A calculation of perihelion precession is presented that utilizes a phase-plane analysis of the general relativistic equations of motion. The equations of motion are reviewed in addition to the phase-plane analysis required for the calculation. “Exact” phase planes for orbital dynamics in the Schwarzschild geometry are discussed, and bifurcations are identified as a dimensionless parameter involving the angular momentum is varied.

1.
M. Carmeli, Classical Fields: General Relativity and Gauge Theory (Wiley, New York, 1982), pp. 218–220;
A. Eddington, The Mathematical Theory of Relativity (Cambridge U.P., Cambridge, 1924), 2nd ed., pp. 88–90;
C. Misner, K. Thorne, and J. Wheeler, Gravitation (Freeman, San Francisco, 1973), pp. 659–670, 1110–1116;
H. Ohanian and R. Ruffini, Gravitation and Spacetime (Norton, New York, 1994), pp. 401–408;
B. Schutz, A First Course in General Relativity (Cambridge U.P., Cambridge, 1990), pp. 275–284;
H. Stephani, General Relativity (Cambridge U.P., Cambridge, 1990), pp. 105–108;
R. Wald, General Relativity (University of Chicago Press, Chicago, 1984), pp. 139–143;
S. Weinberg, Gravitation and Cosmology: Principles and Applications of the General Theory of Relativity (Wiley, New York, 1972), pp. 194–197, 230–233.
2.
N.
Anderson
and
G. R.
Walsh
, “
Phase-Plane Methods for Central Orbits
,”
Am J. Phys.
58
(
6
),
548
551
(
1990
).
3.
B.
Davies
, “
Derivation of Perihelion Precession
,”
Am. J. Phys.
51
(
10
),
909
911
(
1983
);
D.
Ebner
, “
Comment on B. Davies’s ‘Derivation of Perihelion Precession, ’ 
Am. J. Phys.
53
(
4
),
374
(
1985
);
Daniel R.
Stump
, “
Precession of the Perihelion of Mercury
,”
Am. J. Phys.
56
(
12
),
1097
1098
(
1988
).
4.
A. P. Arya, Introduction to Classical Mechanics (Prentice–Hall, Englewood Cliffs, NJ, 1990), pp. 222–252;
H. C. Corben and P. Stehle, Classical Mechanics (Dover, Mineola, NY, 1994), 2nd ed., pp. 90–100;
G. Fowles and G. Cassiday, Classical Dynamics of Particles and Systems (Harcourt-Brace, Orlando, FL, 1993), 5th ed., pp. 191–216;
H. Goldstein, Classical Mechanics (Addison–Wesley, Reading, MA, 1980), 2nd ed., pp. 94–102;
A. S. Kompaneyets, Theoretical Mechanics (Dover, New York, 1962), 2nd ed., pp. 41–48;
J. Marion and S. Thornton, Analytical Mechanics (Harcourt–Brace, Orlando, FL, 1995), 4th ed., pp. 291–321;
A. Roy, Orbital Dynamics (Hilger, Redcliffe Way, Bristol, 1982), 2nd ed., pp. 69–100;
K. Symon, Mechanics (Addison–Wesley, Reading, MA, 1971), pp. 128–134.
5.
J. L. Martin, General Relativity—A First Course for Physicists (Prentice–Hall International, Hertfordshire, UK, 1996), Revised ed., pp. 58–60.
6.
S. Strogatz, Nonlinear Dynamics and Chaos—with Applications to Physics, Biology, Chemistry, and Engineering (Addison–Wesley, New York, 1994). Also see problem #6.5.7, p. 186.
7.
M. Tabor, Chaos and Integrability in Nonlinear Dynamics: An Introduction (Wiley, New York, NY, 1989), pp. 13–30.
8.
L.
Bombelli
and
E.
Calzetta
, “
Chaos around a Black Hole
,”
Class. Quantum Grav.
9
(
12
),
2573
2599
(
1992
);
S.
Suzuki
and
K.
Maeda
, “
Chaos in Schwarzschild Space-Time: The Motion of a Spinning Particle
,”
Phys. Rev. D
55
,
4848
4859
(
1997
).
9.
R. A.
Hulse
and
J. H.
Taylor
, “
Discovery of a Pulsar in a Binary Star System
,”
Astrophys. J.
195
,
L51
L53
(
1975
).
10.
Using x rather than 1/x for the horizontal axis pushes the singularity at r=0 to infinity. As a result, the relative locations of fixed points are more easily scaled and plotted in the phase plane.
11.
Also termed homoclinic orbit in the literature on nonlinear analysis.
12.
These are actually precessing hyperbolic orbits if one allows negative r values (although nonphysical—shown to the left of the y axis in Fig. 4).
13.
But for an ordinary massive object M, the trajectories never reach the event horizon as it lies within the object’s surface.
14.
S. Chandrasekhar, The Mathematical Theory of Black Holes (Oxford U.P., Clarendon, New York, 1983), pp. 96–122.
15.
J. Hale and H. Kocak, Dynamics and Bifurcations (Springer-Verlag, New York, 1991), p. 425;
J. M.
Mao
and
J. B.
Delos
, “
Hamiltonian Bifurcation Theory of Closed Orbits in the Diamagnetic Kepler Problem
,”
Phys. Rev. A
45
,
1746
1761
(
1992
).
16.
Incidentally, x⃗2* of Fig. 4 (and Fig. 3) is classified as a nonlinear center; see Strogatz (Ref. 6, p. 114). 
This content is only available via PDF.
AAPT members receive access to the American Journal of Physics and The Physics Teacher as a member benefit. To learn more about this member benefit and becoming an AAPT member, visit the Joining AAPT page.