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Geodesic motion in Euclidean Schwarzschild geometry
Emmanuele Battista1, Giampiero Esposito2,3
1Department of Physics, University of Vienna, Boltzmanngasse 5, 1090 Vienna, Austria.
This study explores geodesic motion in Euclidean Schwarzschild geometry, finding no elliptic-like orbits exist. Only specific unbounded orbits are permitted, differing from general relativity predictions.
Area of Science:
- Theoretical physics
- General relativity
- Differential geometry
Background:
- Geodesic motion describes the path of objects in spacetime.
- Schwarzschild geometry is a solution to Einstein's field equations describing a non-rotating, uncharged black hole.
- Euclidean geometry differs from Lorentzian geometry in its fundamental properties.
Purpose of the Study:
- To systematically investigate geodesic motion within the equatorial plane of Euclidean Schwarzschild geometry.
- To explicitly derive the mathematical form of these geodesics.
- To compare the characteristics of these geodesics with those in Lorentzian spacetime.
Main Methods:
- The study focuses on the equatorial plane of the Euclidean Schwarzschild geometry.
- Mathematical derivations are performed to obtain the explicit form of geodesic motion.
- Analysis involves the use of incomplete elliptic integrals of the first, second, and third kinds.
Main Results:
- The explicit form of geodesic motion is determined using incomplete elliptic integrals.
- No elliptic-like orbits are found in Euclidean Schwarzschild geometry, contrasting with Lorentzian patterns.
- Among unbounded orbits, only those of the first kind are permissible.
Conclusions:
- The nature of geodesic motion in Euclidean Schwarzschild geometry is fundamentally different from that in Lorentzian spacetime.
- The absence of elliptic-like orbits and the restriction on unbounded orbits highlight unique characteristics of this geometry.
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