This problem is solved by analyzing the given conditions alongside the equations of motion and energy.
The formulas for potential and kinetic energy are as follows:
The problem states that \(KE = 3 \times PE\).
\(\frac{1}{2}mv^2 = 3 \times mgh\)
\(v^2 = 6gh\) (Equation 1)
By the principle of conservation of energy, the total mechanical energy at the start equals the total mechanical energy at height \(h\).
Equating the initial and current energies:
\(mgS = mgh + \frac{1}{2}mv^2\)
\(mgS = mgh + 3mgh\) (since KE = 3PE)
\(mgS = 4mgh\)
\(gS = 4gh\)
\(h = \frac{S}{4}\) (Equation 2)
Substituting Equation 2 into Equation 1 yields the velocity:
\(v^2 = 6g \left(\frac{S}{4}\right)\)
\(v^2 = \frac{3gS}{2}\)
\(v = \sqrt{\frac{3gS}{2}}\)
Consequently, the particle is at a height of \(\frac{S}{4}\) from the surface, and its speed is \(\sqrt{\frac{3gS}{2}}\).
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 
