A problem in rigid body dynamics

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SUMMARY

The discussion centers on a rigid body dynamics problem involving a disc of mass M and radius r, which is connected to a horizontal spring and subjected to a tangential collision by a particle of mass m with velocity v. The key equations utilized are the conservation of linear momentum and conservation of angular momentum. The final velocity of the system is derived using the moment of inertia and angular velocity, with the participant questioning the book's equation regarding momentum conservation, specifically the treatment of the center of mass. The impact of friction on angular momentum conservation is also debated, concluding that the brief impulse from the collision does not significantly affect the normal force.

PREREQUISITES
  • Understanding of conservation of linear momentum
  • Knowledge of conservation of angular momentum
  • Familiarity with moment of inertia calculations
  • Basic principles of rigid body dynamics
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  • Study the derivation of angular momentum equations in rigid body systems
  • Explore the implications of friction in collision problems
  • Learn about the moment of inertia for various shapes and its application in dynamics
  • Investigate the effects of impulse and its duration on momentum conservation
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vijayramakrishnan
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Homework Statement


A disc of mass M and radius r is kept on a horizontal,frictional plane and is connected to a horizontal spring at the centre.A particle of mass m strikes the topmost point of the disc,tangentially and sticks to it.Assume that the mass of the particle is m and it's velocity is v.Find out the velocity after the collision.Can you apply the law of conservation of angular momentum?if so write down the equation and find ω of the system.[/B]

Homework Equations



conservation of momentum
conservation of angular momentum[/B]

The Attempt at a Solution



i know that conservation of momentum and conservation of angular momentum should be applied.
initial angular momentum = mvR
let vf be the final velocity of topmost point and vcm be the velocity of centre of mass of disc.
conservation of angular momentum about centre(not centre of mass as it changes after particle strikes)
final angular momentum should be moment of inertia about centre of mass of disc (angular velocity) + m vfR

vf = vcm + ω(distance of centre of mass from particle)

conservation of momentum:
mv= Mvcm + mvf

but in my book it is written that in momentum conservation mv=(M+m)vcm
i don't understand it aren't they moving with different velocity,so individual momentum should be added or momentum of centre of mass should be taken.
Also correct any of the other steps which i have done wrong
Please help
[/B]
 
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I agree with both of your equations (linear and angular momentum). I cannot explain the book's equation.
 
haruspex said:
I agree with both of your equations (linear and angular momentum). I cannot explain the book's equation.
thank you very much sir for replying.
 
I thought conservation of angular momentum cannot be applied since there is friction?
 
kinemath said:
I thought conservation of angular momentum cannot be applied since there is friction?
The impulse from the collision is assumed to be very brief, i.e. an unlimitedly large force acting for an infinitesimal time. Since the impulse is horizontal, it does not affect the normal force, so that, and hence the corresponding friction, remain strictly limited in magnitude. As a result, the contribution to momentum is negligible.
That said, it does bother me that the question specifies a frictional surface. Either that is a trap, making you think you do need to consider friction, or they should have specified something more like a toothed gear set on a rack.
 

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