Why Mass Not Conserved in Weak Quark Interactions?

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In summary, mass is not conserved in most weak quark interactions, as seen in the example of d → u + W-, where the mass of the down quark is about 4.8 MeV, the up quark is about 2.4 MeV, and the W- mass is 80.4 GeV. This is due to energy conservation, which allows for the production of a virtual W-boson that quickly decays into other particles. In simpler terms, while energy and momentum are conserved, the sum of rest masses is not.
  • #1
potatobabe
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Hi, this may be a stupid and obvious question but its my first post so allow me to ask:

Why is mass not conserved in most weak quark interactions e.g : d → u + W-
the mass of the down quark is about 4.8 MeV
and the up quark is about 2.4 MeV
and the W- mass is 80.4 GeV!
And even accounting for the constituent quark mass the equation doesn't add up,
could someone clear this up for me? Thanks.
 
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  • #2
There is no mass conservation.
There is energy conservation - and your process cannot produce a real W-boson for that reason. It can, however, produce a virtual W-boson (that can violate the energy-momentum relation for the W) which quickly decays into other particles.
 
  • #3
okay thanks for clearing that up for me :)
 
  • #4
look at the simple example

[tex]e^+ + e^- \to 2\gamma[/tex]

Energy E and momentum p are conserved. The invariant mass m is conserved, too:

[tex]E = E_{e^+} + E_{e^-}[/tex]
[tex]p = p_{e^+} + p_{e^-}[/tex]
[tex]m^2 = E^2 - p^2[/tex]

and

[tex]E' = E'_{\gamma_1} + E'_{\gamma_2}[/tex]
[tex]p' = p'_{\gamma_1} + p'_{\gamma_2}[/tex]
[tex]m'^2 = E'^2 - p'^2[/tex]

with

[tex]m = m'[/tex]

But of course the sum of the rest masses is not conserved

[tex]m_{e^+} +m_{e^-} \neq 2 m_{\gamma}[/tex]
 

Related to Why Mass Not Conserved in Weak Quark Interactions?

1. Why is mass not conserved in weak quark interactions?

The concept of mass conservation is a fundamental principle in physics, but it does not hold true in weak quark interactions. This is because in these interactions, particles can change into their antiparticles, resulting in a decrease in the total mass of the system. Additionally, the energy-mass equivalence principle allows for the creation and annihilation of particles, further contributing to the non-conservation of mass in weak quark interactions.

2. How does the Higgs field play a role in mass non-conservation?

The Higgs field is responsible for giving particles their mass through the Higgs mechanism. In weak quark interactions, the Higgs field can interact with the quarks, changing their masses and therefore contributing to the non-conservation of mass in these interactions. The Higgs boson, which was discovered in 2012, is a manifestation of the Higgs field and plays a crucial role in our understanding of mass in the universe.

3. Does the non-conservation of mass violate the law of conservation of energy?

No, the non-conservation of mass in weak quark interactions does not violate the law of conservation of energy. In these interactions, mass is converted into energy or vice versa, but the total energy of the system remains conserved. This is due to the energy-mass equivalence principle, which states that mass and energy are interchangeable.

4. Are there any other interactions in which mass is not conserved?

In addition to weak quark interactions, there are other interactions in which mass is not conserved. For example, in nuclear reactions and particle collisions, mass can be converted into energy or vice versa. Mass is also not conserved in certain cosmological events, such as the expansion of the universe and the formation of black holes.

5. How does the non-conservation of mass affect our understanding of the universe?

The non-conservation of mass in weak quark interactions and other interactions plays a crucial role in our understanding of the universe. It allows for the creation of new particles and the transformation of matter into energy, which are essential processes in the evolution of the universe. The non-conservation of mass also contributes to the understanding of the fundamental forces and particles that govern the universe, as well as the study of dark matter and dark energy.

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