Special & General Relativity: CTC Metrics in Cylindrical Coordinates

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SUMMARY

This discussion focuses on the conversion of metrics exhibiting Closed Timelike Curves (CTCs) into cylindrical coordinates, specifically examining the Tipler, Godel, and Kerr metrics. The Godel metric's coordinate transformation is expressed as ##x^{\alpha}=(t, r\cos{\phi}, r\sin{\phi}, z)##, while its cylindrical metric components are detailed as ##g_{t,t}=c^2##, ##g_{r,r}=1/(1+(r/2a)^2)##, and ##g_{\phi,\phi}=-r^2(1-(r/2a)^2)##. The Tipler cylinder metric is represented as ##ds^2 = H(dr^2+ dz^2 ) + Ldϕ^2 + 2Mdϕdt − Fdt^2##. The discussion also touches on the relationship between the Kerr metric and the Tipler cylinder, particularly regarding the conditions under which CTCs may arise.

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  • Knowledge of CTCs and their implications in spacetime
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YRC
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I am studying metrics that exhibit CTCs. I was looking at a few different metrics...
Tipler's solution
Godel metric
Kerr metric
For starters to compare them, I am trying to convert said metrics into cylindrical coordinates. Thanks in advance for any help😃
 
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YRC said:
I am trying to convert said metrics into cylindrical coordinates.
What have you found in sources that you have looked at? For the last two, at any rate, it should be easy to find expressions for the metrics in cylindrical coordinates.
 
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PeterDonis said:
What have you found in sources that you have looked at? For the last two, at any rate, it should be easy to find expressions for the metrics in cylindrical coordinates.
I understand that the coordinate transform for the Godel metric would look like this, ##x^{\alpha}=(t, x, y, z)=(t, r\cos{\phi}, r\sin{\phi}, z)## for cartesian and cylindrical coordinates. The cylindrical metric itself is given by ##g_{t,t}=c^2##,##g_{r,r}=1/(1+(r/2a)^2)##, ##g_{\phi,\phi}= -r^2(1-(r/2a)^2)##, ##g_{z,z}=-1## and ##g_{t,\phi}=r^2*c/(\sqrt{2}a), g_{\phi,t}=r^2*c/(\sqrt{2}a)## right? That's what I found for Godel, For the Tipler cylinder I found it in cylindrical coordinates... ds^2 = H(dr^2+ dz^2 ) + Ldϕ^2 + 2Mdϕdt − Fdt^2 , What about the Kerr metric that is commonly expressed in Boyer-Lindquist coordinates?

Mentors' note: The Latex was posted without the required delimiters. We've edited in the delimiters but have not otherwise cleaned up the formatting. OP, would you please finish this cleanup?
 
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YRC said:
I am studying metrics that exhibit CTCs.
I don't know if this helps, but any (locally Minkowski) metric can exhibit CTC. For example the flat metric
$$ds^2=dt^2-dx^2$$
contains CTC's if we interpret it as a spacetime with cylindrical topology in which ##t## and ##t+2\pi## are identified. The point is that cylinder admits a flat metric, so when we say that the metric is flat, we have not excluded a possibility that it is a cylinder.

EDIT: It's not valid for any metric, but it's valid for any metric with timelike Killing vector.
 
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Demystifier said:
I don't know if this helps, but any (locally Minkowski) metric can exhibit CTC. For example the flat metric
$$ds^2=dt^2-dx^2$$
contains CTC's if we interpret it as a spacetime with cylindrical topology in which ##t## and ##t+2\pi## are identified. The point is that cylinder admits a flat metric, so when we say that the metric is flat, we have not excluded a possibility that it is a cylinder.
Yes thanks, the Tipler cylinder metric does reduce to the Minkowski line element in cylindrical coordinates when the angular velocity is 0. I was wondering about using the Kerr metric to describe the exterior of the rotating Tipler cylinder. How would that work? Would that work? In a configuration where we have a metric describing the negative energy density required, and this exterior, would CTCs arise in a confined region bounded by the cylinder?
 

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