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An asteroid is moving directly towards t...

An asteroid is moving directly towards the centre of the earth. When at a distance of 4R (R is the radius of the earth) from the earths centre, it has a speed of `2sqrt2` km/s. Neglecting the effect of earths atmosphere, what will be the speed of the asteroid when it hits the surface of the earth (escape velocity from the earth is 11.2 km/s)? Give your answer to the nearest integer in kilometer/s _________.

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To solve the problem, we will apply the principle of conservation of mechanical energy. The total mechanical energy (kinetic energy + gravitational potential energy) of the asteroid at a distance of 4R from the center of the Earth will be equal to its total mechanical energy just before it hits the surface of the Earth. ### Step-by-Step Solution: 1. **Identify the initial conditions:** - Initial distance from the center of the Earth, \( r_i = 4R \) - Initial speed of the asteroid, \( v_i = 2\sqrt{2} \) km/s - Escape velocity from the Earth, \( v_e = 11.2 \) km/s 2. **Calculate the initial kinetic energy (KE) and gravitational potential energy (PE):** - Kinetic Energy at \( r_i \): \[ KE_i = \frac{1}{2} m v_i^2 = \frac{1}{2} m (2\sqrt{2})^2 = \frac{1}{2} m \cdot 8 = 4m \text{ (in km}^2\text{/s}^2\text{)} \] - Gravitational Potential Energy at \( r_i \): \[ PE_i = -\frac{GMm}{r_i} = -\frac{GMm}{4R} \] 3. **Identify the final conditions:** - Final distance from the center of the Earth, \( r_f = R \) - Final speed of the asteroid, \( v_f \) (unknown) 4. **Calculate the final kinetic energy (KE) and gravitational potential energy (PE):** - Kinetic Energy just before hitting the Earth: \[ KE_f = \frac{1}{2} m v_f^2 \] - Gravitational Potential Energy at the surface of the Earth: \[ PE_f = -\frac{GMm}{R} \] 5. **Apply conservation of mechanical energy:** \[ KE_i + PE_i = KE_f + PE_f \] Substituting the expressions we have: \[ 4m - \frac{GMm}{4R} = \frac{1}{2} m v_f^2 - \frac{GMm}{R} \] 6. **Cancel the mass \( m \) from the equation:** \[ 4 - \frac{GM}{4R} = \frac{1}{2} v_f^2 - \frac{GM}{R} \] 7. **Rearranging the equation:** \[ \frac{1}{2} v_f^2 = 4 - \frac{GM}{4R} + \frac{GM}{R} \] \[ \frac{1}{2} v_f^2 = 4 + \frac{3GM}{4R} \] 8. **Substituting \( \frac{GM}{R} \) using escape velocity:** \[ v_e^2 = \frac{2GM}{R} \Rightarrow GM = \frac{v_e^2 R}{2} \] Substituting \( v_e = 11.2 \) km/s: \[ GM = \frac{(11.2)^2 R}{2} \] 9. **Substituting back into the equation:** \[ \frac{1}{2} v_f^2 = 4 + \frac{3 \cdot \frac{(11.2)^2 R}{2}}{4R} \] \[ \frac{1}{2} v_f^2 = 4 + \frac{3 \cdot 11.2^2}{8} \] 10. **Calculating \( 11.2^2 \):** \[ 11.2^2 = 125.44 \] \[ \frac{3 \cdot 125.44}{8} = 47.04 \] \[ \frac{1}{2} v_f^2 = 4 + 47.04 = 51.04 \] 11. **Solving for \( v_f^2 \):** \[ v_f^2 = 2 \cdot 51.04 = 102.08 \] 12. **Taking the square root to find \( v_f \):** \[ v_f = \sqrt{102.08} \approx 10.1 \text{ km/s} \] 13. **Rounding to the nearest integer:** \[ v_f \approx 10 \text{ km/s} \] ### Final Answer: The speed of the asteroid when it hits the surface of the Earth is approximately **10 km/s**.

To solve the problem, we will apply the principle of conservation of mechanical energy. The total mechanical energy (kinetic energy + gravitational potential energy) of the asteroid at a distance of 4R from the center of the Earth will be equal to its total mechanical energy just before it hits the surface of the Earth. ### Step-by-Step Solution: 1. **Identify the initial conditions:** - Initial distance from the center of the Earth, \( r_i = 4R \) - Initial speed of the asteroid, \( v_i = 2\sqrt{2} \) km/s - Escape velocity from the Earth, \( v_e = 11.2 \) km/s ...
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