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A particle is projected vertically upwar...

A particle is projected vertically upward with with velocity `sqrt((2)/(3)(GM)/(R ))` from the surface of Earth. The height attained by it is (G, M, R have usual meanings)

A

3R

B

`(R )/(2)`

C

2R

D

`(R )/(3)`

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The correct Answer is:
To solve the problem of finding the height attained by a particle projected vertically upward with a specific velocity from the surface of the Earth, we can use the principle of conservation of energy. Here’s a step-by-step solution: ### Step-by-Step Solution: 1. **Identify Given Values**: - Initial velocity \( v = \sqrt{\frac{2}{3} \frac{GM}{R}} \) - Mass of the Earth \( M \) - Radius of the Earth \( R \) - Gravitational constant \( G \) 2. **Apply Conservation of Energy**: The total mechanical energy at the surface of the Earth must equal the total mechanical energy at the maximum height \( h \) reached by the particle. \[ \text{Total Energy at Surface} = \text{Total Energy at Height } h \] This can be expressed as: \[ \text{K.E. at surface} + \text{P.E. at surface} = \text{K.E. at height } h + \text{P.E. at height } h \] 3. **Calculate Kinetic and Potential Energy**: - **At the surface**: - Kinetic Energy (K.E.) = \( \frac{1}{2} mv^2 \) - Potential Energy (P.E.) = \( -\frac{GMm}{R} \) - **At height \( h \)**: - K.E. = 0 (at the maximum height, the velocity is 0) - P.E. = \( -\frac{GMm}{R+h} \) 4. **Set Up the Equation**: \[ \frac{1}{2} mv^2 - \frac{GMm}{R} = 0 - \frac{GMm}{R+h} \] 5. **Substitute the Initial Velocity**: Substitute \( v \) into the equation: \[ \frac{1}{2} m \left(\sqrt{\frac{2}{3} \frac{GM}{R}}\right)^2 - \frac{GMm}{R} = -\frac{GMm}{R+h} \] Simplifying the left side: \[ \frac{1}{2} m \cdot \frac{2}{3} \cdot \frac{GM}{R} - \frac{GMm}{R} = -\frac{GMm}{R+h} \] \[ \frac{GMm}{3R} - \frac{GMm}{R} = -\frac{GMm}{R+h} \] 6. **Combine Terms**: \[ \frac{GMm}{3R} - \frac{3GMm}{3R} = -\frac{GMm}{R+h} \] \[ -\frac{2GMm}{3R} = -\frac{GMm}{R+h} \] 7. **Cancel \( GMm \)**: Since \( GMm \) is common on both sides, we can cancel it out: \[ \frac{2}{3R} = \frac{1}{R+h} \] 8. **Cross-Multiply**: \[ 2(R+h) = 3R \] \[ 2R + 2h = 3R \] 9. **Solve for \( h \)**: \[ 2h = 3R - 2R \] \[ 2h = R \] \[ h = \frac{R}{2} \] ### Final Answer: The height attained by the particle is \( h = \frac{R}{2} \).
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