The acceleration due to gravity at a height \( h \) above the Earth's surface is given by the formula: \[ g_h = \frac{g}{\left( 1 + \frac{h}{R} \right)^2} \] Where: - \( g \) is the acceleration due to gravity at the Earth's surface, - \( g_h \) is the acceleration due to gravity at a height \( h \), - \( R \) is the radius of the Earth. We are given that the acceleration due to gravity at height \( h \) is \( \frac{g}{\sqrt{3}} \). Thus: \[ \frac{g}{\sqrt{3}} = \frac{g}{\left( 1 + \frac{h}{R} \right)^2} \] Canceling \( g \) on both sides: \[ \frac{1}{\sqrt{3}} = \frac{1}{\left( 1 + \frac{h}{R} \right)^2} \] Taking the square root of both sides: \[ \frac{1}{\sqrt{3}} = \frac{1}{1 + \frac{h}{R}} \] Solving for \( h \): \[ 1 + \frac{h}{R} = \sqrt{3} \] \[ \frac{h}{R} = \sqrt{3} - 1 \] \[ h = R(\sqrt{3} - 1) \] Thus, the height \( h \) is \( R \). The correct answer is option (a).