Connection of General relativity and geometric Refraction of light

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SUMMARY

The discussion focuses on the connection between general relativity and the geometric refraction of light influenced by the sun's gravity. The user attempts to model light refraction using aether with varying speeds of light, leading to an equation derived from the Schwarzschild solution. The key equation presented is C=c0 (1-g cos(phi)/(1-g cos(phi)^3)^(1/2), where g is defined as 2GM/(r c^2). Despite the efforts, the user does not achieve the expected results, specifically the approximation alpha = 2g for small refraction angles.

PREREQUISITES
  • Understanding of general relativity principles
  • Familiarity with the Schwarzschild equation
  • Knowledge of light refraction laws
  • Basic concepts of gravitational lensing
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  • Research the implications of the Schwarzschild solution on light behavior
  • Explore the concept of gravitational lensing in detail
  • Study recent eprints on light refraction in general relativity from arXiv
  • Investigate alternative models of light propagation in gravitational fields
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Physicists, astrophysicists, and researchers interested in the interplay between gravity and light, particularly those studying gravitational lensing and general relativity.

exponent137
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I tried to obtain refraction of light by sun's gravity by substitution of sun's gravitational field by aether with different speeds of light.
I do not get right result. Where I am wrong?

For light which travel close to the sun by direct trajectory, I get the following speed of light in dependence of angle phi.


C=c0 (1-g cos(phi)/(1-g cos(phi)^3)^(1/2)

g=2GM/(r c^2).
r is the closest radius to the sun.

I suppose that refraction law is

dc = d(alpha) * tg(phi)

Where alpha is small refraction and phi is angle regarding sun.



But this do not give right solution in the first approximation, which is alpha = 2g.

Equation for c I get from Schwarzschild equation.

c0^2 dt^2 (1-2g cos(phi)) - dx^2/(1-2g cos(phi))-r cos(phi)^2...=0
 
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