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A small body of mass m falls to the eart...

A small body of mass m falls to the earth from infintie distance away. What will be its velocity or reaching the earth? (Radius of the earth = R, acceleration due to gravity on the surface of the earth is g) :-

A

`gR`

B

2gR

C

`sqrt(gR)`

D

`sqrt(2gR)`

Text Solution

AI Generated Solution

The correct Answer is:
To find the velocity of a small body of mass \( m \) falling to the Earth from an infinite distance, we can use the principle of conservation of mechanical energy. Here’s a step-by-step solution: ### Step 1: Understand the Initial and Final States - **Initial State**: The body is at an infinite distance from the Earth. At this point, both the potential energy and kinetic energy are zero. \[ U_i = 0, \quad K_i = 0 \] - **Final State**: The body reaches the surface of the Earth. At this point, it has potential energy and kinetic energy. \[ U_f = -\frac{G M m}{R}, \quad K_f = \frac{1}{2} m v^2 \] where \( G \) is the gravitational constant, \( M \) is the mass of the Earth, and \( R \) is the radius of the Earth. ### Step 2: Apply Conservation of Mechanical Energy According to the conservation of mechanical energy: \[ U_i + K_i = U_f + K_f \] Substituting the values: \[ 0 + 0 = -\frac{G M m}{R} + \frac{1}{2} m v^2 \] ### Step 3: Rearranging the Equation Rearranging the equation gives: \[ \frac{1}{2} m v^2 = \frac{G M m}{R} \] ### Step 4: Cancel the Mass \( m \) Since \( m \) is present on both sides of the equation, we can cancel it out (assuming \( m \neq 0 \)): \[ \frac{1}{2} v^2 = \frac{G M}{R} \] ### Step 5: Solve for Velocity \( v \) Multiplying both sides by 2: \[ v^2 = \frac{2 G M}{R} \] Taking the square root gives: \[ v = \sqrt{\frac{2 G M}{R}} \] ### Step 6: Relate \( G \) to \( g \) We know that the acceleration due to gravity \( g \) at the surface of the Earth is given by: \[ g = \frac{G M}{R^2} \] From this, we can express \( G M \) in terms of \( g \) and \( R \): \[ G M = g R^2 \] ### Step 7: Substitute \( G M \) in the Velocity Equation Substituting \( G M \) back into the velocity equation: \[ v = \sqrt{\frac{2 g R^2}{R}} = \sqrt{2 g R} \] ### Final Answer Thus, the velocity of the body when it reaches the surface of the Earth is: \[ v = \sqrt{2 g R} \]
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