Skip to main content
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