Comment Re:"some storage" (Score 1) 260
With all due respect to your calculations, I'm willing to believe an authority figure more than math.
FTFY. Simply because he's correct on some things, doesn't mean he's infallible.
With all due respect to your calculations, I'm willing to believe an authority figure more than math.
FTFY. Simply because he's correct on some things, doesn't mean he's infallible.
called a IRBM.
Yeah I know it exists
the lowest possible temp is -273.15C or -459F, or 0 kelvin. (absolute zero). Increase in flame temp when combusted with air will be approx +10.4C.. (0.04 * 2483K) + (0.96 * 2223K) - 2223K = +10.4K.
You've got a mistake there, 2223K is the flame temp for CH4. Natural gas is 2233K or 10K higher (because it's not pure CH4). The difference, however, is largely inconsequential, it's a 1% increase in absolute flame temperature (exactly like I said), at best (actually 0.44%, but we'll let that go).
+10.4K/(2223K-290K(ore 323C)) = 0.53%(17C) to 0.55%(50C) increase in efficiency to help offset 4% H2's 2.71% reduction in energy content. Since most applications are direct thermal usage(water/hot air/etc) no additional losses will be incurred.
Now hang on, you can't just take the flame temperature and call that your working fluid temperature, that's not how it works in heat engines. Gas-based heat engines (CCGT - the most efficient ones, not talking about ICBs, those have very poor efficiency) use the hot flame to heat a working fluid (typically superheated steam), which is much cooler than the flame itself. I used an 18C coolant temperature (cold water) and 60% efficiency to back-calculate the minimum ideal working fluid temperature (~454C hot vs. 18C cold will give you ~60%). So a 1% increase in absolute flame temperature can at best give you a 1% increase in absolute working fluid temperature, which means your working fluid goes from 454C (727K) to 461C (734K). However, the gains here will be much more modest because you can't just step over a heat exchanger's maximum temperature willy-nilly, or bad things will happen to it, which is why I rounded to 460C (I'm a generous guy, I know
Now as for "direct thermal usage (water/hot air/etc)", these applications are not heat engines, they don't convert heat energy into work (J -> J/s is a heat engine, J -> J is not), so for them an increase in flame temperature means nothing. For example, it takes the same amount of heat to raise 1kg of water by 1C, regardless if the absolute temperature of the heating source is 100C or 500C, it's still 4.18kJ/kg.C.
The analyses collectively indicate that the two reactors appear to be able to achieve their design objectives: The RBWR-AC provides an equilibrium-cycle breeding ratio of slightly above 1.0, thus providing for a self-sustaining fuel cycle in which depleted uranium is used for the makeup fuel. The RBWR-TB2 is capable of unlimited continuous recycling of TRU while consuming on the order of 10% of the loaded TRU per recycle (after accounting for the newly generated TRU). Most results confirmed the values estimated by Hitachi. Some differences among the predicted reactivity coefficients need to be evaluated further.
This has the potential to be a game-changer if true, as we could simply use existing reactor designs such as the ABWR (of which there are several operating already) to both burn waste and breed fuel indefinitely from U238 feedstock.
Also weird, is Hitachi already has a TRU burning design, the S-PRISM
It's possible they're having trouble getting a dedicated TRU burner design approved and built (there might be little economic incentive and much public opposition to new nuclear plants, no matter the safety of the technology), hence why they might be motivated to try and design fuel that can consume TRUs in standard BWRs, of which Japan already has quite a few.
With your bare hands?!?