Unitless constants and unitized forces

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Discussion Overview

The discussion revolves around the classification of coupling constants as unitized or unitless, particularly focusing on the weak coupling constant and its relationship to forces. Participants explore the implications of unitless constants in theoretical physics, including their potential as ratios of forces, and the impact of unit choice on these classifications.

Discussion Character

  • Debate/contested
  • Conceptual clarification
  • Technical explanation

Main Points Raised

  • Some participants assert that coupling constants can be either unitized or unitless, with examples like charge (e) and gravity (G) being unitized, while constants like the fine structure constant (\alpha) are unitless ratios where units cancel out.
  • There is a question about whether the weak coupling constant is a ratio of forces similar to the fine structure constant, with some participants seeking clarification on this point.
  • One participant challenges the classification of coupling constants as unitful or unitless, suggesting that any three universal constants can be set to 1, resulting in a unitless system, but this does not necessarily imply that all constants are unitless in physical terms.
  • Another participant points out that using units where c, G, and h are set to 1 does not make the value of a force unitless, arguing that the fine structure constant retains units of charge under such conditions.
  • There is a discussion about the implications of the weak angle being a unitless coupling constant and whether it indicates a ratio of two forces, with some participants questioning the nature of these forces.
  • Clarification is sought regarding the term "Lorentzian \beta," with some participants noting it refers to a relativistic quantity rather than a coupling constant.

Areas of Agreement / Disagreement

Participants express differing views on the classification of coupling constants, whether the weak coupling constant is a ratio of forces, and the implications of unit choice. No consensus is reached on these points, indicating ongoing debate and exploration of the topic.

Contextual Notes

Limitations include the dependence on definitions of unitless and unitized constants, as well as unresolved questions regarding the nature of forces associated with the weak coupling constant.

enotstrebor
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Coupling constants are unitized or unitless. Forces are associated to unitized coupling constants like charge (e), gravity (G), etc. All unitless coupling constants that I know of, like the fine structure constant (\alpha), or the Lorentzian \beta, etc are ratios where the units cancel out.

As the weak coupling constant is unitless;
Does this mean it is a ratio of forces like the fine structure constant? If not why not.
 
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enotstrebor said:
Coupling constants are unitized or unitless. Forces are associated to unitized coupling constants like charge (e), gravity (G), etc. All unitless coupling constants that I know of, like the fine structure constant (\alpha), or the Lorentzian \beta, etc are ratios where the units cancel out.
What do you mean when you refer to the "Lorentzian \beta?" To me this suggests the relativistic \beta=v/c, which isn't a coupling constant.

I don't think it makes sense to classify coupling constants as unitful or unitless. The SI has three basic units, for length, time, and mass. You can pick any three universal constants you like and set them equal to 1, and then you get a system of units where everything is unitless. For instance, if you pick c=1, G=1, and h=1, you get a system of units where everything is unitless, and the Planck distance equals 1. Of c, G, and h, one (G) is clearly a coupling constant, another (c) could be considered to be one, and one (h) is not. Suppose I choose to set c=1, h=1, and the mass of the electron=1. Then I get a system of units where G does not equal 1, but it's unitless, because everything is unitless. I could also just set c=1 and h=1, and then G would have units.

As the weak coupling constant is unitless;
Does this mean it is a ratio of forces like the fine structure constant? If not why not.

Above the electroweak unification energy, the weak interaction is unified with the EM interaction, so aren't the coupling constants the same?
 
bcrowell said:
What do you mean when you refer to the "Lorentzian \beta?" To me this suggests the relativistic \beta=v/c, which isn't a coupling constant.

I don't think it makes sense to classify coupling constants as unitful or unitless. The SI has three basic units, for length, time, and mass. You can pick any three universal constants you like and set them equal to 1, and then you get a system of units where everything is unitless. For instance, if you pick c=1, G=1, and h=1, you get a system of units where everything is unitless, and the Planck distance equals 1. Of c, G, and h, one (G) is clearly a coupling constant, another (c) could be considered to be one, and one (h) is not. Suppose I choose to set c=1, h=1, and the mass of the electron=1. Then I get a system of units where G does not equal 1, but it's unitless, because everything is unitless. I could also just set c=1 and h=1, and then G would have units.



Above the electroweak unification energy, the weak interaction is unified with the EM interaction, so aren't the coupling constants the same?

But the beauty of the coupling constants is that their value does not depend on your choice of units. So in units where h=c=G=1 the value of alpha, the EM coupling constant, is still 1/137 (approx.), and it stays that way whatever your choice of units is.
 
No coupling constant does not per se be unitless, look at

\lambda \, \phi^3

a fully allowed term in a lagrangian.

is \lambda

unitless here? (in the choice where c = hbar = 1 and unitless)
 
bcrowell said:
What do you mean when you refer to the "Lorentzian \beta?" To me this suggests the relativistic \beta=v/c, which isn't a coupling constant.
?
My appologies I meant to say unitless constants in the first part.
 
bcrowell said:
You can pick any three universal constants you like and set them equal to 1, and then you get a system of units where everything is unitless. For instance, if you pick c=1, G=1, and h=1, you get a system of units where everything is unitless

Using c=\hbar=1 does not make the value of a force unitless. For instance if you were really setting c=\hbar=1 then the units of the fine structure constant alpha=e^2/(c*h)=e^2/(1*1) would not be unitless but have the units of charge. The use of thetype conventions are just a mathematical convenience. They do not make things unitless.

The question is, if the weak angle is a unitless coupling constant does that imply that it is the ratio of two forces just like the fines structure constant is ther ratio of two forces (charge and spin).

If not why not?

If so, what are the components of weak angle ratio (what are the two forces?).
 
Last edited:
enotstrebor said:
The question is, if the weak angle is a unitless coupling constant does that imply that it is the ratio of two forces just like the fines structure constant is ther ratio of two forces (charge and spin).

As was pointed out in https://www.physicsforums.com/showthread.php?t=365156", charge and spin are not forces.
 
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