Originally posted by: So
Originally posted by: SunnyD
Originally posted by: So
...Snip...
I'll cut to the chase in the hopes that you do as well oh resident expert.
Answer the original question then. HOW efficient is... say... the energy output of a nuclear reactor from the raw form(s) that it produces and the form(s) which are directly utilized in powering the turbine which produces said electricity?
How much potential energy is lost from the core material that is never recovered in terms of ALL possible forms of energy output, particularly the forms which we don't/can't utilize with current technology?
Finally, I'd be interested in finding out exactly how much of the electrical output from the turbine actually is utilized in terms of efficiency across the grid that it serves.
I know there's several questions there, so go ahead and do your best, and feel free to be technical - no need to dumb it down unless you really want to.
Please, please read the article on carnot efficiency I linked. A nuclear fuel bundle produces heat. That heat has to be converted to work (power) by some process. With nuclear reactors, the only known process that can produce significant amounts of power is a steam turbine, driven by the rankine cycle. The efficiency of that process is limited by the carnot efficiency. This all depends on the design of the turbine, and if it's a pressurized water reactor, the heat exchanger. I'm an electrical engineer, so my thermo days are long past me, but no matter how many efficiency improvements you do, ANY process that converts heat into energy is limited by the carnot efficiency. I really don't feel like doing the calcs to get you concrete numbers, and I'm betting that PWR / BWR reactor heat rates are at least corporate secrets. Basically, we're already doing well for generators (see http://en.wikipedia.org/wiki/Combined_cycle) -- this article says as much as 85% efficient, which given that this: (http://en.wikipedia.org/wiki/C...versible_heat_engines) gives us an ideal equation, which will yield an ideal efficiency of 85.3%, (with a Tc of 852.15k and a Th of 1172.15k) so we're pretty darn close to the best possible.
And this is (partly) what I'm talking about. We're limited to utilizing nuclear "fuel" to generate heat, even though it gives off another fairly potent type of energy (radiation). This is all part of my (abstract) line of thinking here... wouldn't it be nice if we could utilize both the heat energy as well as the energy from the free radiation that isn't converted into heat? How much potential energy of that nuclear "fuel" itself that decay is converting into liberated energy is being utilized by our current processes? I'm guessing here, but I'd venture that it's not close to the realm of 85%. It may be we're utilizing the heat energy to that point, but not the entire sum energy types that are being produced by said fuel.
