Conservation of Mechanical Energy — Question 4

Section 8-4 · Physics pages 1078–1079

Question 4 Completing a loop requires more than reaching its height Neglect friction and air resistance, take g = 10 m/s2, and treat all stated guides as fixed. A small bead slides on the inside of a smooth vertical circular track of radius R. It starts from rest at height h above the bottom on a connecting track. The contact force can push inward but cannot pull. R mg + N bottom At the top both gravity and an inward normal force point toward the center. (a) Find speed squared at the top in terms of h and R. (b) Derive the minimum release height for continuous contact through the loop. (c) Why is the energy-only threshold h=2R insufficient?
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Question 4 - Solution Completing a loop requires more than reaching its height R mg + N bottom (a) Use the top height of 2R. Conserve energy between release and the top, whose height is 2R: mgh = 1 2mv2 t + 2mgR ⇒v2 t = 2g(h −2R) . (b) Impose nonnegative contact force. At the top, inward radial dynamics require mg + N = mv2 t R , N ≥0 ⇒v2 t ≥gR. 2g(h −2R) ≥gR ⇒hmin = 5 2R . More generally, at angle θ from the bottom, N/(mg) = 2h/R −2 + 3 cos θ, minimized at the top. (c) Check dynamics at the proposed threshold. The energy-only threshold h = 2R gives vt = 0 ⇒N = −mg < 0. The track cannot pull outward on the bead. Loss of contact occurs before the assumed full circular trajectory is completed.

Question 4

Completing a loop requires more than reaching its height

Neglect friction and air resistance, take g=10g=10 m/s2^2, and treat all stated guides as fixed. A small bead slides on the inside of a smooth vertical circular track of radius R. It starts from rest at height h above the bottom on a connecting track. The contact force can push inward but cannot pull.

Diagram shown in the original SVG worksheet.

  1. Find speed squared at the top in terms of h and R.

  2. Derive the minimum release height for continuous contact through the loop.

  3. Why is the energy-only threshold h=2R insufficient?

Question 4 - Solution

Completing a loop requires more than reaching its height

Diagram shown in the original SVG worksheet.

(a) Use the top height of 2R.

Conserve energy between release and the top, whose height is 2R2R: mgh=12mvt2+2mgR⇒vt2=2g(h−2R).mgh=\tfrac12mv_t^2+2mgR\Rightarrow\boxed{v_t^2=2g(h-2R)}.

(b) Impose nonnegative contact force.

At the top, inward radial dynamics require mg+N=mvt2R,N≥0⇒vt2≥gR.mg+N=\frac{mv_t^2}{R},\qquad N\geq0\Rightarrow v_t^2\geq gR. 2g(h−2R)≥gR⇒hmin=52R.2g(h-2R)\geq gR\Rightarrow\boxed{h_{\min}=\frac52R}. More generally, at angle θ\theta from the bottom, N/(mg)=2h/R−2+3cos⁡θN/(mg)=2h/R-2+3\cos\theta, minimized at the top.

(c) Check dynamics at the proposed threshold.

The energy-only threshold h=2Rh=2R gives vt=0⇒N=−mg<0.v_t=0\Rightarrow N=-mg<0. The track cannot pull outward on the bead. Loss of contact occurs before the assumed full circular trajectory is completed.