Infinitesimal coordinate transformation of the metric

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SUMMARY

The discussion focuses on the infinitesimal coordinate transformation of the metric in the context of general relativity. The user encounters a sign issue when calculating the partial derivative of the coordinate transformation, specifically when transitioning from the inverse form of the transformation. The correct expression for the transformed metric is identified as ##g'_{\mu\nu}=g_{\mu\nu}-\partial_\mu \varepsilon_\nu - \partial_\nu \varepsilon_\mu##, emphasizing the importance of proper index labeling to avoid confusion and errors in calculations.

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  • Understanding of general relativity and metric tensors
  • Familiarity with coordinate transformations and partial derivatives
  • Knowledge of tensor notation and index manipulation
  • Experience with infinitesimal transformations in differential geometry
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shinobi20
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Homework Statement
The metric transforms as ##g'_{\mu\nu}(x') = \frac{\partial x^\alpha}{\partial x'^\mu} \frac{\partial x^\beta}{\partial x'^\nu} g_{\alpha\beta}(x)##. Show that under the infinitesimal transformation ##x^\alpha \rightarrow x'^\alpha = x^\alpha + \epsilon^\alpha## (##\epsilon^\alpha## is small), ##g'_{\mu\nu}(x^\mu + \epsilon^\mu) = g_{\mu\nu}(x) + (\partial_{\mu} \epsilon^\mu + \partial_{\nu} \epsilon^\nu) g_{\mu\nu}(x) = g_{\mu\nu}(x) + \partial_{\mu} \epsilon_\nu + \partial_{\nu} \epsilon_\mu##.
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I kinda know how to do this problem, it is just that I hit a sign problem. If I take the partial derivative of the coordinate transformation with respect to ##x'^\mu##, I get

writing it first in the inverse form, ##x^\alpha = x'^\alpha - \epsilon^\alpha##

##\frac{\partial x^\alpha}{\partial x'^\mu} = \delta^\alpha_\mu - \partial'_\mu \epsilon^\alpha = \delta^\alpha_\mu - \frac{\partial x^\alpha}{\partial x'^\mu} \partial_\alpha \epsilon^\alpha##

transposing terms,

##\frac{\partial x^\alpha}{\partial x'^\mu} (1 + \partial_\alpha \epsilon^\alpha) = \delta^\alpha_\mu##

##\frac{\partial x^\alpha}{\partial x'^\mu} \approx \delta^\alpha_\mu - \delta^\alpha_\mu \partial_\alpha \epsilon^\alpha \quad## (to first order)

Now this is going to give me a minus sign instead of a plus sign in the right hand side of the equation to be shown. Did I do something wrong?
 
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Mmm... I'm not sure, but maybe you're right and should be ##g'_{\mu\nu}=g_{\mu\nu}-\partial_\mu \varepsilon_\nu - \partial_\nu \varepsilon_\mu##.
But in any case, be very careful in how you label the indices, in more than one expression you give the same symbol to different indices, what can lead to errors or, at least, to confuse the people who are trying to read it.
 

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