GR metric gauge transformation, deduce 'generating' vector

In summary, the conversation discusses the problem of finding the value of ##C_u## when ##g_{uv}'=g_{uv}+\nabla_v C_u+\nabla_u C_v## and ##g_{uv}## is given by ##ds^2=dx^2+dy^2##. The solution involves setting ##C_u=2\epsilon(f(y),0)## and using the fact that ##g_{xx}=g'_{xx}## and ##g_{yy}=g'_{yy}## to solve for ##C_x## and ##C_y##.
  • #1
binbagsss
1,254
11
1. Problem

##g_{uv}'=g_{uv}+\nabla_v C_u+\nabla_u C_v##

If ##g_{uv}' ## is given by ##ds^2=dx^2+2\epsilon f'(y) dx dy + dy^2##
And ##g_{uv}## is given by ##ds^2=dx^2+dy^2##, Show that ## C_u=2\epsilon(f(y),0)##?

Homework Equations



Since we are in flatspace we have ##g_{uv}'=g_{uv}+\partial_v C_u+\partial_u C_v##

The Attempt at a Solution


[/B]
Since ##g_{xx}=g'_{xx}## and ##g_{yy}=g'_{yy}##

I get ##\partial_x C_x=\partial_y C_y=0##

##\implies C_x=c(y)##, ##c(y)## the constant of ##x## from integration, some function of ##y##
##C_y=k(x)## ##k(x)## some function of ##x##

From the cross term ##g_{xy}'=g_{yx}'=\epsilon f'(y)## I get:

## \epsilon f'(y)=\partial_x C_y + \partial_y C_x ##

So ## \epsilon f'(y)= k'(x) + c'(y) ##

I have no idea what to do now..

Many thanks in advance
 
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  • #2
bump please. thank you very much.
 

Related to GR metric gauge transformation, deduce 'generating' vector

What is a GR metric gauge transformation?

A GR metric gauge transformation is a mathematical tool used in general relativity to describe the behavior of spacetime under different coordinate systems. It involves changing the values of the metric tensor, which represents the curvature of spacetime, under different coordinate transformations.

What does it mean to "deduce" a generating vector in this context?

In the context of GR metric gauge transformations, deducing a generating vector means determining the vector field that generates the coordinate transformation. This vector field is used to calculate the new values of the metric tensor under the transformed coordinates.

What are the applications of GR metric gauge transformations?

GR metric gauge transformations are used in general relativity to study the curvature of spacetime and its effects on the motion of particles and objects. They are also important in cosmology, astrophysics, and other fields that involve the study of gravity and spacetime.

How do GR metric gauge transformations relate to Einstein's theory of general relativity?

Einstein's theory of general relativity is based on the idea that gravity is the curvature of spacetime. GR metric gauge transformations provide a mathematical framework for understanding this curvature and how it changes under different coordinate systems.

Can GR metric gauge transformations be applied to other theories besides general relativity?

Yes, GR metric gauge transformations can be applied to other theories that involve the study of spacetime and gravity, such as string theory and loop quantum gravity. They are a fundamental tool for understanding the behavior of spacetime in these theories.

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