Special & General Relativity: CTC Metrics in Cylindrical Coordinates

In summary: The Kerr metric is not valid for describing the exterior of the rotating Tipler cylinder, but it is valid for describing the negative energy density required.
  • #1
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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  • #2
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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  • #3
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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  • #5
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?
 

FAQ: Special & General Relativity: CTC Metrics in Cylindrical Coordinates

What are CTC metrics in the context of relativity?

CTC stands for Closed Time-like Curves, which are solutions to the equations of general relativity that allow for paths through spacetime that loop back on themselves. In the context of relativity, CTC metrics describe the geometrical structure of spacetime that permits these closed paths, enabling the possibility of time travel to the past.

How are cylindrical coordinates used in CTC metrics?

Cylindrical coordinates provide a convenient way to describe systems with cylindrical symmetry. In the context of CTC metrics, cylindrical coordinates allow for the analysis of spacetime geometries that exhibit this symmetry, such as rotating black holes or certain cosmological models, making it easier to derive and understand the properties of CTCs in those geometries.

What are the implications of CTCs for causality in physics?

CTCs challenge the conventional understanding of causality, as they allow for scenarios where an event can be both a cause and an effect of itself. This raises questions about the consistency of physical laws, the nature of time, and the possibility of paradoxes, such as the famous "grandfather paradox," where a time traveler could potentially prevent their own existence.

Are CTCs physically realizable in our universe?

While CTCs are mathematically valid solutions in general relativity, their physical realizability is still a matter of debate. Many physicists believe that the conditions required for CTCs, such as exotic matter with negative energy density, may not exist in our universe. Additionally, quantum mechanics may impose restrictions that prevent the formation of CTCs, thus preserving causality.

What are some examples of CTC metrics in cylindrical coordinates?

One well-known example of a CTC metric in cylindrical coordinates is the Gödel metric, which describes a rotating universe that permits closed time-like curves. Other examples include certain solutions involving rotating black holes, such as the Kerr solution, when expressed in cylindrical coordinates, which can also exhibit CTCs under specific conditions.

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