Where does exp(-4pi^2) appear in physics?

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Discussion Overview

The discussion centers around the appearance of the factor exp(-4π²) in various physics contexts. Participants explore different scenarios, equations, and models where this term might emerge, including potential energy functions, heat diffusion equations, and transmission lines.

Discussion Character

  • Exploratory
  • Debate/contested
  • Technical explanation

Main Points Raised

  • One participant seeks examples of physics problems involving exp(-4π²).
  • Another participant discusses the work done against a potential described as -exp(-x) when moving a unit mass to x = 4π².
  • A different viewpoint introduces a mass unit defined as \hat{m} = m e^(4π²) and relates it to Newton's second law.
  • One participant presents a solution to the heat diffusion equation, indicating that the temperature at a midpoint after 1 second is predicted to be exp(-4π²) under specific initial conditions.
  • Some participants challenge the relevance of the examples, arguing that the emergence of exp(-4π²) can be arbitrary depending on the chosen parameters or context.
  • Another participant suggests that the term can arise naturally in various physical contexts, such as transmission lines, and encourages exploration of minimal adjustments needed to derive it.
  • There is a discussion about the nature of "natural" versus "unnatural" choices of length scales and parameters in physics.
  • One participant mentions that obtaining a π² term is not particularly difficult and suggests using higher-dimensional phase space to derive it.

Areas of Agreement / Disagreement

Participants express differing views on the arbitrariness of the examples provided and the natural emergence of the term exp(-4π²). There is no consensus on the validity of the original question or the examples discussed.

Contextual Notes

Participants note that the emergence of exp(-4π²) can depend heavily on the chosen parameters, definitions, and contexts, which may lead to varying interpretations of its significance in physics.

franoisbelfor
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This is a somewhat unusual question.
I am looking for any physics problem
in which the number or factor exp(-4pi^2)
appears.

If you know one, I'd like to hear about it!

François
 
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Given a potential described as -exp(-x), what is the work done against the potential when moving a unit mass from infinity to x = 4\pi^2 ?
 
Introduce the new mass unit, \hat{m}\equiv{m}{e}^{4\pi^{2}}, where m is the standard unit of mass.

Then, Newton's second law of motion reads:
F=e^{-4\pi^{2}}\hat{m}a
 
Here's one that's less arbitrary: the solution of

\frac{\partial u(x,t)}{\partial t}=\frac{\partial^2 u(t,x)}{\partial x^2}

is

u(x,t)=\sum_{n=1}^\infty A_n\exp^{-(n\pi/L)^2t}\sin\frac{n\pi x}{L}

where A_n is calculated from the initial conditions. But the upshot is, because the above equation governs heat diffusion by conduction, if you had a bar of material with length 0.5 m, thermal diffusivity 1 m2 s-1, end temperatures of 0°C (i.e., u(0,t)=u(L,t)=0), and an initial sinusoidal temperature distribution with maximum temperature 1°C (i.e., u(x,0)=\sin(\pi x/L)), the temperature at the midpoint after 1 second is predicted to be \exp(-4\pi^2), which is the term you're looking for.
 
How is that less arbitrary? You still have to pick a material with the right size and properties.
 
Vanadium 50 said:
How is that less arbitrary? You still have to pick a material with the right size and properties.

It's less arbitrary because the exponential function and the \pi^2 term come out of the physics rather than being input as variables or functions, as in the other two cases (although we do need to specify a sinusoidal initial temperature distribution). And the values aren't fixed; it could be a 10\,\mu m long microfabricated silicon beam (thermal diffusivity 8\times 10^{-5}\,\mathrm{m^2}\,\mathrm{s^{-1}}) after 5\,\mu s, for example. Don't you think it's interesting that the \pi^2 emerges naturally here?
 
Mapes said:
It's less arbitrary because the exponential function and the \pi^2 term come out of the physics rather than being input as variables or functions, as in the other two cases (although we do need to specify a sinusoidal initial temperature distribution). And the values aren't fixed; it could be a 10\,\mu m long microfabricated silicon beam (thermal diffusivity 8\times 10^{-5}\,\mathrm{m^2}\,\mathrm{s^{-1}}) after 5\,\mu s, for example. Don't you think it's interesting that the \pi^2 emerges naturally here?

Not really. Pretty much any time-harmonic or complex number system you can probably easily massage out an exp(\pi) and exp(\pi^2) dependence of some kind. I could specify a transmission line and given a certain length and loss I could get you an attenuation of exp(-4\pi^2).

The OP is just posing a really bad question. It is completely arbitrary because, like arildno shows, when it comes to picking out a constant you can get it from just about any kind of equation from judicious choice of your units, scale, or choice of parameters.
 
Born2bwire said:
I could specify a transmission line and given a certain length and loss I could get you an attenuation of exp(-4\pi^2).

Go for it! That's what the poster seems to be looking for: physical circumstances in which the term arises naturally. Maybe he or she saw the term on a blackboard once, or a poster (or a tattoo!), and wants to know what the context might have been. I don't know. But I don't think it's a bad question; in fact, I was looking forward to comparing the responses to get a sense of the... grand interconnectedness of physics. Consider it a challenge: what's the least amount of massaging needed to get \exp(-4\pi^2), without inputting it directly?
 
"physical circumstances in which the term arises naturally"

What is natural, or unnatural about a particular choice of length scale??

Yet, they are also part of physics..:smile:
 
  • #10
Getting a pi^2 is not horribly difficult; have a 4 or 5 dimensional volume in phase space. You'll have to turn a 1/2 or an 8/15 into a 4, but that shouldn't be hard. Then find a reason to exponentiate it...e.g. as a partition function.

This is contrived, of course, but no more so than a length of one meter, time of one second, capacitance of one farad, etc.

As far as the context, I fear it's not a blackboard, poster or tattoo. A search of other messages here will perhaps provide some enlightenment.
 
  • #11
Vanadium 50 said:
As far as the context, I fear it's not a blackboard, poster or tattoo. A search of other messages here will perhaps provide some enlightenment.

Ah, got it. I was originally thinking it was something innocuous like https://www.physicsforums.com/showthread.php?t=257304".
 
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