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A particle is projected radially outward...

A particle is projected radially outwards from the surface of a planet with an initial speed of `4.0km//s`. Maximum height attained by the particle is `h=900km`. Find the radius of the planet taking `g=10m//s^(2)`.

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To solve the problem, we will use the conservation of mechanical energy principle. The total mechanical energy (kinetic + potential) at the surface of the planet will be equal to the total mechanical energy at the maximum height. ### Step-by-Step Solution: 1. **Identify the Known Values:** - Initial speed \( v_i = 4.0 \, \text{km/s} = 4000 \, \text{m/s} \) - Maximum height \( h = 900 \, \text{km} = 900000 \, \text{m} \) - Acceleration due to gravity \( g = 10 \, \text{m/s}^2 \) 2. **Write the Conservation of Energy Equation:** At the surface of the planet: - Initial kinetic energy (KE) = \( \frac{1}{2} m v_i^2 \) - Initial potential energy (PE) = \( -\frac{GMm}{R} \) At the maximum height: - Final kinetic energy (KE) = 0 (since the particle stops momentarily) - Final potential energy (PE) = \( -\frac{GMm}{R + h} \) The conservation of energy gives us: \[ \frac{1}{2} m v_i^2 - \frac{GMm}{R} = -\frac{GMm}{R + h} \] 3. **Simplify the Equation:** Canceling \( m \) from both sides (assuming \( m \neq 0 \)): \[ \frac{1}{2} v_i^2 - \frac{GM}{R} = -\frac{GM}{R + h} \] Rearranging gives: \[ \frac{1}{2} v_i^2 = \frac{GM}{R} - \frac{GM}{R + h} \] 4. **Combine the Terms:** The right-hand side can be combined: \[ \frac{GM}{R} - \frac{GM}{R + h} = GM \left( \frac{1}{R} - \frac{1}{R + h} \right) = GM \left( \frac{(R + h) - R}{R(R + h)} \right) = \frac{GMh}{R(R + h)} \] Thus, we have: \[ \frac{1}{2} v_i^2 = \frac{GMh}{R(R + h)} \] 5. **Substitute \( GM \) Using \( g \):** From the formula \( g = \frac{GM}{R^2} \), we can express \( GM \) as: \[ GM = gR^2 \] Substituting this into our equation gives: \[ \frac{1}{2} v_i^2 = \frac{gR^2h}{R(R + h)} = \frac{gRh}{R + h} \] 6. **Rearranging for \( R \):** Rearranging gives: \[ R + h = \frac{gRh}{\frac{1}{2} v_i^2} \] \[ R + h = \frac{2gRh}{v_i^2} \] \[ R(1 - \frac{2gh}{v_i^2}) = -h \] \[ R = \frac{h}{\frac{2gh}{v_i^2} - 1} \] 7. **Substituting the Values:** Substitute \( g = 10 \, \text{m/s}^2 \), \( h = 900000 \, \text{m} \), and \( v_i = 4000 \, \text{m/s} \): \[ R = \frac{900000}{\frac{2 \times 10 \times 900000}{4000^2} - 1} \] Calculate \( \frac{2 \times 10 \times 900000}{4000^2} \): \[ = \frac{18000000}{16000000} = 1.125 \] Thus, \[ R = \frac{900000}{1.125 - 1} = \frac{900000}{0.125} = 7200000 \, \text{m} = 7200 \, \text{km} \] ### Final Answer: The radius of the planet is approximately \( 7200 \, \text{km} \).
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