Collection of Science Jokes P2

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SUMMARY

This forum discussion centers around a collection of science jokes, particularly those involving mathematics and physics. Notable jokes include a mathematician with a dog and cow discussing knot theory, and a play on Heisenberg's uncertainty principle. The humor often relies on advanced concepts such as the Jones polynomial and topological invariants, showcasing a blend of wit and scientific terminology. The conversation also touches on the cultural significance of these jokes within the scientific community.

PREREQUISITES
  • Understanding of knot theory and the Jones polynomial
  • Familiarity with Heisenberg's uncertainty principle
  • Basic knowledge of topology and topological invariants
  • Awareness of mathematical humor and its conventions
NEXT STEPS
  • Explore the concept of knot theory in mathematics
  • Learn about the Jones polynomial and its applications
  • Study Heisenberg's uncertainty principle in quantum mechanics
  • Investigate the role of humor in scientific communication
USEFUL FOR

Mathematicians, physicists, educators, and anyone interested in the intersection of humor and science will benefit from this discussion.

  • #871
Frank wasn't a monster. Frank made a monster.
 
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Physics news on Phys.org
  • #872
Only a monster would have made such a monster.
 
  • #873
hBE9AACB1.jpg
 

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  • #874
Graffiti in a men's bathroom in Leipzig's university:

Heisenberg might have been here
 
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  • #875
I swear this is a real quote from a math source. As a physicist, it made me laugh (might not be funny to mathematicians!)


Cayley's theorem, which says that any group is isomorphic to a certain subgroup of that group's group of isomorphisms.
 
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  • #876
nrqed said:
Cayley's theorem, which says that any group is isomorphic to a certain subgroup of that group's group of isomorphisms.
Do you have a quote? I know Cayley as ##G \leq \operatorname{Sym}_{|G|}## in the finite case.
 
  • #878
nrqed said:
Thanks, and yes, that's the proof, but I don't see that ##f_a## are isomorphisms, only bijections! E.g. ##f_a(1)=a \stackrel{i.g.}{\neq}1##. That was my problem: permutations are no homomorphisms. We have ##G \longrightarrow \operatorname{Sym}(G)## not ##\operatorname{Aut}(G)##. If we restricted ourselves to conjugations, we would get all central elements in the kernel, so that doesn't work. Where are the automorphisms?

All we have are automorphisms in the category ##\mathcal{Set}## but this is a very misleading wording in this context, and to say "its isomorphisms" is wrong - at least as far as I know.
 
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  • #880
44052897_1908269762555226_7629610935753113600_n.jpg?_nc_cat=105&_nc_ht=scontent.fymq2-1.jpg
 

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  • #881
That explains global warming, too!

Anthropomorphic global warming. :wink:
 
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  • #882
aBKwpRQ_700b_v2.jpg
 

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  • #883
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  • #884
fresh_42 said:
Don't forget the paper! We were supposed to save paper!
Actually, I think that we have reached a point of diminishing paper. I basically no longer get any paper invoices and I read the newspapers online. Looking at the students, more and more are buying the textbooks as e-books and many assignments go directly from their computer to mine with no wood-derived product in-between.
 
  • #885
Except in between their ears...?
No, I'm sure your students are better than that!
 
  • #886
DrClaude said:
Actually, I think that we have reached a point of diminishing paper.
All diagrams I can find on the internet are ##O(t)## since 1950. I haven't found a worldwide chart and the ones I've found ended in 2005 or so, which is why I don't post them. Yes, some paper traffic has gone electric, but the vast majority of papers are the n-th copy of a meeting protocol, the 10th-copy of a joke going around in emails, or the private copies of anything. Paper is still cheap and everybody is a Gutenberg. A few online invoices don't change the trend.
 
  • #887
fresh_42 said:
I haven't found a worldwide chart and the ones I've found ended in 2005
https://www.statista.com/statistics/270317/production-volume-of-paper-by-type/
Definition:
Graphic papers products are all around you and can be found in almost any home, office or business. These include a very wide variety of paper products for uses such as newspapers, inserts, supplements, A4 copy paper and printer paper, book paper, envelopes, forms, writing pads, high-quality magazines and brochures, company magazines, catalogues and annual reports.
 
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  • #888
3eXgkj4P3dajeT9wKW2Q2QjSSoZvENtv8ErfXaiN-nE.jpg
 

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  • #889
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  • #890
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  • #891
DennisN said:
@Greg Bernhardt , when will PF/Latex support hieroglyphs?
Haven't you noticed? It already does:
DarMM said:
$$H(g,\kappa) = H_{\phi,\kappa} + H_{\psi,\kappa} + g\colon\bar{\psi}\phi\psi\colon - \delta m^2(g,\kappa) - E(g,\kappa)$$
I think it says: 'Ptolemy was here', but Ptah only knows.
 
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  • #892
DennisN said:
@Greg Bernhardt , when will PF/Latex support hieroglyphs?
upload_2018-11-7_21-18-42.png
 

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  • #893

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  • #895
That's funny.
He better be back before his supper gets cold, or if he's lucky maybe she will keep it warm in the oven.:wink:
 
  • #896
Bandersnatch said:
Haven't you noticed? It already does:

I think it says: 'Ptolemy was here', but Ptah only knows.
It's the Hamiltonian for the Yukawa theory, fairly standard QFT, you'd see it in intro books.
 
  • #897
Oh, humour. That elusive beast.
 
  • #898
Bandersnatch said:
Oh, humour. That elusive beast.
I know it's a joke Mr. Silly, just thought I'd explain what it actually was. :smile:
 
  • #900
Keith_McClary said:
I’m Going on a Random Walk
In case this is not in your Physics curriculum:
Once again, however, our focus is on simple diffusion or the nearest-neighbor random walk. For these processes, the possibility of a diffusing particle making arbitrarily large excursions before certain trapping takes place leads to an infinite mean lifetime. On the other hand, the recurrence of diffusion in one dimension means that the particle must eventually return to its starting point. This dichotomy between infinite lifetime and certain trapping leads to a variety of extremely surprising first-passage-related properties both for the semi-infinite interval and the infinite system.
Section 3.1 (and the referenced Chapters 1-2).
 

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