Graduate Lie Bracket * Matrix * vector (Need proof)

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The discussion revolves around proving the commutation relationship involving skew symmetric matrices W and S derived from vector components. The goal is to demonstrate that W*S*W*s equals S*W*W*s, leading to the conclusion that the Lie Bracket [W,S]*W*s equals zero. The participants emphasize the importance of specifying vector and matrix dimensions, particularly noting that if the dimension exceeds two and W is invertible, [W,S] generally does not equal zero. The final resolution involves recognizing that the Lie Bracket represents a cross product of parallel vectors, confirming the initial assertion. The conversation highlights the complexities of the proof and the necessity for clarity in mathematical definitions.
Trying2Learn
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TL;DR
Relationship of Skew Symmetry, vectors, cross product and Lie Bracket
As an aside, fresh_42 commented and I made an error in my post that is now fixed. His comment, below, is not valid (my fault), in that THIS post is now fixed.Assume s and w are components of vectors, both in the same frame

Assume S and W are skew symmetric matrices formed from the vector components

I want to prove this (that I CAN commute the first two terms on each side)

W*S*W*s = S*W*W*s

Thus, I want to prove

W*S*W*s - S*W*W*s = 0

(W*S-S*W)*W*s =0

However, the parenthetical is the Lie Bracket. Thus

[W,S]*W*s = 0

So, is the above, true?

I can show it works for any general skew symmetric system, using the symbolic manipulator in Matlab

But can someone explain why this is true?
 
Last edited:
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You need to specify the dimensions of the vectors are taken from, or the dimension of the matrices. And what is ##s## for? Did you mean ##V=S## and what does ##W,V## consists of the components of ##v,w## mean?

If the dimension is greater than two, and ##s\neq \vec{0}##, and ##W## is invertible, then ##[W,S]\neq 0## in general, i.e. for arbitrary ##S##.

Maybe you can give an example because your question is too flawed to answer.
 
fresh_42 said:
You need to specify the dimensions of the vectors are taken from, or the dimension of the matrices. And what is ##s## for? Did you mean ##V=S## and what does ##W,V## consists of the components of ##v,w## mean?

If the dimension is greater than two, and ##s\neq \vec{0}##, and ##W## is invertible, then ##[W,S]\neq 0## in general, i.e. for arbitrary ##S##.

Maybe you can give an example because your question is too flawed to answer.

The dimension of all is 3.
w is related to an angular velocity vector
s are the position vector

In the process, I derive this term that I KNOW must be zero (I just can't prove it):
W*S*W*s = S*W*W*s

I can REASON my way around it like this:

I want to prove

W*S*W*s - S*W*W*s = 0

Thus, I want to prove

(W*S-S*W)*W*s =0

However, the parenthetical is the Lie Bracket (A Commutation relationship). Thus

[W,S]*W*s = 0

OK, so v = W*s is a vector perpendicular to w and s

The Lie Bracket is a skew matrix representing a vector perpendicular to w and s

This means that [W,S] and v are parallel

Thus, their cross product must be zero

However I do not like that proof. It seems to be a lot of handwaving and too much reliance on the cross product.
 
fresh_42 said:
You need to specify the dimensions of the vectors are taken from, or the dimension of the matrices. And what is ##s## for? Did you mean ##V=S## and what does ##W,V## consists of the components of ##v,w## mean?

If the dimension is greater than two, and ##s\neq \vec{0}##, and ##W## is invertible, then ##[W,S]\neq 0## in general, i.e. for arbitrary ##S##.

Maybe you can give an example because your question is too flawed to answer.
And I apologize: there was no need for v or V. I meant s and S.

I have corrected that mistake in my original post.
 
I still have difficulties understanding it. If ##[W,S]Ws=0## and ##W## is regular, then ##[W,S]=0## but this isn't the case for arbitrary skewsymmetric matrices of dimension three. So either ##s\in \ker W## or ##Ws \in \ker [W,S].## Hence we need to look at your additional geometric conditions. However, I don't see how to apply them.
 
fresh_42 said:
I still have difficulties understanding it. If ##[W,S]Ws=0## and ##W## is regular, then ##[W,S]=0## but this isn't the case for arbitrary skewsymmetric matrices of dimension three. So either ##s\in \ker W## or ##Ws \in \ker [W,S].## Hence we need to look at your additional geometric conditions. However, I don't see how to apply them.
I am sorry for confusing you: it is my fault for lack of precision (which actually derives directly from my very confusion)

So here... I wrote a Symbolic Manipulator Matlab script. This script gives me the result of ZERO.

I now wish to prove this

---------------------------------------------------Test.m-----------------------------------
% Declare symbolic varitables to be real
syms w1 w2 w3 s1 s2 s3 v1 v2 v3 real

% Create two symbolic vectors
w = [w1;w2;w3]
s = [s1;s2;s3]

% Create their associated skew symmetric form (as if to be used in the cross product)
W =[0,-w3,w2;w3,0,-w1;-w2,w1,0]
S =[0,-s3,s2;s3,0,-s1;-s2,s1,0]

%Perform the operation
T=simplify((expand(W*S*W*s-S*W*W*s)))

I get the components of a zero vector!
I get exactly what I want.
(This is from the realm of rigid body dynamics -- nothing advanced as you would find it relativity or advanced geometric space-time, etc.)
Why?
 
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Trying2Learn said:
Thank you!

t
Maybe you can shorten the calculationn by splitting ##W=W_0+W_1\, , \,S=S_0+S_1## into upper and lower triangular matrices and use the facts that they are multiplicative closed and ##W_1=-W_0^\tau\, , \,S_1=-S_0^\tau .##
 
  • #10
fresh_42 said:
Maybe you can shorten the calculationn by splitting ##W=W_0+W_1\, , \,S=S_0+S_1## into upper and lower triangular matrices and use the facts that they are multiplicative closed and ##W_1=-W_0^\tau\, , \,S_1=-S_0^\tau .##

Actually, I found a better way.

Remember, in my problem, s and w were the vectors
S and W were the corresponding skew symmetric forms.

We already know that Ws and Sw are manifestations of the cross product.
Thus:
Ws is perpendicular to w and s
Sw is perpendicular to w and s.

Next, I investigate:
[W,S] = WS - SW

I use an alternating tensor to represent a skew symmetric form.

I find any skew symmetric form has elements such that:

Wij = -eijk wk
Sij = -eijk sk

Then I go through the process of forming
[W,S]ij = (WS - SW)ij

I find that that last form is ALSO perpendicular to w and s.

Thus,
[W,S] * Ws represents a cross product of two parallel vectors
[W,S] * Sw represents a cross product of two parallel vectors[W,S]Ws = 0
[W,S]Sw = 0

And I am done
 
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