How Does Reflecting a Particle Stream Affect the Force on a Surface?

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Homework Help Overview

The discussion revolves around a one-dimensional stream of particles reflecting off a surface and the resulting force on that surface. Participants are examining the momentum changes associated with the incoming and outgoing particle streams, considering factors such as particle density and velocity.

Discussion Character

  • Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants explore the relationship between incoming and outgoing momentum, questioning whether the particle density remains constant after reflection. There are discussions about how velocity affects particle spacing and density.

Discussion Status

Some participants have provided mathematical expressions for momentum and force, while others are questioning the assumptions made about density and conservation principles. The conversation reflects a mix of interpretations and attempts to clarify the underlying physics.

Contextual Notes

There is an ongoing debate about the conservation of momentum in the context of the problem, with references to real-world analogies such as racing cars to illustrate points about particle spacing and timing.

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Homework Statement


A one-dimensional stream of particles of mass ##m## with density ##\lambda## particles per unit length, moving with speed ##v##, reflects back from a surface, leaving with a different speed ##v'##, as shown. Find the force on the surface

Homework Equations

The Attempt at a Solution


The incoming momentum of the particle stream is ##\lambda m v^2## and the outgoing momentum is ##\lambda m v'^2##, thus the change in momentum of the particle stream by the mirror is ##\lambda m (v^2 + v'^2)##. Thus the force on the mirror is also ##\lambda m (v^2 + v'^2)##.

Is this correct?
 
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Nearly.
Mr Davis 97 said:
and the outgoing momentum is ##\lambda m v'^2##
How did you get this?

Is the particle density still the same for the outgoing stream?
 
Well, ##\lambda## is particles per unit length. If we multiply by m we get the mass of the stream per unit length, which is ##\lambda m## If we multiply this by v we get the momentum per unit length, and if we multiply by v again we get the momentum per second, which is exactly the incoming change in momentum. So ##\lambda m v^2## is the incoming change in momentum. Now it seems that the outgoing change in momentum would be ##\lambda m v'^2##, but you are saying that the particle density may not be the same for the outgoing stream, but I don't see how the velocity of the particles changes the number of particles per unit length... Wouldn't they all be the same length from each other, except going slower?
 
Mr Davis 97 said:
Well, ##\lambda## is particles per unit length. If we multiply by m we get the mass of the stream per unit length, which is ##\lambda m## If we multiply this by v we get the momentum per unit length, and if we multiply by v again we get the momentum per second, which is exactly the incoming change in momentum. So ##\lambda m v^2## is the incoming change in momentum. Now it seems that the outgoing change in momentum would be ##\lambda m v'^2##, but you are saying that the particle density may not be the same for the outgoing stream, but I don't see how the velocity of the particles changes the number of particles per unit length... Wouldn't they all be the same length from each other, except going slower?

Have you ever watched a motor race? Like the formula 1. What happens when the cars get to the fastest part of the track? And the slowest?
 
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What is the conserved quantity in the stream? It is not the density.
 
Is the momentum conserved?
 
Mr Davis 97 said:
Is the momentum conserved?
Given you are calculating the force caused by the change in momentum, that can hardly be conserved.

You didn't answer my question about the racing cars. It's the time interval not the spatial interval that remains constant. Think about it.
 
The initial momentum is P1=λmv^2t .
(you that that by P1=M*v , M=λd , d is the distance between the last particle that hits the mirror during t and mirror , d=v*t ->P1=λmv^2t ) .
Each particle must be reflect (same M) -> P2=(-M*v')=(-λmvv't) .
F=|P2-P1|/t=λm(v^2+vv') .
I hope I helped.
Sorry for my poor english.
 
Voicu said:
The initial momentum is P1=λmv^2t .
(you that that by P1=M*v , M=λd , d is the distance between the last particle that hits the mirror during t and mirror , d=v*t ->P1=λmv^2t ) .
Each particle must be reflect (same M) -> P2=(-M*v')=(-λmvv't) .
F=|P2-P1|/t=λm(v^2+vv') .
I hope I helped.
Sorry for my poor english.
The thread is over two years old,
 

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