CERN’s Large Hadron Collider achieves the hottest manmade temperatures ever
blogs.nature.com
blogs.nature.com
It's even a sub-nuclear soup. It's not obvious until you think to it, but an atom is just enormous when you're talking at nuclear scale: a typical nucleus in its atom is like a tennis ball in a stadium! http://public.web.cern.ch/public/en/research/MinChall-en.htm...
Years ago I addressed "hot" in terms of molecular speed, applying relativistic limits, calculating an upper limit on temperature and finding a large, but not inconceivable, maximum. Alas I've lost the paper (which was probably wrong anyway, but it was a fun exercise). The question has long bugged me: is there a real upper limit on temperature?
There is no relativistic limit to temperature. You probably calculated temperature by using the speed of the particle (and assumed it to max out a c), but at relativistic speeds this is wrong, you should use the energy of the particle instead.
The question is: Does particle A impart energy to particle B, or does it take away energy? Whichever is faster imparts energy to the slower one. It makes no difference that the speed is limited - one particle can always have more energy than the other, and can therefor impart energy to it. It's not possible to actually reach that speed, so no matter how fast a particle is moving, you can always increase its speed.
Time dilation should cause some very interesting artifacts though, I have no idea how to go about calculating what would happen. Length dilation is even more interesting - you may find your particles are so small that they pass each other and don't collide.
However it's not actually the particle that collides, it's the electric fields that collide. But electric fields travel at the speed of light - so the fields won't really have time to notice each other.
And finally at these energies a collision is unlikely to bounce, instead it would create some new particles, using up the energy and cooling rapidly.
Technical limitations aside, not really. However, there's the Planck temperature of 1.42×10^32 K where our physical models break down.
The first (utterly naive) guess that springs to my mind would be that at that point the vibration would be sufficiently fast that when sampled at a Planck time interval, there'd be no motion at all. Like overflow of an unsigned int. This is almost surely wrong. :)
According to wikipedia (heh), quark-gluon plasma is not really a plasma so much as a liquid. Presumably, that means the modes are still roughly momentum modes, and you can literally think of a hotter QGP as faster quarks and gluons sliding around and slamming into one another. It's a Fermi liquid, though, which means the exclusion principle has significant effect. (I'm a physics grad student, but not a high-energy theorist, so take that for what it's worth.)
Molecules will break apart above a few thousand degrees. If you take a gas (say Helium) above a certain temperature (probably ~1e4 K) the collisions between the atoms will knock the electrons off and you'll be left with a plasma.
Confining a plasma could either be done with magnets (e.g. a fusion reactor), or with more plasma! (in the case of stars, where the gravity keeps itself from exploding).
Above 1e7 K you start to get fusion of Hydrogen, and I think above 1e11 K pretty much any nucleus will fuse/break down.
So it's difficult to say there's a maximum temperature, as it's quite hard to define.
What's your maximum temperature? About 41'C... above that and you'll die...
Hopefully there is some clarification to explain how I won't die...
BTW, as a teen I remember playing out in the sun at a good 52°C. Don't think I died :)
And yes, these are well above biologically-friendly temperatures. :)
Many people are familiar with temperature as characterized by "average thermal velocity" of, say, air molecules. However, in statistical mechanics (the physics of many particle systems), temperature is defined in terms entropy and energy.
Specifically, temperature is the rate-of-change of energy with respect to entropy. (In math: T = dU/dS.) This arises as a natural definition if you think of temperature as "the thing that is equal between two systems in thermal equilibrium".
Think about it this way: A cup of water and an ocean have VASTLY different energies. Similarly, the ocean has an enormous entropy compared to the cup. However, if they're at the same temperature, the unit change of entropy per energy added is the same.
Coming back to the article, the temperature being reported by ALICE is derived from the entropy and energy of the collisions. Specifically, they're looking at quark-gluon plasma from the heavy-ion collision at LHC.
Under normal conditions, quarks and gluons are confined to hadrons like protons and neutrons. Quark-gluon plasma occurs only at extreme energies, and in these collisions it is a essentially a chaos of quarks and gluons. The chaos (entropy) is not a thermal property but rather largely comes from the nature of the strong force. So, changing the energy of a quark-gluon plasma doesn't have a huge effect on its entropy. Conversely, you could say it takes a lot of energy to change the entropy, and so by the definition of temperature, you get a very large value!
They're claiming 5.5 trillion degrees Celsius. My mind is unable to comprehend that. A billion times hotter than the surface of the Sun...
Also, any scientific paper should use units. But to be fair, even though the difference between Farenheit and Celsius is huge at this scale, I can't really imagine it or compare it.
NIF press release, 522.6TW and 1.855MJ - https://lasers.llnl.gov/newsroom/project_status/index.php
NIF is applying a large amount of energy to a small but macroscopic amount of matter. The LHC and RHIC are colliding mere nuclei, so the amount of matter is roughly 22 orders of magnitude less. The LHC and RHIC collisions are vastly higher temperature (energy per particle) than NIF, but the total energy is vastly less.
Presumably, the temperature is inferred by measuring the various energies of the outcoming particles (just like in a normal collision) and noting that they are distributed thermally (i.e. according to Bose-Einstein or Fermi-Dirac statistics). This distribution is tell-tale evidence that the particles exchanged energy through scattering many times.
I guess you could call this thermal imagining, although "thermal imaging camera" denotes something that looks at infrared radiation and measures its distribution (in order to infer the temperature of the matter that radiated it). In this case, the particles themselves (and their decay products) are exploding outwards and having their energies measured.
There are some problems with describing the energy of a particle accelerator as a "temperature", but it makes the article more accessible and understandable, which is surely a good thing.
At a certain point, dumbing stuff down strips it of all meaning. Our species is going to have to start taking collective responsibility for its collective intelligence if we want a high tech future.
"The cost [...] has been evaluated, taking into account realistic labor prices in different countries. The total cost is X (with a western equivalent value of Y) [where Y>X]
source: LHCb calorimeters : Technical Design Report
ISBN: 9290831693 http://cdsweb.cern.ch/record/494264
about integrity:
"Message from the Director-General
CERN is an Equal Opportunities employer. Our Equal Opportunities policy is founded on four main pillars:
in recruitment and career development, the Organization will not discriminate against any applicant or employee on the grounds of sex, ethnic origin, disability, sexual orientation, religion, nationality or age; respect and dignity for all in the workplace; support for working parents; work-life balance." --
http://equal-opportunities.web.cern.ch/equal-opportunities/W...