Gravitational Forces at Triangle Centroid
Example 8.2: Three masses at vertices of an equilateral triangle
Example
Question:
Three equal masses of \(m\) kg each are fixed at the vertices of an equilateral triangle \(ABC\).
(a) What is the force acting on a mass \(2m\) placed at the centroid \(G\) of the triangle?
(b) What is the force if the mass at the vertex \(A\) is doubled?
Take \(AG = BG = CG = 1\,\mathrm{m}\).
Solution:
(a) The angle between \(GC\) and the positive \(x\)-axis is \(30^\circ\) and so is the angle between \(GB\) and the negative \(x\)-axis. The individual forces in vector notation are:
\[
\vec{F}_{GA} = \frac{Gm(2m)}{1} \hat{j}
\]
\[
\vec{F}_{GB} = \frac{Gm(2m)}{1} (-\hat{i}\cos 30^\circ - \hat{j}\sin 30^\circ)
\]
\[
\vec{F}_{GC} = \frac{Gm(2m)}{1} (+\hat{i}\cos 30^\circ - \hat{j}\sin 30^\circ)
\]
The resultant gravitational force \(\vec{F}_R\) on \(2m\) at \(G\) is:
\[
\vec{F}_R = \vec{F}_{GA} + \vec{F}_{GB} + \vec{F}_{GC}
\]
\[
\vec{F}_R = 2Gm^2\hat{j} + 2Gm^2(-\hat{j}\sin 30^\circ) = 0
\]
Thus, by symmetry, the resultant force is zero.
(b) Now if the mass at vertex \(A\) is doubled,
\[
\vec{F'}_{GA} = \frac{G(2m)2m}{1} \hat{j} = 4Gm^2\hat{j}
\]
\[
\vec{F'}_R = \vec{F'}_{GA} + \vec{F}_{GB} + \vec{F}_{GC} = 2Gm^2\hat{j}
\]
Results:
Net force on centroid mass (2m): 0 N
Force components:
x-component: 0 N
y-component: 0 N
Physics Explanation:
This simulation demonstrates the gravitational forces acting on a mass placed at the centroid of an equilateral triangle with masses at its vertices.
Case (a): All masses equal (m)
The gravitational force from each vertex mass cancels out at the centroid due to symmetry. The net force is zero.
Case (b): Mass at vertex A doubled (2m)
When the mass at vertex A is doubled, the forces no longer cancel completely. The resultant force is:
\[ F_R = F_{GA} + F_{GB} + F_{GC} \]
Where:
- \( F_{GA} = \frac{G(2m)(2m)}{1^2} \hat{j} = 4Gm^2 \hat{j} \)
- \( F_{GB} = \frac{Gm(2m)}{1^2} (-\cos30^\circ \hat{i} - \sin30^\circ \hat{j}) \)
- \( F_{GC} = \frac{Gm(2m)}{1^2} (\cos30^\circ \hat{i} - \sin30^\circ \hat{j}) \)
The x-components from B and C cancel out, while the y-components add up to:
\[ F_R = 2Gm^2 \hat{j} \]



