What is an example of a proper rotation in physics?

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A proper rotation in physics refers to transformations where the determinant of the transformation matrix is +1, maintaining the orientation of a right-handed coordinate system. This ensures that the transformation is physically realizable. In contrast, an improper rotation has a determinant of -1, which reverses the orientation, transforming a right-handed system into a left-handed one. Such transformations are deemed improper as they cannot be physically realized, effectively "turning space inside out." Understanding these distinctions is crucial in the study of rotations and Lorentz transformations in physics.
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An example being its use in the beginning of this document:

http://isites.harvard.edu/fs/docs/icb.topic1288789.files/Rotations-Lorentz-Transformations.pdf

I haven't read the whole document yet so forgive me if it explains what it means later on.
 
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'proper' usually means the determinant of the transformation matrix is +1.
 
Meir Achuz comment is correct, as far as it goes. If the determinant is +1, a right-handed coordinate system is transformed into a right-handed coordinate system; this is a "proper" (or physically realizable) transformation.

If the determinant is -1, the transformation is "improper" which is to say that a right-handed system is transformed into a left-handed system, and vice versa. This is improper in that it cannot be realized physically because "it turns space inside out."
 
For simple comparison, I think the same thought process can be followed as a block slides down a hill, - for block down hill, simple starting PE of mgh to final max KE 0.5mv^2 - comparing PE1 to max KE2 would result in finding the work friction did through the process. efficiency is just 100*KE2/PE1. If a mousetrap car travels along a flat surface, a starting PE of 0.5 k th^2 can be measured and maximum velocity of the car can also be measured. If energy efficiency is defined by...

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