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1\u002F3 = ~0.47 D\u002Fs。大多数情况下，由于 H 的产量通常远高于 D，消耗掉的燃料大多会是 H，因此你可以近似地把实际减产量视为 200 H\u002Fmin（如果需要更精确的数值，可使用 190 H\u002Fmin）。D 的消耗约为 ~10\u002Fmin，因为它通常约为 H 速率的 4-5%。\\n\\n由于消耗值只取决于燃料类型及其基础产量的比例（因为它们会随矿物利用等比例提升），对于某颗巨行星来说，每个采集器造成的资源绝对损失是固定的。因此，在采矿速度较低时，基础产量较低的巨行星会把大部分产出都损失在维持消耗上。在这种情况下，先研究前几级矿物利用，对于让采集器真正盈利至关重要。\\n\\n例如：假设一颗巨行星的基础产量为 0.5 可燃冰\u002Fs 和 0.25 氢\u002Fs，基础采矿速度（100%）使采集速度 = x8，之后升级到矿物利用 5 级，即采矿速度 150%（使采集速度 = 8 * 1.5 = 12x）。\\n将采矿速度从 100% 提高到 150%（矿物利用从 0 级到 5 级）会使 FI 和 H 的产量都提高约 **3.5 倍**（约 +250%，而不是它对采矿机等设备产生的 +50% 效果）。在这种情况下，即使只是矿物利用的前两级（对大多数采矿机器仅提供 +20%），也基本能让采集器的输出翻倍。不过在更高的矿物利用等级，或基础产率较高的巨行星上，这种效果就不那么明显了。\\n原始（消耗前）和实际（消耗后）的资源产量可按如下方式计算：（其他矿物利用\u002F采矿速度数值的计算留给感兴趣的读者作为练习）\\n\\n{| class=\\\"wikitable\\\"\\n! 气态巨行星基础产量 !! 资源的能量值 !! 能量值合计 || 占总能量比例 !! 轨道采集器消耗 !! 采矿速度 100% 时的原始产量 !! 采矿速度 100% 时的实际产量 !! 采矿速度 150% 时的原始产量 !! 采矿速度 150% 时的实际产量\\n|-\\n| 0.5 **可**燃**冰**\u002Fs\\n| 4.8 MJ\u002FFI * 0.5 FI\u002Fs = **2.4 MW**\\n| rowspan=\\\"2\\\"| 2.4 MW + 2.25 MW = **4.65 MW**\\n| 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