The Kinetic Energy of Rolling — Question 6

Section 11-2 · Physics pages 1582–1583

Question 6 A height measurement can reject an impossible inertia model A rigid object rolls from rest through h = 0.50 m with no losses. All its mass lies within outer radius R, and I = βMR2. An instrument reports V = 2.0 m/s. Take g = 9.8 m/s2. β V 1 √2gh √gh Allowed inertia range 0 ≤β ≤1 sets the lossless rolling speed range. (a) Infer the apparent β and test the assumptions. (b) Find the smallest possible final speed under those assumptions.
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Question 6 - Solution A height measurement can reject an impossible inertia model β V 1 √2gh √gh (a) Derivation and calculation The measured speed would imply β = 2gh V 2 −1 = 2(9.8)(.50) (2.0)2 −1 = 1.45 . But r ≤R for every mass element requires I = ∫ r2 dm ≤MR2 ⇒β ≤1. The measurement and the complete stated ideal model are incompatible. (b) Result and interpretation The speed decreases with increasing β: V (β) = √ 2gh 1 + β . Its smallest admissible value occurs at β = 1: Vmin = √ gh = √ 4.90 = 2.214 m/s . A loss, measurement error, or failure of the radius/no-slip assumptions must explain the lower reported speed. Physical check The reported 2.0 m/s is below the allowed minimum even for a hoop-like inertia distribution.

Question 6

A height measurement can reject an impossible inertia model

A rigid object rolls from rest through h=0.50mh=0.50\,\mathrm m with no losses. All its mass lies within outer radius RR, and I=βMR2I=\beta MR^2. An instrument reports V=2.0m/sV=2.0\,\mathrm{m/s}. Take g=9.8m/s2g=9.8\,\mathrm{m/s^2}.

Diagram shown in the original SVG worksheet.

  1. Infer the apparent β\beta and test the assumptions.

  2. Find the smallest possible final speed under those assumptions.

Question 6 - Solution

A height measurement can reject an impossible inertia model

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

The measured speed would imply β=2ghV2−1=2(9.8)(.50)(2.0)2−1=1.45.\beta=\frac{2gh}{V^2}-1=\frac{2(9.8)(.50)}{(2.0)^2}-1 =\boxed{1.45}. But r≤Rr\le R for every mass element requires I=∫r2dm≤MR2⇒β≤1.I=\int r^2\,dm\le MR^2\Rightarrow\beta\le1. The measurement and the complete stated ideal model are incompatible.

(b) Result and interpretation

The speed decreases with increasing β\beta: V(β)=2gh1+β.V(\beta)=\sqrt{\frac{2gh}{1+\beta}}. Its smallest admissible value occurs at β=1\beta=1: Vmin=gh=4.90=2.214m/s.\boxed{V_{\min}=\sqrt{gh}=\sqrt{4.90}=2.214\ \mathrm{m/s}}. A loss, measurement error, or failure of the radius/no-slip assumptions must explain the lower reported speed.

Physical check

The reported 2.0 m/s is below the allowed minimum even for a hoop-like inertia distribution.