Assume that a tunnel is dug across the earth (radius = R) passing through its centre. Find the time a particle takes to cover the length of the tunnel if it is projected into the tunnel with a speed of √gR
Let M be the total mass of the earth.
At any position x,
∴M′M=ρ×(43)π×x3ρ×(43)π×R3=x3R3⇒M′=Mx3R3
So force on the particle is given by,
∴Fx=GM′mx2=GMmR3x ....(1)
So, acceleration of the mass 'M' at that position is given by,
ax=GMR2x⇒axx=w2=GMR3=gR (∴g=GMR2)
So, T=2π√Rg=Time period of oscillation.
a) Now, using velocity- displacement equation.
V=ω√(A2−R2) [Where, A=amplitude]
Given when, y=R, v=√gR,ω=√gR
⇒√gR=√gR√(A2−R2) [because ω=√gR]
⇒R2=A2−R2⇒A=√2R
[Now, the phase of the particle at the point P is greater than π2 but less than π and at Q is greater
than π but less than 3π2. Let the times taken by the particle to reach the positions P and Q be t1&t2
respectively, then using displacement time equaion]
y=r sin ωt
We have, R=√2 R sin ωt1 ⇒ωt1=3π4
&−R=√2 R sin ωt2 ⇒ωt2=5π4
So, ω(t2−t1)=π2⇒t2−t1=π2ω=π2√(Rg)sec