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A particle of mass 5 m at rest suddenly...

A particle of mass 5 m at rest suddenly breaks on its own into three fragments . Two fragments of mass m of each move along mutully perpendicular direction with speed v each . The energy released suring the process is

A

`4/3mv^(2)`

B

`3/5mv^(2)`

C

`5/3mv^(2)`

D

`3/2mv^(2)`

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The correct Answer is:
To solve the problem, we need to determine the energy released when a particle of mass \(5m\) breaks into three fragments, two of mass \(m\) moving at speed \(v\) in mutually perpendicular directions, and one fragment of mass \(3m\). ### Step-by-Step Solution: 1. **Identify Initial Conditions**: - The initial mass of the particle is \(5m\). - The initial velocity of the particle is \(0\) (it is at rest). - Therefore, the initial kinetic energy (\(KE_i\)) is: \[ KE_i = \frac{1}{2} \times 5m \times 0^2 = 0 \] 2. **Final Conditions After Breaking**: - Two fragments of mass \(m\) each move with speed \(v\) in mutually perpendicular directions. - Let’s assume: - Fragment 1 (mass \(m\)) moves in the positive x-direction with speed \(v\). - Fragment 2 (mass \(m\)) moves in the positive y-direction with speed \(v\). - Fragment 3 (mass \(3m\)) has an unknown velocity \(v'\). 3. **Conservation of Momentum**: - Since there are no external forces, the momentum before and after the break must be conserved. - Initial momentum (\(p_i\)) is \(0\) (since the particle is at rest). - Final momentum (\(p_f\)) can be expressed as: \[ p_f = m \cdot v \hat{i} + m \cdot v \hat{j} + 3m \cdot v' \] - Setting initial momentum equal to final momentum gives: \[ 0 = mv + mv + 3m \cdot v' \] - This simplifies to: \[ 0 = mv + mv + 3m \cdot v' \implies 0 = 2mv + 3mv' \implies v' = -\frac{2v}{3} \] 4. **Calculate Final Kinetic Energy**: - The kinetic energy of each fragment after the break: - For Fragment 1: \[ KE_1 = \frac{1}{2} m v^2 \] - For Fragment 2: \[ KE_2 = \frac{1}{2} m v^2 \] - For Fragment 3: \[ KE_3 = \frac{1}{2} (3m) \left(-\frac{2v}{3}\right)^2 = \frac{1}{2} (3m) \cdot \frac{4v^2}{9} = \frac{2mv^2}{3} \] 5. **Total Final Kinetic Energy**: - The total final kinetic energy (\(KE_f\)) is: \[ KE_f = KE_1 + KE_2 + KE_3 = \frac{1}{2} mv^2 + \frac{1}{2} mv^2 + \frac{2mv^2}{3} \] - Combining the terms: \[ KE_f = mv^2 + \frac{2mv^2}{3} = \frac{3mv^2}{3} + \frac{2mv^2}{3} = \frac{5mv^2}{3} \] 6. **Calculate Energy Released**: - The energy released during the process is the difference between the final and initial kinetic energy: \[ \text{Energy Released} = KE_f - KE_i = \frac{5mv^2}{3} - 0 = \frac{5mv^2}{3} \] ### Final Answer: The energy released during the process is: \[ \frac{5mv^2}{3} \]

To solve the problem, we need to determine the energy released when a particle of mass \(5m\) breaks into three fragments, two of mass \(m\) moving at speed \(v\) in mutually perpendicular directions, and one fragment of mass \(3m\). ### Step-by-Step Solution: 1. **Identify Initial Conditions**: - The initial mass of the particle is \(5m\). - The initial velocity of the particle is \(0\) (it is at rest). - Therefore, the initial kinetic energy (\(KE_i\)) is: ...
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