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Handwaving to match orders of magnitude |
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| Dec6-12, 01:46 PM | #1 |
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Handwaving to match orders of magnitude
Hello
This is my first post here. Although I've often read posts in Physics Forums, I've never actually contributed anything - so here goes! I always enjoy a good hand-waving argument on orders of magnitude; when I first started my astrophysics degree, one homework question was "estimate how many piano tuners there are in this town" - that was it, no other clues! Of course, it was designed to get us to think of ways of solving a problem by making realistic guestimations. Another argument I admired goes that there cannot be an infinitie number of stars in the universe otherwise there would be an infinite amount of light in the sky, so we would not expereience darkness at night. Anyway, I was sitting in the library today (should have been working on a Solid State problem) and started wondering: if I took the energy of a photon as a "rest mass" and multiplied it by the number of photons in the universe would that be anywhere close to the estimated figure for dark matter? So I looked up some figures from not-very-reputable sources (this is just hand-waving, after all) and got this: Number of photons in the universe: 10^91 (source: Science Blog) "Rest Mass" of a photon: 4.2 * 10^-40 kg (source: Wikipedia) So, total estimated photon "Rest Mass" = 4.2 * 10^52 kg. Now compare to Dark Matter in the Universe: 3.5 * 10^52 kg (source: Wikipedia) They match within 20% - well within an order of magnitude! Well, I thought it was interesting even if doesn't mean anything! Anyone got any other hand-waving examples that they can think of? |
| Dec6-12, 03:47 PM | #2 |
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Photon has no rest mass, so I have no idea what you are doing. Or why.
Your estimates cannot be remotely right, however. They suggest that gravitational mass in radiation is significantly greater than gravitational mass of matter in the universe. That would, indeed, result in our sky being a touch on the bright side. |
| Dec6-12, 05:18 PM | #3 |
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Mentor
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Have you ever seen a graph with error bars on the data points? The upper limit is basically the top edge of the error bar, with the actual data point being at somewhere around zero. |
| Dec6-12, 06:39 PM | #4 |
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Handwaving to match orders of magnitude
I think estimating the strength of a nuclear blast using some bits of paper ranks pretty highly.
then again, I think both that example and the piano tuning are due to Enrico Fermi. Heres a nice little story on it for those curious: http://sci.mercer.edu/handouts/fermi_calculations.htm |
| Dec7-12, 02:15 AM | #5 |
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Thank-you for taking time to reply!
Is your argument that a finite number of stars are visible (so the sky is dark at night) but an infinite amount of stars could exist at an infinite distance so that we would never see their light (i.e. a non-bigbang solution)? |
| Dec7-12, 02:18 AM | #6 |
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| Dec7-12, 02:23 AM | #7 |
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Thanks for reply!
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| Dec7-12, 02:54 AM | #8 |
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[tex]\int_0^\infty \frac{dN}{r^2} = \int_0^\infty 4\pi\frac{r^2 \rho dr}{r^2} = \int_0^\infty 4\pi\rho dr = \infty[/tex] So we will get infinite luminosity. Now imagine, instead, that stars are grouped into clusters of density ρ. These clusters are spread out a bit more from each other, so if you take average density across groups of clusters, the new density is some ρ'<ρ. These groups are also clustered, and that gives you density on even larger scale to be ρ''<ρ'<ρ. Because we live near a star, which belongs to a cluster, which belongs to a group of clusters, etc, locally we have the highest density of stars, and it drops with distance. So ρ(r) is now a decreasing function. Say, ρ(r)=ρ0exp(-λr) just for illustration. Now the total luminosity is different. [tex]\int_0^\infty \frac{dN}{r^2} = \int_0^\infty 4\pi \rho_0 e^{-\lambda r} dr = \frac{4\pi \rho_0}{\lambda}[/tex] We get a finite quantity. Notice that this kind of structure is similar to what we really have. In our immediate vicinity, density of stars is very high. 1 star for a moderately small volume. As we look at the scale of the galaxy, the density is significantly lower. If we look at local group, the density of stars is much lower, on average, than in a galaxy. And so on. This sort of fractal structure allows for a finite amount of light to be reaching us from the sky despite effectively infinite number of stars out there. Note that stellar dust would not make a difference. If stars were uniformly distributed, interstellar dust would reach thermal equilibrium with the stars and would glow just as hot. |
| Dec7-12, 08:08 AM | #9 |
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Mentor
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The Cosmic Energy Inventory
The upper limit on a photon mass, according to the particle data group, is <10-18 eV (or <10-26 eV with a specific model). This corresponds to 2*10-54kg as upper limit per photon. |
| Dec8-12, 04:22 AM | #10 |
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btw, great links - thanks |
| Dec8-12, 04:35 AM | #11 |
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While individual photons will be absorbed, won't the total number available will remain constant? Sorry if that's a little confusing, but, again, thanks for the reply - it's very interesting. |
| Dec25-12, 09:06 AM | #12 |
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the light from each ring that reaches earth will be the same. And we are adding up an infinite amount of rings. the intensity falls off as 1/r^2 but the further we go out
there will be r^2 more stars to add to the light so the light from each ring will be the same no matter the distance. |
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