Conservation of relativistic energy, collision of particles

AI Thread Summary
The discussion revolves around the conservation of relativistic energy and momentum in particle collisions, specifically focusing on the creation of pions from a proton-antiproton pair. Participants explore the assumption that all created pions could have zero momentum, allowing energy to be fully converted into their rest masses. Calculations indicate that with a total energy of 3752 MeV, approximately 28 pions can be produced, assuming the pions have a rest mass of about 134 MeV each. There is also mention of the need for the proton-antiproton pair to be in a spin-coupled state to conserve angular momentum, although this concern is deemed secondary for the exercise. Overall, the conversation emphasizes the complexities of relativistic energy calculations in particle physics.
milkism
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Homework Statement
Collision of a proton and antiproton forming bunch of pions, what's the maximum amount?
Relevant Equations
$$E=\gamma mc^2$$
Question:
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With maximum do they mean that the speed of the pions is the same as the proton and an antiproton? Otherwise there will be two unknowns, and if I use both relativistic-energy and momentum conservation equations I get difficult equations.
 
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milkism said:
With maximum do they mean that the speed of the pions is the same as the proton and an antiproton?
No reason to think that. To find the maximum number of pions, what might you assume about their speeds?
 
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Doc Al said:
No reason to think that. To find the maximum number of pions, what might you assume about their speeds?
I have no idea 😭😥,I'm sorry.
 
What's the total momentum of the system?
 
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Zero.
 
Right! So how about assuming that all the created pions have zero momentum -- all the energy goes into their rest masses.
 
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Doc Al said:
What's the total momentum of the
Doc Al said:
Right! So how about assuming that all the created pions have zero momentum -- all the energy goes into their rest masses.
Wouldn't that be $$E=nmc^2$$, with n amount.
 
You're given the rest mass of the pions. How much total energy does the system have to create particles with?
 
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Doc Al said:
You're given the rest mass of the pions. How much total energy does the system have to create particles with?
3752 MeV?
 
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milkism said:
3752 MeV?
You should at least sketch out why you think that. You're right, but you may have made two cancelling mistakes.

So how many pions can you get from that?
 
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  • #11
Ibix said:
You should at least sketch out why you think that. You're right, but you may have made two cancelling mistakes.

So how many pions can you get from that?
Using $$E=\gamma mc^2$$, calculating the Lorentz factor with the given velocity will be 2, so E becomes 2mc², but because both proton and antiproton have same mass and velocity, the total energy will be 4mc², that's how I got 3752 MeV.
So we have 3752 = nmc² = > 3752 MeV= n *134 MeV => 28 pions.
If the pions had the same velocity as the proton and antiproton it would have be 14 pions, that's what I had at first.
 
  • #12
Right.

Note that they've fudged the numbers so it comes out nice and round. The neutral pion mass is nearly 135MeV, while protons are only a bit over 938MeV. You'd need to speed your protons up a bit more to have enough energy for 28 pions.
 
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  • #13
milkism said:
So we have 3752 = nmc² = > 3752 MeV= n *134 MeV => 28 pions.

Good! (Thanks for jumping in, @Ibix -- I got called away.)
 
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  • #14
Doc Al said:
Thanks for jumping in, @Ibix -- I got called away.
Thanks for not saying "butting in". 😁
 
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  • #15
Doc Al said:
What's the total momentum of the system?
Of course, the proton-antiproton pair must be spin-coupled in the singlet state to conserve angular momentum as well. That might be a bit tricky to achieve in a particle collider.
 
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  • #16
kuruman said:
Of course, the proton-antiproton pair must be spin-coupled in the singlet state to conserve angular momentum as well. That might be a bit tricky to achieve in a particle collider.
Indeed. For the purpose of this exercise I think those worries can be ignored. :wink:
 
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