takeTwo
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Maybe this has already been discussed. I have read the thread, but it didn't stand out. It is fairly easy to fuse some fraction of the fuel in two beams. But all current designs for either magnetic confinement fusion energy (MFE) or inertial confinement fusion (ICF) ask that the fusion products be used to help burn some more of the fuel. For D-T, the "alpha" particles (He ions) must not escape so fast that they don't contribute to the heating of the fuel. If they can be contained, then the fusion burn will be efficient. For ICF, the alphas must heat the unburned fuel prior to escaping the small, compressed pellet (stopping power = compressed-density * radius > x grams/cm^2, x ~ 5-10). Similar for MFE. The alphas heat the plasma faster than the total heat loss, be it via particles or radiation. I've forgotten the details, but think of density*temperature as proportional the probability per unit time that fusion will occur. Add confinement time (for the heat); density*temperature*time. This then is proportional to the fraction of fuel that will burn; i.e. efficiency.
Both approaches have produced fusion energy, but neither has yet met the so-called Lawson criterion which deals with the requirement that the energy deposition of the (initial) fusion products either substantially completes the burn (ICF) or sustains the burn (substains the required plasma temperature) for literally many seconds (MFE).
see. http://en.wikipedia.org/wiki/Lawson_criterion
For beams, I would guess that the problem is in recycling the un-burnt fuel back to a chamber that can extract the heat for boiling water. Somebody mentioned that these beams should be neutral, and probably so if the current is high. So, how does one recycle these beams such that the collision point occurs in an (expensive) central piece of a power plant... where the "heat" is used to boil water?
By the way, word has it that NIF will achieve scientific break-even earlier than expected, perhaps by mid 2010.
Both approaches have produced fusion energy, but neither has yet met the so-called Lawson criterion which deals with the requirement that the energy deposition of the (initial) fusion products either substantially completes the burn (ICF) or sustains the burn (substains the required plasma temperature) for literally many seconds (MFE).
see. http://en.wikipedia.org/wiki/Lawson_criterion
For beams, I would guess that the problem is in recycling the un-burnt fuel back to a chamber that can extract the heat for boiling water. Somebody mentioned that these beams should be neutral, and probably so if the current is high. So, how does one recycle these beams such that the collision point occurs in an (expensive) central piece of a power plant... where the "heat" is used to boil water?
By the way, word has it that NIF will achieve scientific break-even earlier than expected, perhaps by mid 2010.