The Angular Momentum of a Rigid Body Rotating About a Fixed Axis — Question 4

Section 11-9 · Physics pages 1718–1719

y Question 4 Annular layers contribute angular momentum in proportion to squared radius A uniform annular plate has mass M, inner radius a and outer radius b. It rotates about its central normal axis at angular speed ω. b a Schematic; labels, not drawing lengths, specify the data. (a) Integrate the ring contributions to find Lz. (b) For a = b/2, find the ratio to a solid disk of the same mass, outer radius and angular speed.
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y Question 4 - Solution Annular layers contribute angular momentum in proportion to squared radius b a (a) Derivation and calculation The uniform surface density and differential ring mass are σ = M π(b2 −a2), dm = 2πσr dr. Integrating, Iz = ∫b a r2 dm = 2πσ ∫b a r3 dr = πσ 2 (b4 −a4), Lz = Izω = 1 2M(a2 + b2)ω . (b) Result and interpretation For a = b/2, Iannulus = 1 2M(b2/4 + b2) = 5 8Mb2. At equal mass, outer radius and angular speed, Lannulus Ldisk = (5/8)Mb2 (1/2)Mb2 = 5 4 . Removing the central region while retaining the same mass concentrates more mass at larger radii. Physical check The formula approaches the disk value at a = 0 and the thin-hoop value as a →b.

Question 4

Annular layers contribute angular momentum in proportion to squared radius

A uniform annular plate has mass MM, inner radius aa and outer radius bb. It rotates about its central normal axis at angular speed ω\omega.

Diagram shown in the original SVG worksheet.

  1. Integrate the ring contributions to find LzL_z.

  2. For a=b/2a=b/2, find the ratio to a solid disk of the same mass, outer radius and angular speed.

Question 4 - Solution

Annular layers contribute angular momentum in proportion to squared radius

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

The uniform surface density and differential ring mass are σ=Mπ(b2−a2),dm=2πσrdr.\sigma=\frac{M}{\pi(b^2-a^2)},\qquad dm=2\pi\sigma r\,dr. Integrating, Iz=∫abr2dm=2πσ∫abr3dr=πσ2(b4−a4),I_z=\int_a^b r^2\,dm=2\pi\sigma\int_a^b r^3\,dr =\frac{\pi\sigma}{2}(b^4-a^4), Lz=Izω=12M(a2+b2)ω.\boxed{L_z=I_z\omega=\tfrac12M(a^2+b^2)\omega}.

(b) Result and interpretation

For a=b/2a=b/2, Iannulus=12M(b2/4+b2)=58Mb2.I_{\mathrm{annulus}}=\tfrac12M(b^2/4+b^2)=\frac58Mb^2. At equal mass, outer radius and angular speed, LannulusLdisk=(5/8)Mb2(1/2)Mb2=54.\boxed{\frac{L_{\mathrm{annulus}}}{L_{\mathrm{disk}}}=\frac{(5/8)Mb^2}{(1/2)Mb^2}=\frac54}. Removing the central region while retaining the same mass concentrates more mass at larger radii.

Physical check

The formula approaches the disk value at a=0a=0 and the thin-hoop value as a→ba\to b.