What is the Dimension of a 3-D Rotation Matrix?

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The discussion centers on the dimensions of various rotation matrices and Lie groups, particularly SO(3, R), SE(3, R), and GL+(3, R). The dimension of the rotation matrix in SO(3, R) is confirmed to be 3, corresponding to the three Euler angles representing rotations about orthogonal axes. SE(3, R) is identified as 6-dimensional, while the dimension of GL+(3, R)/GL+(2, R) is calculated to be 5, assuming the positive determinant condition does not reduce the dimensions further. The conversation also touches on the nature of manifolds and coordinate systems, emphasizing the importance of understanding these concepts for grasping the dimensions of the discussed groups. Overall, the thread provides insights into the mathematical framework surrounding rotation matrices and their dimensions.
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I have a similar question about rotation matrices. I'm trying to understand the dimension of the matrix given below which is a 3-D rotation. I think that its dimension is 3 but unsure. Any help appreciated. Thanks, John

[(cosx sin x 0), (-sinx cosx 0), (0 0 1)] with ( ) = row,
 
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Fredrik,

Thanks for your comment. Sorry for not being clearer. I mean the dimension of the vector space of 3 X 3 matrices R in SO(3, R). In other words, the number of elements in the basis. SO(3,R) is nxn real matrices such that RR^T = I & detR = 1.

I think that the answer is 3 but I'm having trouble to list them.

My ultimate goal is to find the dimension of the vector space of the following:
1) SE(3, R) = {g in R^(4x4) | g in [(R r), (000,1)], detg = 1, R in SO(3, R), r in R^3} which, I think, is 6.
2) GL+(3,R)/GL+(2,R) where GL+(n, R) = {M in R^(nxn) | detM >0}

Thanks, John
 
SO(3) doesn't have a natural vector space structure, since the sum of two of its members isn't in SO(3). It's a 3-dimensional Lie group (a 3-dimensional manifold that's also a group and satisfies an additional technical requirement).
 
Fredrik,

Thanks for clarifying this. Since a 3-dim. manifold, what do its 3 dimensions represent? By this, I mean are they the rotation matrices (or angles) for rotations about three orthogonal axes ?

SE(3,R) & GL+(3,R) also are Lie groups so how does one get dimensions of these manifolds ?

Sorry to be so clumsy about this !

Thanks, John
 
oldmathguy said:
Thanks for clarifying this. Since a 3-dim. manifold, what do its 3 dimensions represent? By this, I mean are they the rotation matrices (or angles) for rotations about three orthogonal axes ?

SE(3,R) & GL+(3,R) also are Lie groups so how does one get dimensions of these manifolds ?
A manifold is always equipped with a bunch of coordinate systems. These are functions from open subsets of the manifold into ℝn for some n. That n is the dimension of the manifold. There are many ways to define a coordinate system on SO(3). One way to do it is to use Euler angles. Three Euler angles specify a rotation uniquely.
 
Fredrik,

Thanks very much for clarifying SO(3, R) using Euler angles. I somewhat understand Euler angles so can see why 3 work.

I found some another good explanation of the dimension of SO(3) by Prof. VVedensky from Imperial College www.cmth.ph.ic.ac.uk/people/d.vvedensky/groups/Chapter7.pdf (p. 116). He also clarifies SE(3,R) being 6-dimensional.

This leaves (thanks to you both) only GL+(3,R)/GL+(2,R). I realize (think !) that dimensions are 9 for GL(3,R) & 4 for GL(2,R) and that this means 5 for GL(3,R)/GL(2,R). However, I'm wondering if the requirement of a positive determinant reduces the dimensions of GL+(3,R), GL+(2,R), & GL+(3,R)/GL+(2,R).

My work concerns the polar decomposition of the deformation gradient F as in F = [v]R where:
F in GL+(3, R)
[v] = {vu | ux = x, u in GL+(3,R), x in R^3, v in Symm+(3, R) diffeomorphic to GL+(3, R)/SO(3,R)}
[v] in GL+(3, R) / N where N = {u | ux = x, u in GL+(3, R), x in R^3} where N is isometric to GL+(2, R)
[v] are equivalence classes of stretches which include both pure stretch & shear
R in SO(3, R)

So, my goal is to understand the dimension of the manifold GL+(3, R) / N.

Thanks again, very much.

John
 

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