How is the weak force related to a change in velocity?

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Discussion Overview

The discussion centers on understanding the weak force and its relation to changes in motion, particularly in the context of particle decay. Participants explore the conceptualization of the weak force as a fundamental interaction and how it fits within the framework of the four fundamental forces, including comparisons to classical mechanics and quantum mechanics.

Discussion Character

  • Exploratory
  • Conceptual clarification
  • Debate/contested
  • Technical explanation

Main Points Raised

  • One participant expresses confusion about how the weak force relates to changes in motion, noting that most explanations focus on radioactive decay rather than on force as a change in motion.
  • Another participant suggests that one could either refer to it as the weak interaction or expand the definition of force to include the weak interaction.
  • A later reply indicates that extending the notion of force to include decay processes is a valid approach, linking it to the role of carrier particles like W and Z bosons.
  • There is a discussion about the limitations of classical concepts like Newton's second law in the context of quantum mechanics, with an emphasis on how quantum mechanics predicts scattering cross-sections rather than classical force relationships.
  • One participant mentions that Coulomb's law does not hold at high energies for quantum particles, suggesting a need for a different understanding of forces in quantum contexts.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the nature of the weak force as a "force" in the traditional sense. There are competing views on whether to redefine force to include weak interactions or to maintain a distinction between traditional forces and interactions like decay.

Contextual Notes

The discussion highlights the challenges of reconciling classical and quantum perspectives on forces, with participants acknowledging the limitations of classical definitions in the quantum realm.

Who May Find This Useful

This discussion may be of interest to those exploring the fundamental forces in physics, particularly students or enthusiasts seeking to understand the weak force and its implications in particle physics.

SamRoss
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TL;DR
Seeking intuitive understanding of how the weak force "pushes" particles.
Hi everyone,

The four fundamental forces are gravity (I understand that G.R. does not look upon gravity as a force but I'm not worried about that here), the Lorentz force, the weak force, and the strong force. I'm familiar with the inverse square law for gravitation and the Lorentz force F=q(E+vxB). I also have the dimmest understanding of how the strong force is related to a change in motion (protons in the nucleus of an atom would want to move away from each other due to the Lorentz force so there must be another force, called the strong force, which changes this desired motion and pushes them back toward each other; that's as far as my understanding goes). However, whenever I search for some explanation of the weak force, I only see how it is related to radioactive decay and I don't see clearly how this can be categorized as a "change in motion" which is what a force is supposed to do. Any help here would be appreciated. Also, similar to how we now think of a=GM/r^2 as an approximation of the motion predicted by G.R., are there analogous approximations of both the strong and weak forces that do not require a high level of understanding of Q.E.D and Q.C.D?
 
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SamRoss said:
Summary:: Seeking intuitive understanding of how the weak force "pushes" particles.

Hi everyone,

decay and I don't see clearly how this can be categorized as a "change in motion" which is what a force is supposed to do. Any help here would be appreciated.

You have two options:

1) Call it the weak interaction;

2) Extent your notion of force to encompass the weak interaction.
 
Vanadium 50 said:
PeroK said:
You have two options:

1) Call it the weak interaction;

2) Extent your notion of force to encompass the weak interaction.

Okay, so we're extending our idea of what we call a "force" to include not only something that results in acceleration but also something that results in particles decaying into other particles. The reason for this extension is that both acceleration and decay are the result of carrier particles (W and Z bosons for decay, photons for electromagnetism, gluons for the strong force, and gravitons for gravity). Is that right?
 
SamRoss said:
Okay, so we're extending our idea of what we call a "force" to include not only something that results in acceleration but also something that results in particles decaying into other particles.
Newton's second law, ##F = ma##, is a classical concept. There's no concept of this in QM, as such. Instead, it emerges from the interaction of many quantum particles. Instead, QM tends to predict scattering cross-sections.

Coulomb's law breaks down, for example, at high energies for quantum particles.
 
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