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The ratio of escape velocity at earth (...

The ratio of escape velocity at earth `(v_(e))` to the escape velocity at a planet `(v_(p))` whose radius and mean density in twice as that of earth is

A

`1 : 2`

B

`1 : 2 sqrt(2)`

C

` 1 : 4 `

D

`1 : 2 `

Text Solution

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The correct Answer is:
To find the ratio of escape velocity at Earth `(v_e)` to the escape velocity at a planet `(v_p)` whose radius and mean density are twice that of Earth, we can follow these steps: ### Step-by-Step Solution: 1. **Define Escape Velocity**: The escape velocity `v` from a celestial body is given by the formula: \[ v = \sqrt{\frac{2GM}{R}} \] where \( G \) is the gravitational constant, \( M \) is the mass of the body, and \( R \) is its radius. 2. **Escape Velocity for Earth**: For Earth, we denote the radius as \( R_e \) and the mass as \( M_e \). Thus, the escape velocity at Earth \( v_e \) is: \[ v_e = \sqrt{\frac{2GM_e}{R_e}} \] 3. **Mass of Earth in terms of Density**: The mass of Earth can be expressed in terms of its density \( \rho \): \[ M_e = \rho \cdot V_e = \rho \cdot \left(\frac{4}{3} \pi R_e^3\right) \] Therefore, substituting this into the escape velocity formula gives: \[ v_e = \sqrt{\frac{2G \left(\rho \cdot \frac{4}{3} \pi R_e^3\right)}{R_e}} = \sqrt{\frac{8\pi G \rho R_e^2}{3}} \] 4. **Escape Velocity for the Planet**: For the planet, its radius \( R_p \) is twice that of Earth, so: \[ R_p = 2R_e \] The density of the planet is also twice that of Earth: \[ \rho_p = 2\rho \] The mass of the planet \( M_p \) can be calculated as: \[ M_p = \rho_p \cdot V_p = 2\rho \cdot \left(\frac{4}{3} \pi (2R_e)^3\right) = 2\rho \cdot \left(\frac{4}{3} \pi \cdot 8R_e^3\right) = \frac{64}{3} \pi \rho R_e^3 \] Now, substituting this into the escape velocity formula for the planet gives: \[ v_p = \sqrt{\frac{2GM_p}{R_p}} = \sqrt{\frac{2G \left(\frac{64}{3} \pi \rho R_e^3\right)}{2R_e}} = \sqrt{\frac{64\pi G \rho R_e^2}{3}} \] 5. **Finding the Ratio**: Now we can find the ratio of the escape velocities: \[ \frac{v_e}{v_p} = \frac{\sqrt{\frac{8\pi G \rho R_e^2}{3}}}{\sqrt{\frac{64\pi G \rho R_e^2}{3}}} \] Simplifying this gives: \[ \frac{v_e}{v_p} = \frac{\sqrt{8}}{\sqrt{64}} = \frac{2\sqrt{2}}{8} = \frac{1}{2\sqrt{2}} \] ### Final Answer: The ratio of escape velocity at Earth to the escape velocity at the planet is: \[ \frac{v_e}{v_p} = \frac{1}{2\sqrt{2}} \]

To find the ratio of escape velocity at Earth `(v_e)` to the escape velocity at a planet `(v_p)` whose radius and mean density are twice that of Earth, we can follow these steps: ### Step-by-Step Solution: 1. **Define Escape Velocity**: The escape velocity `v` from a celestial body is given by the formula: \[ v = \sqrt{\frac{2GM}{R}} ...
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