What Happens to Mass During the Annihilation of an Electron-Positron Pair?

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Discussion Overview

The discussion revolves around the concept of mass during the annihilation of an electron-positron pair, particularly in the context of relativistic mass versus invariant mass. Participants explore the implications of the mass-energy equation and how mass is perceived in different reference frames, touching on theoretical and conceptual aspects of physics.

Discussion Character

  • Debate/contested
  • Conceptual clarification
  • Technical explanation

Main Points Raised

  • Some participants assert that invariant mass remains constant across reference frames, while relativistic mass varies depending on kinetic energy.
  • Others argue that relativistic mass is frame-dependent and that mass is not conserved in the classical sense, but rather mass-energy is conserved.
  • There is a contention regarding the definition of mass, with some participants defining it in terms of relativistic mass and others in terms of invariant mass.
  • One participant suggests that the photons produced in electron-positron annihilation should be assigned mass based on their momentum, while another counters that photons have zero mass.
  • Concerns are raised about the implications of assigning mass to photons, particularly in relation to photon absorption and the consistency of the model.
  • Some participants emphasize the importance of using the conservation of mass-energy in understanding the annihilation process.

Areas of Agreement / Disagreement

Participants express differing views on the nature of mass in relativistic contexts, with no consensus reached on whether relativistic mass should be considered or how to interpret the mass of photons. The discussion remains unresolved with competing perspectives on mass conservation and definitions.

Contextual Notes

Participants highlight the complexity of mass definitions and the implications of reference frames in relativistic physics. There are unresolved assumptions regarding the treatment of mass in different contexts, particularly in relation to energy and momentum conservation.

trichop
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After a dispute on the nature of kinetic energy on a previous topic,
a new question has arised.
If kinetic energy is different for each reference frame,
then what happens with mass, considering the mass-energy
equation?
 
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trichop said:
After a dispute on the nature of kinetic energy on a previous topic,
a new question has arised.
If kinetic energy is different for each reference frame,
then what happens with mass, considering the mass-energy
equation?

Depends on which kind of mass you're asking about. The "invariant mass" a.k.a. "proper mass" a.k.a. "rest mass" doesn't change. The "relativistic mass" depends on the kinetic energy:

[tex]m_{rel} c^2 = m_0 c^2 + K[/tex]
 
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So for different reference frames we have different relativistic mass.
Can this be true?
 
trichop said:
So for different reference frames we have different relativistic mass.
Can this be true?

This is definitely true. Only the invariant mass is the same for different frames.
 
trichop said:
So for different reference frames we have different relativistic mass.
Can this be true?
Yep. That is 100% true.

Pete
 
trichop said:
So for different reference frames we have different relativistic mass.
Can this be true?

In relativistic terms, you add mass to the variant variables. It is no longer frame-independent. Don't let incredulity make you skeptical. The way physics works is sometimes not "common sense" to everyday experience.

Also, in a swing from classical mechanics, mass is also no longer conserved. Instead, the total mass-energy of the system is conserved. That's how we get nuclear fusion for example.
 
mezarashi said:
In relativistic terms, you add mass to the variant variables. It is no longer frame-independent. Don't let incredulity make you skeptical. The way physics works is sometimes not "common sense" to everyday experience.

Also, in a swing from classical mechanics, mass is also no longer conserved. Instead, the total mass-energy of the system is conserved. That's how we get nuclear fusion for example.
Mass is always conserved, whether you call "mass" relativistic mass or you call it the magnitude of the total 4-momentum.

Pete
 
pmb_phy said:
Mass is always conserved, whether you call "mass" relativistic mass or you call it the magnitude of the total 4-momentum.

Pete

How do you explain the annihilation of an electron-positron pair?
 
mezarashi said:
How do you explain the annihilation of an electron-positron pair?

People (like Pete) who use "mass" to refer to relativistic mass say that the photons produced in the annihilation have mass, and the sum of the masses of the electron and positron before the annihilation equals the sum of the masses of the photons afterwards.

People (like me) who use "mass" to refer to invariant mass, defined by

[tex](mc^2)^2 = E^2 - (pc)^2[/tex]

say that the mass of the system of electron and positron before the annihilation equals the mass of the system of two photons afterwards. In calculating the mass of a system, you use the total energy and the total (vector) momentum in the equation above.

In this view, the mass of a system of particles does not equal the sum of the masses of the individual particles, unless the particles are at rest with respect to each other.

[added] Also in this view, the mass of a photon is zero, because [itex]E = pc[/itex] for a photon.
 
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  • #10
I prefer using the conservation of mass-energy. As in the case of the electron-positron annihilation, it is rather odd to assign a mass to the photon. It would then be difficult then to explain photon absorption using that model. There seems to be too many inconsistencies as far as I can see.
 
  • #11
mezarashi said:
How do you explain the annihilation of an electron-positron pair?
Assumption: To make the derivationn easy we assum that all observations will be made from the zero momentum frame.

Since each of the two particles have the same proper mass then for momentum to be conserved the two photons produced in the resulting annihilation must have the same frequenecy, f and therefore the same energy E = hf and hence same momentum |p| = E/c.

According to the mass = relativistic mass people: The mass of each photon is defined as the ratio of the magnitude of the photon's momentum to the speed of light. This equals the ratio of the energy over c2, i.e. m = hf/c2. Since energy is conserved then so too is the total (relativistic) mass. Actually the conservation of mass can be proven to be a consequence of two facts (1) that (mc, p) is a 4-vector and (2) that p is conserved.

If you question whether a photon has a non-zero mass recall the definition of mass; m = p/v (E.g. Special Relativity, A.P. French, page 16 - See footnote #2 as well). Almost any text that uses rel-mass will explain that fact

According to the mass = magnitude of 4-momentum 4-vector - The magnitude of the 4-vector is simply proportional to the energy of the system. For the energy to remain constant then so too does the system mass.

For all the glorious details please see -
http://www.geocities.com/physics_world/sr/invariant_mass.htm

Ohanian has a nice discussion in his GR text.

Pete
 
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