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を燃やす方法があります。\\n\\n建物を隣り合わせに配置し、[[dsp.term.sorters|Sorters]] を使って燃料を1基から次の1基へ送ることで、連結して運用することもできます。これによりベルトの使用量を減らせるうえ、発電所群の設置スペースを節約できます。ただし、連結した 火力発電所 は単一の燃料タイプとの相性が最も良いです。混在した燃料をチェーンに流し込むと、最初の発電所がフィルターの役割を果たし、後続の発電所は想定と異なる燃料タイプを受け取ったときに停止してしまうことがあります。\\n\\n実用面でいくつか押さえておくと、火力発電所 はより効率よく使いやすくなります。\\n\\n- 幅広い種類の燃料を燃やせますが、何でも使えるわけではありません。[[dsp.term.deuteron_fuel_rod|Deuteron Fuel Rod]]、[[dsp.term.antimatter_fuel_rod|Antimatter Fuel Rod]]、[[dsp.term.accumulator|Accumulator]]（Full）は代わりに専用施設で処理されます。\\n- 燃料消費は電力網の需要に応じて変動するため、燃料1個あたりの総エネルギーは常に同じです。負荷が高いほど、単に燃える速度が速くなるだけです。\\n- [[dsp.term.orbital_collector|軌道採集機]] を研究すると、水素 と メタンハイドレート が再生可能な投入資源になり、資源が [[dsp.term.space_warper|空間歪曲器]] で輸送されていない限り、火力発電所 を再生可能電源として運用できるようになります。\\n- 燃料生産にもそれ自体のエネルギーコストがかかるため、高性能燃料が必ずしも純増になるとは限りません。場合によっては、より高密度の燃料を製造し、[[dsp.term.sorter|仕分機]] で運搬するために使う電力が、その利点の大半を相殺してしまうことがあります。\\n\\n火力発電所 は小型ながら出力が高く、早期から中盤にかけての産業を支える実用的な手段です。より大規模な再生可能電源や高密度電源システムが主流になるまで、十分に活躍します。\",\"hero_image\":\"\u002Fimages\u002Fdyson-sphere-program\u002Fthermal-power-plant.png\",\"category\":\"power\",\"power_generation_kw\":2160,\"name\":\"dsp.term.thermal_power_plant\",\"tips\":\"===燃焼速度===\\n燃料1個がどれだけ持続するかは、そのMJ値に基づきます。火力発電所は効率の悪さにより20%の損失があります。燃料1個がどれだけ持つかを計算するには、そのMJエネルギーに80%（または0.8）を掛け、それを発電機が1秒あたりに発生させる2.16MWで割ります。その結果の数値が、その燃料1個が持続する時間になります。\\n\\n例1：石炭のエネルギー密度は2.7MJです。効率損失を差し引く（2.7 * 0.8）と、2.16MJが残ります。これを火力発電機の最大出力（2.16MJ \u002F 2.16MW）で割ると、石炭1個は最大稼働時に1秒間燃焼することが分かります。\\n例2：水素燃料棒のエネルギー密度は40MJです。効率損失を差し引く（40MJ * 0.8）と、32MJが残ります。これを火力発電機の最大出力（32MJ \u002F 2.16MW）で割ると、燃料棒1本は最大稼働時に14.8秒間燃焼することが分かります。\\n{| class=\\\"wikitable\\\"\\n|+負荷100%時の燃料燃焼時間\\n|-\\n! 燃料 !! エネルギー !! TPSでの80% !! 燃焼時間\\n|-\\n| 植物燃料 || 500 KJ || 400 KJ || 0.185 s \u002F 5 sごとに  27個 \u002F 1分あたり324個\\n|-\\n| 木材 || 1.5 MJ || 1.2 MJ || 0.555 s \u002F 5 sごとに  9個 \u002F 1分あたり108個\\n|-\\n| 石炭 || 2.7 MJ || 2.16 MJ || 1.000 s \u002F 1 sごとに  1個 \u002F 1分あたり60個\\n|-\\n| 可燃ユニット || 9.72 MJ ||7.776 MJ || 3.6 s \u002F 18 sごとに  5個 \u002F 1分あたり16.67個\\n|-\\n| 高エネルギーグラファイト || 6.75 MJ || 5.4 MJ || 2.500 s \u002F 5 sごとに  2個 \u002F 1分あたり24個\\n|-\\n| 原油 || 4.05 MJ || 3.24 MJ || 1.500 s \u002F 3 sごとに  2個 \u002F 1分あたり40個\\n|-\\n| 精製油 || 4.5 MJ || 3.6 MJ || 1.667 s \u002F 5 sごとに  3個 \u002F 1分あたり36個\\n|-\\n| 水素 & 重水素 || 9 MJ || 7.2 MJ || 3.333 s \u002F 10 sごとに  3個 \u002F 1分あたり18個\\n|-\\n| メタンハイドレート || 4.8 MJ || 3.84 MJ || 1.777 s \u002F 16 sごとに  9個 \u002F 1分あたり33.75個\\n|-\\n| 水素燃料棒 || 54 MJ || 43.2 MJ || 20.00 s \u002F 20 sごとに  1個 \u002F 1分あたり3個\\n|}\\n燃料は電力需要に応じた速度で消費されることに注意してください。満足度が100%未満の場合、火力発電所は（上記の）最大燃焼時間で燃料を燃やし、満足度が常に100%の場合は、より遅い燃焼速度で燃料が消費されます。\\n\\n===燃料生産コスト===\\n燃料の生産自体にもエネルギーコストがかかるため、専用の発電を行う場合は、加工によって高密度化した燃料が、その材料をそのまま使う場合に比べて正味の利益になるかどうかを考慮する必要があります。\\n例1：石炭のエネルギー密度は2.7MJです。石炭は2:1の比率で高エネルギーグラファイトに製錬でき、これは6.3MJのエネルギー密度を持ち、16%多いエネルギーになります。しかし、高エネルギーグラファイトの製錬には720 kJが必要で、製錬所にアクセスするためのソーターでさらに約36 kJが加わります。その結果、加工後に石炭より得られる増分はわずか5.6kJに過ぎず、一方でオーバーヘッド消費が増えるため、同じ利用可能電力を得るにはより多くの火力発電機が必要になります。\\n\\n===連結===\\n火力発電所は互いに隣接して配置し、ソーターで燃料を1つの発電所から次の発電所へ移動させることで連結できます。連結を使うと、発電施設に必要なベルトの数と総設置面積を抑えるのに役立ちます。\\n\\n===混合燃料タイプ===\\n1つの火力発電所は複数の種類の燃料を受け取り、使用できます。発電出力は一定（最大2.16MW）に保たれますが、燃料の燃焼時間はそのエネルギー量に応じて変化します。火力発電所を連結している場合、チェーン内で最初の発電所が拾った燃料タイプだけが、チェーン内の他の発電所へ受け渡せることに注意してください。最初の発電所がフィルターとして機能します。\\n\\n=== 副産物の処分 ===\\n火力発電所は、大量に生成される不要な副産物（例：メタンハイドレートをグラフェンに精製する際に発生する水素）を燃やすことで、一種の廃棄処理施設としても機能します。これらは貯蔵施設の直後に配置でき、貯蔵が完全に満杯になった後にだけ余剰分が燃やされます。これにより、副産物が施設の出力を詰まらせるのを防げます。\\n\\nCategory:アイテム\\nCategory:建造物\\nCategory:電力施設\"}","【DSP】火力発電所の性能・使い方","Dyson Sphere Programの火力発電所について、燃料の種類、稼働特性、効率と出力の特徴、給燃料の注意点を分かりやすく解説します。","2026-06-10 19:48:49","2026-05-09 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수집기\"],\"zh-CN\":[\"轨道采集器\",\"吸尘器\",\"采集器\"]}","\u002Fimages\u002Fdyson-sphere-program\u002Forbital-collector.webp","{\"ja\":{\"value\":\"軌道採集機\"},\"en\":{\"value\":\"Orbital Collector\"}}","軌道採集機","building\u002Forbital-collector",{"id":447,"category":50,"canonical_en":448,"aliases":449,"related_terms":389,"icon_url":450,"translations":451,"name":452,"e":453},"dsp.term.fire_ice","Fire ice","{\"ja\":[\"メタンハイドレート\"],\"ko\":[\"고체 메탄\"],\"zh-CN\":[\"可燃冰\"]}","\u002Fimages\u002Fdyson-sphere-program\u002Ffire-ice.webp","{\"ja\":{\"value\":\"メタンハイドレート\"},\"en\":{\"value\":\"Fire 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연료봉\"],\"zh-CN\":[\"氘核燃料棒\",\"氘棒\",\"核棒\",\"绿棒\"]}","\u002Fimages\u002Fdyson-sphere-program\u002Fdeuteron-fuel-rod.webp","{\"ja\":{\"value\":\"重陽子燃料棒\"},\"en\":{\"value\":\"Deuteron Fuel Rod\"}}","重陽子燃料棒","item\u002Fdeuteron-fuel-rod",{"id":479,"category":50,"canonical_en":480,"aliases":481,"related_terms":389,"icon_url":482,"translations":483,"name":484,"e":485},"dsp.term.energetic_graphite","Energetic graphite","{\"ja\":[\"高エネルギーグラファイト\"],\"ko\":[\"활성 흑연\"],\"zh-CN\":[\"高能石墨\",\"石墨\"]}","\u002Fimages\u002Fdyson-sphere-program\u002Fenergetic-graphite.webp","{\"ja\":{\"value\":\"高エネルギーグラファイト\"},\"en\":{\"value\":\"Energetic 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