How to Calculate Invariant Mass for Negligible Particle Mass?

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Homework Help Overview

The discussion revolves around calculating the invariant mass of an electron-proton system, where the mass of the electron is considered negligible. Participants explore the implications of energy conservation and the relationship between energy, momentum, and mass in relativistic contexts.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the initial total energy of the system and question how to incorporate the negligible mass of the electron into the invariant mass calculation. There is confusion regarding the necessity of velocity in the equations and the implications of momentum conservation.

Discussion Status

The discussion is active, with participants providing insights into the equations involved and clarifying misconceptions about massless particles and momentum. Some participants suggest that the invariant mass can be approximated using the energy-momentum relationship, while others question the assumptions made regarding momentum.

Contextual Notes

Participants are operating under the constraint of neglecting the mass of the electron, which raises questions about how this affects the calculations and interpretations of momentum and energy in the system.

tnibbz
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Homework Statement
A 2 GeV electron is incident on a proton with rest mass mpc^2 = .938 GeV at rest. Calculate the invariant mass of the electron proton pair in the center of mass, neglect the mass of the electron.
Relevant Equations
E^2 = p^2*c^2 + m^2*c^4
E = K + E0
So I know that since we are ignoring the mass of the electron, and the proton starts at rest, the proton has no KE and the electron has no rest energy.

So the initial total energy of the system would be

rest energy of proton + KE of electron = 2GeV + .938GeV = 2.938 GeV

and since energy is conserved this would also be the total energy of the final state as well correct?

Now with the equation
E2 = p2*c2 + m2*c4

I can subsitute in 2.938GeV for E, however from here I get confused, because I need both the resulting velocity of the system and the mass.

Or is the mass of the system in this case just the mass of the proton because we are neglecting the mass of electron? But in that case would the invariant mass of the system just be the mass of the proton?
 
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tnibbz said:
Homework Statement:: A 2 GeV electron is incident on a proton with rest mass mpc^2 = .938 GeV at rest. Calculate the invariant mass of the electron proton pair in the center of mass, neglect the mass of the electron.
Homework Equations:: E^2 = p^2*c^2 + m^2*c^4
E = K + E0

because I need both the resulting velocity of the system and the mass.
Why would you need the velocity? There is no velocity in that equation.
 
well doesn't p=ϒmv?
 
That is irrelevant. You already know p.
 
Oh because the momentum is conserved? So the final momentum p would be equal to the initial momentum of the system, since the proton was at rest and the electron is essentially massless is the momentum 0? So I would just plug in the E I found earlier and 0 into the equation

E2 = p2*c2 + m2*c4
and solve for m?
 
That the electron is massless does not mean momentum is zero. What is the momentum of a massless particle?
 
well if it is not zero than it cannot be p= ϒmv. Could we treat it like a photon and use E=pc?
 
tnibbz said:
Could we treat it like a photon and use E=pc?
##E^2 = (pc)^2 + m^2c^4## is true for all systems. If you just consider a massless particle, you get ##E=pc## so this is true for any massless particle. In general, ##E^2 = (pc)^2 + m^2c^4## is a much more useful relation than ##p = m\gamma v##.
 
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Okay that makes sense, I did not realize that was where the E = pc formula was derived from, for some reason I thought it only held for photons. I believe I can solve the problem from here, thank you for all your help.
 
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tnibbz said:
Okay that makes sense, I did not realize that was where the E = pc formula was derived from, for some reason I thought it only held for photons. I believe I can solve the problem from here, thank you for all your help.

If ##E^2 = p^2c^2 + m^2c^4##, then for a particle whose mass can be neglected, compared to its energy, we have:

##E^2 \approx p^2c^2##

That equation only hold exactly for massless particles. But, it is also a sufficient approximation for particles with small mass.
 

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