To determine the side length of the square, we will analyze the given information and conditions systematically:
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:
\(\left( \frac{2 \sqrt{2} + 1}{32} \right) \frac{G m^2}{L^2}\)
Each particle at a vertex experiences gravitational forces from the other three particles:
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:
2. Force originating from the diagonally opposite particle:
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:
\(\left(2 + \frac{\sqrt{2}}{2}\right) \frac{G m^2}{L^2} = \left( \frac{2\sqrt{2} + 1}{32} \right) \frac{G m^2}{L^2}\)
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 \(L = 4L\).
Consequently, the side length of the square is determined to be 4L, aligning with the option '4L'.
Net gravitational force at the center of a square is found to be \( F_1 \) when four particles having masses \( M, 2M, 3M \) and \( 4M \) are placed at the four corners of the square as shown in figure, and it is \( F_2 \) when the positions of \( 3M \) and \( 4M \) are interchanged. The ratio \( \dfrac{F_1}{F_2} = \dfrac{\alpha}{\sqrt{5}} \). The value of \( \alpha \) is 
