The two-body problem consists of a system of two particles, one of mass m1= M and the other of mass m2= m. The sole forces on the system are the result of a Newtonian gravitational force field that has a potential energy function
(a) For this system, show that the linear momentum of the system is conserved and that the center of mass C moves at a constant speed in a straight line. In addition, show that
Here, r¯ is the position vector of the center of mass.
(b) Show that the angular momentum of the system of particles relative to C is conserved.
(c) Show that the total energy of the system of particles is conserved.
(d) Show that the differential equations governing the motions of m1and m2can be written in the following forms:26
(e) Argue that the results of Section 2.8 can be applied to (4.44) to determine the orbital motions of the particles about their center of mass C.
Chapter 5
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