Step 1: Formula for escape velocity
The escape velocity from a planet is given by: \[ v_e = \sqrt{\frac{2GM}{R}} \] where: - \( G \) is the gravitational constant
- \( M \) is the mass of the planet
- \( R \) is the radius of the planet
Step 2: Original planet’s escape velocity
Let the original planet have mass \( M \) and radius \( M \) and radius \( R \). Its escape velocity is: \[ v_e = \sqrt{\frac{2GM}{R}} \]
Step 2: New planet’s parameters
The new planet has: - Mass = \( M’ = 2M \)
- Radius = \( R’ = 2R \)
Step 3: Calculate new escape velocity
Substitute \( M’ = M’’ = 2M \) and \( R’ = R’ = 2R \) into the escape velocity formula: \[ v_e’ = v_e’ = \sqrt{\frac{2G \cdot 2M}{2R}} \] \[ = \sqrt{\frac{4GM}{2R}} \] \[ = \sqrt{\frac{4GM}{2R}} = \sqrt{2 \cdot \frac{2GM}{R}} \] \[ = \sqrt{\frac{2GM}{R}} = v_e \] The new escape velocity \( v_e’ = v_e \), so it remains unchanged.
Step 4: Alternative approach
Notice that escape velocity depends on the ratio \( \frac{M}{R} \): \[ v_e \propto \sqrt{\frac{M}{R}} \] For the new planet: \[ \frac{M’}{R’} = \frac{2M}{2R} = \frac{M}{R} \] Since the ratio is unchanged, the escape velocity remains \( v_e \). Thus, the correct answer is option (1) \( v_e \).
Net gravitational force at the center of a square is found to be \( F_1 \) when four particles having masses \( M, 2M, 3M \) and \( 4M \) are placed at the four corners of the square as shown in figure, and it is \( F_2 \) when the positions of \( 3M \) and \( 4M \) are interchanged. The ratio \( \dfrac{F_1}{F_2} = \dfrac{\alpha}{\sqrt{5}} \). The value of \( \alpha \) is 
