Surfaces and geodesics in General Relativity

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SUMMARY

The discussion focuses on proving that a curve ¡, which pierces a family of null hypersurfaces orthogonally, is a null geodesic in General Relativity. The problem requires demonstrating that the tangent vector ka is collinear with the normal vector na at the point of intersection and finding the condition under which the geodesic equation simplifies to ka||bka = 0. The key equation involved is the geodesic equation: \ddot{x}e + \Gammaemb\dot{x}m \dot{x}b = 0, where \Gamma represents the Christoffel symbols associated with the null hypersurface.

PREREQUISITES
  • Understanding of General Relativity concepts, particularly null hypersurfaces.
  • Familiarity with geodesic equations and their significance in curved spacetime.
  • Knowledge of vector fields and their properties in differential geometry.
  • Basic proficiency in tensor calculus and Christoffel symbols.
NEXT STEPS
  • Study the properties of null hypersurfaces in General Relativity.
  • Learn about the derivation and implications of the geodesic equation in curved spacetime.
  • Explore the relationship between waves and rays in the context of General Relativity.
  • Investigate the role of Christoffel symbols in the geodesic equation.
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Students and researchers in physics, particularly those studying General Relativity, as well as mathematicians interested in differential geometry and its applications to theoretical physics.

student85
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Hi all. This is one of the problems that I was asked to do for my General Relativity class. I know this may look a little long, but if anyone can help me out with ANYTHING about this problem, I will greatly appreciate it.

Homework Statement


Consider the family of hypersurfaces where each member is defined by the constancy of the function S(xc) over that hypersurface and further require that each hypersurface be a null hypersurface in the sense that its normal vector field, na = S|a , be a null vector field.
Let ¡ be a member of the family of curves that pierces each such hypersurface orthogonally, meaning that the tangent vector to ¡, say ka, is everywhere collinear with the vector na at the point of piercing. Show that ¡ is a null geodesic and find the condition on the relation between na and ka that allows the geodesic equation to be written in the simple form ka||bka = 0.
Interpret your results in terms of waves and rays.


Homework Equations


The geodesic equation: \ddot{x}e + \Gammaemb\dot{x}m \dot{x}b = 0


The Attempt at a Solution


By reading through the problem it is not very hard to get the hang of what it is saying, and it seems pretty clear that \Gamma must be a null surface. But I don't know where to get started in showing that it is a "null geodesic", and how to derive at the simple geodesic equation they give. I'm just very stuck here. If anyone can give me a little hint I would appreciate it. Thanks in advance.
 
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No relativists here? :S
 

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