Perihelion precession of Mercury

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    Mercury Precession
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SUMMARY

The discussion focuses on the perihelion precession of Mercury as described in "Spacetime and Geometry" by Sean Carroll. The key formula presented is r = L² / GM(1 + e cos((1 - α)φ), which indicates that the perihelion advances by Δφ = 2πα per orbit. Participants clarify that the total angle traversed from one perihelion to the next is 2π plus the precession angle, leading to a refined understanding of the precession phenomenon. Additionally, there is confusion regarding the visualization of the orbital plane, which remains constant despite the elliptical orbit's movement.

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  • Understanding of classical mechanics and orbital dynamics
  • Familiarity with the concepts of perihelion and aphelion
  • Knowledge of angular momentum (L) and gravitational constant (G)
  • Basic grasp of trigonometric functions and their applications in physics
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  • Study the derivation of perihelion precession in general relativity
  • Explore visualizations of orbital mechanics, particularly the precession of orbits
  • Learn about the implications of precession in celestial mechanics
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LAHLH
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Hi,

It's found it Carroll that r=\frac{L^2}{GM(1+e\cos{((1-\alpha)\phi)}}. He states that this means we've found that during each orbit the perihelion advances by \Delta\phi=2\pi\alpha, I'm not sure that I follow this. Perihelion is the min value of r, and thus should correspond to whenever \cos{((1-\alpha)\phi)} is at a max, namely (1-\alpha)\phi_n =2n\pi therefore \Delta\phi= \phi_{n+1}-\phi_{n}=\frac{2(n+1)\pi}{1-\alpha}-\frac{2n\pi}{1-\alpha}=\frac{2\pi}{1-\alpha}=2\pi+2\pi\alpha+O(\alpha^2) =2\pi(1+\alpha). Yet this is not what he states...

Also more generally, the figure shown of the precession (5.6) seems to show the orbital plane itself changing, I was expecting things to remain in a plane, but the ellipse to move around (like flat flower petals), just wondering how I should visualise this precession and if anyone has any good links/vids to see it
 
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LAHLH said:
It's found it Carroll that r=\frac{L^2}{GM(1+e\cos{((1-\alpha)\phi)}}. He states that this means we've found that during each orbit the perihelion advances by \Delta\phi=2\pi\alpha, I'm not sure that I follow this. Perihelion is the min value of r, and thus should correspond to whenever \cos{((1-\alpha)\phi)} is at a max, namely (1-\alpha)\phi_n =2n\pi therefore \Delta\phi= \phi_{n+1}-\phi_{n}=\frac{2(n+1)\pi}{1-\alpha}-\frac{2n\pi}{1-\alpha}=\frac{2\pi}{1-\alpha}=2\pi+2\pi\alpha+O(\alpha^2) =2\pi(1+\alpha). Yet this is not what he states...

What you've computed there is the total angle the planet has traversed from one perihelion to the next. If there was no precession at all, this would be 2pi, so the precession is the total angle minus 2pi. If you subtract 2pi from your expression, you get (2pi alpha)/(1-alpha), which is essentially 2pi alpha for sufficiently small alpha.

LAHLH said:
Also more generally, the figure shown of the precession (5.6) seems to show the orbital plane itself changing, I was expecting things to remain in a plane, but the ellipse to move around (like flat flower petals), just wondering how I should visualise this precession and if anyone has any good links/vids to see it

The orbital plane doesn't change. I haven't checked Carroll's figure, but it shouldn't show any change in the orbital plane, if it's just talking about the precession of an orbit.
 
Thanks a lot,makes sense..

Yeah I didn't think the plane should change, maybe I'm just looking at the fig weirdly, looks like a slinky to me, whereas I guess it's intended to look like flat flower petals
 

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