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Physics · Ch 6 — Gravitation

Superposition Principle for Gravitational Field

6.2.2

Superposition Principle for Gravitational Field

The superposition principle. When nn different masses m1,m2,…,mnm_1, m_2, \dots, m_n are all present, the total gravitational field they produce together at any point PP is simply the vector sum of the individual fields each one would produce alone:

E⃗total=E⃗1+E⃗2+⋯+E⃗n=−∑i=1nGmiri2r^i.(6.20)\vec{E}_{total}=\vec{E}_1+\vec{E}_2+\cdots+\vec{E}_n=-\sum_{i=1}^{n}\frac{Gm_i}{r_i^2}\hat{r}_i. \qquad (6.20)

If instead of discrete point masses we have a continuous distribution of total mass MM, the same idea is applied using integration.

Worked example (two masses on the axes). Masses m1m_1 and m2m_2 sit on the yy- and xx-axes respectively, each a distance aa from the origin, and we want the field at the origin PP. The field due to m1m_1 alone points along −j^-\hat{j} (toward m1m_1) with magnitude Gm1/a2Gm_1/a^2; the field due to m2m_2 alone points along −i^-\hat{i} with magnitude Gm2/a2Gm_2/a^2. Adding them as vectors,

E⃗total=−Gm1a2j^−Gm2a2i^=−Ga2(m2i^+m1j^),\vec{E}_{total}=-\frac{Gm_1}{a^2}\hat{j}-\frac{Gm_2}{a^2}\hat{i}=-\frac{G}{a^2}\left(m_2\hat{i}+m_1\hat{j}\right),

and if m1=m2=mm_1=m_2=m, this simplifies (using i^+j^\hat{i}+\hat{j} as a single diagonal direction) to E⃗total=−2 Gma2\vec{E}_{total}=-\dfrac{\sqrt{2}\,Gm}{a^2} pointing diagonally back toward the origin from the midpoint of m1m_1 and m2m_2 -- the resultant direction is fixed purely by the relative sizes of m1m_1 and m2m_2. …

Figure 6.11Superposing two gravitational fields

What this figure shows. Two source masses each produce their own field vector, E1 and E2, at a common point P; the diagram shows these two vectors being added tip-to-tail (vector addition) to construct the single resultant vector E_total, which is the actual, net field a test mass at P would experience from both sources acting tog …