A nucleus moving with velocity →v emits an α−particle. Let the velocities of the α−particle and the remaining nucleus be →v1 and →v2 and their masses be m1 and m2, then:
A
→v,→v1, and →v2 must be parallel to each other
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B
none of the two of →v,→v1, and →v2 should be parallel to each other
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C
→v1+→v2 must be parallel to →v
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D
m1→v1+m2→v2 must be parallel to →v
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Solution
The correct option is Cm1→v1+m2→v2 must be parallel to →v Momentum of the system is conserved. If mi is the initial mass. Applying momentum conservation. miv=m1v1+m2v2 Hence v is parallel (along the direction of) v1+v2 Hence option D is correct.