How Do You Calculate the Distance of Closest Approach in a Particle Collision?

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Homework Help Overview

The discussion revolves around calculating the distance of closest approach in a particle collision involving an alpha particle and a Beryllium nucleus. The problem is set within the context of nuclear physics and involves concepts of energy conservation, potential energy, and kinetic energy in a collision scenario.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants explore the relationship between kinetic energy and potential energy at the point of closest approach, questioning the assumption that all energy converts to potential energy. There is discussion about the center of mass frame and the implications of particle speeds in that frame.

Discussion Status

Participants are actively engaging with each other's reasoning, identifying potential errors and clarifying assumptions. Some guidance has been offered regarding the validity of certain assumptions about potential energy at the start of the problem. Multiple interpretations of the energy conservation principles are being explored.

Contextual Notes

There are mentions of specific values and conditions, such as the potential difference of 20 kV and the masses and charges of the particles involved. Participants express uncertainty about the initial conditions and the treatment of potential energy in the problem setup.

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Homework Statement


An alpha particle is accelerated from rest through a potential dierence of 20 kV. It travels directly towards a stationary Beryllium nucleus (4 protons, 5 neutrons). Calculate the distance of closest approach.

The problem definitely wants a solution that takes into account the recoil of the stationary nucleus on approach.

Homework Equations


VCM=m1v1+m2v2/m1+m2
U=Q1Q2/4πε0d
T=mv2/2

The Attempt at a Solution


Let the oncoming alpha particle have speed v. VCM=4v/13. In the CM frame, we have a particle of mass 4m, charge 2e, speed 9v/13 heading towards on of mass 9m, charge 4e, speed -4v/13.

Initially, T=18mv2/3. This all becomes PE which will be 2e2/πε0d for closest approach d. Equating given d=e2/3πε0mv2. T=qV for a p.d V so v2=2qV/m. Then d=e/3πε0V. Plugging in the numbers given d=96fm.

I don't have a solution so would appreciate somebody having a check. I'm unsure about my approach because it assumes that the initial scenario (i.e as soon as the alpha particle has finished being accelerated through the p.d) has the PE as zero, which isn't realistic and the question doesn't indicate this is valid. Thanks.
 
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You went wrong when you said all the energy becomes PE. That's not the case. At closest approach both particles are moving at speed VCM
 
dauto said:
You went wrong when you said all the energy becomes PE. That's not the case. At closest approach both particles are moving at speed VCM

But I'm working in the CM frame?
 
Last edited:
dauto said:
You went wrong when you said all the energy becomes PE. That's not the case. At closest approach both particles are moving at speed VCM
Fayled has transformed the problem into the CM frame, where VCM is zero. So the approach is correct.

But I did spot two mistakes or typos.
fayled said:

The Attempt at a Solution


Let the oncoming alpha particle have speed v. VCM=4v/13. In the CM frame, we have a particle of mass 4m, charge 2e, speed 9v/13 heading towards on of mass 9m, charge 4e, speed -4v/13.
Looks good so far.

Initially, T=18mv2/3.
It should be "/13" at the end, not "/3". Do you agree?

This all becomes PE which will be 2e2/πε0d for closest approach d. Equating given d=e2/3πε0mv2.
Agree, once you fix the earlier mistake.

T=qV for a p.d V so v2=2qV/m.
I agree.

Then d=e/3πε0V.
I don't think that follows. Can you show the steps leading up to this expression (following the v^2=\frac{2qV}{m} result)? What are you using for q?

Plugging in the numbers given d=96fm.

I don't have a solution so would appreciate somebody having a check. I'm unsure about my approach because it assumes that the initial scenario (i.e as soon as the alpha particle has finished being accelerated through the p.d) has the PE as zero, which isn't realistic and the question doesn't indicate this is valid. Thanks.
It is safe to assume this is valid. The alpha should be a considerable distance from the berylium when it exits the accelerator, so there would be negligible PE at that time.
 
Last edited:
Redbelly98 said:
Fayled has transformed the problem into the CM frame, where VCM is zero. So the approach is correct.

But I did spot two mistakes or typos.

Looks good so far.It should be "/13" at the end, not "/3". Do you agree?Agree, once you fix the earlier mistake.I don't think that follows. Can you show the steps leading up to this expression? What are you using for q?It is safe to assume this is valid. The alpha should be a considerable distance from the berylium when it exits the accelerator, so there would be negligible PE at that time.

Right:

Yes I agree! In fact a follow up question of mine was going to be why doesn't TLAB=TTCM+T', with T' the KE of a particle of the total mass of the system moving at speed VCM? That error solves that (should have known better than thinking physics had broken and I hadn't made an error).

So T=18mv2/13

U=2e2/πε0d

d=13e2/9πε0mv2

Now v2=eV/m. Before I had v2=2qV/m. But I would then need q=2e,m=4m (i.e I should have used M say - I think this confused you).

d=13e/9πε0V=416fm (simply substituting the above expression into the one above it).

Hopefully that's right. Thanks for your help!
 
Last edited:
Looks good. You're welcome! :smile:

p.s. You're right, I was confused about m vs. 4m.
 

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