Solve Relativity Q: Electron-Proton CM Velocity, New Particles Energy

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The discussion revolves around calculating the center-of-momentum (CM) velocity of a system where a 10 GeV electron strikes a stationary proton, and determining the energy available for new particle production. The participant successfully calculated the CM velocity but struggled with the subsequent energy calculations in the lab frame. Key equations involving conservation of energy and momentum were discussed, emphasizing the need to express energy in terms of the initial electron energy. The participant was advised to maintain the same gamma factor for all particles post-collision and to use the CM frame's velocity to find the energy available for new particles. The conversation highlights the complexities of relativistic collisions and the importance of accurate arithmetic in these calculations.
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Homework Statement


An electron of energy 10GeV strikes a proton at rest. What is the velocity of the electron-proton CM system? What energy is available to produce new particles?


Homework Equations





The Attempt at a Solution


I've done the first part, but am stuck on the second. I was thinking that in the CM frame after the collision, as the sum of momenta is zero, if the max amount of energy possible went into new particles,

ECM = mc^2 + Mc^2 + E*

where m is the mass of an electron, M the mass of a proton and E* the energy going into new particles. I have ECM from the first part, so I can get E*. However I don't know how to transform this energy into energy in the lab frame.

I (hopefully) won't need a full solution, just some pointers on how to approach this please!
 
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Suppose that only one neutral particle with a non-zero rest mass m1 is produced. It’s also at rest in the CM frame. The max energy will be made available when the P and e are also at rest after collision, provided they are not destroyed. So, all three are traveling with v in lab frame after collision. The energy in CM frame of new particle is m1c^2, which is equal to your E*. If energy available in CM frame is m1c^2, then it must be m1*gamma*c^2 in lab frame. Express it as a function of initial electron energy Ee.
 
Thanks but I still can't get it. This is what I did after your help:

Conservation of energy in CM frame: ECM = mec^2 + mpc^2 + m1c^2

i.e. the initial energy in the CM frame equals the sum of the rest masses

Conservation of energy in lab frame: Ee + mpc^2 = Ee1 + Ep1 + En (En is energy of new particle in lab frame)


so Ee + mpc^2 = gamma(mec^2 + mpc^2 + m1c^2)
as they all have the same velocity they must have the same gamma in lab frame


so Ee + mpc^2 = gamma*ECM


This gives a gamma of about 2, and then doing

En = gamma*m1c^2 = gamma*(ECM - mec^2 - mpc^2)


gives the wrong answer (it should be 4.4 GeV)
 
joker_900 said:
Thanks but I still can't get it. This is what I did after your help:

Conservation of energy in CM frame: ECM = mec^2 + mpc^2 + m1c^2

i.e. the initial energy in the CM frame equals the sum of the rest masses

Conservation of energy in lab frame: Ee + mpc^2 = Ee1 + Ep1 + En (En is energy of new particle in lab frame)


so Ee + mpc^2 = gamma(mec^2 + mpc^2 + m1c^2)
as they all have the same velocity they must have the same gamma in lab frame

Up to here, all seems to be fine. But gamma is dependent only on the velo of the CM frame. You should not have to find gamma(v) afterward. I presume that you can find the velo of the CM frame. Suppose it’s v.

In the lab frame,

Ee + Mpc^2 = (Mp + Me + m1)*gamma(v)*c^2.

From this, you can find m1*gamma(v)*c^2 = E_available in terms of the other quantities.

(Note that by CM frame here, I mean the centre of momentum frame, i.e. in which the total momentum vanish.)
 
Sorry I'm being really slow. Gamma changes after the collision right? So how do I find the new velocity of the CM frame in the lab frame? When I did this for the first part of the question, my method required knowing the masses of the electreon and proton and the energy of the electron in the lab frame. After the collision I don't know these?
 
The whole point is that for maximum energy to be available, all three particles should be at rest in the CM frame. The velocity of the CM frame does not change. So, you calculate that before the collision, and use it to find the reqd energy after the collision.
 
But I'm doing that and it's giving me the wrong answer :(

The velocity of the CM frame in the first part is 0.914c. So gamma = (1 - 0.914^2)^-0.5 = 2.46

Mpc^2 = 938 MeV Mec^2 = 0.512 Ee = 10000MeV

And putting this in i get m1*gamma*c^2 = 8625 MeV

!
 
Are you sure you've done the arithmetic correctly...? Anyway, try this formula for now, until I can verify your calc.

Energy available = sqrt([2Mp*c^2*Ee + (Mp*c^2)^2 + (Me*c^2)^2]
 
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