Understanding the Residual Strong Force on Hadrons - Explained

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Discussion Overview

The discussion centers around the nature of the residual strong force acting on hadrons, particularly focusing on why hadrons, which carry no net color charge, still experience this force. Participants explore theoretical aspects, calculations of force strength, and the implications of quantum mechanics versus classical mechanics in understanding these interactions.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants inquire about the origin of the residual strong force and its implications for hadrons that carry no net color charge.
  • Links to external resources are provided to clarify the concept of the residual strong force.
  • Participants present calculations of the average strong force between neutrons and protons, with one participant stating it to be approximately 456 N, while another questions the use of mass units to express force strength.
  • There is a discussion about the meaning of "average" in the context of force calculations, with some participants suggesting that the force may vary significantly depending on the distance between particles.
  • One participant argues that the strong force does not drop to zero at 3 fm, challenging the notion of well-defined boundaries for protons and neutrons and emphasizing the overlap of their wave functions.
  • Another participant asserts that classical mechanics is inappropriate for nuclear scales, while others defend the occasional use of classical theory for estimations.
  • Disagreements arise regarding the validity of classical mechanics in the context of quantum mechanics, with some participants asserting that quantum mechanics provides a more accurate framework for understanding these forces.

Areas of Agreement / Disagreement

Participants express multiple competing views regarding the nature of the strong force, the appropriateness of classical mechanics at nuclear scales, and the interpretation of force calculations. The discussion remains unresolved with no consensus reached on these points.

Contextual Notes

Participants highlight limitations in the definitions and assumptions used in their discussions, particularly regarding the interpretation of force strength and the applicability of classical versus quantum mechanics in nuclear interactions.

Garlic
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Hello everyone,
Why does the residual strong force arise?
Hadrons carry no net color charge, so why are they experiencing the strong force?
 
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The average strong force between a neutron and a proton is about 46kg.
 
kiwaho said:
The average strong force between a neutron and a proton is about 46kg.

I'm sorry, I don't understand what you mean. How can you show the force strength with a mass unit?
 
Garlic said:
I'm sorry, I don't understand what you mean. How can you show the force strength with a mass unit?
OK, the said strong force should be 456N.
 
Last edited:
Or ~3 MeV/fm. What does "average" mean? Averaged over what? The order of magnitude is certainly right, but 456 N looks very specific.
 
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mfb said:
Or ~3 MeV/fm. What does "average" mean? Averaged over what? The order of magnitude is certainly right, but 456 N looks very specific.
The 456N is calculated from classical kinematic equation Work = Average_Forece*Distance.
I use the data of deuterium. The binding energy is 2.22456MeV, and given 1MeV= 1.602*10^(-13)J.
The Distance = 3 - 2.22 = 0.78fm, because after 3fm, the strong force is 0, and the 2.22fm is the minimum distance between neutron and proton in deuterium. When 2 particles are kissing together, their distance equals to the sum of their radii, and both radii of proton and neutron are officially given.
Now we have: the Work= 2.22456* 1.602*10^(-13)J = 0.78*10^(-15) *Average_Force.
So the Average_Force= 2.22456* 1.602*10^(-13)J/0.78*10^(-15) = 456N
The max force occurs while 2 hadrons kissing together, of course, it will be far greater than the Average_Force 456N.
If the strong force is reduced to 0 at 3fm linearly, then the max force = 2* Average_Force = 912N, but probably the attenuation is not by linear but by exponential, so the max force may be a couple of thousands Newtonian level.
 
kiwaho said:
after 3fm, the strong force is 0
This is not true.
kiwaho said:
and the 2.22fm is the minimum distance between neutron and proton in deuterium. When 2 particles are kissing together, their distance equals to the sum of their radii
And this is completely wrong.
Proton and neutron are not billard balls. Their wave functions overlap. And they don't have a well-defined boundary either. The radius value is usually the root mean square of something (charge, mass, or whatever).
 
  • #10
mfb said:
This is not true.And this is completely wrong.
Proton and neutron are not billard balls. Their wave functions overlap. And they don't have a well-defined boundary either. The radius value is usually the root mean square of something (charge, mass, or whatever).
The specific weight of neutron is very very high, so it is the hardest matter in universe! do you think they can overlap concentrically?
Even the minimum distance is not the sum of their radii, the split distance may be doubled, that means the average force will be half of 456N, still in the same order of magnitude.
 
  • #11
kiwaho said:
The specific weight of neutron is very very high, so it is the hardest matter in universe!
This is just nonsense.
kiwaho said:
do you think they can overlap concentrically?
I don't just "think" so, I work with the consequences of it (parton collisions at high energy) every day.
kiwaho said:
Even the minimum distance is not the sum of their radii, the split distance may be doubled, that means the average force will be half of 456N, still in the same order of magnitude.
This does not make sense.

As Orodruin and ZapperZ already told you here: quantum mechanics is not classical mechanics on a smaller scale, it is completely different.
Feel free to ask questions, but don't claim things that are simply wrong.
 
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  • #12
mfb said:
This is just nonsense.I don't just "think" so, I work with the consequences of it (parton collisions at high energy) every day.This does not make sense.

As Orodruin and ZapperZ already told you here: quantum mechanics is not classical mechanics on a smaller scale, it is completely different.
Feel free to ask questions, but don't claim things that are simply wrong.
I believe quantum mechanics QM is right. But for estimation, why not to hug classical theory occasionally? You know, QM only talks about potential or energy, but never quantitizes force although QM often talks about force.
Bohr calculated the radius of hydrogen atom by method of classical mechanics, even the controversial "classic radius of electron" 2.8fm has the same base.
 
  • #13
kiwaho said:
But for estimation, why not to hug classical theory occasionally?

Classical mechanics is inappropriate to use at nuclear scales.

kiwaho said:
Bohr calculated the radius of hydrogen atom by method of classical mechanics

Yes, and he got the wrong answer by a factor of 3/2.

mfb said:
Feel free to ask questions, but don't claim things that are simply wrong.

Exactly.
 
  • #14
kiwaho said:
I believe quantum mechanics QM is right.
Then I suggest you learn quantum mechanics.
kiwaho said:
You know, QM only talks about potential or energy, but never quantitizes force although QM often talks about force.
You can calculate forces in quantum mechanics, but they are rarely single values, and rarely useful.
kiwaho said:
Bohr calculated the radius of hydrogen atom by method of classical mechanics
Not purely classical mechanics, he used something between classical mechanics and quantum theory. And he got it wrong, as V50 noted already.
kiwaho said:
even the controversial "classic radius of electron" 2.8fm has the same base.
And we know today this is not the electron radius. If it has a radius at all, it has to be much smaller.
 
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