Gravitation Inside Earth — Question 9

Section 13-4 · Physics pages 1968–1969

Question 9 A shorter chord tunnel has the same ideal transit time In a uniform nonrotating sphere,⃗g = −k⃗r with k = gs/R. A narrow straight frictionless tunnel follows a chord at perpendicular distance b < R from the center. Let s measure distance along the chord from its midpoint. A particle is released from an endpoint; ignore removed mass. b Cross-section of a spherically symmetric mass distribution. (a) Find its along-tunnel equation and endpoint-to-endpoint travel time, using ¨s = −ω2s ⇒T = 2π/ω. (b) Find the wall-force magnitude and explain why travel time does not depend on chord length.
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Question 9 - Solution A shorter chord tunnel has the same ideal transit time b (a) Derivation and calculation Write⃗r = sˆs + bˆb. Projecting gravity along the tunnel, ¨s =⃗g · ˆs = −ks, s0 = √ R2 −b2. Thus s(t) = s0 cos( √ k, t), ttransit = π/ √ k = π √ R/gs . (b) Result and interpretation The particle has no transverse acceleration, requiring −mkbˆb +⃗N =⃗0 =⇒⃗ N = mkbˆb, N = mkb . The maximum speed is vmax = √ k s0 = √ k(R2 −b2). Distance and speed scale with the same amplitude s0, leaving transit time independent of the chord length. Physical check At b = 0 the wall force vanishes and the result reduces to the diameter tunnel.

Question 9

A shorter chord tunnel has the same ideal transit time

In a uniform nonrotating sphere, g→=−kr→\vec g=-k\vec r with k=gs/Rk=g_s/R. A narrow straight frictionless tunnel follows a chord at perpendicular distance b<Rb<R from the center. Let ss measure distance along the chord from its midpoint. A particle is released from an endpoint; ignore removed mass.

Diagram shown in the original SVG worksheet.

  1. Find its along-tunnel equation and endpoint-to-endpoint travel time, using s̈=−ω2s⇒T=2π/ω\ddot s=-\omega^2s\Rightarrow T=2\pi/\omega.

  2. Find the wall-force magnitude and explain why travel time does not depend on chord length.

Question 9 - Solution

A shorter chord tunnel has the same ideal transit time

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Write r→=sŝ+bb̂\vec r=s\hat s+b\hat b. Projecting gravity along the tunnel, s̈=g→⋅ŝ=−ks,s0=R2−b2.\ddot s=\vec g\cdot\hat s=-ks,\qquad s_0=\sqrt{R^2-b^2}. Thus s(t)=s0cos⁡(k,t),ttransit=π/k=πR/gs.s(t)=s_0\cos(\sqrt k,t),\qquad \boxed{t_{\mathrm{transit}}=\pi/\sqrt k=\pi\sqrt{R/g_s}}.

(b) Result and interpretation

The particle has no transverse acceleration, requiring −mkbb̂+N→=0→⇒N→=mkbb̂,N=mkb.-mkb\hat b+\vec N=\vec0\quad\Longrightarrow\quad \boxed{\vec N=mkb\hat b,\quad N=mkb}. The maximum speed is vmax=ks0=k(R2−b2).v_{\max}=\sqrt k\,s_0=\sqrt{k(R^2-b^2)}. Distance and speed scale with the same amplitude s0s_0, leaving transit time independent of the chord length.

Physical check

At b=0b=0 the wall force vanishes and the result reduces to the diameter tunnel.