Gravitation and the Principle of Superposition — Question 7

Section 13-2 · Physics pages 1924–1925

Question 7 A semicircular arc pulls toward its occupied half A uniform thin semicircular arc of radius R and mass M occupies angles 0 ≤θ ≤π above the x axis. Find the field at the circle center. x y R Schematic; labels, not drawing lengths, specify the data. (a) Integrate the Cartesian field components. (b) Compare its magnitude with placing all the mass at the top of the arc.
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Question 7 - Solution A semicircular arc pulls toward its occupied half x y R (a) Derivation and calculation The arc length is πR, so dm = (M/π)dθ. Resolving sourceward contributions,⃗ g = GM πR2 ∫π 0 (cos θˆi + sin θ ˆj) dθ. gx = GM πR2 [sin θ]π 0 = 0, gy = GM πR2 [−cos θ]π 0 = 2GM πR2 . (b) Result and interpretation Placing the entire mass at the top would produce gpoint = GM/R2, garc/gpoint = 2/π ≃0.63662 . The reduction is the mass-weighted vertical projection: ⟨sin θ⟩= 1 π ∫π 0 sin θ dθ = 2 π. Physical check Left-right symmetry removes horizontal components; the surviving field points toward the occupied upper half.

Question 7

A semicircular arc pulls toward its occupied half

A uniform thin semicircular arc of radius RR and mass MM occupies angles 0≤θ≤π0\le\theta\le\pi above the xx axis. Find the field at the circle center.

Diagram shown in the original SVG worksheet.

  1. Integrate the Cartesian field components.

  2. Compare its magnitude with placing all the mass at the top of the arc.

Question 7 - Solution

A semicircular arc pulls toward its occupied half

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

The arc length is πR\pi R, so dm=(M/π)dθdm=(M/\pi)d\theta. Resolving sourceward contributions, g→=GMπR2∫0π(cos⁡θî+sin⁡θĵ)dθ.\vec g=\frac{GM}{\pi R^2}\int_0^\pi (\cos\theta\,\hat i+\sin\theta\,\hat j)\,d\theta. gx=GMπR2[sin⁡θ]0π=0,gy=GMπR2[−cos⁡θ]0π=2GMπR2.g_x=\frac{GM}{\pi R^2}[\sin\theta]_0^\pi=0,\quad \boxed{g_y=\frac{GM}{\pi R^2}[-\cos\theta]_0^\pi=\frac{2GM}{\pi R^2}}.

(b) Result and interpretation

Placing the entire mass at the top would produce gpoint=GM/R2,garc/gpoint=2/π≃0.63662.g_{\mathrm{point}}=GM/R^2,\qquad \boxed{g_{\mathrm{arc}}/g_{\mathrm{point}}=2/\pi\simeq0.63662}. The reduction is the mass-weighted vertical projection: ⟨sin⁡θ⟩=1π∫0πsin⁡θdθ=2π.\langle\sin\theta\rangle=\frac1\pi\int_0^\pi\sin\theta\,d\theta=\frac2\pi.

Physical check

Left-right symmetry removes horizontal components; the surviving field points toward the occupied upper half.