Gravitation and the Principle of Superposition — Question 4

Section 13-2 · Physics pages 1918–1919

Question 4 Removing one corner mass can be solved by subtracting its field Four equal point masses M originally occupy the corners (±a, ±a) of a square. The mass at (a, a) is removed. removed Schematic; labels, not drawing lengths, specify the data. (a) Find the field at the center without summing three separate vectors. (b) Give its magnitude and direction.
Show solutionHide solution
Question 4 - Solution Removing one corner mass can be solved by subtracting its field removed (a) Derivation and calculation By symmetry, the full square has⃗gfull = 0. The removed source contributes⃗ gremoved = GM aˆi + aˆj ( √ 2a)3 = GM 2 √ 2a2 (ˆi + ˆj). Therefore⃗ gremaining =⃗gfull −⃗gremoved = −GM 2 √ 2a2 (ˆi + ˆj) . (b) Result and interpretation Its norm and unit direction are |⃗g| = GM 2a2 , ˆg = − ˆi + ˆj √ 2 . The field points toward (−a, −a), opposite the empty corner. Subtraction is a superposition calculation, without introducing physical negative mass. Physical check The remaining field has exactly the magnitude of the removed contribution and the opposite direction.

Question 4

Removing one corner mass can be solved by subtracting its field

Four equal point masses MM originally occupy the corners (±a,±a)(\pm a,\pm a) of a square. The mass at (a,a)(a,a) is removed.

Diagram shown in the original SVG worksheet.

  1. Find the field at the center without summing three separate vectors.

  2. Give its magnitude and direction.

Question 4 - Solution

Removing one corner mass can be solved by subtracting its field

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

By symmetry, the full square has g→full=0\vec g_{\mathrm{full}}=0. The removed source contributes g→removed=GMaî+aĵ(2a)3=GM22a2(î+ĵ).\vec g_{\mathrm{removed}}=GM\frac{a\hat i+a\hat j}{(\sqrt2a)^3} =\frac{GM}{2\sqrt2a^2}(\hat i+\hat j). Therefore g→remaining=g→full−g→removed=−GM22a2(î+ĵ).\boxed{\vec g_{\mathrm{remaining}}=\vec g_{\mathrm{full}}-\vec g_{\mathrm{removed}} =-\frac{GM}{2\sqrt2a^2}(\hat i+\hat j)}.

(b) Result and interpretation

Its norm and unit direction are |g→|=GM2a2,ĝ=−î+ĵ2.\boxed{|\vec g|=\frac{GM}{2a^2}},\qquad \hat g=-\frac{\hat i+\hat j}{\sqrt2}. The field points toward (−a,−a)(-a,-a), opposite the empty corner. Subtraction is a superposition calculation, without introducing physical negative mass.

Physical check

The remaining field has exactly the magnitude of the removed contribution and the opposite direction.