Conservation of relativistic energy, collision of particles

In summary, the conversation discusses the concept of maximum number of pions that can be created in a system, and the factors that must be considered to determine this number. These factors include the assumption of pions having zero momentum and the total energy available for particle creation. The conversation also mentions the difficulty in achieving spin-coupling in a particle collider.
  • #1
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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  • #2
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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  • #3
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.
 
  • #4
What's the total momentum of the system?
 
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  • #5
Zero.
 
  • #6
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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  • #7
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.
 
  • #8
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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  • #9
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?
 
  • #10
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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FAQ: Conservation of relativistic energy, collision of particles

What is the principle of conservation of relativistic energy in particle collisions?

The principle of conservation of relativistic energy states that the total energy of a closed system remains constant during any interaction, including particle collisions. In relativistic contexts, this includes both the kinetic energy and the rest mass energy of the particles involved.

How does relativistic energy differ from classical energy in particle collisions?

In classical mechanics, energy is typically separated into kinetic and potential forms, and mass is treated as invariant. In relativistic mechanics, however, energy and mass are interrelated through Einstein's equation \(E = mc^2\). This means that the total energy includes contributions from both the rest mass and the kinetic energy, which become significant at high velocities near the speed of light.

What role does the invariant mass play in relativistic collisions?

The invariant mass (or rest mass) of a system of particles is a key quantity that remains unchanged regardless of the reference frame. During relativistic collisions, while individual particles may gain or lose kinetic energy, the total invariant mass of the system is conserved. This is crucial for analyzing the outcomes of high-energy particle collisions.

How can we calculate the total energy in a relativistic collision?

The total energy in a relativistic collision can be calculated using the formula \(E^2 = (pc)^2 + (mc^2)^2\), where \(E\) is the total energy, \(p\) is the momentum, \(m\) is the rest mass, and \(c\) is the speed of light. This equation takes into account both the rest mass energy and the kinetic energy of the particles.

What are some common examples of relativistic particle collisions in physics?

Common examples of relativistic particle collisions include interactions in particle accelerators, such as those at CERN's Large Hadron Collider, where protons and other particles are accelerated to near-light speeds and collided to study fundamental particles and forces. Another example is cosmic ray interactions with the Earth's atmosphere, which can produce high-energy particle showers.

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