Timelike geodesics in Schwarzschild Metric.

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SUMMARY

The discussion focuses on deriving timelike geodesics in the Schwarzschild Metric using the Euler-Lagrange equations. The Lagrangian is defined as F = gμν(dxμ/ds)(dxν/ds), specifically for the Schwarzschild metric in the equatorial plane as F = (1-2m/r)⁻¹(dr/ds)² + r²(dθ/ds)² - (1-2m/r)(dt/ds)². Three first integrals are identified: one for the t coordinate, one for the θ coordinate, and the Lagrangian F itself. The final result can be expressed as a differential equation for r(θ).

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  • Understanding of the Schwarzschild Metric
  • Familiarity with the Euler-Lagrange equations
  • Knowledge of differential equations
  • Basic concepts of general relativity
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Nilupa
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Please explain me how to derive the Timelike geodesics in Schwarzschild Metric.

Thank you.
 
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To derive the geodesics for any metric, write out and solve the Euler-lagrange equations for the Lagrangian F = gμν(dxμ/ds)(dxν/ds).

For Schwarzschild this is (in the equatorial plane) F = (1-2m/r)-1(dr/ds)2 + r2(dθ/ds)2 - (1-2m/r)(dt/ds)2 . There are three first integrals: one for the t coordinate, one for the θ coordinate, and F itself. The result can be expressed as a differential equation for r(θ).
 
Thank you so much Bill K.

I derived the equations.
 

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