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Problem 13 from Chapter 6 of Goldstein's "Classical Mechanics" reads:
Show that the relativistic motion of a particle in an attractive
inverse square law of force is a precessing ellipse. Compute the
precession of the perihelion of Mercury resulting from this
effect. ( The answer, about 7" per century, is much smaller than
the actual precession of 40" per century which can be accounted
for correctly only by general relativity.)
Can someone kickstart my brain with a hint as to what approach I should
consider to solve this problem?
A somewhat similar problem is sometimes offered: [Phys 4222 UFlorida]
"Suppose that the sun were surrounded by a dust cloud of uniform
density which extended at least as far as the orbital radius of the
Earth. The effect of the dust cloud is to modify the gravitational
force experienced by the Earth, so that the potential energy of the
Earth is (neglecting the effects of the planets)
U(r) = -GMm/r + 1/2 kr^2
where M is the mass of the sun, m is the mass of the Earth, G is the
gravitational constant, and k = 4 pi rho mG/3 (note that k > 0, so
this additional term is attractive). The effect of the dust cloud is
to cause elliptical orbits about the sun to precess slowly."
Does this provide any traction, I wonder?
Leigh,
You're showing your age, that is the problem in the first edition. It
is now problem 26 in chapter 7.
Leigh,
Apparently the assignment is to apply special, but not general
relativity. I suppose I'd try to solve the equation
-G M r_vec/r^2 = d(gamma v_vec)/dt
separating out the radial and azimuthal components and performing
something like the usual small amplitude radial oscillation analysis
to find the apsidal angle.
But maybe that isn't saying anything you hadn't already thought of
and the stumbling block lies further along that path.
Oh good that's the ed. I can't find. Cost < $10.
My first thought was somewhere I'd heard one could expand and use the
first and second? terms. Thereby, adding a cubic term to the force.
(quad potential, naturellement). Some theorem, I think, that only the
linear and quad central force result in no precession. That's why some
early on suggested gravity was not exactly inverse square.