Geometry of SO(3): Reflection, Composition & Rotation

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Homework Help Overview

The discussion revolves around the properties and compositions of reflections and rotations in three-dimensional space, specifically within the context of the special orthogonal group SO(3) and the orthogonal group O(3). Participants explore the implications of composing reflections, the characteristics of rotation matrices, and the relationships between angles and axes of rotation.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants inquire about the nature of matrices in SO(3) and O(3)/SO(3), the behavior of points under reflections, and the composition of reflections in R3 compared to R2. There are questions regarding the derivation of rotation matrices from given angles and axes, as well as the implications of determinant properties in the context of reflections and rotations.

Discussion Status

Several participants have shared their understanding of the mathematical concepts involved, while others express uncertainty about specific aspects, such as the composition of reflections in three dimensions. There is an ongoing exploration of how to derive rotation matrices from given parameters, indicating a productive exchange of ideas without a clear consensus yet.

Contextual Notes

Participants are navigating complex relationships between geometric transformations, and some express confusion regarding the application of known results from two dimensions to three dimensions. The discussion includes references to specific properties of reflections and rotations, as well as the need for orthonormal bases in certain contexts.

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1) Let P,Q be planes through the origin in R3. Let Rp, Rq be the corresponding reflections. Is Rp*Rq (where * denotes "composition") in SO(3) or O(3)/SO(3)? What is the axis of rotation of Rp*Rq?


2) For a fixed A in SO(3) show that there are infinitely many pairs of planes P,Q such that A=Rp*Rq.


3) For arbitrary A,B in SO(3) find the axis and angle of rotation of AB.
 
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1. What does it mean for a matrix to be in SO(3)? How about O(3)/SO(3)? What can you say about the matrices Rp and Rq? What happens to any point on the axis of rotation of Rp*Rq under the action of Rp*Rq itself? What happens to any point in P under the action of Rp?

2. Do you know that in R², if you take a reflection about a line whose angle with the origin is x, and a line whose angle is y, then composing the reflections gives a rotation through an angle of x-y? Note that x-y = (x+a)-(y+a).

3. What have you tried?
 
Last edited:
1) SO(3) are all orthogonal matrices with det 1, and represents the rotation group in R3.

I know what the rotation matrices in R3 look like, but don't know what the reflection ones do, so I can't say what happens to a point on the axis of reflection.

2) I do know that the composition of reflections in R2 is the sum of the acute angles, but I can't figure it out for 3 dimensions and for planes (for R2 I did it with lines). So, how can I compose two reflections of planes in R3?

3) I know that the axis of rotation of AB is:
+- (cos(a/2)sin(b/2)Ub)+- (sin(a/2)cos(b/2)Ua)+- (sin(a/2)sin(b/2)sin(c)Uab) where Ua, Ub, Uab are the unit vectors.

And I know that the angle of rotation is:
2sin^-1(cos^2(a/2)sin^2(b/2)+sin^2(a/2)cos^2(b/2)+sin^2(a/2)sin^2(b/2)sin^2(c))^1/2

So I know the answer, but can't figure out how to arrive at it... any thoughts?
 
1. Do you know that det(AB) = det(A)det(B)? A reflection in the plane P fixes all points in P. Rotation about a line L fixes all points in L.

2. I don't know what you mean by "the composition of reflection in R2 is the sum of the acute angles," but did you note what I said?

Do you know that in R², if you take a reflection about a line whose angle with the origin is x, and a line whose angle is y, then composing the reflections gives a rotation through an angle of x-y? (EDITED)

If anything, it would be the difference of the acute angles. Anyways, that means that a reflection about a line with angle x, followed by a reflection about a line with angle y produces the same rotation as a reflection about a line with angle x+a, followed by a reflection about a line with angle y+a, and there are an infinite number of a's to choose from. So, if you take two lines, and rotate them together, then you still end up with the same rotation after composing the new reflections. Can you think of what you can do with two planes?

3. Given a rotation with the angle and axis specified, can you find it's matrix? Conversely, given a matrix in SO(3), can you find the angle and axis?
 
3) No I don't know how to find the associated matrix... can you help?
 
A rotation about the z axis through an angle x is represented by the matrix:
Code:
(cosx  -sinx  0)
(sinx   cosx  0)
(0      0     1)
So the matrix through an angle x about an another axis will be a similar matrix to the one above, all you need is a change of basis matrix that changes the z axis into your axis of rotation. Make sure to pick an orthonormal right-handed basis. You may not need such a basis, perhaps any basis with the third vector being on the rotation axis will do, but I'm not sure since this is just coming off the top of my head, so it's probably better to play it safe. Actually, I'm pretty sure you'd want an orthogonal basis otherwise a rotation about one vector won't guarantee that your rotation is in the plane spanned by the other two vectors, whereas when you have an orthogonal basis like your standard basis, a rotation about the z axis is the same as a rotation in the plane spanned by the other two vectors, x and y, and this matrix representation (I believe) only works when it's set up like this.
 

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