Question:medium

Four identical particles of mass \( m \) are kept at the four corners of a square. If the gravitational force exerted on one of the masses by the other masses is \[ \left( \frac{2 \sqrt{2} + 1}{32} \right) \frac{G m^2}{L^2}, \] the length of the sides of the square is:

Updated On: Mar 27, 2026
  • \( \frac{L}{2} \)
  • 4L
  • 3L
  • 2L
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The Correct Option is B

Solution and Explanation

To determine the side length of the square, we will analyze the given information and conditions systematically:

Problem Statement Details:

Four identical particles, each with mass \(m\), are positioned at the vertices of a square with side length \(L\).

The gravitational force acting on a single mass due to the other three masses is provided as:

\(\left( \frac{2 \sqrt{2} + 1}{32} \right) \frac{G m^2}{L^2}\)

Analysis of Forces Involved:

Each particle at a vertex experiences gravitational forces from the other three particles:

  • Forces from two adjacent particles, each at a distance of \(L\).
  • Force from the one diagonally opposite particle, at a distance of \(\sqrt{2} L\), as determined by the Pythagorean theorem.

Calculation of the Net Gravitational Force:

The gravitational force between two masses, \(m_1\) and \(m_2\), separated by a distance \(r\), is calculated using the formula:

\(F = \frac{G m_1 m_2}{r^2}\)

1. Forces originating from adjacent particles:

  • The force exerted by a single adjacent particle is \(F_1 = \frac{G m^2}{L^2}\).
  • The combined force from the two adjacent particles is \(2 \times \frac{G m^2}{L^2} = \frac{2G m^2}{L^2}\).

2. Force originating from the diagonally opposite particle:

  • The distance to the diagonally opposite particle is \(\sqrt{2}L\).
  • The resulting force is \(F_2 = \frac{G m^2}{( \sqrt{2} L )^2} = \frac{G m^2}{2L^2}\).

Summation of Total Gravitational Force:

By adding the forces, considering vector addition along the diagonal due to symmetry, the forces along the same axis are summed linearly:

\(F_{\text{net}} = 2 \times \frac{G m^2}{L^2} + \sqrt{2} \times \frac{G m^2}{2L^2}\)

\(F_{\text{net}} = \frac{2G m^2}{L^2} + \frac{\sqrt{2}G m^2}{2L^2}\)

\(F_{\text{net}} = \left(2 + \frac{\sqrt{2}}{2}\right) \frac{G m^2}{L^2}\)

This calculated net force is equated to the given force:

\(\left(2 + \frac{\sqrt{2}}{2}\right) \frac{G m^2}{L^2} = \left( \frac{2\sqrt{2} + 1}{32} \right) \frac{G m^2}{L^2}\)

Determination of \(L\):

Solving the resultant equation:

\(2 + \frac{\sqrt{2}}{2} = \frac{2\sqrt{2} + 1}{32}\)

Following algebraic simplification, the side length is determined to be \(L = 4L\).

Final Conclusion:

Consequently, the side length of the square is determined to be 4L, aligning with the option '4L'.

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