Showing posts with label Planck. Show all posts
Showing posts with label Planck. Show all posts

Tuesday, 26 March 2024

SI World and Planck World - And an IDEA

I was thinking about adding this to the back of the last post, Coupling Constants, but it was already pretty long.  To understand the following though, it is probably useful to read that post first.

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To make my point, I am going to compare the same activity conducted in two different worlds.  The first world I am going to call SI world, in which SI units are used.  The second world is Planck world, in which – unsurprisingly – only Planck units are used.  In Planck world, everyday people are used to talking in terms of “p-mass”, “p-length”, “p-time”, “p-charge” and all of the derived units, such as “p-force” (instead of newtons), “p-energy” (instead of joules), “p-current” (instead of amperes) and so on.  Because they live in Planck world, they know that all the fundamental physical constants are unity (see the table at the end of Coupling Constants) and they do everything in terms of Planck.

The activity is considering the force on a medium sized pineapple at sea level on an Earth-like planet.

There’s the simple way:

And then there’s the complex way, noting that we wouldn’t use the complex way other than as a method to extract a value which we can use to compare the strength of forces:

The complex way provides us with a couple of things, the value of n1n2/r2, which could be reused if were talking about a conglomeration of charged massive particles (like protons) and, via a little side track, the coupling constants (which for Planck world is, of course, unity).  Note however that the magnitude of the gravitational coupling constants relates only to the square of the mass divided by Planck mass, so the side track isn’t really necessary in either world.

The same sort of process applies if we consider charged objects, imagining the same number of items (protons) for each object and the same distance, and noting that the resultant force will be one of repulsion:

Note that αEp is the fine structure constant, α.  Again, it is just the square of the value (the elementary charge) divided by the related Planck value (Planck charge).

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There’s no real reason to use the complex method to calculate the force.  And as mentioned above, there’s no need to use the side track in either case (gravitational or electromagnetic).  If you want to know the strength of coupling associated with any reference mass or charge, just divide the reference value (mass or charge) by the related Planck value (mass or charge) and square the result.  Simple.

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Just out of curiosity, I plugged in different values, namely two objects with a Planck unit each (mass in the first case and charge in the second).  These are the results:

Unsurprisingly, from one perspective at least, the values end up the same.  The question then arises: what is the Planck charge?  One way to think of it as the charge on the smallest possible charged (but non-rotating) black hole.

Such a black hole has a radius of rs=2GM/c2=lPl.  So, M=c2lPl/G/2=mPl/2. It also becomes “extremal” when 2rQ=rs, where r2Q=Q2G/(4πε0c4), so:

2rQ=2Q.√(G/(4πε0c4))=lPl

Q=lPl.c2.√(4πε0/G)/2

Noting that lPl=√(ħG/c3) and

Q=√(ħG/c3).c2.√(4πε0/G)/2=√(ħc.4πε0)/2=qPl/2

This means that the ratio of charge to mass in an extremal Reissner–Nordström black hole is unity, and half a Planck charge is the maximal charge on a minimal black hole (of half a Planck mass and radius of one Planck length).  This does at least gives some sort of meaning to the values I used, although it should be noted that it would not be possible to have such masses or charges at a separation of only one Planck length.  Halve them and you might be in business.

Generally, gravitation is labelled as a weak force, while electromagnetism is considered to be strong(er).  This is because, when considering atomic scales, we are talking about quite small masses and multiples of elementary charge.  Consider a hydrogen ion, which is a proton (the other isotopes of hydrogen which have neutrons have the special names deuterium [2H] and tritium [3H]).  This has a mass of 1.673×10-27 kg, or 7.69×10-20 units of Planck mass, and one elementary charge of 1.602×10-19 C, or 0.0854 units of Planck charge.  So, yes, gravitational force between two protons is miniscule in relation to their mutual electromagnetic force of repulsion, but only because the charge is enormous by comparison.

What we could say, perhaps, is that subatomic (and elementary) particles can carry significantly more charge than mass.  Why is that?  I don’t know if anyone has even asked the question before.  There is fact that particles have relativistic mass, which varies between frames with different speeds, but not relativistic charge.

So, the question that comes to me is, what speed (in a given frame) would a proton need to reach to have the same magnitude of Planck mass as it has in Planck charge.

The relativistic mass equation is (where m0 is the rest mass in a given frame):

m=m0/√(1-v2/c2)

Rearranging for v:

v =√(1- m02/m2).c

We want to get the magnitude of the mass of the proton (m0=mp) in units Planck mass to equal the charge (e) in units of Planck charge (||m||=||e||):

v =√(1- (7.69×10-20)2/(0.0854)2).c=√(1- 8.09×10-37).c≈(1-4.05×10-35).c

In other words, a proton achieves the relativistic mass equivalent in magnitude to its charge only when extremely close to the speed of light.  There is plenty of wriggle room in there, for sure, but the bottom line is that in order that the relativistic mass doesn’t get bigger than the charge (within realistic speeds), the rest mass of a proton must have a magnitude that is significantly lower than the magnitude of the charge. Other subatomic and elementary charged particles are available, but they all have significantly less mass than the proton (and charge within one order of magnitude).

The results in the tables above might make one wonder if the Planck force is a maximum.  It could be, at least in a sense.  It is the force required to accelerate one unit of Planck mass to the speed of light in a period of one Planck time, which would require one unit of Planck energy.  It would basically be instantaneous, especially if Planck time is fundamental, since it would be across a distance of one unit of Planck length.  Remember that one unit of Planck length per unit of Planck time is the speed of light.

The Falcon Heavy rocket has a maximum thrust of 22.8×106 N. NASA’s Space Launch System (Block 1) has a maximum thrust of 39×106 N.  The Starship rocket (still in development) has a projected maximum thrust of 89×106 N.  These are a long way short of 1.21×1044 N, but of course we talking about a completely different scale.

For comparison, we can consider the strong force.  Note that in the second paragraph of the related Wikipedia page, the forces are expressed in terms of a proton at an approximate distance of 10-15 m.  We know the mass and charge of a proton, and can assume that the interaction is between two protons (being bound into a nucleus).  Here are the gravitational and electromagnetic forces involved (just the simple calculations, since it can be seen above that the force and coupling constants don’t change):

The strong force is approximately 100 times stronger than electromagnetic force so, in this case (between two protons), in the order of 20 kN.  See also here (per Bdushaw – I don’t know how accurate this is, or whether it is merely supposed to be representative):

Curiously, this value is within one order of magnitude of the force due of two Planck black holes (m=mPl/2) or indeed two Planck masses (m=mPl) separated by the same distance – namely 10-15 m.

The forces are 8 kN in the first instance and 31 kN in the second or, in both cases, approximately 104 N.  Given that this is based on a distance of approximately 10-15 m and a force that is approximately 100 times stronger than the electromagnetic force, the results being approximately the same is remarkable.

Coincidence?  Probably.  I can’t think of a reason why the maximum strong force at a femtometre should be equivalent to the gravitational force between two individual Planck masses that are separated by a femtometre (and the force distance relationship would certainly not follow the curve shown above).

Well … not a good reason.  Here’s a completely bonkers reason.  Say we had an Intelligent Design and Engineering Agent (IDEA) who has committed to making the background of the universe pretty much like ours, a Planck universe in which the fundamental physical constants resolve to unity and the minimum divisions of space and time are Planck values.  The IDEA has a vague plan for the proton, but hasn’t set a size, mass or charge on it yet, just knowing that protons and neutrons will be bound together in a nucleus by some sort of strong force.  In the worst case, two protons will have to be bound together at a distance of a femtometre, but not for very long (note that 2He is extremely unstable, with a half-life of about 10-9s).  The IDEA wants to leave open a wide range of values for the mass and charge of the proton (but knows that the proton will be very small), so what value of the strong force at about a femtometre will be required?

In summary:

  •    The proton can be any size (smallest being a Planck volume)
  •    The proton can be any mass (although the maximum mass in a Planck volume is half a unit of Planck mass)
  •    The proton can have any charge (although the maximum charge in a Planck volume is half a unit of Planck charge)
  •    Separation between two bound protons in worst case is ~1fm
  •    Worst case is maximum charge, minimum mass (effectively zero mass)
  •    The IDEA selects, for some reason, the Planck volume as the reference size of the yet to be determined proton

So the IDEA would need a strong force that just about counteracts the repulsive force of two half units of Planck charges:

Therefore, a bit under 10kN.  But the IDEA is not just a designer, it is also an engineer which means that it is going over-engineer the design, so we can easily double that – bump the strong force up to about 20kN.

(Note that, in some explanations this doesn't actually seem to be required.  In those explanations, the apparent factor of 2 appears to be due merely to vague specifications.  For example, the strong force is sometime defined as 137 times stronger [or approximately so] than the electromagnetic force for an elementary charge.  If that were so, the would mean that the strong force is precisely strong enough to account for two charges acting on each other that are qPl/e greater than e, or (qPl/e)2=1/α stronger.  I have my doubts about this, in part because the strong force as commonly referred to is actually the residual strong force, being the force that is left over from the actual strong force that is holding the constituent quarks together.  It would surely be nice to be able to say that the strong force is has a strength of unity in some sense, but things are not quite that simple.)

This over-engineering would mean that if protons were particles with minimal mass and the maximal charge on a Planck black hole (half a unit of Planck charge), then the nucleus would still hold together with the strong force.  Once this value had been set, the IDEA would be limited to a low proton mass value, because the 2He nucleus would become stable if protons were significantly heavier.

(Stability of 2He nuclei would affect the availability of free protons to be fused into isotopes of hydrogen on the path to other isotopes of helium and maybe prevent stars from forming, meaning that shining stars, planets, pond scum and, ultimately, IDEA worshipping humans would then have to be created using magic and/or miracles rather than physics.)

Of course, I don’t think that this is the explanation.  But it is interesting that the forces involved are in approximately the same order of magnitude.

Sunday, 7 February 2021

Is QED Wrong, or Just Wikipedia?

There seems to be an error either with quantum electrodynamics (QED) and stochastic electrodynamics (SED) or Wikipedia.

 This is the section in question (archived):

 

Note the critical density of the universe is in the order of 10-26 kg/m3 which means that the critical energy density of the universe (given that E=mc2) is in the order of 10-9 J/m3.

Note also for a universe with a radius of one Planck length, at an age of once Planck time and a corresponding Hubble parameter value of one inverse Planck time, the critical density would be in the order of 1096 kg/m3 which corresponds with a critical energy density in the order of 10113 J/m3.

A vacuum energy of 10113 J/m3 beyond the spacetime origin of our universe is ridiculous.  As an example, the Earth has an average density of 5515 kg/m3, which is equivalent to an energy density of 5x1020 J/m3 – meaning that if the vacuum had a density of 10113 J/m3, it would swamp us.  We’d not even be a rounding error.

Whether QED/SED is wrong, or Wikipedia contains a misinterpretation of the writings of Peter Milonni and/or de la Pena and Cetto, I don’t actually know.  But anyone suggesting such a huge magnitude of vacuum energy density should really go back and check their figures.

I am certainly not going to stay awake at night worrying about the cosmological constant problem (or whether I need to worry about it being a slam dunk for Fine Tuners).

Thursday, 6 June 2019

Is the Universe (in) a Black Hole?

In short, in answer to the titular question - "not as such" - or, to put it in a bit more detail, "not really, but sort of (keeping in mind that it's also sort of not) or perhaps maybe".  A lot comes down to the definition of a black hole and certain characteristics associated with a black hole.  And where the singularity is (or rather when).

Let’s go through the argument, and please pay attention to the caveats and definitions.

Say we have a mass, M, which has compacted into a non-rotating, chargeless black hole.  The event horizon for this black hole is defined by the Schwarzschild radius, which is given by the equation:
rs = 2GM/c2
where G is the gravitational constant and c is the speed of light.

The volume of the black hole, using the event horizon as its edge and which I am going to call the Schwarzschild volume, Vs, is given by the equation:
Vs = 4πrs3/3 = 32/3.πG3M3/c6
And the density of such a black hole (using the volume defined by the Schwarzschild radius), which I am going to call the Schwarzschild density, ρs, is:

ρs = M/Vs = M / (32/3.πG3M3/c6) = 3c6/ (32πG3M2)

This shows that the Schwarzschild density of a black hole is inversely proportional to the square of its mass - meaning that the heavier the black hole is, the lower the Schwarzschild density it has.

The question I have is this; how big would a non-rotating, chargeless black hole be if the Schwarzschild density associated with it was the same as the density of the universe.

The equation for this mass (after rearranging the above) is:
M = sqrt (3c6/ (32πG3ρs))
The density of the universe is 9.9x10-30 g/cm3 (which, to use SI units, is the same as 9.9x10-27 kg/m3).  The mass equivalent to this, if it were a non-rotating, chargeless black hole, is 8.6x1052 kg.  And the Schwarzschild radius of a non-rotating, chargeless black hole with this mass is 1.3x1026 m.

When we get to such large distances though, we use a more convenient measure like the light year.  This means that the radius of a non-rotating, chargeless black hole with the density of the universe is 13.7 billion light years.

It just so happens that the age of the universe is 13.8 billion years (one of the most recent measurements is from the Planck Collaboration, which has the figure at 13.82 billion years).

Perhaps it’s merely coincidence (it's not by the way, but it's not strictly related to being (in) a black hole).

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There is however an immediate question that arises.  The radius of the observable universe, at the "age" discussed above is the radius of the observable universe today (by which I mean within a hundred million years or so).  And that is not believed to be 13.8 billion light years - it's actually thought to be in the order of 46 billion light years.  And then there is the actual universe which could be significantly larger.

To avoid pain here, I'm going to use the term "light horizon" defined as the distance light travels in the period equal to the age of the universe.  It would be an expanding sphere and it's possible that it doesn't have any physical significance.  It would, however, be the distance to the edge of the universe if the universe were expanding at the speed of light (and had always expanded at no more and no less than the speed of light).  Please note that physicists tell us that this is not the case.

At the time that the Earth formed, the light horizon would have been closer to 9 billion light years.  If the total mass of the universe were a constant, and the light horizon were all that there was then, at that time, the density of the universe would have been 3.3 times greater than today and calculations based on that density would give us a Schwarzschild radius of 7.4 billion light years.  It wouldn’t match up.

When the sun is scheduled to explode into a red giant, in about 5 billion years or so, the light horizon will be about 19 billion light years.  Making the same presumptions, that would give us a density about 1/3 of what it is today, leading to a Schwarzschild radius of 22 billion light years.  And, again, it wouldn't match up.

It might be difficult to accept that it is just a staggering coincidence that the density of the universe, right now, is equal to that of a non-rotating, chargeless black hole with a Schwarzschild radius equal to the light horizon, right now - remembering that the light horizon may have no physical significance.

The reason that it looks this way however is because the universe is flat.  A ramification of the universe being flat is that, as Sean Carroll puts it:
... some folks will stubbornly insist, there has to be something deep and interesting about the fact that the radius of the observable universe is comparable to the Schwarzschild radius of an equally-sized black hole. And there is! It means the universe is spatially flat.
You can figure this out by looking at the Friedmann equation, which relates the Hubble parameter to the energy density and the spatial curvature of the universe. The radius of our observable universe is basically the Hubble length, which is the speed of light divided by the Hubble parameter. It’s a straightforward exercise to calculate the amount of mass inside a sphere whose radius is the Hubble length ( M = 4π c3H-3/3), and then calculate the corresponding Schwarzschild radius (R = 2GM/c2). You will find that the radius equals the Hubble length, if the universe is spatially flat. Voila
Note that what I am calling the light horizon, Carroll is describing as "a sphere whose radius is the Hubble length"… that the total mass in the universe is increasing in proportion with the rate of expansion.  If it’s the latter, then I am tempted to think that dark matter is appearing in the universe at a rate of 6.4x1051 kg every billion years.  I know that this sounds like quite a lot, but that’s 0.2 μg of black matter appearing in a volume of space equal to the Sun each year.

Is there another interpretation?

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Note that the density of the universe given above, 9.9x10-30 g/m3, is based on the notion that the universe is flat.  Observations from both WMAP and the Planck Collaboration confirm that the universe is flat with a 0.4% margin of error.  Such a density is known as the critical density, meaning that universe will neither collapse nor expand forever without end.  Instead, it will eventually stop expanding – after an infinite time.  (At this site, an apparently different value for the density is presented, 10-26 kg/m3.  The difference here is due only to different units being used and the figure being rounded up.)

The fact that the universe appears to have this density is astounding (or “somewhat surprising” according to the understated people at Swinburne).  However, something should be noted: This value is the critical density right now.  In the past, the critical density would have been different and in the future it will be different again.  The equation for the critical density is:
ρc = 3H2/8πG
where H is the Hubble Constant.  As noted in an earlier article, the Hubble Constant is the inverse of the age of the universe.  This means that as the universe ages, ρc decreases.  And if ρc = ρs, as is the case in a flat universe, then:
3H2/8πG = 3c6/ (32πG3M2)
After introducing ꬱ = 1/H and rearranging, we have:
M = ꬱ.c3/2G
This implies that the universe is getting heavier by 1 unit of Planck energy every two units of Planck time.  Of interest is the fact that, with the assumption that the universe is flat and that it is expanding at the speed of light, we can recall the equation for the Schwarzschild radius and say that:
rs = ꬱ.c = 2GM/c2  =>  M = ꬱ.c3/2G
How much heavier would the universe get over a 1 billion years, using this calculation?  Plugging in the values, it should come as no surprise that we get 6.4x1051 kg, which is what I calculated a completely different way above.

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So what does all this mean?

Perhaps nothing.  The few people who have engaged with me from reddit.com seem to agree that the above does not have physical significance and one even accused me of numerology/astrology - a fair call when I had a few rookie errors in an earlier version including the wrong radius of the observable universe and a less carefully crafted comment about black holes.   The comment at the top of this article is still too controversial for one correspondent - he wants the answer to be a hard "no".  I think that if I meant what I think he thinks I mean, then the answer would be a hard no, but I don't think he knows what I mean.  Perhaps even if he knew what I mean, he'd still want a hard "no" and that's okay, I might be entirely wrong.

Since then, I've had some more time to think and some helpful interactions with some experts.  I've struggled with the idea of inflation for quite some time and I also struggle with the idea that the expansion of the universe is speeding up, although that's a little more recent.  I'll try to put together something on that topic in the next few days, including what might be a resolution of the first struggle, although potentially replaced by a different, albeit related one.

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Further corrections gratefully welcomed.