Given a basis $\displaystyle \beta$ for $\displaystyle V$ define $\displaystyle \det(T) = \det([T]_\beta)$. Prove that the definition is independent of choice of an ordered basis for V (i.e. if $\displaystyle \beta$ and $\displaystyle \gamma$ are ordered basis for $\displaystyle V$ then $\displaystyle \det([T]_\beta) = \det([T]_\gamma)$).

I don't have much in the form of a proof. I tried working out an example but it got me nowhere. So what I have as an example is:

let $\displaystyle T(a,b) = (a+b,a-2b)$ and $\displaystyle \beta=\{(1,0), (0,1)\} \ \gamma = \{(1,2),(1,-1)\}$ then under the transformation we have

$\displaystyle [T]_\beta = \begin{pmatrix} 1 & 1 \\ 1 & -2 \end{pmatrix}$ where $\displaystyle \det[T]_\beta = -3$

and for

$\displaystyle [T]_\gamma= \begin{pmatrix} 0 & 3 \\ 1 & -1 \end{pmatrix}$ where $\displaystyle \det[T]_\gamma= -3$

where $\displaystyle [T]_\gamma= \begin{pmatrix} 0 & 3 \\ 1 & -1 \end{pmatrix}$ was obtained by $\displaystyle [T]_\gamma^\beta= \begin{pmatrix} 3 & -3 \\ 0 & 3 \end{pmatrix}$ and $\displaystyle [\hat{T}] = \frac{1}{3} (a+b,2a-b)$ which gives the desired result.

Now I'm thinking it has something with the eigenvalues and corresponding eigenvectors but that got nowhere, since I'm not to sure on how to proceeds.