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by pfdietz
1793 days ago
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The cost of the reactor will be proportional to its size, so the cost/power will be inversely proportional to the power density. Lawrence Lidsky (who was also at MIT) (and also a similar argument from Pfirsch and Schmitter in Germany) famously pointed out back in the 1980s that DT fusion reactors will inherently have terrible power density compared to fission reactors, and this will render them noncompetitive. Despite putative rebuttals at the time, nothing we've seen since contradicts their devastating argument. http://orcutt.net/weblog/wp-content/uploads/2015/08/The-Trou... https://ui.adsabs.harvard.edu/abs/1987oepn.book.....P/abstra... Note that Helion wants to go with D-3He, and use direct conversion for at least some of the energy recovery. This might be the only hope for making fusion compete. But of course you need 3He; making it with DD fusion requires even more aggressive plasma physics. ARC at least isn't quite as absurd as a tokamak the size of ITER, which has a gross fusion power density another order of magnitude lower. |
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>Fusion will almost certainly have a lower power density than fission and therefore will require a larger plant to produce the same output. Suppose a fusion plant had to be ten times as big and therefore likely ten times as costly — as a present-day fission plant to produce the same amount of power.
Fission is currently not cost-competitive due to the expense of ensuring that fission reactors do not pose an unacceptable risk of radioactive contamination in their vicinity. However, fusion is not subject to this constraint, or anyway suffers from it much less. There are no long-lived radioactive byproducts, and judicious selection of the construction materials (already implemented) can ensure that neutron activation of the walls is not a problem either. Furthermore, the inherently unfavorable nature of fusion reactions mean that criticality accidents ('meltdowns'; a la Chernobyl) are not possible.
From Pfirsch and Schmitter:
>It is shown that the claims made therein for the economic prospects of pure fusion with tokamaks, when discussed on the basis of the present-day technology, do not stand up to critical examination.
The analysis in the fulltext relies on a variety of plasma parameters estimated based on technology available in 1987. I cannot immediately determine if it generalizes to designs using HTS, but the comments on pp 1473-4 about the achievable B field strengths and corresponding betas suggests that they do not. Cf. this paragraph:
>Another possibility is to use higher magnetic fields: 6 T instead of 5 T would increase fw to values between 1.3 and 2.0 MW/m2, which are still very low. The latter comes close to the value of 3 MW/m2 obtained in Sec. IV.A.l from thermal wall load constraints. Higher fields would, of course, again increase the cost.
Overall I don't think that these links provide nearly as strong an argument as you suggest they do.