Adjoint transformation (inverse)

mnb96
Messages
711
Reaction score
5
Hi,
in the text I am reading I found the following implicit definition of an adjoint transformation:

\overline{f}( \textbf{a}) \ast \textbf{b} = \textbf{a} \ast f(\textbf{b})

then it is said that \overline{f^{-1}} = (\overline{f})^{-1}. Basically the inverse and ajoint are interchangeable, and this property is (supposed to be) easily shown from the definition above.
Unfortunately I have problems figuring out how to prove it. Any ideas?
 
Physics news on Phys.org
it's been a really long time since i did anything math related, but i think if you * the inverse of everything to both sides (i.e. step 1, * (f^bar(a))^-1 to both sides, step 2 * b^1 to both sides, step 3 * a^1 to both sides, step 4 * (f(b))^-1 to both sides) you should end up with

<br /> \textbf{a}^{-1} \ast f(\textbf{b})^{-1} = \textbf{b}^{-1} \ast \overline{f}( \textbf{a})^{-1}<br />

does that give you what you want? sorry, it's been a long time since I've done this type of stuff. i think this is probably wrong, but it may give you a step in the right direction.
 
When you say, step1 * f^bar(a))^-1 to both sides do you mean the following?

\overline{f}\\^{-1}(\textbf{a}) \ast \overline{f}( \textbf{a}) \ast \textbf{b} = \overline{f}\\^{-1}(\textbf{a}) \ast \textbf{a} \ast f(\textbf{b})<br />
 
actually i meant this:

<br /> (\overline{f}\\(\textbf{a}))^{-1} \ast \overline{f}( \textbf{a}) \ast \textbf{b} = (\overline{f}\\(\textbf{a}))^{-1} \ast \textbf{a} \ast f(\textbf{b})<br /> <br />

i'm not that great with latex, or i would have tried to explain it better; my apologies. i think the equation in my post is actually incorrect now that i look at it, but if you follow the method i described i think it gets you somewhere.

after you simplify you get

<br /> \textbf{b} = (\overline{f}\\(\textbf{a}))^{-1} \ast \textbf{a} \ast f(\textbf{b})<br /> <br />

and then you continue to * inverses on both sides (i don't want to say multiply because * is an operator not always multiplication... is there a better word for that?)
 
I found a solution when the operation * is cancellative (which I can assume to be my case):

\overline{f^{-1}}(a) * f(b) = a * f^{-1}(f(b)) = a * b = \overline{f}(\overline{f}^{-1}(a)) * b = \overline{f}^{-1}(a) * f(b)

However if you check from wikipedia http://en.wikipedia.org/wiki/Hermitian_adjoint#Properties this seems to be a property of linear operators, but I wonder how you can prove it without assuming cancellativity (y*x = z*x \\ \Rightarrow \\ y=z)
 
Thread 'Derivation of equations of stress tensor transformation'
Hello ! I derived equations of stress tensor 2D transformation. Some details: I have plane ABCD in two cases (see top on the pic) and I know tensor components for case 1 only. Only plane ABCD rotate in two cases (top of the picture) but not coordinate system. Coordinate system rotates only on the bottom of picture. I want to obtain expression that connects tensor for case 1 and tensor for case 2. My attempt: Are these equations correct? Is there more easier expression for stress tensor...
Back
Top