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Liquid Fluoride Thorium Reactor |
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| Nov28-12, 07:54 AM | #171 |
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Liquid Fluoride Thorium Reactor"In addition to the intergranular corrosion problem, the standard Hastelloy-N used in the MSRE is not suitable for use in the MSBR because its mechanical properties deteriorate to an unacceptable level when subjected to the higher neutron doses which would occur in the higher power density, longer-life MSBR." Note that MSRE was only 8 MW (without the electrical generation system, and with off-line batch processing), while the MSBR was planned for 2250 MWt (1000 MWe) and use of on-line continuous processing. See Table III, p. 21 of WASH-1222. Nickel is problematic in any neutron environment. It absorbs neutrons and becomes active (producing Co-58 and some Co-60) and suffers from an (n,α) reaction. An alloy with lower Ni content would be preferable, something more along the lines of more Cr-Mo (Hastelloys are Ni-Cr-Mo). Several other technical issues are mentioned. The MSBR concept proposes high temerpature steam cycle, and that presents a challenge, particularly with respect to the heat exchanger, which basically can't be allowed to fail (leak), and then there is the materials compatibility issues between the steam and salt loop. The chemical separation part of the plant would also be challenging. Storage of Xe, Kr, I would be challenging, as well as ultimate disposition of the other fission products (ostensibly they would be converted to oxides and vitrified). A large scale LFTR would not be a trivial undertaking. |
| Nov28-12, 09:18 AM | #172 |
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| Nov28-12, 09:59 AM | #173 |
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You had asked: "Does this mean a chemical analysis the interaction of most of the elements in the periodic table against Hasteloy N must be done under LFTR conditions?" No, its imperative to be more careful about allowing opinion to get in the way before looking at the facts. |
| Nov28-12, 10:33 AM | #174 |
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On page 30 I noticed the report starts by talking about how the ORN scientists wanted to 'freeze' the salt along the walls to prevent corrosion in the flourinator, seems like a pretty clever idea, but is it feasable? The author thinks no but this report was not written by the scientists actually working on the project who had experience working with similar techniques; Time frame 8:16: http://www.youtube.com/watch?v=ENH-j...layer_embedded So now come the questions, how hard would it be? how much energy does it use? what is the cost of a system like this? From my own experience in refrigeration I don't think this would be difficult to add on. What is your opinion? |
| Nov28-12, 11:51 AM | #175 |
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Do you see the materials for the reactor as being the largest obstacle? On another note, I don't see why we have to remove 'most every element below U' if their concentration is almost undectectable and there is little to no effect on the reactor itself. It would seem more important to concentrate on the elements that effect the lifecycle of the reactor i.e. materials longevity, efficiency, waste, etc. |
| Nov28-12, 01:32 PM | #176 |
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| Nov28-12, 01:41 PM | #177 |
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I'm suggesting that along with the advantage comes a problem. While the dispersal of fission products throughout the reactor makes them removable, if the chemical means are put in place, it also means the reactor structural containment must accommodate contact with all of those products which accumulate over long periods. PS One speculative idea that comes to mind: After a high fuel burnup, dump the salt, say, every ten years. The MSR is designed for this for safety reasons in any case. Give it some decay time (short because of the low concentration of actinides in a Thorium cycle), then bury/dispose? The idea might be a step in the wrong direction, i.e. away from passive, walk away safety. As it implies a design that it a *dump* maintenance is neglected the structural containment is at threat of failure. |
| Nov28-12, 02:03 PM | #178 |
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As far as your graph link I was simply pointing out it was for the wrong fissile material, your new link is much better, thanks for posting it. |
| Nov28-12, 02:11 PM | #179 |
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For instance, for every mole of U233 consumed, 2% of a mole of some fission product (with atomic weight 85) is produced, 7% Zr, 6% Cs and so on. Burn another mole of U233, get another 2%, 7%, 6%, ... which the remains in the reactor, unless it has a fast decay path thus becoming something else, or unless it happens to have a high neutron capture cross section thus becoming something else, ... |
| Nov28-12, 03:06 PM | #180 |
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With this data we can simply calculate the accumulation of this element of the course of say a 30 year life cycle based off of anticipated (MWt energy of a reactor)/(energy per fission)*time for a rough estimate. Astronuc, can you point us in the direction of a source with more detail of the fission products from U233? Nevermind, found it, here is a link for anyone interested in running some calculations: http://www-nds.iaea.org/relnsd/vchart/ |
| Nov28-12, 06:08 PM | #181 |
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PWR typical burnup is around 50 GWdays/ton, or 5% of the fuel. Up to 500 GWdays/ton is expected in an experimental reactor, says the wiki. LFTR supposedly will have very high burnup, so optimistically assume 500 GWdays/ton, or ~120GWdays per 1000 moles of U, or given a 33% efficient reactor, 40GWe-days/1000 moles, or ~11GWe-years/1e5 moles U. So for every 11 years of operation, and again following the fission products curve, a 1GWe reactor produces 7e3 moles of Zr, 6e3 moles of Cs, etc, for the high probability products. Or, all products with amu's from 82 to 105, and 127 to 150 would accumulate 5e2 moles, or higher, in 11 years. Those concentrations will change through decay or neutron capture. The consequence of the result would depend on chemistry of the particular element in contact with the alloy which is beyond me. |
| Nov28-12, 07:42 PM | #182 |
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2250MWtx24hoursx365daysx30years/((MeV per fission)x(4.4504902416667x10^(-17))) = total number of fissions for the life cycle of the reactor. From here we can just multiply by the Cumulative Fission Yields to get: 4.9x10^21 Ga atoms produced, or .0081mols Using your method I get .0025mols Ga for the same time frame. If we are correct Gallium will not be an issue. Granted we could also account for Ga production from U235 since small amounts will also appear in this reactor but that lowers our values since they are an order of magnitude less in production of Ga in the thermal spectrum. Also, as Astronuc pointed out in the other thread, 8-10% of fission in LFTR will be fast neutrons, however this value is comparitively insignificant as well for this particular case. |
| Nov28-12, 07:53 PM | #183 |
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As for the remainder, calculations for the rest of the elements produced along with their constituent isotopes (and variations) would be helpful but improvement is needed on how calculations are performed to get decent sig figs. Any thoughts? |
| Nov28-12, 08:08 PM | #184 |
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* Independent fission yield (%): number of atoms of a specific nuclide produced directly (not
via radioactive decay of precursors) in 100 fission reactions * Cumulative fission yield (%): total number of atoms of a specific nuclide produced (directly and via decay of precursors) in 100 fission reactions From http://www-nds.iaea.org/publications...ecdoc-1168.pdf These may not include activation (n-capture). -------------------------------------------------- Fission product pairs for U (Z, 92-Z; A, 234-A for U235 or 232-A for U233), assuming 2 neutrons released per fission. The neutrons affect A, not Z. Code:
Z A 92-Z 234-A for U-235; 232-A for U-233 63 Eu 29 Cu 62 Sm 30 Zn 61 Pm 31 Ga 60 Nd 32 Ge 59 Pr 33 As 58 Ce 34 Se 57 La 35 Br 56 Ba 36 Kr 55 Cs 37 Rb 54 Xe 38 Sr 53 I 39 Y 52 Te 40 Zr 51 Sb 41 Nb 50 Sn 42 Mo 49 In 43 Tc 48 Cd 44 Ru 47 Ag 45 Rh 46 Pd 46 Pd Another factor to consider is the delayed neutron precusors that leave the core. Delayed neutrons are important with respect to control the reactor as well as irradiating the structure and piping outside the core. Reactivity control is another consideration, so a large MSBR may require use of control elements. The graphite must be supported, so there is a core support plate (not graphite), which will receive a neutron flux.Differences in thermal expansion between graphite and the structural alloy will have to be investigated. Hideout of the molten salt could be an issue. Note the MSRE operated 4 years and surface defects of 7 mils were found. Larger defects may propagate. Also, a 40 to 60 year lifetime is preferable. The numerous technical issues should be listed and discussed separately. |
| Nov28-12, 08:34 PM | #185 |
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I recieved an email from FliBe energy giving a link to the pdf files of the ORNL research program on the MSR. There is a substantial amount of information: http://energyfromthorium.com/pdf/ This should be helpful. |
| Nov28-12, 09:15 PM | #186 |
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| Nov28-12, 10:01 PM | #187 |
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http://www.youtube.com/watch?v=ZbtVk8r6-3U Calculating for if they are neccessary would be good, however there are many things Astronuc suggested that seem like viable avenues to look at. This is already a proven technology and it would seem the question is whether it is needed or not; it is reasonable to assume regulatory agencies could insist on such measures as they are a standard today even if shown to be unneccesary for LFTR. |
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