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#1596 |
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Romulan Interpreter
Jun 2011
Thailand
3·3,221 Posts |
Actually, what some guys want to do now, they want to create carbon fiber structures that are filled with helium first, to balance the pressure, then the helium is released slowly as the structure goes up, ending up closer to the top of the atmosphere, and vacuumed inside. These structures are intended to be kind of "permanent" things, you can not replace (so easy) the lost helium. So, once there, they will stay there (the pumps can work solar and maintain the vacuum level) and "never" return down. Another problem would be to shield them against the sun and UV, and of course the Earth's whatever belts they can find there up.
Re: 150 atm inside (crosspost), you can make a sphere of (whatever) and fill it with a high pressure fluid (gas), and it will resist, because the material would need to be teared apart for the fluid to go out. The "tearing apart" force is very high. How about you try to put 150 atm outside, and 1 atm/nothing inside? The material in this case will only need to be "bent", where the force is much lower. See the divers who take empty iron or tin canisters when they dive, and the canisters are squashed by the underwater pressure starting from the first meters. The same canisters will get a rounded form if you put some pressure inside, but they will not break. Last fiddled with by LaurV on 2015-08-24 at 05:24 |
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#1597 | |
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Bamboozled!
"𒉺𒌌𒇷𒆷đ’€"
May 2003
Down not across
2·5,393 Posts |
Quote:
Pump it into pressurized containers and drop them (including the pumps) as ballast. Pick up the containers when they reach the surface and re-use. About all that wouldn't be recyclable would be the parachute subsystem. |
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#1598 |
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Romulan Interpreter
Jun 2011
Thailand
3×3,221 Posts |
Well, pumps you can't drop, you will need them to compensate the lose of vacuum. If you say that you don't need strong pumps for that, then well, you don't need strong pumps for anything, as you raise, the pressure is lower and the helium from the balloon would go out by itself
What do you have against me going up there and staying there ? I won't come down to bother you... only maybe pee on you from there above, when you upset me, :p.
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#1599 | |
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Bamboozled!
"𒉺𒌌𒇷𒆷đ’€"
May 2003
Down not across
2×5,393 Posts |
Quote:
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#1600 | |
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"Gang aft agley"
Sep 2002
1110101010102 Posts |
Exclusive: Secretive fusion company claims reactor breakthrough
Now holds plasma for 5 milliseconds Quote:
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#1601 | |
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Romulan Interpreter
Jun 2011
Thailand
3×3,221 Posts |
Quote:
They said that "it would be stupid to release the helium into the atmosphere and lose it in space", and that "all the equipment to compress it in polyethylene bags till they are heavier than the atmosphere would not be heavier than 100 kilos or so. Well...
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#1602 | |
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"Gang aft agley"
Sep 2002
2×1,877 Posts |
Why the world is running out of helium
Quote:
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#1603 | |
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∂2ω=0
Sep 2002
RepĂşblica de California
19·613 Posts |
After a week of intense debate, Stephen Hawking and his colleagues are still puzzled by black holes | WaPo
Re. the black hole confab: Speaking of much-neglected 'dusty old' theories, I find the pervasive lack of mention (or perhaps better, misrepresentation) of the second law of thermodynamics in the context of the alleged information paradox exceedingly curious. After all the 2LOT tells us - in stark contrast to the assertions made in the piece like 'Information isn't supposed to disappear' - that information is in fact destroyed (in the sense of being rendered irretrievably nonrecoverable) all the time. The term is 'irreversibility', and in many ways it defines the blurry transition zone from the microscopic world, in which 'all individual transactions are time-reversible' to the macroscopic, in which the resulting collective behavior is not. Boltzmann, anyone? Equally curious is that Hawking himself in his groundbreaking earlier work in which he achieved the first plausible (albeit piecemeal) unification of quantum field theory with classical (= relativistic but continuum-based) gravitation, came up with a strikingly lovely result regarding blackbody (= diffuse, i.e. entropy-maximized, i.e. all-detailed-information-lost) radiation from black holes and the entropy of same. So the present extreme aversion to the idea of information loss in the process of black hole accretion among the 'thought leaders' in the field -including Hawking himself - strikes me as bizarre. Perhaps it's simply the natural research bias that confirming (in this case by extending to encompass novel phenomena which were unknown when the original theory was being developed) existing theories is inherently 'less sexy' that publishing 'radical paradigm-smashing' new ones. From another phys.org perspective on the issue: [The idea of black hole information loss] posed a huge problem for the field of physics because it meant that information inside a black hole could be permanently lost when the black hole disappeared — a violation of quantum mechanics, which states that information must be conserved. Uh, QM may say this for individual microscopic events, but again, what about large-scale statistics of collective behavior? Even though QM is now accepted as underpinning all macroscopic physics, I've never heard of any luminary claiming that the second law of thermo is thus a dead letter in the macroscopic realm where, last time I checked, information continues to be merrily and profligately destroyed and entropy thus keeps increasing. Why should matter (i.e. mass/energy) falling into a black hole be an exception? Sure, there may be some wacky stuff happening to spacetime near (and inside) the event horizon, but there is no reason to believe that the infalling stuff suddenly stops being subject to the rules of statistical thermodynamics. Similarly, here: The entropy of black holes: Quote:
Paul, am I overlooking something blatantly obvious in my take here? |
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#1604 | |
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"Gang aft agley"
Sep 2002
1110101010102 Posts |
Three years ago someone on Physics Stack Exchange asked: Why is information indestructible?
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#1605 | |
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Bamboozled!
"𒉺𒌌𒇷𒆷đ’€"
May 2003
Down not across
2·5,393 Posts |
Quote:
AIUI (meaning imperfectly) information is "lost" in classical thermodynamics when you cease to pay attention to individual particles but instead decide to work with ensemble averages. The particles themselves continue to preserve information in terms of their momenta, etc, and if you were prepared to re-record their properties all the original information will still be there. A particular "random" state taken from the large number of random states which are a close enough approximation to a distribution in thermal equilibrium is unique --- it differs from all other states taken from any distribution and requires exactly the same amount of information to specify it as any other state whether taken from a distribution near or far from equilibrium. The problem with GR and QM, again AIUI, is that the former doesn't know how to treat what happens at a singularity. On the face of it, nothing can happen at a singularity because by definition almost everything is either infinite or zero in size. GR allows a black hole to posess abitrary values only for its mass, angular momentum and electric charge. Everything else is either uniquely determined by those quantities or can not be determined at all. Information appears to fall into the latter class. |
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#1606 |
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"Mike"
Aug 2002
5·17·97 Posts |
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