How Thick Should the Wall Be to Scatter Half the Particle Beam?

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Homework Help Overview

The problem involves determining the thickness of a wall that will allow half of a particle beam to penetrate without scattering. The context includes a wall with a specific atomic density and the behavior of atoms modeled as spheres.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the relationship between the wall's thickness and the surface area covered by the atoms. There is mention of calculating the microscopic cross-section based on the atomic radius and using it to find the macroscopic cross-section.

Discussion Status

Some participants have suggested methods for approaching the problem, including the use of the exponential attenuation formula. However, there is no explicit consensus on the exact steps to take, and some uncertainty remains regarding the wall area and how it factors into the calculations.

Contextual Notes

Participants note the absence of information regarding the wall area, which may affect the calculations. There are also references to specific equations related to mean free path and cross-sections that are relevant to the problem.

leviathanX777
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Homework Statement



A beam of particles strike a wall containing 2 x 10^29 atoms per m^3. each atom behaves like a sphere of radius 3 x 10^-15 m. Find the thickness of the wall that exactly half the particles will penetrate without scattering. What thickness would be needed to stop all but one particle in 10^6

Homework Equations



the mean free path (λ) = 1/nσ


The Attempt at a Solution



I'm not sure how to start the solution. I can't find an equation that will bring the thickness of the wall into the problem

Cheers.
 
Last edited:
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hmmm... you could consider the surface area effectivley covered by the spheres... what is that relative to the wall area in terms of the thickness?
 
I do not know the wall area, it didn't say.
 
Cool problem. I would approach it this way: The microscopic cross-section is ~ the area presented by a single nucleus, so in this case \sigma = \pi*(3x10-15 m)2 = 2.83 x 10-29 m2

Once you have that, you can calculate the macroscopic cross section using \Sigma=N\sigma and then you can use the exponential attenuation formula I = I0exp(-\Sigmat) to solve for the penetration depth t.
 

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