Assuming the earth to be of uniform density, drill a hole
through the Earth between any two points on the surface of the
earth. Install a frictionless tube, and evacuate all the air. Show
that the motion of a subway car placed in this tube is simple
harmonic motion and evaluate the period of the motion. (HINT: Use
gravitational equivalent of Gauss's Law.)
PROVE THE GENERAL CASE ALONG ANY CHORD BETWEEN ANY TWO POINTS. NOT
JUST THE CASE WHERE IT TRAVELS ALONG A DIMATER
Putting the z axis pointing from the center of the Earth to the
middle point of the tunnel,
and the x axis parallel to the tunnel, the tunnel equation
are
z=z0
y=0
In polar coordinates,
r cos(theta) = R cos(theta0)
phi = 0
where R is Earth radius and R cos(theta0) = z0.
The tunnel goes from theta=-theta0 to theta=theta0.
Gravitational force:
Only the mass contained into a sphere of radius r contributes to
the gravitational force, so
F(r) = G M(r)m/r^2 = G (rho (4/3) pi r^3)m/r^2 =
= G rho (4/3) pi m r
F(R) = g m = G rho (4/3) pi m R, then
F(r) = g m r/R
Potential energy
U(r) = g m r^2/(2R) =
= [g m z_0^2/(2R)]/cos^2(theta))
Velocity:
r cos(theta) = R cos(theta0)
then
dr/dt cos(theta) - r d theta/dt sin(theta) = 0
or
dr/dt = r d theta/dt tan(theta)
v^2 = (dr/dt)^2 + r^2 (d theta/dt)^2=
= r^2 (d theta/dt)^2 (1+tan^2(theta))=
= r^2 (d theta/dt)^2 / cos^2(theta) =
= z_0^2 (d theta/dt)^2 / cos^4(theta)
Lagrangian:
L = T-U =
= (m z_0^2/2) (d theta/dt)^2 / cos^4(theta) -
- [g m z_0^2/(2R)]/cos^2(theta))
Assuming that theta0<<1, then we can approximate the
lagrangian as
L = m z_0^2/2 (d theta/dt)^2 + g m z_0^2/(2R) theta^2
and hence the equation of motion will be
d^2 theta/dt^2 + g/R theta = 0 ==> Motion is Simple
Harmonic Motion
Then
theta(t) = A cos(sqrt(g/R) t + phi)
Period: T = 2pi/omega = 2 pi sqrt(R/g)
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