This tutorial is set by the author to use the CC By-NC-ND protocol.
This tutorial is only applicable to E2ES, version V1.37!Because the magic has changed the heat dissipation and heat, it cannot be copied in other bags!
Unfortunately, E2ES eventually needs 4 锎 RTG, so it is necessary to obtain 锎 250, and E2ES also modify the heat and fuel heat of the cooler. ThereforeThe numerical values are re -simulated.This strategy will give me a available 锎 250 route.At the same time, in order to maximize the efficiency of fuel, oxidation fuel is used.At the same time, high density and low density differences are very different on the upper and lower limit requirements of the reactor, so they are completely two routes.
Cooler
The usage method is omitted because it is not modified.
Cooling Dalva Laws 20 Red Stone 80 quartz 80 gold 120 Shothta 120 Golden Stone 100 Diamond 120 氦 120 Last Shadow 140 Crown Ice 140 Iron 60 Copper 140 Tin 80 Magnesium 100 100 100
Fuel meter
Save flow: The duration of fuel is halved, the power generation increases to 6 times, and the heat of the hair becomes 1.2 times.
The duration of fuel power generation (T) a single total power generation (RF) TBU36021.67200025,920,000 oxidation TBU504277200036,288,000 Low -density uranium 23386472327,648,000 low -density uranium oxide 2331209.6903200038, 707,200 High -density uranium 233345643232000110,592,000 High -density uranium oxide 2334838.454032000154,828,800 Low -density uranium 235720603600025,920,000 Low -density uranium oxide 2351008753600036,288,000 High -density uranium 235288036036000103,680,000 High -density uranium oxide 2354032450145,152,000 low density Digital 鎿 236540435100027,540,000 Low -density oxidation 鎿 236756545100038,556,000 High -density 鎿 2362160259.251000110,160,000 High -density oxidation 鎿236302432451000154,224,000 Low density 钚 239630484600028,980,000 Low density oxidation 钚 239882604600040,572,000 High -density 钚 239252028846000115,920,000 High -density oxidation 钚 2393528366 046000162,288,000 low density 钚 241990843000029,700,000 low -density oxidation 钚 24113861053000041,580,000 high density 钚 2413960504300118,800,000 high densityOxidation 氧 2415544630300166,320,000 MOX239932.4694200039,160,800 MOX24114 2.81412700043,545,600 High -density 镅 2424608676.827000124,416,000 High -density oxidation 镅 2426451.284627000174,182,400 Low density 锔 24312601342600032,760,000 Low -density oxidation4 24317641682600045,864,000 High -density 锔 2435040806.42600013131,040,000 High -density oxidation 锔 2437056100826000183,456,000 Low density 锔 24597281.63400033,048,000 Low -density oxidation 锔 24 51360.81023400046,267,200 High -density 锔 2453888489.634000132,192,000 High -density oxidation 锔 2455443.261234000185,068,800 Low density 锔 24782864.83900032,292,000 lowDensity oxidation 锔 2471159.2813900045,208,800 High -density 锔 2473312388.839000129,168,000 High -density oxidation 锔 2474636.848639000180,835,200 Low density 锫 24881062.4434,830,000,830,000 Low -density oxidation 8 2481134784300048,762,000 High -density 锫 2483240374.443000139,320,000 High -density oxidation 锫 248453646843000195,048,000 Low density 锎 2491296139.23000038,880,000 low density oxidation 锎 2491814.41743000054,432,000 high density 锎 2495184835.2300155,520,000
High -density oxidation 9 2497257.6104430000217,728,000 Low density 锎 25113501442900039,150,000 Low -density oxidation 锎 25118901802900054,810,000 High -density 锎 251540086429000156,600,000 high density Oxidation 氧 2517560108029000219,240,000 IC2 concentrated uranium fuel 68256126608,634,120 IC2 MOX119888888400117,883,200 ER Yellow Uranus 6405345002,880,000 ER Blue Tablet ingots 6405345002,880,000 Uranium ingots 6004824001,440,000 Low -density routes
Low -density routes are: 2 232 → uranium oxide 233+uranium 238 (uranium ingot) → oxidation 钚 239+ oxidation 钚 242 → oxidation 锔 243+oxidation 锔 246 → oxidation 锫 247 氧 247 → oxidation 锎 249+ oxidation 锎 252 252→ oxidation 锎 250 → 锎 250
The synthesis of low -density routes is: TBU fuel → oxidation TBU fuel → low -density uranium oxide 233 fuel → low density oxidation 钚 239 fuel → low density 锔 243 fuel → low density 锫 248 fuel → low density 锎 249 fuel
After the calculation of the ME synthetic unit, 4 锎 250 is produced, and a total of 954 ingots and 1,496 uranium ingots are required.All fuel takes about 260 hours in total, even if 11 times it takes nearly 24 hours
The highest heating is 9 249, 174Hu/T
3*3*3 1 reactor
The most efficiency of the SLR reactor is the highest, but the slowest.
3*3*3 2 reactor
3*3*3 11 reactor
Under the conditions of 3*3, speed up the reaction rate as much as possible to speed up the product acquisition.The last shadow can be replaced with 冰 ，, which has no effect.
5*3*5 32 reactor
In order to speed up the progress, there is nothing to say in order to speed up the progress.
High -density route
High -density routes are direct than low -density routes, but the required raw materials are doubled.
High -density routes are: uranium ingot → uranium 235+ uranium 238 → oxidation 钚 239+ oxidation 钚 242 → oxidation 锔 246 oxidation 锔 246 → oxidation 锫 247 oxidation 锫 247 → 锎 250
The synthesis of high -density routes is: high -density uranium 235 fuel → high -density uranium oxide 235 fuel → high -density oxidation 钚 239 fuel → high density 锔 245 fuel → high density 锫 248 fuel → 锎 250
After the calculation of the ME synthetic unit, 4 锎 250 is produced, and a total of 65,772 uranium ingots are required. All fuels need a total of about 1066 hours.The main reason is that high -density materials require 4 scarce materials, so the materials have doubled.
The highest heating is 5 245, 612HU/T
3*3*3 1 reactor
3*3*3 4 reactor
3*3*3 should not be stuffed more.
5*5*5 16 reactor
Self -use reactor
The contents of the following reactors are based on uranium oxide 235 fuels. Because it is easy to obtain, it is best used.
3*3*3 3 reactor 388%efficiency
4*3*4 4 reactor 500%efficiency
5*5*4 6 reactor 588%efficiency
Improved from here, because the heat dissipation/thermal efficiency is different.
5*3*5 4 reactor 600%efficiency
9*5*9 16 reactor 800%efficiency
Similar expansion ideas as the previous.
