Timeline for Correct order for tensor operations, when expressed in matrix form
Current License: CC BY-SA 4.0
7 events
when toggle format | what | by | license | comment | |
---|---|---|---|---|---|
Jan 11 at 12:03 | vote | accept | Tiago | ||
Jan 11 at 10:49 | comment | added | basics | I performed the product you need in the edit at the end of the answer. Now, you should easily realize that the "lq" component of the 2-nd order tensor $\eta \hspace{-4pt} \eta \cdot \mathbb{A} \cdot \eta \hspace{-4pt} \eta $ is $ \eta_{li} A^{ik} \eta_{kq}$, and thus this should solve your doubts. | |
Jan 11 at 10:47 | history | edited | basics | CC BY-SA 4.0 |
added 970 characters in body
|
Jan 11 at 10:38 | comment | added | basics | Try to compute $\mathbb{B} \cdot \mathbb{A}$ with the notation I used above. And then try to compute $\eta \hspace{-4pt} \eta \cdot \mathbb{A} \cdot \eta \hspace{-4pt} \eta$ and compare it with $\eta \hspace{-4pt} \eta\cdot \eta \hspace{-4pt} \eta \cdot \mathbb{A} $ or any other combination you like | |
Jan 11 at 9:22 | comment | added | Tiago | This does not explain why the right order is $(A_{\alpha\beta}) = (\eta_{\alpha\mu})(A^{\mu\nu})(\eta_{\nu\beta})$. | |
Jan 10 at 20:08 | comment | added | basics | In the answer above, the vectors $\mathbf{b}^j$ are vectors of the reciprocal base of the base $\mathbf{b}_i$, defined as $\mathbf{b}^j \cdot \mathbf{b}_i = \delta_i^j$, so that it's easier to evaluate the dot product. | |
Jan 10 at 20:06 | history | answered | basics | CC BY-SA 4.0 |