Did I Make a Mistake in Finding the Determinant of an Orthogonal 2x2 Matrix?

Click For Summary

Discussion Overview

The discussion revolves around the properties and determinant of orthogonal 2x2 matrices, specifically focusing on the derivation of their general form and the implications of their determinants. Participants explore various mathematical approaches and relationships between the elements of the matrix.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • One participant proposes that the general form of an orthogonal 2x2 matrix can be expressed as $ \begin{bmatrix}a&b\\c&d\end{bmatrix}$ and notes that the determinant must be $\pm 1$.
  • Another participant corrects a mathematical expression regarding the inverse of the matrix, suggesting that there may have been a mistake in the signs used.
  • There is a discussion about the relationships between the elements of the matrix, with one participant stating that $d = a$, $-c = b$, and $-b = c$, leading to a determinant condition of $|A| = 1$.
  • One participant expresses confusion about the signs of $c$ and $d$, indicating that they expected $c = -\sin \theta$ and $d = \cos \theta$.
  • Another participant provides a solution for the matrix $A$ in terms of sine and cosine, noting that the solutions can vary based on the signs of the sine and cosine terms.
  • There is a mention of comparing the derived matrix with the standard 2D rotation matrix, which is a common form of orthogonal matrices.
  • A participant introduces the equation $A \times A^T = I$ (identity matrix) and derives additional conditions, such as $ac + bd = 0$, suggesting that if $a$ and $b$ are positive, one of $c$ or $d$ must be negative.

Areas of Agreement / Disagreement

Participants express differing views on the correct signs for the elements of the orthogonal matrix, particularly regarding $c$ and $d$. There is no consensus on the resolution of these discrepancies, and multiple interpretations of the determinant and matrix properties remain present.

Contextual Notes

The discussion includes various assumptions about the definitions of the matrix elements and the conditions under which the determinant is evaluated. Some mathematical steps remain unresolved, particularly regarding the implications of the determinant being $\pm 1$ and the relationships between the matrix elements.

ognik
Messages
626
Reaction score
2
Find the general form of an orthogonal 2 x 2 matrix = $ \begin{bmatrix}a&b\\c&d\end{bmatrix}$

I used $det(A)=\pm 1$ (from an earlier exercise) - and the special form of $ A_{2 \times 2}^{-1} = \frac{ \begin{bmatrix}d&-b\\-c&a\end{bmatrix}}{|A|} $ using $|A| = +1$ first, to get an 'alternative' $ A = \left(A^{-1}\right)^T = \begin{bmatrix}d&-c\\-b&a\end{bmatrix}$

This gave me $ a=Cos\theta, b=Sin \theta $ as expected so far.

But if I do something similar for c and d I get $ c=Cos\theta, d=Sin \theta $, which can't be right 'cos that would be singular.

So using |A| = -1, I get a 2nd 'alternate' $A = -\begin{bmatrix}d&-c\\-b&a\end{bmatrix} = \begin{bmatrix}-d&c\\-b&a\end{bmatrix} $ This is clearly wrong, but can't see what I've done wrong?
 
Physics news on Phys.org
Uhh...$-\begin{bmatrix}d&-c\\-b&a\end{bmatrix} = \begin{bmatrix}-d&c\\b&-a\end{bmatrix}$
 
ognik said:
Find the general form of an orthogonal 2 x 2 matrix = $ \begin{bmatrix}a&b\\c&d\end{bmatrix}$

I used $det(A)=\pm 1$ (from an earlier exercise) - and the special form of $ A_{2 \times 2}^{-1} = \frac{ \begin{bmatrix}d&-b\\-c&a\end{bmatrix}}{|A|} $ using $|A| = +1$ first, to get an 'alternative' $ A = \left(A^{-1}\right)^T = \begin{bmatrix}d&-c\\-b&a\end{bmatrix}$
Stop it here.
[math]A = \left ( A^{-1} \right )^T[/math]

[math]\left ( \begin{matrix} a & b \\ c & d \end{matrix} \right ) = \left ( \begin{matrix} d & -c \\ -b & a \end{matrix} \right )[/math]

So by comparison we know that d = a, -c = b, -b = c, a = d. And |A| = 1. That will give you the rest.

-Dan
 
Deveno said:
Uhh...$-\begin{bmatrix}d&-c\\-b&a\end{bmatrix} = \begin{bmatrix}-d&c\\b&-a\end{bmatrix}$
You mean Duh - I was stuck in Det mode :-)
 
topsquark said:
Stop it here.
[math]A = \left ( A^{-1} \right )^T[/math]

[math]\left ( \begin{matrix} a & b \\ c & d \end{matrix} \right ) = \left ( \begin{matrix} d & -c \\ -b & a \end{matrix} \right )[/math]

So by comparison we know that d = a, -c = b, -b = c, a = d. And |A| = 1. That will give you the rest.

-Dan
That gave me $ Det\left ( \begin{matrix} d & -c \\ c & d \end{matrix} \right ) = d^2 + c^2 = 1, ie \:c=Sin \theta etc \:$
But I know the 2nd row of A should be $c=-Sin \theta, d= Cos \theta $
 
topsquark said:
Stop it here.
[math]A = \left ( A^{-1} \right )^T[/math]

[math]\left ( \begin{matrix} a & b \\ c & d \end{matrix} \right ) = \left ( \begin{matrix} d & -c \\ -b & a \end{matrix} \right )[/math]

So by comparison we know that d = a, -c = b, -b = c, a = d. And |A| = 1. That will give you the rest.

-Dan

ognik said:
That gave me $ Det\left ( \begin{matrix} d & -c \\ c & d \end{matrix} \right ) = d^2 + c^2 = 1, ie \:c=Sin \theta etc \:$
But I know the 2nd row of A should be $c=-Sin \theta, d= Cos \theta $
d = a, -c = b implies [math]A = \left ( \begin{matrix} a & b \\ -b & a \end{matrix} \right )[/math] and |A| = 1.

From the determinant we get [math]|A| = a^2 + b^2 = 1[/math].

The solutions for A are:
[math]\left ( \begin{matrix} \pm sin( \theta ) & \pm cos( \theta ) \\ \mp cos(\theta) & \pm sin(\theta) \end{matrix} \right )[/math]

and
[math]\left ( \begin{matrix} \pm cos( \theta ) & \pm sin( \theta ) \\ \mp sin(\theta) & \pm cos(\theta) \end{matrix} \right )[/math]
where the choice of [math]\pm[/math] on the sines is independent of the [math]\pm[/math] on the cosines.

-Dan
 
that makes sense of course, so I wonder why my book said to compare the answer with the 2-D rotation matrix?

So I was looking for something that would give that...
 
ognik said:
that makes sense of course, so I wonder why my book said to compare the answer with the 2-D rotation matrix?

So I was looking for something that would give that...
Given any number of definitions of your x and y axes they are all rotation matrices. Note that
[math]\left ( \begin{matrix} cos( \theta) & -sin( \theta ) \\ sin( \theta) & cos(\theta) \end{matrix} \right )[/math]
is the "usual" rotation matrix.

-Dan
 
I think I found what I was looking for... $A \times A^T$ = identity matrix. Solving gives 2 equations - we already knew $ a^2 + b^2 =1 $, but we also get ac + bd = 0, ac = -bd which tells me that if a and b are positive one of c or d must be negative. This way there is also no doubt about using $A^{-1}$ as 1 or -1 and its a simpler solution (assuming I got it right)
 

Similar threads

  • · Replies 33 ·
2
Replies
33
Views
2K
  • · Replies 1 ·
Replies
1
Views
4K
  • · Replies 5 ·
Replies
5
Views
2K
  • · Replies 24 ·
Replies
24
Views
3K
  • · Replies 10 ·
Replies
10
Views
3K
  • · Replies 13 ·
Replies
13
Views
3K
  • · Replies 8 ·
Replies
8
Views
3K
  • · Replies 12 ·
Replies
12
Views
2K
  • · Replies 7 ·
Replies
7
Views
3K
  • · Replies 1 ·
Replies
1
Views
2K