Gravitation Inside Earth — Question 1

Section 13-4 · Physics pages 1952–1953

Question 1 A uniform spherical shell has no preferred interior resting point A thin uniform spherical shell has radius R and mass M. Use the shell theorem: its gravitational field is zero everywhere strictly inside and equals a central point-mass field outside. A test particle is released from rest at r = .7R. m Thin spherical shell; the particle is offcenter inside the empty cavity. (a) Describe its motion if the shell is fixed and no other forces act. (b) If it is instead given a small velocity, explain whether the interior equilibrium restores its original position.
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Question 1 - Solution A uniform spherical shell has no preferred interior resting point m (a) Derivation and calculation The shell theorem gives⃗g =⃗0 everywhere strictly inside. Therefore m¨⃗r = m⃗g =⃗0,⃗ r(t) =⃗r0 +⃗v0t. For release from rest,⃗ v(t) =⃗0,⃗ r(t) =⃗r0 , |⃗r0| = .7R. The particle remains at its initial point. (b) Result and interpretation With a small imposed velocity,⃗ r(t) =⃗r0 +⃗v0t , |⃗r(t)| < R. A displacement alone leaves another equilibrium, since δ⃗g =⃗0. There is no restoring force; the particle drifts until it reaches the shell boundary. Physical check The interior motion is uniform only while it remains within the cavity and encounters no other force.

Question 1

A uniform spherical shell has no preferred interior resting point

A thin uniform spherical shell has radius RR and mass MM. Use the shell theorem: its gravitational field is zero everywhere strictly inside and equals a central point-mass field outside. A test particle is released from rest at r=.7Rr=.7R.

Diagram shown in the original SVG worksheet.

  1. Describe its motion if the shell is fixed and no other forces act.

  2. If it is instead given a small velocity, explain whether the interior equilibrium restores its original position.

Question 1 - Solution

A uniform spherical shell has no preferred interior resting point

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

The shell theorem gives g→=0→\vec g=\vec0 everywhere strictly inside. Therefore mr→̈=mg→=0→,r→(t)=r→0+v→0t.m\ddot{\vec r}=m\vec g=\vec0,\qquad \vec r(t)=\vec r_0+\vec v_0t. For release from rest, v→(t)=0→,r→(t)=r→0,|r→0|=.7R.\boxed{\vec v(t)=\vec0,\qquad \vec r(t)=\vec r_0},\qquad |\vec r_0|=.7R. The particle remains at its initial point.

(b) Result and interpretation

With a small imposed velocity, r→(t)=r→0+v→0t,|r→(t)|<R.\boxed{\vec r(t)=\vec r_0+\vec v_0t},\qquad |\vec r(t)|<R. A displacement alone leaves another equilibrium, since δg→=0→.\delta\vec g=\vec0. There is no restoring force; the particle drifts until it reaches the shell boundary.

Physical check

The interior motion is uniform only while it remains within the cavity and encounters no other force.