Gravitational field due to spherical shell A point mass m is a distance d from the center of a thin spherical shell of mass M and radius R. The magnitude of the gravitational force on the point mass is given by the
F(d)=GMm4π∫2π0∫π0(d−Rcosφ)sinφ(R2+d2−2Rdcosφ)3/2dφ dθ,
where G is the gravitational constant.
a. Use the change of variable x = cos φ to evaluate the integral and show that if d > R, then F(d)=GMmd2, which means the force is the same as if the mass of the shell were concentrated at its center.
b. Show that if d < R (the point mass is inside the shell), then F = 0.

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