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1. A thin, uniform bar of length L and mass M is supported by a frictionless horizontal surface. A ball of mass m travels to

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Given . Mass of bar = M. mass of ball am velocity of ball = 3 Акт () mot v → Ball d - - strikes at a distance from centre ofSo, linear momentum is conserved (Pi =P ) combined let vf be the velocity of is bar and ball mv + MV = (m+ M) VA V→ initial vAngular velocity of system Since there is no external torque acting in the system So, Angular momentum (2) is conserved Pakinmoment of inertia of bar about its centre of mass = Me moment of inertiá of: ball about o = mer? Lsystem el present euro frPART (6) Collision is elastie -) » 1. of Energy is conserved y Ball comes to rest & This time ball doesnt I stick to bas ? 1=) muto= o+N Vf As external torque es absent, So, angular momentum O is conserved. Li a lf n 7) mvby) Ibar w s Angular momentAs colliscon is elastic Energy is conserved - £mv² = £mvh + 2 MV 2 a) {mv? 0+ Vz? a) į mi a { MV2 + Escolese - Now putting va을뤄씀 루 서 NK ON K NS 는 뚱 일 은 시루 서 두 77 |

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