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If an object is projected vertically ...

If an object is projected vertically upwards with speed , half the escape speed of earth , then the aximum height attained by it is [ R is radius of earth ]

A

R

B

`R/2`

C

`2 R`

D

`R/3`

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To solve the problem of finding the maximum height attained by an object projected vertically upwards with a speed equal to half the escape speed of Earth, we can use the principle of conservation of energy. ### Step-by-Step Solution: 1. **Identify Escape Velocity**: The escape velocity \( V_E \) from the surface of the Earth is given by the formula: \[ V_E = \sqrt{2gR} \] where \( g \) is the acceleration due to gravity at the surface of the Earth, and \( R \) is the radius of the Earth. 2. **Determine Initial Velocity**: The initial velocity \( V \) of the object is half the escape velocity: \[ V = \frac{V_E}{2} = \frac{1}{2} \sqrt{2gR} = \frac{\sqrt{2gR}}{2} \] 3. **Calculate Initial Kinetic Energy**: The initial kinetic energy \( KE_i \) of the object when it is projected is given by: \[ KE_i = \frac{1}{2} m V^2 = \frac{1}{2} m \left(\frac{\sqrt{2gR}}{2}\right)^2 = \frac{1}{2} m \left(\frac{2gR}{4}\right) = \frac{mgR}{4} \] 4. **Calculate Initial Potential Energy**: The initial potential energy \( PE_i \) of the object at the surface of the Earth is: \[ PE_i = -\frac{GMm}{R} \] where \( G \) is the gravitational constant and \( M \) is the mass of the Earth. 5. **Set Up Conservation of Energy Equation**: At the maximum height \( H \), the kinetic energy will be zero, and the potential energy will be: \[ PE_f = -\frac{GMm}{R + H} \] By conservation of energy, we have: \[ KE_i + PE_i = KE_f + PE_f \] Substituting the values we calculated: \[ \frac{mgR}{4} - \frac{GMm}{R} = 0 - \frac{GMm}{R + H} \] 6. **Simplify the Equation**: Rearranging the equation gives: \[ \frac{mgR}{4} - \frac{GMm}{R} = -\frac{GMm}{R + H} \] Multiplying through by \( R(R + H) \) to eliminate the denominators: \[ \frac{mgR^2(R + H)}{4} - GMm(R + H) = -GMmR \] 7. **Substituting \( GM \)**: We know from the definition of \( g \) that \( g = \frac{GM}{R^2} \), thus \( GM = gR^2 \). Substituting this into the equation: \[ \frac{mgR^2(R + H)}{4} - gR^2(R + H) = -gR^2 \] 8. **Solving for Height \( H \)**: Rearranging gives: \[ \frac{mgR^2(R + H)}{4} = gR^2(R + H) - gR^2 \] Simplifying further, we can isolate \( H \): \[ \frac{mgR^2}{4} = gR^2 - gR^2\frac{R}{R + H} \] Solving this will yield: \[ H = \frac{R}{3} \] ### Final Answer: The maximum height attained by the object is: \[ H = \frac{R}{3} \]
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