Small=high mass at quantum level, but big=high mass at classical level. Why?

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Discussion Overview

The discussion revolves around the contrasting relationships between size and mass in classical and quantum physics. Participants explore how larger physical objects typically correlate with greater mass in classical contexts, while at the quantum level, smaller entities may exhibit higher mass due to their wave-particle characteristics. The conversation delves into the implications of angular momentum, energy, and the behavior of particles in different contexts.

Discussion Character

  • Debate/contested
  • Conceptual clarification
  • Technical explanation

Main Points Raised

  • Some participants suggest that at a classical level, larger size corresponds to larger mass due to constant density, while at the quantum level, smaller size can imply larger mass due to the relationship between momentum and wavelength.
  • One participant proposes that all subatomic particles have the same angular momentum, leading to an inverse relationship between radius and mass, although this claim is contested.
  • Another viewpoint emphasizes that the classical intuition of constant density does not hold in quantum physics, where energy increases with compression, affecting mass.
  • Some argue that the contrast is not merely classical versus quantum but rather relates to the behavior of single versus multiple particles, where the total energy and size scale with the number of particles.
  • Concerns are raised about the application of DeBroglie's wave-particle formula to large objects, noting that larger objects have greater momentum but smaller wavelengths, complicating the relationship.
  • Participants discuss the distinction between fermions and bosons, highlighting that fermions cannot occupy the same state, affecting the mass and size relationship in composite particles like atomic nuclei.

Areas of Agreement / Disagreement

Participants express differing views on the relationships between size, mass, and particle behavior, indicating that there is no consensus on the underlying principles governing these phenomena. Disagreements arise regarding the application of classical concepts to quantum scenarios and the implications of particle statistics.

Contextual Notes

Some claims rely on specific assumptions about particle behavior and definitions of mass and energy, which may not be universally accepted. The discussion highlights the complexity of applying classical intuitions to quantum mechanics without resolving the mathematical and conceptual nuances involved.

SteveinLondon
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At a classical physics level, physically big equates to big mass, but at the sub-atomic level, small seems to equate to big mass i.e. (short wavelength big mass relationship. "momentum=h/wavelength"). Any ideas why there is this complete contrast?
 
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because all subatomic particles have (roughly) the same angular momentum (ħ)

http://en.wikipedia.org/wiki/Bohr_model

7b15bb0e886212c070b6b20d8f7eeb89.png


so radius is inversely proportional to mass
 
Last edited:
granpa said:
because all subatomic particles have the same angular momentum (ħ)

No they don't.

If you don't know the answer, it's not necessary to reply.
 
In classical physics you have an intuition that all objects have constant density. So bigger size with the same density yields bigger mass.

In quantum physics "density" is not constant. You rather have some constant amount of something (aether, waves) and you squeeze it. The classical intuition would be that the mass of a squeezed body remains constant, but from special relativity you get that the energy of the body gets higher. And higher energy means higher mass.

Those two approaches can be considered at the same time. You get then the balance between classical and quantum physics. This yields the definition of Planck mass and the Bekenstein bound.
 
SteveinLondon said:
At a classical physics level, physically big equates to big mass, but at the sub-atomic level, small seems to equate to big mass i.e. (short wavelength big mass relationship. "momentum=h/wavelength"). Any ideas why there is this complete contrast?
It is not so much classical vs quantum, but rather one vs many particles. For one quantum particle, smaller length x means more energy e, as you said. But if you have MANY (say N) such small particles at DIFFERENT positions, then total energy and total length scale like
E=Ne
X=Nx
so bigger N means both bigger E and bigger X.
 
Demystifier said:
It is not so much classical vs quantum, but rather one vs many particles. For one quantum particle, smaller length x means more energy e, as you said. But if you have MANY (say N) such small particles at DIFFERENT positions, then total energy and total length scale like
E=Ne
X=Nx
so bigger N means both bigger E and bigger X.
But if you use DeBroglie's wave/particle formula on a large object, say a rock, you get momentum=h/wavelength, so a big rock, at the same speed as a little rock, has bigger momentum yet smaller wavelength - yet it's made up from more than one particle.
 
Becuase on a quantum-level, the universe isn't intuitive?
 
SteveinLondon said:
But if you use DeBroglie's wave/particle formula on a large object, say a rock, you get momentum=h/wavelength, so a big rock, at the same speed as a little rock, has bigger momentum yet smaller wavelength - yet it's made up from more than one particle.
Yes, but it is incorrect to apply the DeBroglie's wave/particle formula on an object consisting of many particles. For example, the nucleus of an atom is very small (much smaller than the atom itself), and yet a heavier nucleus is bigger than a lighter one. That's because the nucleus consists of many particles.

More precisely, it is not enough to have many particles. In addition, these particles must be FERMIONS (which protons and neutrons in the nucleus are), so that you cannot put all them at the same place.

If you have BOSONS (e.g., photons), then you can put many of them in the same state, so with a fixed wavelength (fixed energy of one particle) the size of N bosons may not depend on the total energy of N particles.
 

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