Tuesday 19 March 2024

Coupling Constants

I revisited Constants that Resolve to Unity recently and I updated the table there, replicated below.

For the most part these were minor changes, correcting the symbols for current and temperature, fixing the column width, making the subscript notation consistent and so on.  But there was a more significant change, which was a mention of the ratio between the square of elementary charge e and Planck charge that is expressed by fine structure constant α.

I had been thinking about doing something similar with another value, the gravitational coupling constant αG, but this is a bit of an odd constant as it’s often poorly defined.  I kept niggling at it, trying to get a good explanation of what all these coupling constants are, including the fine structure constant.  I noticed that there is a mathematical similarly between α and αG, beyond them both using alpha as their notation.  Namely, that α=e2/qPl2 and αG=m2/mPl2 (where m is the mass of whatever you are using as the basis of the gravitational coupling constant, which you can clarify by using a subscript to both the m term and after the G in the αG term, but they often don’t).

The clearest explanation for these coupling constants that I found was here, but there is an error in it and it is not completely clear, so I will have a hack at it in a way that totally avoids the introduction of that error.

Thanks to Professor Watkins, who has since retired.

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I will start with gravitational coupling since this is the most intuitive and then go back to charge coupling.

We know that a body with mass m1 that is a distance r away from a second body with mass m2 will experience a force of gravity FG given by:

FG=Gm1m2/r2

We could think of m1 and m2 being accumulations of unspecified numbers n1 and n2 of neutrons that each have mass mn such that m1=n1mn and m2=n2mn.  This means that the force FG varies by the number of neutrons involved and the distance and is mediated by a constant value (dubbed a “force constant” by Watkins, with the choice to use φ to denote it being mine).  So:

φG=G.mn2

And:

FG=Gm1m2/r2=φG.(n1n2/r2)

Watkins then introduces the term ħc and shows, numerically, that:

φG/ħc=αG

where αG is specifically the gravitational coupling constant for a neutron, so to be more accurate, after rearranging:

αGn=φGn/ħc=mn2.(G/ħc)

Note that the value of Planck mass is mPl=(ħc/G).  Therefore, G/ħc=1/mPl2 and so:

αGn=mn2/mPl2

Watkins does not explain the introduction of the term ħc, so I suggest a slightly different approach.

The term φG, or rather φGn, can be broken down further into two terms, one that carries the units and one that is dimensionless, noting that the dimensionless term mPl2/mPl2=1:

φGn=G.mn2.mPl2/mPl2=(mn2/mPl2).(GmPl2)

The ratio of the two masses is, of course, dimensionless and can therefore be assigned as αGn.  We know that mPl=(ħc/G) so the second term becomes:

GmPl2=G.((ħc/G))2= G.ħc/G=ħc

So we arrive at φGn expressed as two terms (the second being the ħc that Watkins introduces without explanation):

φGnGn.ħc

or, rearranged:

αGn=φGn/ħc [=mn2.(G/ħc)]

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Note that the derivation above was done in terms of a neutron mass mn but there was no stage at which the value of mn needed to be specified.  Therefore, the exact same logic applies irrespective of what mass we use, so we could say:

αGx=mx2/mPl2

where x can refer to any mass; that of a neutron, electron, proton, Planck mass and any other random mass you want.  Filling in the first four, we arrive at:

 


The error that Watkins introduced was with the value of αGn.  For some reason, Watkins arrives at 3.76915×10-39 as the ratio between 1.871855×10-64 and 3.1616×10-26, which is clearly wrong (1.871855/3.1616=0.5920594, with the small variation in magnitude being due to a difference in our values for G).  This error was irrelevant to the logic of the derivation.

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The same sort of process as above can be used to derive an electromagnetic coupling constant via the formula:

F=q1q2/4πε0r2

Using the same logic, thinking of q1 and q2 as unspecified numbers n1 and n2 of units of elementary charge e, we see that q1=n1e and q2=n2e.  There is another force constant φE implied here (E for electromagnetic):

φE=e2/4πε0

Watkins just introduces ħc, so that we get:

αEE/ħc=e2/(4πε0.ħc)

And, because qPl=(ħc.4πε0):

αE=e2/qPl2

The electromagnetic coupling constant associated with the elementary charge isn’t normally called that, but is rather referred to as the fine structure constant, and the subscript E is not used.  So:

α=e2/qPl2

As with the gravitational case, the φE term can be broken down, this time using qPl2/qPl2=1:

φE=e2/4πε0.qPl2/qPl2=(e2/qPl2).(qPl2/(4πε0))

The ratio of the two charges is dimensionless and can be assigned as α.  Noting that qPl=(ħc.4πε0), the second term becomes:

qPl2/(4πε0)=ħc.4πε0/(4πε0)=ħc

So:

φE= α.ħc

Or, rearranged:

αEE/ħc [=e2/(4πε0.ħc)]

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Note also that ke=1/4πε0, so:

αE=e2/(4πε0.ħc)=e2/(ħc/ke)

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Similarly with the gravitational coupling constant derived above, a particular charge was selected with the electromagnetic coupling constant (or fine structure constant) relating specifically to the elementary charge.  Other charges are available, such as the charge on up and down quarks, +2e/3 and -e/3 respectively, or the Planck charge.

Therefore, as per the logic above, we could say that:

αEx=qx2/qPl2

where x can refer to any charge.  This gives us, for the options above:

 

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Note that I have included two terms αGPl and αEPl.  These could be referred to as the “natural coupling constants” (gravitational and electromagnetic respectively).  For the purposes of adding to the suite of constants that resolve to unity, this means I now have two more.  Doing so demotes the fine structure constant to what it actually is, just the square of the ratio between the charge selected to represent (so, the elementary charge) and the natural unit (the Planck charge).  The same applies to whatever variant of the gravitational coupling constant you would like to talk about.  The natural value is unity, and any other value is merely the square of the ratio of the mass selected and the Planck mass.

Of course, it would no longer be possible, if anyone actually does this, to say that the fine structure constant tells the universe what the relationship between the elementary charge and the Planck charge is.  But it doesn’t, the fine structure constant is merely something that falls out of the fact that the elementary charge has a specific value.

I remain totally unconvinced that the fine structure constant tells us anything more than the ratio between the elementary charge and the Planck charge.  The physical interpretations given at Wikipedia all seem to fall out of this ratio.  (I plan to write something on this in a later post.)

The same logic applies to the various options for the gravitational coupling constant.

To ram the point home further, we could establish the gravitational coupling constant in terms of standard duck masses (mduck), because the equation is, very simply:

αGduck=mduck2/mPl2

And the same if we use the standard charge on a post-launch duck (qduck), in which case the duck centred fine structure constant becomes:

αduck=qduck2/qPl2

By careful selection of the values of mduck or qduck, a sufficiently motivated researcher could come up with startling numbers the coupling constants – much more exciting one than ~1/137.  Want it to equal pi to ten significant figures, just make qduck=3.3233509704×10-18C.

The immediate response is (or should be) that this duck centred fine structure constant (αduck=π) doesn’t mean anything.  It certainly wouldn’t tell us why the standard charge on a post-launch duck (qduck) had that value, if it did.  The value of the αduck would simply be a different way of saying that qduck has the value that it has (qduck= qPl.√αduck) – a simple truism.

Similarly, none of the variants of the gravitational coupling constant nor the fine structure constant are really telling us anything useful in themselves.

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There are (at least) two other coupling constants (associated with weak and strong interaction), but I don’t really want to get into them.  I don’t think they would relate to Planck units, having done a quick check.  Perhaps someone else with a better knowledge of such things could have a good think about it and let me know.

It is possible that they tell us something, but it is equally possible that these coupling constants are similar to the gravitational and electromagnetic coupling constants in at least that sense and tell us nothing new at all.  My brief and patently inadequate check indicated that while the wording “coupling constant” is used for all four, and the meaning is comparable between the weak and strong interactions, they are not actually the same sort of thing as we talking about with respect to electromagnetic and gravitational force coupling.

That said, it is interesting to note that the strong force is usually thought of having a relative strength of 1.  Maybe you might thing, ah, but that's different.  Note however, that while the relative strength is listed at the link above as being in the order o10-3, it's more often listed as being in the order of 10-2 and frequently more specifically as 1/137 (or more precisely, α).  Sadly, however, if you dig a bit deeper, you will find that the strong force is only approximated as 1, and sometimes has a value closer to 14.5 (or the inverse thereof, the explanation I saw was a bit vague on that point), and - in terms of a nucleus - is only the residual force left over from holding the constituent quarks of a proton or neutron together. 

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Finally, here is the updated table of constants that resolve to unity (noting that I have removed the charge to structure ratio as irrelevant, added some more formulas for clarity and also changed to a font that makes the difference between a large “i” and a small “L” a little more distinct):

And, for ease of reference, a clean version with the greyed-out items removed:

All unity, as far as the eye can see.  Truly beautiful.

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