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	Manual section on uranium enrichment
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							| @@ -343,6 +343,162 @@ There's one more iron alloy in the game: stainless steel.  It is managed | ||||
| in a completely regular manner, created by alloying carbon steel with | ||||
| chromium. | ||||
|  | ||||
| ### uranium enrichment ### | ||||
|  | ||||
| When uranium is to be used to fuel a nuclear reactor, it is not | ||||
| sufficient to merely isolate and refine uranium metal.  It is necessary | ||||
| to control its isotopic composition, because the different isotopes | ||||
| behave differently in nuclear processes. | ||||
|  | ||||
| The main isotopes of interest are U-235 and U-238.  U-235 is good at | ||||
| sustaining a nuclear chain reaction, because when a U-235 nucleus is | ||||
| bombarded with a neutron it will usually fission (split) into fragments. | ||||
| It is therefore described as "fissile".  U-238, on the other hand, | ||||
| is not fissile: if bombarded with a neutron it will usually capture it, | ||||
| becoming U-239, which is very unstable and quickly decays into semi-stable | ||||
| (and fissile) plutonium-239. | ||||
|  | ||||
| Inconveniently, the fissile U-235 makes up only about 0.7% of natural | ||||
| uranium, almost all of the other 99.3% being U-238.  Natural uranium | ||||
| therefore doesn't make a great nuclear fuel.  (In real life there are | ||||
| a small number of reactor types that can use it, but technic doesn't | ||||
| have such a reactor.)  Better nuclear fuel needs to contain a higher | ||||
| proportion of U-235. | ||||
|  | ||||
| Achieving a higher U-235 content isn't as simple as separating the U-235 | ||||
| from the U-238 and just using the required amount of U-235.  Because | ||||
| U-235 and U-238 are both uranium, and therefore chemically identical, | ||||
| they cannot be chemically separated, in the way that different elements | ||||
| are separated from each other when refining metal.  They do differ | ||||
| in atomic mass, so they can be separated by centrifuging, but because | ||||
| their atomic masses are very close, centrifuging doesn't separate them | ||||
| very well.  They cannot be separated completely, but it is possible to | ||||
| produce uranium that has the isotopes mixed in different proportions. | ||||
| Uranium with a significantly larger fissile U-235 fraction than natural | ||||
| uranium is called "enriched", and that with a significantly lower fissile | ||||
| fraction is called "depleted". | ||||
|  | ||||
| A single pass through a centrifuge produces two output streams, one with | ||||
| a fractionally higher fissile proportion than the input, and one with a | ||||
| fractionally lower fissile proportion.  To alter the fissile proportion | ||||
| by a significant amount, these output streams must be centrifuged again, | ||||
| repeatedly.  The usual arrangement is a "cascade", a linear arrangement | ||||
| of many centrifuges.  Each centrifuge takes as input uranium with some | ||||
| specific fissile proportion, and passes its two output streams to the | ||||
| two adjacent centrifuges.  Natural uranium is input somewhere in the | ||||
| middle of the cascade, and the two ends of the cascade produce properly | ||||
| enriched and depleted uranium. | ||||
|  | ||||
| Fuel for technic's nuclear reactor consists of enriched uranium of which | ||||
| 3.5% is fissile.  (This is a typical value for a real-life light water | ||||
| reactor, a common type for power generation.)  To enrich uranium in the | ||||
| game, it must first be in dust form: the centrifuge will not operate | ||||
| on ingots.  (In real life uranium enrichment is done with the uranium | ||||
| in the form of a gas.)  It is best to grind uranium lumps directly to | ||||
| dust, rather than cook them to ingots first, because this yields twice | ||||
| as much metal dust.  When uranium is in refined form (dust, ingot, or | ||||
| block), the name of the inventory item indicates its fissile proportion. | ||||
| Uranium of any available fissile proportion can be put through all the | ||||
| usual processes for metal. | ||||
|  | ||||
| A single centrifuge operation takes two uranium dust piles, and produces | ||||
| as output one dust pile with a fissile proportion 0.1% higher and one with | ||||
| a fissile proportion 0.1% lower.  Uranium can be enriched up to the 3.5% | ||||
| required for nuclear fuel, and depleted down to 0.0%.  Thus a cascade | ||||
| covering the full range of fissile fractions requires 34 cascade stages. | ||||
| (In real life, enriching to 3.5% uses thousands of cascade stages. | ||||
| Also, centrifuging is less effective when the input isotope ratio | ||||
| is more skewed, so the steps in fissile proportion are smaller for | ||||
| relatively depleted uranium.  Zero fissile content is only asymptotically | ||||
| approachable, and natural uranium relatively cheap, so uranium is normally | ||||
| only depleted to around 0.3%.  On the other hand, much higher enrichment | ||||
| than 3.5% isn't much more difficult than enriching that far.) | ||||
|  | ||||
| Although centrifuges can be used manually, it is not feasible to perform | ||||
| uranium enrichment by hand.  It is a practical necessity to set up | ||||
| an automated cascade, using pneumatic tubes to transfer uranium dust | ||||
| piles between centrifuges.  Because both outputs from a centrifuge are | ||||
| ejected into the same tube, sorting tubes are needed to send the outputs | ||||
| in different directions along the cascade.  It is possible to send items | ||||
| into the centrifuges through the same tubes that take the outputs, so the | ||||
| simplest version of the cascade structure has a line of 34 centrifuges | ||||
| linked by a line of 34 sorting tube segments. | ||||
|  | ||||
| Assuming that the cascade depletes uranium all the way to 0.0%, | ||||
| producing one unit of 3.5%-fissile uranium requires the input of five | ||||
| units of 0.7%-fissile (natural) uranium, takes 490 centrifuge operations, | ||||
| and produces four units of 0.0%-fissile (fully depleted) uranium as a | ||||
| byproduct.  It is possible to reduce the number of required centrifuge | ||||
| operations by using more natural uranium input and outputting only | ||||
| partially depleted uranium, but (unlike in real life) this isn't usually | ||||
| an economical approach.  The 490 operations are not spread equally over | ||||
| the cascade stages: the busiest stage is the one taking 0.7%-fissile | ||||
| uranium, which performs 28 of the 490 operations.  The least busy is the | ||||
| one taking 3.4%-fissile uranium, which performs 1 of the 490 operations. | ||||
|  | ||||
| A centrifuge cascade will consume quite a lot of energy.  It is | ||||
| worth putting a battery upgrade in each centrifuge.  (Only one can be | ||||
| accommodated, because a control logic unit upgrade is also required for | ||||
| tube operation.)  An MV centrifuge, the only type presently available, | ||||
| draws 7 kEU/s in this state, and takes 5 s for each uranium centrifuging | ||||
| operation.  It thus takes 35 kEU per operation, and the cascade requires | ||||
| 17.15 MEU to produce each unit of enriched uranium.  It takes five units | ||||
| of enriched uranium to make each fuel rod, and six rods to fuel a reactor, | ||||
| so the enrichment cascade requires 514.5 MEU to process a full set of | ||||
| reactor fuel.  This is about 0.85% of the 6.048 GEU that the reactor | ||||
| will generate from that fuel. | ||||
|  | ||||
| If there is enough power available, and enough natural uranium input, | ||||
| to keep the cascade running continuously, and exactly one centrifuge | ||||
| at each stage, then the overall speed of the cascade is determined by | ||||
| the busiest stage, the 0.7% stage.  It can perform its 28 operations | ||||
| towards the enrichment of a single uranium unit in 140 s, so that is | ||||
| the overall cycle time of the cascade.  It thus takes 70 min to enrich | ||||
| a full set of reactor fuel.  While the cascade is running at this full | ||||
| speed, its average power consumption is 122.5 kEU/s.  The instantaneous | ||||
| power consumption varies from second to second over the 140 s cycle, | ||||
| and the maximum possible instantaneous power consumption (with all 34 | ||||
| centrifuges active simultaneously) is 238 kEU/s.  It is recommended to | ||||
| have some battery boxes to smooth out these variations. | ||||
|  | ||||
| If the power supplied to the centrifuge cascade averages less than | ||||
| 122.5 kEU/s, then the cascade can't run continuously.  (Also, if the | ||||
| power supply is intermittent, such as solar, then continuous operation | ||||
| requires more battery boxes to smooth out the supply variations, even if | ||||
| the average power is high enough.)  Because it's automated and doesn't | ||||
| require continuous player attention, having the cascade run at less | ||||
| than full speed shouldn't be a major problem.  The enrichment work will | ||||
| consume the same energy overall regardless of how quickly it's performed, | ||||
| and the speed will vary in direct proportion to the average power supply | ||||
| (minus any supply lost because battery boxes filled completely). | ||||
|  | ||||
| If there is insufficient power to run both the centrifuge cascade at | ||||
| full speed and whatever other machines require power, all machines on | ||||
| the same power network as the centrifuge will be forced to run at the | ||||
| same fractional speed.  This can be inconvenient, especially if use | ||||
| of the other machines is less automated than the centrifuge cascade. | ||||
| It can be avoided by putting the centrifuge cascade on a separate power | ||||
| network from other machines, and limiting the proportion of the generated | ||||
| power that goes to it. | ||||
|  | ||||
| If there is sufficient power and it is desired to enrich uranium faster | ||||
| than a single cascade can, the process can be speeded up more economically | ||||
| than by building an entire second cascade.  Because the stages of the | ||||
| cascade do different proportions of the work, it is possible to add a | ||||
| second and subsequent centrifuges to only the busiest stages, and have | ||||
| the less busy stages still keep up with only a single centrifuge each. | ||||
|  | ||||
| Another possible approach to uranium enrichment is to have no fixed | ||||
| assignment of fissile proportions to centrifuges, dynamically putting | ||||
| whatever uranium is available into whichever centrifuges are available. | ||||
| Theoretically all of the centrifuges can be kept almost totally busy all | ||||
| the time, making more efficient use of capital resources, and the number | ||||
| of centrifuges used can be as little (down to one) or as large as desired. | ||||
| The difficult part is that it is not sufficient to put each uranium dust | ||||
| pile individually into whatever centrifuge is available: they must be | ||||
| input in matched pairs.  Any odd dust pile in a centrifuge will not be | ||||
| processed and will prevent that centrifuge from accepting any other input. | ||||
|  | ||||
| industrial processes | ||||
| -------------------- | ||||
|  | ||||
|   | ||||
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