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A mass is taken to a height R from the s...

A mass is taken to a height R from the surface of earth and then is given horizontal velocity v. The minimum value of v so that mass escapes to infinity is `sqrt((GM)/(nR))`. Find the value of n.

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To solve the problem, we need to determine the minimum horizontal velocity \( v \) that a mass must have when taken to a height \( R \) above the Earth's surface in order to escape the Earth's gravitational field. The formula given for this minimum velocity is \( v = \sqrt{\frac{GM}{nR}} \), and we need to find the value of \( n \). ### Step-by-Step Solution: 1. **Understand the Situation**: - The mass is taken to a height \( R \) above the Earth's surface. - The distance from the center of the Earth to the mass at this height is \( R + R = 2R \). 2. **Use Conservation of Energy**: - The total mechanical energy at the height \( R \) must equal the total mechanical energy at infinity. - At infinity, the potential energy (U) is zero, and we want the kinetic energy (K) to also be zero for the minimum escape velocity. 3. **Write the Energy Conservation Equation**: \[ K_i + U_i = K_f + U_f \] - Where: - \( K_i = \frac{1}{2} mv^2 \) (initial kinetic energy) - \( U_i = -\frac{GMm}{2R} \) (potential energy at height \( R \)) - \( K_f = 0 \) (final kinetic energy at infinity) - \( U_f = 0 \) (potential energy at infinity) Thus, the equation becomes: \[ \frac{1}{2} mv^2 - \frac{GMm}{2R} = 0 \] 4. **Simplify the Equation**: - Rearranging gives: \[ \frac{1}{2} mv^2 = \frac{GMm}{2R} \] - Dividing both sides by \( m \) (mass of the object): \[ \frac{1}{2} v^2 = \frac{GM}{2R} \] 5. **Solve for \( v^2 \)**: - Multiply both sides by 2: \[ v^2 = \frac{GM}{R} \] 6. **Relate to the Given Formula**: - We want to express \( v \) in the form \( v = \sqrt{\frac{GM}{nR}} \). - From our derived formula, we have: \[ v^2 = \frac{GM}{R} \] - Comparing this with \( v^2 = \frac{GM}{nR} \), we can see that: \[ n = 1 \] ### Conclusion: The value of \( n \) is \( 1 \).
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