Parallel transport and geodecics

In summary: Is this what you were looking for?Yes, but since parallel transport also preserves the dot product I think that you could probably generalize it to arbitrary vectors.
  • #1
Kidphysics
164
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So from what I understand if you pass a vector (using parallel transport) through a closed curve where there is curvature in the interior, the vector will come back not to it's original vector but with a changed sense. However if the vector is on a geodesic it will not change its sense after it gets parallel transported but isn't this a contradiction (since it's a closed curve with curvature in the interior) or is this just the definition of a geodesic?
 
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  • #2
Kidphysics said:
So from what I understand if you pass a vector (using parallel transport) through a closed curve where there is curvature in the interior, the vector will come back not to it's original vector but with a changed sense. However if the vector is on a geodesic it will not change its sense after it gets parallel transported but isn't this a contradiction (since it's a closed curve with curvature in the interior) or is this just the definition of a geodesic?

I don't think it is possible to have a closed curve geodesic, since a geodesic is a world line for a particle in free fall. You can form a closed curve comprised of segments of geodesics, and if you parallel transport around one of these, the vector will change its sense.

Chet
 
  • #3
Chestermiller said:
I don't think it is possible to have a closed curve geodesic, since a geodesic is a world line for a particle in free fall. You can form a closed curve comprised of segments of geodesics, and if you parallel transport around one of these, the vector will change its sense.

Chet
I think kidphysics is thinking of the often quoted example of transporting a vector along a great circle around a sphere which is an analogy to a geodesic.
 
  • #4
Kidphysics said:
So from what I understand if you pass a vector (using parallel transport) through a closed curve where there is curvature in the interior, the vector will come back not to it's original vector but with a changed sense. However if the vector is on a geodesic it will not change its sense after it gets parallel transported but isn't this a contradiction (since it's a closed curve with curvature in the interior) or is this just the definition of a geodesic?

A geodesic parallel transports its own tangent vector, [itex]\triangledown _{\mathbf{U}}\mathbf{U} = 0[/itex]; nothing is being said about arbitrary vectors being transported along the curve.
 
  • #5
WannabeNewton said:
A geodesic parallel transports its own tangent vector, [itex]\triangledown _{\mathbf{U}}\mathbf{U} = 0[/itex]; nothing is being said about arbitrary vectors being transported along the curve.
Yes, but since parallel transport also preserves the dot product I think that you could probably generalize it to arbitrary vectors.
 
  • #6
DaleSpam said:
Yes, but since parallel transport also preserves the dot product I think that you could probably generalize it to arbitrary vectors.
Yes indeed it does but generalize what sorry?
 
  • #7
yuiop said:
I think kidphysics is thinking of the often quoted example of transporting a vector along a great circle around a sphere which is an analogy to a geodesic.

yes this is what I was referencing sorry for not including this. So this was during a susskind lecture and he was saying that if you parallel transport a vector along the geodesic then it returns full circle and is not displaced by any angle. I assume this is just a property of geodesics they are the only closed paths which has curvature in the interior such that when a vector is parallel transported along that closed path it is invariant to changing orientation. I was just looking for an affirmative.
 
  • #8
WannabeNewton said:
Yes indeed it does but generalize what sorry?
If a closed geodesic parallel transports its own tangent vector then it must parallel transport all other vectors also since it preserves the dot product also, right?
 
  • #9
Kidphysics said:
yes this is what I was referencing sorry for not including this. So this was during a susskind lecture and he was saying that if you parallel transport a vector along the geodesic then it returns full circle and is not displaced by any angle. I assume this is just a property of geodesics they are the only closed paths which has curvature in the interior such that when a vector is parallel transported along that closed path it is invariant to changing orientation. I was just looking for an affirmative.
It is true for geodesics on a sphere, but I am not sure that it is true in other manifolds.
 
  • #10
Kidphysics said:
yes this is what I was referencing sorry for not including this. So this was during a susskind lecture and he was saying that if you parallel transport a vector along the geodesic then it returns full circle and is not displaced by any angle. I assume this is just a property of geodesics they are the only closed paths which has curvature in the interior such that when a vector is parallel transported along that closed path it is invariant to changing orientation. I was just looking for an affirmative.

DaleSpam said:
It is true for geodesics on a sphere, but I am not sure that it is true in other manifolds.

I don't think so. Try a closed geodesic path on a cone that encloses the apex.
 
  • #11
A.T. said:
a closed geodesic path on a cone that encloses the apex.
Is there such a geodesic on a cone? I didn't think that a cone had any closed geodesics, but I must admit that I am having trouble visualizing it for sure. I am definitely less confident about this than most of my posts.
 
  • #12
DaleSpam said:
If a closed geodesic parallel transports its own tangent vector then it must parallel transport all other vectors also since it preserves the dot product also, right?

Well the geodesic will maintain [itex]\triangledown _{\mathbf{U}}g(U,U) = 0[/itex], with [itex]\mathbf{U}[/itex] being the tangent to the geodesic, but I'm not seeing why this or the definition of the geodesic would imply [itex]\triangledown _{\mathbf{U}}\mathbf{V} = 0[/itex] for some arbitrary vector [itex]\mathbf{V}[/itex]. I'm probably missing something so I apologize in advance.
 
  • #13
No need to apologize, I am not confident that I am right either.
 
  • #14
Chestermiller said:
I don't think it is possible to have a closed curve geodesic, since a geodesic is a world line for a particle in free fall.

A *timelike* geodesic is, yes. And a null geodesic is a world line for a light ray in "free fall" (i.e., no waveguides or other stuff present). But there are also spacelike geodesics. Those can be closed if the manifold is curved. For example, yuiop gave the example of a great circle on a sphere.

(There are spacetimes, such as the Godel universe, where there are closed timelike curves; but I'm not sure whether those curves can be geodesics. I think they can, but I'm not positive.)

A.T. said:
I don't think so. Try a closed geodesic path on a cone that encloses the apex.

The apex is a singularity of the manifold; I believe there is a theorem that says parallel transport around a closed geodesic brings all vectors back to the same vectors, but only if the closed geodesic doesn't enclose a singularity.
 
  • #15
DaleSpam said:
No need to apologize, I am not confident that I am right either.

Sorry, I was thinking of segments of geodesics being connected together to form a closed loop. But yeah for a single closed geodesic I agree with what you said before.
 
  • #16
DaleSpam said:
Is there such a geodesic on a cone? I didn't think that a cone had any closed geodesics
If the opening angle is less than 60° it has closed geodesics around the apex.
PeterDonis said:
The apex is a singularity of the manifold
Replace the pointy tip with a small spherical dome. Or simply look at the geodesics on an ellipsoid of revolution.
 
  • #17
A.T. said:
If the opening angle is less than 60° it has closed geodesics around the apex.
Cool, I didn't know that.
 
  • #18
DaleSpam said:
Cool, I didn't know that.
Me neither. I figured it out after you questioned it. So better check it. It seems that the direction change after a loop around the apex is:

2*pi*sin(opening_angle / 2)
 
  • #19
The surface of a cone is metrically equivalent to flat space. A cone is flat space with a sector removed and the two "edges" glued together. The geodesics on it are straight lines. It will be possible to have a geodesic that hits both "edges" if and only if the sector you removed is greater than 180o, and if so, it will go all the way around.
 
  • #20
Bill_K said:
The surface of a cone is metrically equivalent to flat space. A cone is flat space with a sector removed and the two "edges" glued together. The geodesics on it are straight lines. It will be possible to have a geodesic that hits both "edges" if and only if the sector you removed is greater than 180o, and if so, it will go all the way around.
That was my idea too. And if you remove more than 270° it will go all the way around twice, right?
 
  • #21
Bill_K said:
It will be possible to have a geodesic that hits both "edges" if and only if the sector you removed is greater than 180o, and if so, it will go all the way around.
Yes, but I don't think that it will be a geodesic. I think it will be straight everywhere except at the place where the edges join where it will have a corner.
 
  • #22
DaleSpam said:
Yes, but I don't think that it will be a geodesic. I think it will be straight everywhere except at the place where the edges join where it will have a corner.
It doesn't have a corner, it is intersecting itself.
 
  • #23
A.T. said:
It doesn't have a corner, it is intersecting itself.
Yes, but I think it is intersecting itself at an angle.
 
  • #24
DaleSpam said:
Yes, but I think it is intersecting itself at an angle.
Yes, that is the point. The direction of a vector changes after being parallel transported along a closed loop on a single geodesic. So this:
I assume this is just a property of geodesics they are the only closed paths which has curvature in the interior such that when a vector is parallel transported along that closed path it is invariant to changing orientation.
is wrong. The orientation is unchanged only in special cases, like the sphere.
 
  • #25
A.T. said:
Yes, that is the point. The direction of a vector changes after being parallel transported along a closed loop on a single geodesic. So this:

is wrong. The orientation is unchanged only in special cases, like the sphere.

I know it is wrong and the example of the cone is perfect. I first thank you and another contributor for helping me.

Now if I can ask why does the definition seem to say that the sense of the vectors remains unchanged??

In the presence of an affine connection, geodesics are defined to be curves whose tangent vectors remain parallel if they are transported along it.

from wikipedia: geodesics
 
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  • #26
PeterDonis said:
The apex is a singularity of the manifold; I believe there is a theorem that says parallel transport around a closed geodesic brings all vectors back to the same vectors, but only if the closed geodesic doesn't enclose a singularity.

this theorem would be great to find! I will try to find it
 
  • #27
A.T. said:
The orientation is unchanged only in special cases, like the sphere.

So what defines the special cases? I see what you mean about the presence of a "singularity" not being the right thing to look for, since you can alter the manifold slightly to eliminate it without eliminating the change in a vector parallel transported around a closed loop, e.g. putting a small spherical dome at the tip of the cone.

Is it constant curvature that defines the special cases? More precisely, is it that the surface enclosed by the closed geodesic has to have constant curvature? That would explain why a sphere is a special case but an ellipsoid of revolution is not.
 
  • #28
Kidphysics said:
this theorem would be great to find! I will try to find it

After seeing A.T.'s follow up post, I think I was mistaken; the theorem, if there is one, won't be that general. It will only cover the "special cases" like a sphere, not all manifolds without singularities.
 
  • #29
A.T. said:
The direction of a vector changes after being parallel transported along a closed loop on a single geodesic.
But then it isn't a geodesic. A geodesic parallel transports it own tangent vector. The path you describe doesn't parallel transport its own tangent vector since it has a bend. Therefore it isn't a geodesic.
 
  • #30
Found an interesting paper titled "Closed Geodesics on Positively Curved Manifolds" which bears on this topic:

http://people.mpim-bonn.mpg.de/hwbllmnn/archiv/Annals82_BTZ.pdf
 
  • #31
PeterDonis said:
Found an interesting paper titled "Closed Geodesics on Positively Curved Manifolds" which bears on this topic:

http://people.mpim-bonn.mpg.de/hwbllmnn/archiv/Annals82_BTZ.pdf

In this paper there was reference to closed hyperbolic geodesics.

this seems a contradiction ,could you explain the geometric meaning of this??

I understood that in a gravitational context hyperbolic orbits were necessarily escape trajectories.
 
  • #32
Austin0 said:
I understood that in a gravitational context hyperbolic orbits were necessarily escape trajectories.

"Hyperbolic" in the paper is a technical term; I believe it refers to the type of differential equation describing the curve, as here:

http://en.wikipedia.org/wiki/Partial_differential_equation#Classification

But I am not really familiar with much of the technical terminology in this paper.

Also, a point of clarification about orbits: yes, hyperbolic orbits are not bound orbits in GR, but bound orbits are not closed geodesics of spacetime either; they are "helical" when the time dimension is included. Their projections into spacelike slices will be closed spacelike curves, but those curves probably won't be geodesics of the spacelike slice.
 
  • #33
PeterDonis said:
"Hyperbolic" in the paper is a technical term; I believe it refers to the type of differential equation describing the curve, as here:

http://en.wikipedia.org/wiki/Partial_differential_equation#Classification

But I am not really familiar with much of the technical terminology in this paper.

Also, a point of clarification about orbits: yes, hyperbolic orbits are not bound orbits in GR, but bound orbits are not closed geodesics of spacetime either; they are "helical" when the time dimension is included. Their projections into spacelike slices will be closed spacelike curves, but those curves probably won't be geodesics of the spacelike slice.

thanks for the link, although mostly over my head.
from what you said is it correct to infer that closed geodesics only refers to static manifolds and that the transport means repositioning vectors as a mathematical operation, with no implication of actual translation through spacetime?
 
  • #34
DaleSpam said:
But then it isn't a geodesic. A geodesic parallel transports it own tangent vector. The path you describe doesn't parallel transport its own tangent vector since it has a bend. Therefore it isn't a geodesic.
Based on this reasoning there is trivially (per definition) no example of "other manifold" that you mention in post #9 (as a counter example to the sphere). Is there?

The entire line extending to infinity is a geodesic which intersects itself. The loop, that the geodesic encloses, is of course not a geodesic if you jump to the other part at the intersection. But it is a closed loop made from a single geodesic segment. The fact the total change in direction at the corner(s) is different from 2pi implies curvature inside the loop. A full great circle on a sphere has no corners at all, so the total corner change in direction is zero which also implies curvature.
 
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  • #35
PeterDonis said:
Is it constant curvature that defines the special cases? More precisely, is it that the surface enclosed by the closed geodesic has to have constant curvature? That would explain why a sphere is a special case but an ellipsoid of revolution is not.
On the ellipsoid of revolution there are some self intersecting geodesics which preserve the direction. On the sphere all of them do. This seems to be due to the higher degree of symmetry on the sphere, which is of course connected to the globally constant curvature.
 
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