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A particle of mass m is projected upward...

A particle of mass m is projected upwards with velocity `v=(v_(e))/(2)`, where `v_(e)` is the escape velocity then at the maximum height the potential energy of the particle is : (R is radius of earth and M is mass of earth)

A

`(-GMm)/(2R)`

B

`(-GMm)/(4R)`

C

`(-3GMm)/(4R)`

D

`(-2GMm)/(3R)`

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem step by step, we will use the principle of conservation of energy. ### Step 1: Understand the given information We have a particle of mass \( m \) projected upwards with a velocity \( v = \frac{v_e}{2} \), where \( v_e \) is the escape velocity. We need to find the potential energy at the maximum height. ### Step 2: Write down the expression for escape velocity The escape velocity \( v_e \) is given by the formula: \[ v_e = \sqrt{\frac{2GM}{R}} \] where \( G \) is the gravitational constant, \( M \) is the mass of the Earth, and \( R \) is the radius of the Earth. ### Step 3: Calculate the initial kinetic energy (KE) and potential energy (PE) at the surface of the Earth The initial kinetic energy at the surface (point A) when the particle is projected is: \[ KE_A = \frac{1}{2} m v^2 = \frac{1}{2} m \left(\frac{v_e}{2}\right)^2 = \frac{1}{2} m \left(\frac{v_e^2}{4}\right) = \frac{m v_e^2}{8} \] The initial potential energy at the surface (point A) is given by: \[ PE_A = -\frac{GMm}{R} \] ### Step 4: Write the total energy at point A The total energy at point A is: \[ E_A = KE_A + PE_A = \frac{m v_e^2}{8} - \frac{GMm}{R} \] ### Step 5: Calculate the potential energy at the maximum height (point P) At the maximum height (point P), the kinetic energy is zero (since the particle stops momentarily). Therefore, the total energy at point P is just the potential energy: \[ E_P = PE_P \] ### Step 6: Apply the conservation of energy principle According to the conservation of energy: \[ E_A = E_P \] Thus, \[ \frac{m v_e^2}{8} - \frac{GMm}{R} = PE_P \] ### Step 7: Substitute the expression for escape velocity Substituting \( v_e^2 = \frac{2GM}{R} \) into the equation: \[ \frac{m \left(\frac{2GM}{R}\right)}{8} - \frac{GMm}{R} = PE_P \] This simplifies to: \[ \frac{mGM}{4R} - \frac{GMm}{R} = PE_P \] ### Step 8: Simplify the equation Taking a common factor of \( \frac{GMm}{R} \): \[ PE_P = \frac{GMm}{R} \left(\frac{1}{4} - 1\right) = \frac{GMm}{R} \left(-\frac{3}{4}\right) \] Thus, we have: \[ PE_P = -\frac{3GMm}{4R} \] ### Final Answer The potential energy of the particle at the maximum height is: \[ PE_P = -\frac{3GMm}{4R} \]
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