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A particle is released from rest from a tower of height 3h. The ratio of time intervals for fall of equal height h i.e. `t_(1):t_(2):t_(3)` is :

A

`sqrt(3):sqrt(2):1`

B

`3:2:1`

C

`9:4:1`

D

`1:(sqrt(2)-1):(sqrt(3)-sqrt(2))`

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To solve the problem of finding the ratio of time intervals \( t_1 : t_2 : t_3 \) for a particle falling from a height of \( 3h \) in equal height segments of \( h \), we can use the equations of motion under uniform acceleration due to gravity. ### Step-by-Step Solution: 1. **Understanding the Problem**: - The particle is released from rest from a height of \( 3h \). - We need to find the time intervals \( t_1 \), \( t_2 \), and \( t_3 \) for each segment of height \( h \). 2. **Using the Kinematic Equation**: - The kinematic equation for distance under uniform acceleration is: \[ s = ut + \frac{1}{2} g t^2 \] - Here, \( u = 0 \) (the initial velocity since the particle is released from rest), \( g \) is the acceleration due to gravity, and \( s \) is the distance fallen. 3. **Calculating \( t_1 \)**: - For the first segment of height \( h \): \[ h = 0 \cdot t_1 + \frac{1}{2} g t_1^2 \] \[ h = \frac{1}{2} g t_1^2 \] \[ t_1^2 = \frac{2h}{g} \] \[ t_1 = \sqrt{\frac{2h}{g}} \] 4. **Calculating \( t_2 \)**: - For the second segment, the particle has already fallen \( h \) and is now falling another \( h \) from a height of \( 2h \). The time taken to fall \( 2h \) (from rest) is: \[ 2h = 0 \cdot (t_1 + t_2) + \frac{1}{2} g (t_1 + t_2)^2 \] \[ 2h = \frac{1}{2} g (t_1 + t_2)^2 \] \[ (t_1 + t_2)^2 = \frac{4h}{g} \] \[ t_1 + t_2 = \sqrt{\frac{4h}{g}} = 2\sqrt{\frac{h}{g}} \] 5. **Calculating \( t_3 \)**: - For the third segment, the particle has fallen \( 3h \) from rest: \[ 3h = 0 \cdot (t_1 + t_2 + t_3) + \frac{1}{2} g (t_1 + t_2 + t_3)^2 \] \[ 3h = \frac{1}{2} g (t_1 + t_2 + t_3)^2 \] \[ (t_1 + t_2 + t_3)^2 = \frac{6h}{g} \] \[ t_1 + t_2 + t_3 = \sqrt{\frac{6h}{g}} = \sqrt{6} \sqrt{\frac{h}{g}} \] 6. **Finding the Ratios**: - We have: - \( t_1 = \sqrt{\frac{2h}{g}} \) - \( t_1 + t_2 = 2\sqrt{\frac{h}{g}} \) - \( t_1 + t_2 + t_3 = \sqrt{6} \sqrt{\frac{h}{g}} \) - From \( t_1 + t_2 \): \[ t_2 = (t_1 + t_2) - t_1 = 2\sqrt{\frac{h}{g}} - \sqrt{\frac{2h}{g}} = \left(2 - \sqrt{2}\right) \sqrt{\frac{h}{g}} \] - From \( t_1 + t_2 + t_3 \): \[ t_3 = (t_1 + t_2 + t_3) - (t_1 + t_2) = \sqrt{6} \sqrt{\frac{h}{g}} - 2\sqrt{\frac{h}{g}} = \left(\sqrt{6} - 2\right) \sqrt{\frac{h}{g}} \] 7. **Final Ratio**: - The ratio \( t_1 : t_2 : t_3 \) becomes: \[ t_1 : t_2 : t_3 = 1 : (2 - \sqrt{2}) : (\sqrt{6} - 2) \]

To solve the problem of finding the ratio of time intervals \( t_1 : t_2 : t_3 \) for a particle falling from a height of \( 3h \) in equal height segments of \( h \), we can use the equations of motion under uniform acceleration due to gravity. ### Step-by-Step Solution: 1. **Understanding the Problem**: - The particle is released from rest from a height of \( 3h \). - We need to find the time intervals \( t_1 \), \( t_2 \), and \( t_3 \) for each segment of height \( h \). ...
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