Earnshaw's theorem for electrostatics rests only on two facts: the potential energy…
PHYSICS · Multi-part · Fermi University Physics · Electricity, Magnetism & Electromagnetism · Relativity & Gravitation · Newtonian gravitation as a field theory
The Boundary-Value Problem, Ch The field as a differential equation: Poisson, Laplace and the well-posed problem
Problem
Earnshaw's theorem for electrostatics rests only on two facts: the potential energy of the test object is proportional to a potential obeying Laplace's equation in the region free of sources, and nothing about the sign of the charge enters the argument. The Newtonian gravitational potential Φ(r) is defined so that the gravitational field is g=−∇Φ and obeys ∇2Φ=4πGρm, with ρm the mass density and G=6.674×10−11Nm2kg−2; in vacuum ∇2Φ=0. The potential energy of a small test mass mq>0 placed at r is U(r)=mqΦ(r). Two point masses, each M=5.0×105kg, are fixed at z=+b and z=−b on the z axis, with b=2.0m, in otherwise empty space; gravity is the only force acting. A small test mass sits at the origin, midway between them.
((a)) Write Φ(z) on the axis for −b<z<b and show the origin is an equilibrium point, dΦ/dz=0 there.
((b)) Find d2Φ/dz2 at the origin and say whether a small axial displacement grows or is restored.
((c)) Using ∇2Φ=0 at the origin (mass-free there) together with the rotational symmetry of the arrangement about the z axis, find ∂2Φ/∂x2 and ∂2Φ/∂y2 at the origin, and say whether a small sideways displacement grows or is restored.
((d)) State whether any fixed arrangement of point masses could make the equilibrium of a test mass stable against a displacement in every direction at once, using the same mean-value argument as Earnshaw's theorem, and say whether the positive sign of mq changes that conclusion.