The use of cross section in a particle collision exercise.

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Homework Help Overview

The discussion revolves around a particle collision exercise involving a beam of protons colliding with a plate characterized by a specific particle density and thickness. The problem includes the concept of cross section and its implications on the intensity of outgoing particles compared to incoming particles.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • The original poster attempts to reason through the relationship between incoming particle intensity and the thickness of the plate, questioning the implications of the cross section on particle behavior post-collision. Participants raise concerns about the assumptions regarding particle momentum and energy loss during collisions.

Discussion Status

Some participants affirm the original poster's assumptions regarding the cross section, while others introduce additional complexities related to particle behavior after collisions. The discussion reflects a mix of agreement and exploration of deeper concepts in particle physics.

Contextual Notes

There is mention of the original exercise being presented with limited information, which may affect the clarity of assumptions regarding the cross section and particle interactions. Participants also note that the discussion may extend beyond the intended scope of the exercise.

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1. Situation: I have no specific exercise in mind but just the general form. ''A beam of protons is colliding with a plate of a given particle density ##\rho## and thickness ##l##. The cross section is ##\sigma##. What should the thickness of the plate be such that the intensity of the outgoing particles on the other side is 0.1 of the incoming intensity'' The exercises we made in class were literally worded like this with no more info.2. Equations: ##W=\rho l \phi \sigma## where ##W## is the amount of elastic collisions per second and ##\phi## the amount of incoming particles per second. 3. My general reasoning is something like this. If I look at a 1 second interval I have an amount ##\phi## of incoming particles, I'd like that the collision rate would be ##0.9 \phi## so that only 0.1 of the particles have not collided. In that case the relevant equation becomes ##0.9= \rho l \sigma##.

CONFUSION:

The point where I'm confused is the given cross section as I underlined. I make an implicit assumption here that this cross section is just the cross section of collision, and that after collision the particles ''dissapear'' so to speak or move very slow relative to the ingoing beam. If this isn't the case then there will be collisions after which particles will keep moving forward without losing all too much momentum and my reasoning would be wrong.

QUESTION:

Is my reasoning of a solution correct? If so, how can I lift my confusion about the meaning of the cross section in this situation?
 
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Your assumption is completely correct. No confusion necessary in this simple case.

For scattering at small angles, there is no simple sigma and an angular dependence comes in.
 
BvU said:
Your assumption is completely correct. No confusion necessary in this simple case.

For scattering at small angles, there is no simple sigma and an angular dependence comes in.

Then what about the particles that keep on having a quite large velocity component in the direction after colliding? Those particles will still contribute to the outgoing beam of particles.
 
Absolutely. In fact for protons with a reasonable kinetic energy that is what normally happens: they lose energy mainly through collisions with bound electrons (which they ionize) through Coulomb interaction. Google Bethe Bloch, browse through http://www.kip.uni-heidelberg.de/~coulon/Lectures/Detectors/Free_PDFs/Lecture2.pdf , or get it all here, but realize that you are by now way beyond the scope and level of the original exercise. Welcome to the wonderful world of elementary particle physics !
 
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