Passive and Active Transformations

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The discussion centers on the distinction between active and passive transformations in 2D rotation matrices. It highlights that one transformation involves changing the coordinates of a point while the other alters the basis vectors. The confusion arises when deriving matrices with inconsistent orientations, particularly when using a clockwise rotation. A consistent approach is essential to avoid errors, as the rotation of basis vectors directly informs the transformation of all vectors. Ultimately, understanding the relationship between the basis and the points being transformed is crucial for accurate matrix representation.
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Alright. I was looking into a 2D rotation matrix and there are two equations: one is through the transformation of the component of p (always with respect to x,y), x,y into x',y' and the other is through the transformation of the unit vectors i,j into i',j'.

In a sense 1 is passive the other is an active transformation. I do understand the difference between the two, but my question is that why do we get the different matrices if when we derive them, we do so with a clockwise orientation?

Hope its clear, If not--I'd be happy to clarify.
 
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Can you clarify. I guess I understand what you mean, but just to be sure.
 
LOL Okay. I got the answer. Welp it seems like they way you derive the matrix you have to say consistent, otherwise you fall in a a trap.
https://en.wikipedia.org/wiki/Active_and_passive_transformation#/media/File:PassiveActive.JPG
Staring at this image for a bit and making sense of this reasoning: http://math.stackexchange.com/quest...erent-representations-of-2d-rotation-matrices

helped. You need to use a point relative to the rotated basis once you rotate the basis. You cannot use a rotated basis on a point relative to a the old basis, but with rotational matrices you only an inverted answer and nothing any more alarming.
 
See this thread for some general comments about "active" vs. "passive" rotations.

The convention that I'm familiar with is to rotate vectors counterclockwise. A rotation is linear, so if we know how the basis vectors are rotated, we will know how all vectors are rotated. If you rotate (1,0) by an angle ##\theta## counterclockwise, the result is ##(\cos\theta,\sin\theta)##. The same rotation applied to (0,1) yields ##(-\sin\theta,\cos\theta)##. It follows immediately from this that the matrix of the rotation operator with respect to the standard ordered basis is
$$\begin{pmatrix}\cos\theta & -\sin\theta\\ \sin\theta & \cos\theta\end{pmatrix}.$$ The rotated basis vectors end up as the columns of the matrix. If you don't understand this, I recommend the FAQ post that I linked to in the post I linked to above.
 
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Hehe alright, thanks. Looking back at it, I was being pretty dense.
 
I am studying the mathematical formalism behind non-commutative geometry approach to quantum gravity. I was reading about Hopf algebras and their Drinfeld twist with a specific example of the Moyal-Weyl twist defined as F=exp(-iλ/2θ^(μν)∂_μ⊗∂_ν) where λ is a constant parametar and θ antisymmetric constant tensor. {∂_μ} is the basis of the tangent vector space over the underlying spacetime Now, from my understanding the enveloping algebra which appears in the definition of the Hopf algebra...

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