Varying dimensional universal constants

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SUMMARY

This discussion centers on the implications of varying the dimensional universal constants, specifically the Planck constant (h) and the speed of light (c). Participants argue that changing these constants would not alter the underlying physics but would instead modify the numerical values of measurements. The conversation highlights the circularity of measuring c in SI units, as it is defined based on the speed of light itself. Ultimately, the consensus is that while hypothetical scenarios can be considered, the fundamental relationships in physics remain unchanged.

PREREQUISITES
  • Understanding of dimensional universal constants, specifically Planck constant (h) and speed of light (c).
  • Familiarity with SI unit definitions and their historical context.
  • Basic knowledge of relativity and its relationship to massless particles.
  • Awareness of dimensionless constants such as the fine-structure constant (α).
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  • Research the implications of changing dimensional constants on physical laws.
  • Explore the historical evolution of SI unit definitions and their impact on modern physics.
  • Study the role of dimensionless constants in quantum mechanics and relativity.
  • Investigate alternative theories of electromagnetism, such as Proca's theory involving massive photons.
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Physicists, students of theoretical physics, and anyone interested in the foundational principles of measurement and the implications of universal constants in scientific theories.

Pnin
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If Planck constant h and light speed constant c were (very) different, would we notice it?

(I know we can change units and make h and c take any numerical value we like. But let‘s stick with one set of units.)

I assume rulers, clocks, coupling constants, all dimensionless constants would change. So would Planck lenght, time and mass.

What would we notice if these constants in some chosen set of units were different?
 
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If you wanted to stick to "one set of units," you should not have picked c and h. The quantity c, for example converts meters to seconds in the same 2.54 cm/in converts inches to centimeters. If you treat space and time on equal footing, you measure time and space using the same units, so c is 1 m/m. What matters are dimensionless quantities, e.g., ##\alpha##, ratios of particle masses, etc.
 
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I do not follow. When we measure the speed of light in meters and seconds we get 299792458 m/s.

We measure it.

My question (rephrased): what would the world look like when would measure ligth traveling at 2 m/s instead?
 
Pnin said:
We measure it.
You can try to measure it by seeing how many meter rules light travels in one second. But the problem is that a meter rule is defined to be 1/299792458 of the distance traveled by light in one second - so the result is 299792458 by definition. It's circular. All you are doing is seeing how well your meter rule matches the definition of a meter.

Prior to 2018 meters were not defined in terms of ##c## and you could measure ##c##. Now meters depend on ##c## and you can no longer measure ##c##.
 
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Pnin said:
what would the world look like when would measure ligth traveling at 2 m/s instead?
You can play with that at MIT
 
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Ok. Then let's use this standard meter stick in Paris, instead. Could I still not measure a different speed of light in principle, because the speed of light is a dimensional universal constant? Which means that a different speed of light would also imply different radii of the atoms that make up this meter stick?
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It is hard enough to understand the universe without changing the numbers.
Why do you ask such a hypothetical question ?

An enormous effort has been invested in a robust definition of SI. Physics is scaleable. So changing the fundamental defined constants does not change the physics, it only changes the numbers.
If the speed of light was 30 km/hr, your mass when running for a train would be relativistic, like the mass and length of the train. Your world would simply run slower.
 
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Pnin said:
Could I still not measure a different speed of light in principle, because the speed of light is a dimensional universal constant?
Only in the trivial sense that any such ruler is probably not exactly the standard length. You don't change the underlying physics just by switching to an older standard - the logic that allows us to define the newer standard is still valid.

If you require that the dimensionless constants be unchanged, you cannot have a different value of ##c## without also having different values of at least one other dimensional constant. These changes will cancel out in any analysis you do of an experiment - either changing your time standard or cancelling out your distance standard change. The "standard" meter is made up of a certain number of atoms, so your atoms' sizes are derived constants (and not measureable), as is the speed of light. They must be consistent.

It's all quite headache-inducing to think about. The modern SI units are set up to minimise the number of arbitrary starting points, encoding as much of the arbitrarily chosen stuff explicitly in the dimensional constants as possible.
 
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The problem here is that thinking about the constant "c" in SI units obscures the physics. If you take "c" to be a meaningful quantity, but do not change ##\alpha##, then, sure the universe would look different, but no one would be here to decide what it means because chemistry can't happen. The velocity of the first Bohr orbit in Hydrogen is ##\alpha c##, so obviously ##\alpha c## is going to determine if atoms can even exist. Now, recall that the definition of the second comes from atomic transitions.

Atomic transition rates are determined by ##\alpha##, the matrix elements between the states and the phase space available for the transition. If you assume that we're still in a universe where chemistry can occur, then saying the speed of light is different means you redefined the units of seconds such that nothing looks any different. All that has changed are the definitions of the meter and the second such that we can be here to define them.

A better, more physically meaningful way to think about this is to stop referring to "c" as the speed of light. Relativity tells you that massless particles propagate at the same speed in every frame. If the photon is massless then light propagates at the same speed in every frame, but whether or not the photon is massless belongs in a theory of E&M. Although that certainly appears to be the case, you can easily construct a theory of E&M with a massive photon (Proca ca. 1913 or 1914). Once you separate relativity from the speed of light, you can stop asking how things "look" if "c" were different, since the "c" in relativity is tied to the speed of light for historical reasons and the fact that Maxwell's equations are correct only if the photon is massless, so that was what led Einstein to use light to discover relativity.

Why the speed of light is still being used to teach relativity rather than mentioned as an historical note is beyond me. But, it's why these sorts of questions come up all the time. SI units are useful because those units address the measuring devices that we find the most convenient to use and the relationships that allow us to choose which relationships we can can choose to get the most precision. If you take the units themselves to be physically meaningful, it's hard untangle the physics from human conventions of measurement.
 
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