Tensor determinant using box product

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Homework Help Overview

The discussion revolves around demonstrating properties of the determinant of a tensor using index notation, specifically focusing on two parts: (a) relating the determinant to a product involving the Levi-Civita symbol and (b) expressing the determinant in terms of specific indices. The subject area is linear algebra and tensor calculus.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the application of index notation and the implications of manipulating the Levi-Civita symbol in relation to the determinant. There is an exploration of how to transition from part (a) to part (b) and the challenges associated with the indices involved.

Discussion Status

Some participants have provided insights into the manipulation of the Levi-Civita symbol and the limitations of standard algebraic techniques in this context. There is recognition of a simpler approach to the problem, although no consensus has been reached on the exact method to proceed.

Contextual Notes

Participants note the complexity of the indices and the summation involved, which complicates direct manipulation. There is also mention of the time spent on the problem, indicating a level of difficulty in understanding the transition between the two parts of the question.

hotvette
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Homework Statement


Using index notation only (i.e. don't expand any sums) show that:
\begin{align*}
&\text{(a) } \epsilon_{ijk} \det \underline{\bf{A}} = \epsilon_{mnp} A_{mi} A_{nj} A_{pk} \\
& \text{(b) } \det \underline{\bf{A}} = \epsilon_{mnp} A_{m1} A_{n2} A_{p3}
\end{align*}

Homework Equations



\begin{align*}
&\text{(1) }\epsilon_{ijk} \det \underline{\bf{A}} = [\underline{\bf{A}} \underline{e}_i, \underline{\bf{A}} \underline{e}_j, \underline{\bf{A}} \underline{e}_k] \\
& \text{(2) } \underline{\bf{A}} = A_{ij} \underline{e}_i \otimes \underline{e}_j \\
& \text{(3) } \underline{\bf{A}} \underline{e}_j= (A_{pq} \underline{e}_p \otimes \underline{e}_q)\underline{e}_j
= (\underline{e}_q \cdot \underline{e}_j) A_{pq} \underline{e}_p = \delta_{qj} A_{pq} \underline{e}_p = A_{pj} \underline{e}_p
\end{align*}

The Attempt at a Solution


I got part (a) by using (3) for each term of the box product, substituting each of those expressions into the box product, and evaluating.

What baffles me is (b). If I multiply \epsilon_{ijk} times (b) and compare to (a), the net result is:
\begin{align*}
&\epsilon_{mnp} (\epsilon_{ijk} A_{m1} A_{n2} A_{p3}) = \epsilon_{mnp} (A_{mi} A_{nj} A_{pk}) \\
& \epsilon_{ijk} A_{m1} A_{n2} A_{p3} = A_{mi} A_{nj} A_{pk}
\end{align*}

But I have no idea what to do with that (the indices look really goofy). Any tips?
 
Last edited:
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hotvette said:
\begin{align*}
&\epsilon_{mnp} (\epsilon_{ijk} A_{m1} A_{n2} A_{p3}) = \epsilon_{mnp} (A_{mi} A_{nj} A_{pk}) \\
& \epsilon_{ijk} A_{m1} A_{n2} A_{p3} = A_{mi} A_{nj} A_{pk}
\end{align*}
You can't go from the first line to the second line by dividing by ##\epsilon_{mnp}## throughout - because there is an summation involved.

To arrive at (b) from (a), consider the value of ##\epsilon_{123}## :wink:
 
Ah, thanks. I was applying standard algebra techniques, which I now see is a mistake. Gosh, the answer is soooooo simple! Thanks.

P.S. I'd fiddled with this thing for probably 2 hours. At one point I was on the right track by looking at how to eliminate \epsilon_{ijk} from (a) to isolate the determinant. I thought about multiplying both sides by \epsilon_{ijk} to get 6 \det(A) = xxx but that didn't look promising. Drat!
 
Last edited:
Haha, I guess the trick is to realize that the only way you can have explicit labels such as 1,2 and 3 appearing in the indices is by setting them to be so - multiplying by other stuff with arbitrary indices can never give you specific indices.
 

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