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Two particles are projected vertically upwards from the surface of the earth with velocities `upsilon_(1) = sqrt((2gR)/3) and upsilon_(2) = sqrt((4gR)/(3))` respectively. If the maximum heights attained by the two particles are `h_(1)` and `h_(2)` respectively, then calculate the ratio `(h_1)/(h_2)`.

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To solve the problem, we will use the principle of conservation of energy. The maximum height attained by a particle projected vertically upwards can be derived from the initial kinetic energy and the change in gravitational potential energy. ### Step-by-Step Solution: 1. **Identify the Given Values:** - For particle 1: \( v_1 = \sqrt{\frac{2gR}{3}} \) - For particle 2: \( v_2 = \sqrt{\frac{4gR}{3}} \) 2. **Use the Conservation of Energy:** The total mechanical energy (kinetic + potential) at the point of projection will equal the total mechanical energy at the maximum height. For a particle projected upwards: \[ \text{Initial Kinetic Energy} = \text{Final Potential Energy} - \text{Initial Potential Energy} \] \[ \frac{1}{2} mv^2 = mgh + \left(-\frac{GMm}{R}\right) \] 3. **Calculate Maximum Height for Particle 1:** \[ \frac{1}{2} m v_1^2 = mg h_1 + \left(-\frac{GMm}{R}\right) \] Substituting \( v_1 \): \[ \frac{1}{2} m \left(\sqrt{\frac{2gR}{3}}\right)^2 = mg h_1 - \frac{GMm}{R} \] Simplifying: \[ \frac{1}{2} m \cdot \frac{2gR}{3} = mg h_1 - \frac{GMm}{R} \] \[ \frac{mgR}{3} = mg h_1 - \frac{GMm}{R} \] Rearranging gives: \[ mg h_1 = \frac{mgR}{3} + \frac{GMm}{R} \] Dividing by \( mg \): \[ h_1 = \frac{R}{3} + \frac{GM}{gR} \] 4. **Calculate Maximum Height for Particle 2:** \[ \frac{1}{2} m v_2^2 = mg h_2 + \left(-\frac{GMm}{R}\right) \] Substituting \( v_2 \): \[ \frac{1}{2} m \left(\sqrt{\frac{4gR}{3}}\right)^2 = mg h_2 - \frac{GMm}{R} \] Simplifying: \[ \frac{1}{2} m \cdot \frac{4gR}{3} = mg h_2 - \frac{GMm}{R} \] \[ \frac{2mgR}{3} = mg h_2 - \frac{GMm}{R} \] Rearranging gives: \[ mg h_2 = \frac{2mgR}{3} + \frac{GMm}{R} \] Dividing by \( mg \): \[ h_2 = \frac{2R}{3} + \frac{GM}{gR} \] 5. **Calculate the Ratio \( \frac{h_1}{h_2} \):** \[ \frac{h_1}{h_2} = \frac{\left(\frac{R}{3} + \frac{GM}{gR}\right)}{\left(\frac{2R}{3} + \frac{GM}{gR}\right)} \] Let \( x = \frac{GM}{gR} \): \[ \frac{h_1}{h_2} = \frac{\frac{1}{3} + x}{\frac{2}{3} + x} \] Cross-multiplying gives: \[ = \frac{1 + 3x}{2 + 3x} \] As \( x \) approaches zero (for large R), this simplifies to: \[ \frac{1}{2} \] 6. **Final Result:** Therefore, the ratio of the maximum heights attained by the two particles is: \[ \frac{h_1}{h_2} = \frac{1}{2} \]
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