Gravitational Forces at Triangle Centroid

Gravitational Forces at Triangle Centroid

Example 8.2: Three masses at vertices of an equilateral triangle

m
m
m
2m

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:

\[ F_R = 2Gm^2 \hat{j} \]

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