Metric Form of ##g_{μν}## - Solving a Challenge

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In summary, the equation states that the sum of the squares of the differences of the angles between two vectors is equal to the sum of the squares of the vectors themselves.
  • #1
hykhor0601
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Does anyone know how to solve this?
##ds^2=g_{μν}(x)dx^μdx^ν= -(r^6/l^6)[1-(Ml^2/r^2)]dt^2+{1/[(r^2/l^2)-M]}dr^2+r^2dΦ^2##

Does anyone know how to solve this?
 
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  • #2
What do you mean by "solve"? There is nothing to "solve", there is just a line-element.
 
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  • #3
Solve in what sense? It appears to be just a statement of a metric, missing a definition of ##l## and assuming ##d\Phi## is a solid angle element.
 
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  • #4
Can you provide some context here? Where di this equation come from? What book course etc...?

and what have you tried so far?

We had to modify your equation using Latex to make it readable:
ds^2=gμν(x)dx^μdx^ν= -(r^6/l^6)[1-(Ml^2/r^2)]dt^2+{1/[(r^2/l^2)-M]}dr^2+r^2dΦ^2

Basically the changes were to bracket the equation on both sides with double # and to replace the gμν with g_{μν} to make them into subscripts.
 
  • #5
jedishrfu said:
Can you provide some context here? Where di this equation come from? What book course etc...?

and what have you tried so far?

We had to modify your equation using Latex to make it readable:Basically the changes were to bracket the equation on both sides with double # and to replace the gμν with g_{μν} to make them into subscripts.
https://arxiv.org/pdf/0909.1347.pdf The metric is given in (9)
 
  • #6
Ibix said:
Solve in what sense? It appears to be just a statement of a metric, missing a definition of ##l## and assuming ##d\Phi## is a solid angle element.
The conditions is in the article below, please help me
https://arxiv.org/pdf/0909.1347.pdf
 
  • #7
hykhor0601 said:
The conditions is in the article below, please help me
https://arxiv.org/pdf/0909.1347.pdf
This still does not answer the question you have been asked about what you mean by ”solve”.
 
  • #8
∂∨μ[(√-g)g∨μν∂∨ν(Φ)]-m^2√(-g)Φ=0
What is the meaning of ∂∨μ,√-g,∂∨ν(Φ) in this equation?

How to give the form of g^μν from the metric (9) in the article?(or how do i get the form of ∂∨μ[(√-g)g∨μν∂∨ν(Φ)]-m^2√(-g)Φ=0 )
https://arxiv.org/pdf/0909.1347.pdf
Please help me, thank you
 
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  • #9
hykhor0601 said:
The conditions is in the article below, please help me
https://arxiv.org/pdf/0909.1347.pdf
Again, what do you mean by "solve"? The metric is not a thing you solve. What are you trying to find out?
 
  • #10
Why are you interested in this particular paper if you are not familiar with basics of general relativity?
 
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  • #11
Ibix said:
Again, what do you mean by "solve"? The metric is not a thing you solve. What are you trying to find out?
just the form of gμν that can be sub into the equation of motion
 
  • #12
hykhor0601 said:
just the form of gμν that can be sub into the equation of motion
You already have ##g_{\nu\nu}##. What is your actual problem?
 
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  • #13
Orodruin said:
You already have ##g_{\nu\nu}##. What is your actual problem?
can you write it in the form after substitude into
∂µ[√ (−g)gµν∂ν(ϕ) ]− m^2√ (−g)ϕ = 0
 
  • #14
I don't understand. You can read off the components of ##g_{\mu\nu}## from the line element and ##g## is just its determinant. Where's the difficulty?

It would also help immensely if you spent a few minutes reading the LaTeX Guide linked below the reply box. Then you could type maths in a way that we could actually read it.
 
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FAQ: Metric Form of ##g_{μν}## - Solving a Challenge

What is the metric form of ##g_{μν}##?

The metric form of ##g_{μν}## is a mathematical representation of the spacetime geometry in the theory of general relativity. It describes the curvature of spacetime and is used to calculate the path of a particle in a gravitational field.

How is the metric form of ##g_{μν}## solved?

The metric form of ##g_{μν}## is solved by using Einstein's field equations, which relate the curvature of spacetime to the distribution of matter and energy. These equations are solved using various mathematical techniques, such as tensor calculus and differential geometry.

What challenges are involved in solving the metric form of ##g_{μν}##?

One of the main challenges in solving the metric form of ##g_{μν}## is the complexity of the equations involved. They require a deep understanding of advanced mathematical concepts and can be difficult to solve without the use of powerful computers. Additionally, the equations may have multiple solutions, making it necessary to carefully analyze and interpret the results.

What are some real-world applications of the metric form of ##g_{μν}##?

The metric form of ##g_{μν}## has many important applications in physics and astronomy. It is used to study the behavior of objects in strong gravitational fields, such as black holes. It also plays a crucial role in the development of technologies like GPS, which rely on accurate measurements of spacetime curvature.

How does the metric form of ##g_{μν}## relate to the theory of general relativity?

The metric form of ##g_{μν}## is a fundamental concept in the theory of general relativity. It is one of the key components of Einstein's theory, which describes the relationship between matter and spacetime. The metric form of ##g_{μν}## is used to calculate the curvature of spacetime, which is essential for understanding the behavior of objects in the presence of gravity.

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