a point in the two-dimensional XY system are known, but we are actually interested in knowing the coordinates of this point in another coordinate system, X'Y', which is related to the XY system by a counter-clockwise rotation by an angle α. As the figure indicates, the coordinates of the given point in the new coordinate system will be: x' = x cos α + y sin α y' = -x sin α + y cos α These transformations are explained in the next two pictures. | |
Obtaining the new x' coordinate: The old x coordinate of P corresponds to the length of the line between points
O and E on the old X axis, |OE|. Similarly, the new x' coordinate of P corresponds to the
length of the line between points O and I on the new X' axis, |OI|; we can see that this
length is the sum of |OF| and |FI|. How does this help? | |
Obtaining the new y' coordinate: It works for the y' coordinate analogously: |
[1] | V. Heine, Group Theory in Quantum Mechanics: An Introduction to
its Present Usage, Pergamon Press: New York, 1960. |
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