Question:

At a height \( h \) above the Earth's surface, the acceleration due to gravity becomes \( \frac{g}{\sqrt{3}} \). What is the value of \( h \) in terms of the Earth's radius \( R \)?

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When working with gravitational problems involving height above the Earth's surface, remember to use the formula for gravity variation with height: \( g_h = \frac{g}{(1 + \frac{h}{R})^2} \).
Updated On: Apr 15, 2025
  • \( R \)
  • \( \sqrt{2}R \)
  • \( 2R \)
  • \( \frac{R}{2} \)
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The Correct Option is A

Solution and Explanation


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).
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