Calculating the Rotational Inertia — Question 3

Section 10-6 · Physics pages 1476–1477

Question 3 An annulus approaches a hoop in the thin-ring limit A uniform flat annulus has mass M, inner radius a and outer radius b. Its axis passes through the center perpendicular to its plane. a b Schematic; labels, not drawing lengths, specify the data. (a) Derive its inertia by summing circular rings. (b) Check the solid-disk and thin-hoop limits without confusing surface density with total mass.
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Question 3 - Solution An annulus approaches a hoop in the thin-ring limit a b (a) Derivation and calculation A ring of radius r and width dr has mass dm = 2πσr dr, where σ = M π(b2 −a2). I = ∫b a r2 dm = 2πσ ∫b a r3 dr = πσ 2 (b4 −a4) = M 2 (a2 + b2) . (b) Result and interpretation The limiting cases at fixed total mass are a = 0 ⇒I = 1 2Mb2 , a, b →R ⇒I →MR2 . In the thin-annulus limit, σ = M/[π(b2 −a2)] increases as the area shrinks. Holding surface density fixed would instead change the mass. Physical check The mean squared radius lies between a2 and b2, so Ma2 ≤I ≤Mb2.

Question 3

An annulus approaches a hoop in the thin-ring limit

A uniform flat annulus has mass MM, inner radius aa and outer radius bb. Its axis passes through the center perpendicular to its plane.

Diagram shown in the original SVG worksheet.

  1. Derive its inertia by summing circular rings.

  2. Check the solid-disk and thin-hoop limits without confusing surface density with total mass.

Question 3 - Solution

An annulus approaches a hoop in the thin-ring limit

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

A ring of radius rr and width drdr has mass dm=2πσrdrdm=2\pi\sigma r\,dr, where σ=Mπ(b2−a2).\sigma=\frac{M}{\pi(b^2-a^2)}. I=∫abr2dm=2πσ∫abr3dr=πσ2(b4−a4)=M2(a2+b2).I=\int_a^br^2\,dm=2\pi\sigma\int_a^br^3\,dr =\frac{\pi\sigma}{2}(b^4-a^4) =\boxed{\frac M2(a^2+b^2)}.

(b) Result and interpretation

The limiting cases at fixed total mass are a=0⇒I=12Mb2,a,b→R⇒I→MR2.a=0\Rightarrow\boxed{I=\frac12Mb^2},\qquad a,b\to R\Rightarrow\boxed{I\to MR^2}. In the thin-annulus limit, σ=M/[π(b2−a2)]\sigma=M/[\pi(b^2-a^2)] increases as the area shrinks. Holding surface density fixed would instead change the mass.

Physical check

The mean squared radius lies between a2a^2 and b2b^2, so Ma2≤I≤Mb2Ma^2\le I\le Mb^2.