Finding Angular Velocity of Man with Gun in Physics Textbook

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Homework Help Overview

The discussion revolves around a physics problem involving angular momentum and the dynamics of a man standing on a massless rod while shooting a bullet. The problem requires finding the angular velocity of the man as a function of the angle the bullet's velocity vector makes with the rod.

Discussion Character

  • Exploratory, Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • Participants discuss the application of conservation of angular momentum and question the relevance of linear momentum in the context of the problem. There are varying opinions on whether the mass of the man should be considered negligible compared to the bullet's mass.

Discussion Status

Some participants express confidence in the use of angular momentum conservation, while others suggest corrections and clarifications regarding the initial and final angular momentum calculations. There is an ongoing exploration of the implications of mass ratios and the fixed nature of the rod on momentum conservation.

Contextual Notes

Participants note that the problem's complexity increases if the mass of the man is not significantly greater than that of the bullet. There is also a recognition that the total angular momentum is zero before the bullet is fired, leading to confusion about the conservation principles being applied.

HSSN19
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Homework Statement



This is a question from the physics textbook Don't Panic Volume I, chapter XIV.

A man, mass M, stands on a massless rod which is free to rotate about its center in the horizontal plane. The man has a gun (massless) with one bullet, mass m. He shoots the bullet with velocity vb, horizontally. Find the anglular velocity of the man as a function of the angle θ which the bullet's velocity vector makes with the rod.

Homework Equations



L = r x mv = mrvsinθ
L = mr2ω

The Attempt at a Solution



Initial L = m(l/2)vbsinθ
Final L = M(l/2)2ω

Therefore, ω = (2mvbsinθ)/Ml

What do guys think? Was I correct in using conservation of angular momentum? It is a very weird question compared to the rest.

Thanks in advance!
 

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Yes it's correct.But should we neglect mass of man in comparison to mass of bullet?
If not then conserve linear momentum along cos component of velocity, i.e.
M*v=-m*vB*cos(θ).
'-' sign indicates man gets velocity in opposite direction of motion of bullet.Then the problem bcms complex bcs. now man's distance from centre of table keeps decreasing.
Check the answer.If it's simple which mostly should be then what you have done is seems correct.
I think you must have missed '2' in (l/2)2 in initial angular momentum term.
 
Nah I don't think linear momentum should be used in problems like this. About the 2, if you're talking about the square, then no there shouldn't be a square. The definition of angular momentum is the cross product between r and linear momentum. The other equation has a square because it's derived for the special case of circular motion.
 
HSSN19 said:
What do guys think? Was I correct in using conservation of angular momentum? It is a very weird question compared to the rest.
I think your answer is fine, but your work needs a little correction. The total angular momentum is--and remains--zero.
 
HSSN19 said:
Nah I don't think linear momentum should be used in problems like this. About the 2, if you're talking about the square, then no there shouldn't be a square. The definition of angular momentum is the cross product between r and linear momentum. The other equation has a square because it's derived for the special case of circular motion.

Oh!Sorry.I didn't think about that.Well then all terms written by you are correct.But linear momentum should be conserved in such problems if mass of man is not much greater than mass of bullet.However in your problem it seems that book has assumed the mass of man to be much greater than mass of bullet.So what you have done seems fine.
 
1994Bhaskar said:
But linear momentum should be conserved in such problems if mass of man is not much greater than mass of bullet.However in your problem it seems that book has assumed the mass of man to be much greater than mass of bullet.
Conservation of linear momentum would not apply here--the rod is fixed on an axis, so linear momentum is not conserved.

No need for any assumption about the relative masses of bullet and man.
 
Doc Al said:
I think your answer is fine, but your work needs a little correction. The total angular momentum is--and remains--zero.

Wait, what? I'm confused now. Why is the total L zero? Don't you mean the change in L is zero (L is conserved)?
 
HSSN19 said:
Wait, what? I'm confused now. Why is the total L zero? Don't you mean the change in L is zero (L is conserved)?
Presumably, before the bullet is fired nothing is moving. So the total angular momentum is zero. And it remains zero, of course.
 
Oh man, I already submitted the homework. I knew my "initial" and "final" L's didn't make any sense since the events are simultaneous. So the answer should be the same but negative now, I guess. Thanks!
 
  • #10
Doc Al said:
Conservation of linear momentum would not apply here--the rod is fixed on an axis, so linear momentum is not conserved.

No need for any assumption about the relative masses of bullet and man.

OK.I understood that.
 

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