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We know that $∂x^ρ /∂x^μ = δ^ρ_μ$

Τhen, $∂x_ρ /∂x^μ = η_{ρμ}$ Should be correct, right?

Similarly, $\frac{∂x_ρ} {∂x_μ} = δ^μ_ρ$

Also, if $x'^μ = e^α x^μ $, then
$∂'_μ$ should be $e^α ∂_μ$

I am new to this topic and I don't know if I am in the right direction. Can someone please help clarify?

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  • $\begingroup$ I can delete the post if it's not up to the requirements of posting questions $\endgroup$
    – Korra
    Commented Aug 15, 2021 at 10:28
  • $\begingroup$ Possible duplicate: physics.stackexchange.com/q/616574 $\endgroup$ Commented Aug 15, 2021 at 12:35
  • $\begingroup$ @Nihar Karve no it's not a duplicate but it was helpful. Thanks! $\endgroup$
    – Korra
    Commented Aug 15, 2021 at 13:34
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    $\begingroup$ I think the big thing here is that "taking a derivative relative to a lowered index" is a bit of a strange concept, since the coordinates are typically represented with raised indices, by convention. I'm not the downvoter, but I presume that's the reason for the downvote. I generally think downvoting without a comment or a close vote is a pretty rude thing to do. $\endgroup$ Commented Aug 15, 2021 at 14:08
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    $\begingroup$ @Jerry Schirmer as I said I am new to this and there are many such questions. $\endgroup$
    – Korra
    Commented Aug 15, 2021 at 14:11

1 Answer 1

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I am also new in this topic and a high school student, my go on this is as:

$1.$ $\displaystyle \frac {\partial x^{\rho}}{\partial x^{\mu}} = \delta_{\mu}^{\rho} $ when we say that $x^\nu$ is component of vector.


$2.$ $\displaystyle \frac {\partial \vec x_{\rho}}{\partial x^{\mu}} = \Gamma^{\nu}_{\rho \mu} \ \ \vec x_{\nu} \ $ where $ \ \displaystyle \vec x_{\nu} \ $ is Basis vectors as lower index show covariance.

Moreover, $\displaystyle \Gamma^{\nu}_{\rho \mu} = \frac {\partial^{2}}{\partial x^{\mu} \partial x^{\rho}} \cdot \partial_{j} \ g^{j\nu} $

(I may be wrong in this part cause we generally not use lowered index for components, but if it is the case : $\displaystyle \frac {\partial x_{\rho}}{\partial x^{\mu}} = g_{\rho \nu} \frac {\partial x^{\nu}}{\partial x^{\mu}} = g_{\rho \nu} \ \delta^{\nu}_{\mu} = g_{\rho \mu} $)


$3.$ $\displaystyle \widetilde {x^{\mu}} = e^{\alpha} x^{\mu} $ This shows us the contravariant old to new transform, using inverse Jacobian. Thus $\displaystyle e^{\alpha} \widetilde {\partial_{\mu}} = \partial_{\mu} $

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  • $\begingroup$ Thanks for your input! I had actually resolved this question in a chatroom. Also , the last one is $e^{-\alpha}$ $\endgroup$
    – Korra
    Commented Aug 30, 2021 at 5:24

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