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Let escape velocity od a body a kept...

Let escape velocity od a body a kept surface of a planet is u , If it is projected at a speed of 200 % more than the escape speed , then its speed in interstellar space will be

A

u

B

`sqrt(3)` u

C

`2u`

D

`2sqrt(2)u`

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem, we need to find the speed of a body in interstellar space after it has been projected at a speed that is 200% more than the escape velocity of the planet. ### Step-by-Step Solution: 1. **Understanding Escape Velocity**: The escape velocity (u) is the minimum speed required for an object to break free from the gravitational attraction of a planet without any additional propulsion. 2. **Calculating the Projected Speed**: The body is projected at a speed that is 200% more than the escape velocity. \[ \text{Projected speed} = u + 200\% \text{ of } u = u + 2u = 3u \] So, the initial speed (v) of the body when projected is \(3u\). 3. **Understanding the Energy Conservation**: When the body is projected, it has both kinetic and potential energy. As it moves away from the planet, the potential energy approaches zero when it reaches interstellar space. 4. **Setting Up the Energy Equation**: The total mechanical energy at the surface of the planet is the sum of kinetic energy (KE) and gravitational potential energy (PE): \[ \text{Total Energy at surface} = KE + PE = \frac{1}{2}mv^2 - \frac{GMm}{R} \] where \(v = 3u\), \(G\) is the gravitational constant, \(M\) is the mass of the planet, and \(R\) is the radius of the planet. 5. **Calculating Initial Total Energy**: Substitute \(v = 3u\): \[ \text{Total Energy} = \frac{1}{2}m(3u)^2 - \frac{GMm}{R} = \frac{9}{2}mu^2 - \frac{GMm}{R} \] 6. **Final Energy in Interstellar Space**: In interstellar space, the potential energy is zero, and the kinetic energy is given by: \[ \text{Total Energy in interstellar space} = \frac{1}{2}mV_1^2 \] where \(V_1\) is the speed in interstellar space. 7. **Setting the Energies Equal**: Since energy is conserved, we can set the total energy at the surface equal to the total energy in interstellar space: \[ \frac{9}{2}mu^2 - \frac{GMm}{R} = \frac{1}{2}mV_1^2 \] 8. **Substituting for \(GM/R\)**: From the escape velocity formula, we know: \[ u^2 = \frac{2GM}{R} \implies \frac{GM}{R} = \frac{u^2}{2} \] Substitute this into the energy equation: \[ \frac{9}{2}mu^2 - \frac{m}{2}u^2 = \frac{1}{2}mV_1^2 \] Simplifying gives: \[ \frac{8}{2}mu^2 = \frac{1}{2}mV_1^2 \implies 4mu^2 = \frac{1}{2}mV_1^2 \] 9. **Solving for \(V_1\)**: Cancel \(m\) from both sides: \[ 4u^2 = \frac{1}{2}V_1^2 \implies V_1^2 = 8u^2 \implies V_1 = \sqrt{8}u = 2\sqrt{2}u \] 10. **Final Result**: The speed of the body in interstellar space is: \[ V_1 = 2\sqrt{2}u \]
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