JPS6337308B2 - - Google Patents
Info
- Publication number
- JPS6337308B2 JPS6337308B2 JP54054495A JP5449579A JPS6337308B2 JP S6337308 B2 JPS6337308 B2 JP S6337308B2 JP 54054495 A JP54054495 A JP 54054495A JP 5449579 A JP5449579 A JP 5449579A JP S6337308 B2 JPS6337308 B2 JP S6337308B2
- Authority
- JP
- Japan
- Prior art keywords
- natural gas
- air
- liquefied natural
- gas
- lng
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired
Links
- 239000003949 liquefied natural gas Substances 0.000 claims description 80
- VNWKTOKETHGBQD-UHFFFAOYSA-N methane Chemical compound C VNWKTOKETHGBQD-UHFFFAOYSA-N 0.000 claims description 32
- 239000007788 liquid Substances 0.000 claims description 29
- 239000007789 gas Substances 0.000 claims description 20
- 238000000034 method Methods 0.000 claims description 20
- 239000003345 natural gas Substances 0.000 claims description 14
- 238000001816 cooling Methods 0.000 claims description 6
- 239000002994 raw material Substances 0.000 claims description 6
- 238000001704 evaporation Methods 0.000 claims description 3
- 230000008020 evaporation Effects 0.000 claims description 3
- 238000010438 heat treatment Methods 0.000 claims description 2
- 230000005611 electricity Effects 0.000 description 14
- 238000009835 boiling Methods 0.000 description 6
- 238000005057 refrigeration Methods 0.000 description 4
- 239000002351 wastewater Substances 0.000 description 4
- 238000007796 conventional method Methods 0.000 description 3
- 238000004519 manufacturing process Methods 0.000 description 3
- 238000010248 power generation Methods 0.000 description 3
- 239000002918 waste heat Substances 0.000 description 3
- CURLTUGMZLYLDI-UHFFFAOYSA-N Carbon dioxide Chemical compound O=C=O CURLTUGMZLYLDI-UHFFFAOYSA-N 0.000 description 2
- 238000002485 combustion reaction Methods 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 239000000446 fuel Substances 0.000 description 2
- 239000003507 refrigerant Substances 0.000 description 2
- 238000003303 reheating Methods 0.000 description 2
- 239000013535 sea water Substances 0.000 description 2
- 239000000126 substance Substances 0.000 description 2
- 230000008016 vaporization Effects 0.000 description 2
- 239000001569 carbon dioxide Substances 0.000 description 1
- 229910002092 carbon dioxide Inorganic materials 0.000 description 1
- 230000006835 compression Effects 0.000 description 1
- 238000007906 compression Methods 0.000 description 1
- 238000009795 derivation Methods 0.000 description 1
- 229930195733 hydrocarbon Natural products 0.000 description 1
- 150000002430 hydrocarbons Chemical class 0.000 description 1
- 239000005416 organic matter Substances 0.000 description 1
- 238000001556 precipitation Methods 0.000 description 1
- 230000001105 regulatory effect Effects 0.000 description 1
- 238000001179 sorption measurement Methods 0.000 description 1
- 239000013526 supercooled liquid Substances 0.000 description 1
- 238000009834 vaporization Methods 0.000 description 1
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 description 1
Classifications
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F25—REFRIGERATION OR COOLING; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS; MANUFACTURE OR STORAGE OF ICE; LIQUEFACTION SOLIDIFICATION OF GASES
- F25J—LIQUEFACTION, SOLIDIFICATION OR SEPARATION OF GASES OR GASEOUS OR LIQUEFIED GASEOUS MIXTURES BY PRESSURE AND COLD TREATMENT OR BY BRINGING THEM INTO THE SUPERCRITICAL STATE
- F25J1/00—Processes or apparatus for liquefying or solidifying gases or gaseous mixtures
- F25J1/0002—Processes or apparatus for liquefying or solidifying gases or gaseous mixtures characterised by the fluid to be liquefied
- F25J1/0012—Primary atmospheric gases, e.g. air
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F25—REFRIGERATION OR COOLING; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS; MANUFACTURE OR STORAGE OF ICE; LIQUEFACTION SOLIDIFICATION OF GASES
- F25J—LIQUEFACTION, SOLIDIFICATION OR SEPARATION OF GASES OR GASEOUS OR LIQUEFIED GASEOUS MIXTURES BY PRESSURE AND COLD TREATMENT OR BY BRINGING THEM INTO THE SUPERCRITICAL STATE
- F25J1/00—Processes or apparatus for liquefying or solidifying gases or gaseous mixtures
- F25J1/003—Processes or apparatus for liquefying or solidifying gases or gaseous mixtures characterised by the kind of cold generation within the liquefaction unit for compensating heat leaks and liquid production
- F25J1/0032—Processes or apparatus for liquefying or solidifying gases or gaseous mixtures characterised by the kind of cold generation within the liquefaction unit for compensating heat leaks and liquid production using the feed stream itself or separated fractions from it, i.e. "internal refrigeration"
- F25J1/004—Processes or apparatus for liquefying or solidifying gases or gaseous mixtures characterised by the kind of cold generation within the liquefaction unit for compensating heat leaks and liquid production using the feed stream itself or separated fractions from it, i.e. "internal refrigeration" by flash gas recovery
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F25—REFRIGERATION OR COOLING; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS; MANUFACTURE OR STORAGE OF ICE; LIQUEFACTION SOLIDIFICATION OF GASES
- F25J—LIQUEFACTION, SOLIDIFICATION OR SEPARATION OF GASES OR GASEOUS OR LIQUEFIED GASEOUS MIXTURES BY PRESSURE AND COLD TREATMENT OR BY BRINGING THEM INTO THE SUPERCRITICAL STATE
- F25J1/00—Processes or apparatus for liquefying or solidifying gases or gaseous mixtures
- F25J1/02—Processes or apparatus for liquefying or solidifying gases or gaseous mixtures requiring the use of refrigeration, e.g. of helium or hydrogen ; Details and kind of the refrigeration system used; Integration with other units or processes; Controlling aspects of the process
- F25J1/0221—Processes or apparatus for liquefying or solidifying gases or gaseous mixtures requiring the use of refrigeration, e.g. of helium or hydrogen ; Details and kind of the refrigeration system used; Integration with other units or processes; Controlling aspects of the process using the cold stored in an external cryogenic component in an open refrigeration loop
- F25J1/0222—Processes or apparatus for liquefying or solidifying gases or gaseous mixtures requiring the use of refrigeration, e.g. of helium or hydrogen ; Details and kind of the refrigeration system used; Integration with other units or processes; Controlling aspects of the process using the cold stored in an external cryogenic component in an open refrigeration loop in combination with an intermediate heat exchange fluid between the cryogenic component and the fluid to be liquefied
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F25—REFRIGERATION OR COOLING; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS; MANUFACTURE OR STORAGE OF ICE; LIQUEFACTION SOLIDIFICATION OF GASES
- F25J—LIQUEFACTION, SOLIDIFICATION OR SEPARATION OF GASES OR GASEOUS OR LIQUEFIED GASEOUS MIXTURES BY PRESSURE AND COLD TREATMENT OR BY BRINGING THEM INTO THE SUPERCRITICAL STATE
- F25J1/00—Processes or apparatus for liquefying or solidifying gases or gaseous mixtures
- F25J1/02—Processes or apparatus for liquefying or solidifying gases or gaseous mixtures requiring the use of refrigeration, e.g. of helium or hydrogen ; Details and kind of the refrigeration system used; Integration with other units or processes; Controlling aspects of the process
- F25J1/0221—Processes or apparatus for liquefying or solidifying gases or gaseous mixtures requiring the use of refrigeration, e.g. of helium or hydrogen ; Details and kind of the refrigeration system used; Integration with other units or processes; Controlling aspects of the process using the cold stored in an external cryogenic component in an open refrigeration loop
- F25J1/0224—Processes or apparatus for liquefying or solidifying gases or gaseous mixtures requiring the use of refrigeration, e.g. of helium or hydrogen ; Details and kind of the refrigeration system used; Integration with other units or processes; Controlling aspects of the process using the cold stored in an external cryogenic component in an open refrigeration loop in combination with an internal quasi-closed refrigeration loop
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F25—REFRIGERATION OR COOLING; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS; MANUFACTURE OR STORAGE OF ICE; LIQUEFACTION SOLIDIFICATION OF GASES
- F25J—LIQUEFACTION, SOLIDIFICATION OR SEPARATION OF GASES OR GASEOUS OR LIQUEFIED GASEOUS MIXTURES BY PRESSURE AND COLD TREATMENT OR BY BRINGING THEM INTO THE SUPERCRITICAL STATE
- F25J1/00—Processes or apparatus for liquefying or solidifying gases or gaseous mixtures
- F25J1/02—Processes or apparatus for liquefying or solidifying gases or gaseous mixtures requiring the use of refrigeration, e.g. of helium or hydrogen ; Details and kind of the refrigeration system used; Integration with other units or processes; Controlling aspects of the process
- F25J1/0243—Start-up or control of the process; Details of the apparatus used; Details of the refrigerant compression system used
- F25J1/0279—Compression of refrigerant or internal recycle fluid, e.g. kind of compressor, accumulator, suction drum etc.
- F25J1/0281—Compression of refrigerant or internal recycle fluid, e.g. kind of compressor, accumulator, suction drum etc. characterised by the type of prime driver, e.g. hot gas expander
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F25—REFRIGERATION OR COOLING; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS; MANUFACTURE OR STORAGE OF ICE; LIQUEFACTION SOLIDIFICATION OF GASES
- F25J—LIQUEFACTION, SOLIDIFICATION OR SEPARATION OF GASES OR GASEOUS OR LIQUEFIED GASEOUS MIXTURES BY PRESSURE AND COLD TREATMENT OR BY BRINGING THEM INTO THE SUPERCRITICAL STATE
- F25J1/00—Processes or apparatus for liquefying or solidifying gases or gaseous mixtures
- F25J1/02—Processes or apparatus for liquefying or solidifying gases or gaseous mixtures requiring the use of refrigeration, e.g. of helium or hydrogen ; Details and kind of the refrigeration system used; Integration with other units or processes; Controlling aspects of the process
- F25J1/0243—Start-up or control of the process; Details of the apparatus used; Details of the refrigerant compression system used
- F25J1/0279—Compression of refrigerant or internal recycle fluid, e.g. kind of compressor, accumulator, suction drum etc.
- F25J1/0292—Refrigerant compression by cold or cryogenic suction of the refrigerant gas
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F25—REFRIGERATION OR COOLING; COMBINED HEATING AND REFRIGERATION SYSTEMS; HEAT PUMP SYSTEMS; MANUFACTURE OR STORAGE OF ICE; LIQUEFACTION SOLIDIFICATION OF GASES
- F25J—LIQUEFACTION, SOLIDIFICATION OR SEPARATION OF GASES OR GASEOUS OR LIQUEFIED GASEOUS MIXTURES BY PRESSURE AND COLD TREATMENT OR BY BRINGING THEM INTO THE SUPERCRITICAL STATE
- F25J2210/00—Processes characterised by the type or other details of the feed stream
- F25J2210/62—Liquefied natural gas [LNG]; Natural gas liquids [NGL]; Liquefied petroleum gas [LPG]
Landscapes
- Engineering & Computer Science (AREA)
- Physics & Mathematics (AREA)
- Mechanical Engineering (AREA)
- Thermal Sciences (AREA)
- General Engineering & Computer Science (AREA)
- Separation By Low-Temperature Treatments (AREA)
Description
本発明は液化天然ガス(以下LNGという。)を
利用した空気液化方法に関する。
従来よりLNGの寒冷を利用することは種々の
分野で提案され、一部は実施されている。このう
ち例えばガスタービン発電に於ける助燃用空気を
燃料用LNGの寒冷を利用して液化貯溜しておき、
電力需要のピーク時にその液体空気を集中的に気
化使用することにより発電を行う方法がある。こ
の方法によると、ガスタービン発電に於ける助燃
用空気を供給するための動力が節約できるので高
効率で発電できる特徴があるが、空気の液化貯溜
に要する動力を節減することが発電コストを低減
させることから望まれる。又一般に空気を液化し
て液体空気を製造する場合、その製造コストの大
部分は動力費であり、この動力費節減のために
LNGの寒冷を利用することが提案される理由で
あるが、実際にはLNGの寒冷費等と相殺され、
実用化に至らないのが現状である。
本発明はこのようなことから、LNGの寒冷を
有効に利用すると共にLNG中に含まれる高沸点
有機物の濃縮対策のために加圧する圧力を利用し
て膨脹タービンを駆動し圧縮機用動力節減を図る
ことにより液体空気製造コストのうち大部分を占
める電力費の低減を実現した方法である。
即ち圧縮空気を冷却液化するためのLNG蒸発
器に低圧にした気化量以上の過剰のLNGを供給
し、気化した天然ガスは天然ガス圧縮機により所
要圧に再加圧・圧送し、高沸点成分の多くなつた
余剰のLNGはポンプで臨界圧以上に加圧し、こ
れを予冷過程の圧縮空気との間接熱交換によつて
加温し、更に必要な場合は海水、温廃水などによ
つて常温以上迄加温した後膨脹タービンに導入し
て膨脹させ、発生した動力によつて前記気化天然
ガスの圧縮機を駆動する。これによつて圧縮空気
を低圧LNGの蒸発によつて低温に冷却できるた
め空気の圧縮圧力を比較的低くし、液化動力を節
減させることができる。同時に膨脹タービン駆動
による回収動力によつて所要動力を節減し得る。
更に本発明に於てはLNGの需要増大時に増大
分のLNGをポンプで臨界圧以上に加圧し、この
高圧LNGを海水・温廃水等により常温以上に加
温した後、膨脹タービンにより膨脹させて動力を
発生させ、これを原料空気圧縮機の動力源とする
ことにより空気液化の所要動力節減を図る方法を
も含む。火力発電所の燃料であるLNGは電力需
要に応じて変動があるが、空気液化の寒冷用に利
用するLNG量は最小需要量即ちベースロード値
に基づいて決めることが空気液化装置を常時安定
運転するために望ましい。従つて電力需要の大き
い昼間は使用LNG量も増加するので、この増加
分のLNGを利用して上記の如く膨脹タービンを
駆動する。即ち、相当大きな電力消費設備である
空気液化装置の空気圧縮機を電動機と膨脹タービ
ンとの両方により駆動し得る様にしておき、電力
需要の少ない夜間は安価な夜間電力を利用して電
動機を駆動源とし、電力需要の多い昼間はこの結
果として駆動する膨脹タービンを主駆動源とする
ことにより空気液化用の動力費の大巾な低減化を
可能としたものである。
以下に本発明の実施例を詳細に説明する。
第1図は火力発電所に供給するLNGを利用し
て液体空気を毎時48000Nm3製造する場合におけ
る本発明方法の一実施例である。管1より30℃の
大気48000Nm3/hが吸入され、冷却器2に於て
LNGにより冷却されたフレオンと熱交換して+
5℃迄冷却され、管24よりの空気と合流して
65000Nm3/hとなり圧縮機3によつて加圧され、
20気圧、+30℃の圧縮空気となつて管6を経、予
冷器7に導入される。圧縮機3の駆動に必要な動
力は10000kWであるが、駆動源は同容量の電動
機4と共に膨脹タービン5を連設しておく。この
膨脹タービン5は後記する如く高圧天然ガスを作
動ガスとし、LNG需要の大きい時期にはその駆
動力を利用することによつて電動機に要する電力
を軽減または不要とする。LNG需要の小さい時
期には膨脹タービン5は作動を停止し、電動機4
のみで圧縮機3を駆動する。予冷器7に導入され
た圧縮空気はここで伝熱管69内を流れる冷媒フ
レオンにより再び冷却され+5℃で導出し、切換
使用される吸着器8a又は8bの片方に導入さ
れ、ここで水分及び炭酸ガスが吸着除去される。
吸着により精製された空気は管9より原料空気予
冷用熱交換器10に導入され後記する気液分離器
18よりの低温気化空気および循環フレオンと熱
交換して−130℃まで冷却され、次いで管11を
経てLNG蒸発器12に導入される。LNG蒸発器
12に於て圧縮精製空気は大気圧のLNGと熱交
換し−155℃まで冷却されて液化する。液化した
空気は管13を経てLNG蒸発器14に導入され、
0.5気圧(絶対)のLNGと熱交換し−168℃に過
冷されて管15より導出する。過冷された液体空
気は更に熱交換器16に導入されて後記する気液
分離器18よりの気化空気と熱交換し一層過冷さ
れて導出し、膨脹弁17に於て1.5気圧に膨脹し
気液分離器18に導入される。気液分離器18の
底部より管19を経て液体空気48000Nm3/hが
取出され弁20を経て液体空気貯槽21に貯蔵さ
れる。一方気液分離器18の低温気化空気
17000Nm3/hは管22より熱交換器16に入つ
て液体空気を過冷し、自身は昇温して導出し、管
23より更に熱交換器10に導入されて圧縮精製
空気を冷却し自身はほぼ常温附近迄昇温して管2
4を経、管1よりの原料空気と合流し圧縮機3の
吸入側へ戻される。
寒冷用LNGは10気圧、−155℃の状態で管25
より供給され、2分してその一部80000Nm3/h
が管26を経て前記した空気の液化用に供され
る。即ち管26のLNGは更に2分してその一部
は弁27を経て大気圧まで降圧し−160℃の状態
でLNG蒸発器12に導入され、空気と熱交換し
て蒸発する。この場合弁27で調整されるLNG
蒸発器12へのLNGの供給量はLNG蒸発器12
で蒸発する量よりも過剰にしておく。従つて
LNG蒸発器12を導出し管28を流れるLNGは
気液混合状態であり、これが気液分離器29に入
つて気液分離され、ガス33000Nm3/hが管30
より導出される。一方空気液化用LNGの分岐流
れは弁31を経てLNG蒸発器14へ導入され、
ここで0.5気圧(絶対)、−170℃の状態で蒸発する
が、この場合も弁31で調整するLNGの供給量
はLNG蒸発器14で蒸発する量よりも過剰にし
ておく。従つて気液混合状態のLNGは管32よ
り気液分離器33に導入され、分離されたガス
12000Nm3/hは電動機34により駆動される真
空ポンプ35により圧縮され、大気圧−110℃の
状態で管36を経て前記管30よりのガスと合流
する。合流して45000Nm3/hとなつたガスは膨
脹タービン37によつて駆動される圧縮機38に
よつて10気圧、+10℃の天然ガスとして管39を
経、後記する他の管52および60よりの天然ガ
スと合流した上、管40より需要先の火力発電所
41に供給される。気液分離器29および33で
分離された液には一般にLNG中に含まれる炭化
水素等の高沸点成分が濃縮されており、これらの
析出によつて蒸発器内が閉塞する不都合が生ず
る。これを防ぐため、高沸点成分の濃縮された
LNGを加圧した後、加温することにより、LNG
中の主成分であるメタンと高沸点成分との比揮発
度を小さくし、メタン気流中に均一に気化される
ようにする必要がある。このため気液分離器29
および33で分離されたLNGは各々管42およ
び43よりポンプ44および45に導入され各々
200気圧に加圧された後合流して管46を経、熱
交換器47に入る。該熱交換器47に於て、後記
する循環フレオンと熱交換し−40℃まで昇温され
て導出し、管48より加熱器49に導入され、こ
こで廃熱源50により+100℃まで加熱された後、
管51より膨脹タービン37に入り、200気圧か
ら10気圧まで膨脹して動力を発生し管52へ導出
する。この場合膨脹タービン37を2段以上とし
て常温以上加熱された最初の高圧天然ガスを先ず
第1段タービンにて中間圧力まで膨脹し、その際
温度降下した出口ガスを再び温廃水等による加熱
によつて常温以上に昇温して次段タービンにて膨
脹させ、最終段タービンの出口ガスを天然ガス圧
送配管52に送る多段式タービンを採用すること
により更に効率を上げることが可能である。
以上に述べた空気液化用のLNGの流れは電力
需要の変動に伴なうLNG量の増減に拘らず定常
的に供給する、いわゆるベースロード用LNGを
利用したものであるが、次に述べるLNGの流れ
は電力需要がピークの時にのみ流されるLNGを
利用したものである。即ち発電所のLNG消費量
が増加した時の増加分で、夜間は実質的に流さず
日中はその使用量に応じて流すLNGの流れを利
用したものである。管25より供給され前記2分
されたLNGの他部は管54よりポンプ55に導
入され200気圧に加圧され弁56に至る。弁56
に於て、電力需要に応じた使用量に調節されて加
熱器57に入り、廃熱源58により+100℃まで
加熱された後管59を経て膨脹タービン5に導入
され、ここで200気圧から10気圧まで膨脹しその
際発生した動力は連設した空気圧縮機3に必要な
動力の一部又は大部分として利用される。膨脹タ
ービン5は2段以上とし前段タービンでの膨脹で
温度降下したガスを再び温廃水等による加熱によ
つて常温以上に昇温した後、後段タービンに導入
する多段再熱式とすることも可能である。膨脹タ
ービン5の出口ガスは管60を経、管39および
52よりのガスと合流し、需要先の火力発電所4
1へ送られる。
次に本発明方法に於てはLNGの寒冷をより有
効且つ安全に利用するためにフレオン冷媒の循環
系が設けられている。管61を流れる10気圧、−
150℃の液状フレオンはポンプ62により圧送さ
れ管63を経て熱交換器10へ導入される。熱交
換器10では精製圧縮空気の冷却源として用いら
れ、自身は昇温して−20℃となり管64より導出
する。次いでこのフレオンの流れは2分し、その
一部は管65を経て冷却器2の伝熱管66内を流
れ原料空気を熱交換してこれを冷却し自身は0℃
迄昇温して管67へ導出する。一方2分した他部
は管68を経て予冷器7の伝熱管69内を流れ、
圧縮原料空気を冷却して自身は昇温し0℃となり
管70へ導出する。管70は前記管67と合流し
て熱交換器47に至り、ここでフレオンは高圧
LNGに冷却されて−150℃となつて導出しポンプ
62により循環する。尚、このフレオン循環系を
用いず、直接圧縮空気とLNGを熱交換しても良
いことは勿論である。
次に本発明の他の実施例について説明する。前
記の如く本発明に於ては膨脹タービンを多段とし
各段の中間に再熱回路を組合せることにより、高
圧天然ガスの膨脹タービンに於ける発生動力を大
ならしめ、電力節減の効果を更に大ならしめるこ
とが可能である。第2図はこの場合の実施例であ
る。管48より供給される200気圧、−40℃の天然
ガスは加熱器49Aに於て廃熱源50により+
100℃迄加熱された後、管51Aより膨脹タービ
ン37Aに導入され、膨脹して45気圧、20℃の状
態となり管52Aを通つて加熱器49Bに入り再
び100℃まで加熱されて管51Bより膨脹タービ
ン37Bに導入される。ここで再び膨脹して10気
圧、+20℃の状態となり、管52Bへ導出する。
膨脹タービン37Aおよび37Bで発生した動力
は共に連設された圧縮機38を駆動する動力とし
て用いられる。一方管54より供給される10気
圧、−155℃のLNGはポンプ55により200気圧に
加圧された後弁56に至り、ここで電力需要に応
じた供給量に調節された上加熱器57Aに入り熱
源58により100℃まで加熱されて管59Aより
膨脹タービン5Aに導入される。ここで高圧の
LNGは膨脹して45気圧、+20℃の状態となり、管
60Aより加熱器57Bに入り、再び熱源58に
より+100℃迄加熱されて管59Bを経、膨脹タ
ービン5Bに入り再び膨脹して10気圧、+20℃の
状態となり管60Bへ導出する。管60Bは前記
52Bおよび39と合流し、管40となつて需要
先の火力発電所に至る。膨脹タービン5Aおよび
5Bは連設されている空気圧縮機3に発生動力を
伝達し、原料空気圧縮に必要な動力の一部又は大
部分を供給する。
本発明は以上の様にLNGに通常含まれる高沸
点有機物が気化過程で濃縮・析出する不都合を解
決するため、該有機物が濃縮されたLNGを加圧
することに着目し、この圧力を有効に利用するこ
とにより圧縮機の動力節減化を図ると共にLNG
の寒冷を最大限に利用して空気の液化率の向上を
可能としたもので、この方法によつて液体空気を
製造した場合の原単位を従来法の場合と比較する
と次の如くになる。今LNGの最終需要先である
火力発電所における消費量が夜間80000Nm3/h、
昼間の電力ピーク時は150000Nm3/hになるもの
と仮定する。即ち第1図の実施例に於て、
LNG80000Nm3/hが常時管26を通つて空気液
化用として流れる一方、管54を流れるLNG量
は夜間は無視し得る程度であり、昼間のピーク時
は70000Nm3/hに達すると仮定すると、各機器
の消費動力、本発明方法の膨脹タービンによる発
生動力、このタービンによる発生動力を圧縮機の
駆動源とした場合の差引必要動力は次表の如くな
る。
The present invention relates to an air liquefaction method using liquefied natural gas (hereinafter referred to as LNG). Utilizing the refrigeration of LNG has been proposed in various fields, and some have already been implemented. Among these, for example, air for combustion support in gas turbine power generation is liquefied and stored using the cooling of LNG for fuel.
There is a method of generating electricity by intensively vaporizing the liquid air during peak electricity demand. This method has the advantage of being able to generate electricity with high efficiency because it saves the power needed to supply air for combustion assistance in gas turbine power generation, but reducing the power required to liquefy and store air reduces power generation costs. Desired because it makes you do something. In addition, when producing liquid air by liquefying air, most of the production cost is power cost, and in order to reduce this power cost,
The reason is that it is proposed to use the refrigeration of LNG, but in reality it is offset by the refrigeration costs of LNG, etc.
The current situation is that it has not been put into practical use. For this reason, the present invention effectively utilizes the cold temperature of LNG, and also uses the increased pressure to drive the expansion turbine to prevent the concentration of high-boiling organic matter contained in LNG, thereby saving power for the compressor. This method has achieved a reduction in electricity costs, which account for the majority of liquid air manufacturing costs. In other words, LNG in excess of the amount of vaporized at a low pressure is supplied to an LNG evaporator that cools and liquefies compressed air, and the vaporized natural gas is repressurized and pumped to the required pressure by a natural gas compressor, and the high-boiling point components are Excess LNG, which has increased in volume, is pressurized above the critical pressure using a pump, heated through indirect heat exchange with compressed air during the pre-cooling process, and, if necessary, heated to room temperature using seawater, heated wastewater, etc. After being heated to the above temperature, it is introduced into an expansion turbine and expanded, and the generated power drives the vaporized natural gas compressor. As a result, the compressed air can be cooled to a low temperature by evaporation of the low-pressure LNG, so the compression pressure of the air can be made relatively low, and the liquefaction power can be saved. At the same time, the required power can be reduced by the recovered power driven by the expansion turbine. Furthermore, in the present invention, when the demand for LNG increases, the increased amount of LNG is pressurized to above the critical pressure using a pump, and after this high-pressure LNG is heated to above room temperature using seawater, hot wastewater, etc., it is expanded using an expansion turbine. It also includes a method for reducing the power required for air liquefaction by generating power and using it as a power source for a raw air compressor. LNG, which is the fuel for thermal power plants, fluctuates depending on the power demand, but the amount of LNG used for cooling air liquefaction is determined based on the minimum demand, that is, the base load value, so that the air liquefaction equipment can operate stably at all times. desirable for. Therefore, since the amount of LNG used increases during the day when the demand for electricity is high, this increased amount of LNG is used to drive the expansion turbine as described above. In other words, the air compressor of the air liquefaction equipment, which is a fairly large power consuming facility, can be driven by both an electric motor and an expansion turbine, and at night when electricity demand is low, the electric motor is driven using cheap nighttime electricity. By using the expansion turbine as the main drive source during the day when the demand for electricity is high, it is possible to significantly reduce the power cost for air liquefaction. Examples of the present invention will be described in detail below. FIG. 1 shows an embodiment of the method of the present invention in which 48,000 Nm 3 of liquid air is produced per hour using LNG supplied to a thermal power plant. 48000Nm 3 /h of air at 30°C is sucked into the cooler 2 through the pipe 1.
By exchanging heat with Freon cooled by LNG
It is cooled down to 5℃ and merges with the air from tube 24.
It becomes 65000Nm 3 /h and is pressurized by compressor 3.
The compressed air at 20 atmospheres and +30°C is introduced into the precooler 7 through the pipe 6. The power required to drive the compressor 3 is 10,000 kW, and the drive source is an electric motor 4 of the same capacity and an expansion turbine 5 installed in series. As will be described later, this expansion turbine 5 uses high-pressure natural gas as a working gas, and during periods of high demand for LNG, the power required for the electric motor is reduced or eliminated by utilizing its driving force. When LNG demand is low, the expansion turbine 5 stops operating and the electric motor 4
The compressor 3 is driven only by the The compressed air introduced into the precooler 7 is cooled again by the refrigerant Freon flowing in the heat exchanger tube 69, and is led out at +5°C.The compressed air is introduced into one of the adsorbers 8a or 8b, which is used selectively, where water and carbon dioxide are removed. Gas is adsorbed and removed.
The air purified by adsorption is introduced into the feed air precooling heat exchanger 10 through the tube 9, where it is cooled down to -130°C by exchanging heat with low-temperature vaporized air from the gas-liquid separator 18 and circulating Freon, which will be described later. 11 and is introduced into the LNG evaporator 12. In the LNG evaporator 12, the compressed purified air exchanges heat with LNG at atmospheric pressure, is cooled to -155°C, and is liquefied. The liquefied air is introduced into the LNG evaporator 14 through the pipe 13,
It exchanges heat with LNG at 0.5 atm (absolute), is subcooled to -168°C, and is discharged from pipe 15. The supercooled liquid air is further introduced into a heat exchanger 16, where it exchanges heat with vaporized air from a gas-liquid separator 18 (to be described later), is further supercooled, and then discharged, and expanded to 1.5 atmospheres at an expansion valve 17. The gas is introduced into the gas-liquid separator 18. 48,000 Nm 3 /h of liquid air is taken out from the bottom of the gas-liquid separator 18 via a pipe 19 and stored in a liquid air storage tank 21 via a valve 20. On the other hand, the low temperature vaporized air of the gas-liquid separator 18
17000Nm 3 /h enters the heat exchanger 16 from the pipe 22, subcools the liquid air, raises its temperature and draws it out, and is further introduced into the heat exchanger 10 through the pipe 23, cools the compressed purified air, and cools the liquid air itself. The temperature of tube 2 was increased to approximately room temperature.
4, joins with the raw material air from the pipe 1, and is returned to the suction side of the compressor 3. LNG for cold use is pipe 25 at 10 atm and -155℃.
80000Nm 3 /h
is provided through the pipe 26 for the aforementioned liquefaction of the air. That is, the LNG in the pipe 26 is further divided into two parts, a part of which is reduced in pressure to atmospheric pressure through the valve 27, and introduced into the LNG evaporator 12 at -160°C, where it is evaporated by exchanging heat with air. In this case the LNG regulated by valve 27
The amount of LNG supplied to the evaporator 12 is
Make sure the amount is in excess of the amount that will evaporate. accordingly
The LNG led out of the LNG evaporator 12 and flowing through the pipe 28 is in a gas-liquid mixed state, and this enters the gas-liquid separator 29 where it is separated into gas and liquid.
It is derived from On the other hand, the branched flow of LNG for air liquefaction is introduced into the LNG evaporator 14 via the valve 31,
Here, the LNG is evaporated at 0.5 atm (absolute) and -170°C, but in this case as well, the amount of LNG supplied that is adjusted by the valve 31 is set to be in excess of the amount evaporated by the LNG evaporator 14. Therefore, LNG in a gas-liquid mixed state is introduced into the gas-liquid separator 33 through the pipe 32, and the separated gas is
12000 Nm 3 /h is compressed by a vacuum pump 35 driven by an electric motor 34, and merges with the gas from the pipe 30 through a pipe 36 at an atmospheric pressure of -110°C. The combined gas becomes 45,000 Nm 3 /h and is passed through a pipe 39 as natural gas at 10 atmospheres and +10°C by a compressor 38 driven by an expansion turbine 37, and then from other pipes 52 and 60, which will be described later. After combining with the natural gas of The liquid separated by the gas-liquid separators 29 and 33 generally contains concentrated high-boiling components such as hydrocarbons contained in LNG, and their precipitation causes the inconvenience of clogging the evaporator. To prevent this, high boiling point components are concentrated.
By pressurizing and heating LNG, LNG
It is necessary to reduce the relative volatility of methane, which is the main component, and high-boiling components so that they can be uniformly vaporized in the methane stream. For this reason, the gas-liquid separator 29
The LNG separated at and 33 is introduced into pumps 44 and 45 through pipes 42 and 43, respectively.
After being pressurized to 200 atmospheres, they join together and enter a heat exchanger 47 via a pipe 46. In the heat exchanger 47, it exchanged heat with circulating freon, which will be described later, and was heated to -40°C and led out, introduced through a pipe 48 to a heater 49, where it was heated to +100°C by a waste heat source 50. rear,
It enters the expansion turbine 37 through the pipe 51, expands from 200 atm to 10 atm, generates power, and leads out to the pipe 52. In this case, the expansion turbine 37 is set to two or more stages, and the first high-pressure natural gas heated above room temperature is first expanded to an intermediate pressure in the first stage turbine, and the outlet gas whose temperature has dropped at that time is heated again by hot waste water or the like. Efficiency can be further improved by employing a multi-stage turbine in which the gas is heated to above room temperature and expanded in the next stage turbine, and the outlet gas of the final stage turbine is sent to the natural gas pressure feeding pipe 52. The flow of LNG for air liquefaction described above uses so-called base load LNG, which is constantly supplied regardless of changes in the amount of LNG due to fluctuations in electricity demand. This flow utilizes LNG, which is flown only during peak electricity demand. In other words, this is the increase when the power plant's LNG consumption increases, and it utilizes the flow of LNG that is virtually not flowed at night but is flowed during the day according to the amount used. The other portion of the LNG, which is supplied through the pipe 25 and divided into two parts, is introduced into the pump 55 through the pipe 54, is pressurized to 200 atmospheres, and reaches the valve 56. valve 56
The amount of electricity used is adjusted according to the electricity demand, enters the heater 57, is heated to +100°C by the waste heat source 58, and is introduced into the expansion turbine 5 via the tube 59, where the temperature is increased from 200 atm to 10 atm. The power generated at this time is used as part or most of the power required for the connected air compressor 3. The expansion turbine 5 may have two or more stages, and may be of a multi-stage reheating type in which the gas whose temperature has been lowered by expansion in the first stage turbine is heated again by hot waste water or the like to rise above room temperature and then introduced into the second stage turbine. It is. The outlet gas of the expansion turbine 5 passes through a pipe 60, joins the gas from the pipes 39 and 52, and is sent to the thermal power plant 4, which is the demand destination.
Sent to 1. Next, in the method of the present invention, a Freon refrigerant circulation system is provided in order to utilize the refrigeration of LNG more effectively and safely. 10 atmospheres flowing through pipe 61, -
Liquid Freon at 150°C is pumped by a pump 62 and introduced into the heat exchanger 10 through a pipe 63. The heat exchanger 10 is used as a cooling source for purified compressed air, and the purified compressed air itself is heated to -20°C and is led out through the pipe 64. Next, this flow of Freon is divided into two parts, and a part of it flows through the tube 65 and inside the heat transfer tube 66 of the cooler 2, exchanging heat with the raw material air and cooling it, so that the temperature itself reaches 0°C.
The temperature is raised to a temperature of 100.degree. On the other hand, the other part, which is divided into two parts, flows through the tube 68 and inside the heat transfer tube 69 of the precooler 7.
The compressed raw material air is cooled and its temperature rises to 0° C. and is led out to the pipe 70. The tube 70 joins the tube 67 to the heat exchanger 47, where the Freon is heated to high pressure.
It is cooled by LNG to −150° C. and circulated by a derivation pump 62. Note that it is of course possible to directly exchange heat between compressed air and LNG without using this Freon circulation system. Next, other embodiments of the present invention will be described. As described above, in the present invention, the expansion turbine is multi-staged and a reheating circuit is combined between each stage, thereby increasing the power generated in the high-pressure natural gas expansion turbine and further increasing the power saving effect. It is possible to make it big. FIG. 2 shows an example of this case. Natural gas at 200 atm and -40°C supplied from pipe 48 is heated to + by waste heat source 50 in heater 49A.
After being heated to 100°C, it is introduced into the expansion turbine 37A through the pipe 51A, where it is expanded to a state of 45 atmospheres and 20°C, passes through the pipe 52A, enters the heater 49B, is heated to 100°C again, and is expanded through the pipe 51B. It is introduced into the turbine 37B. Here, it expands again to a state of 10 atmospheres and +20°C, and is led out to the pipe 52B.
The power generated by the expansion turbines 37A and 37B is used as power to drive the compressor 38 connected together. On the other hand, the LNG at 10 atm and -155°C supplied from the pipe 54 is pressurized to 200 atm by the pump 55, and then reaches the valve 56, where it is supplied to the upper heater 57A where the supply amount is adjusted according to the electricity demand. It is heated to 100° C. by the input heat source 58 and introduced into the expansion turbine 5A through the pipe 59A. Here the high pressure
The LNG expands to 45 atmospheres and +20°C, enters the heater 57B from the pipe 60A, is heated again to +100°C by the heat source 58, passes through the pipe 59B, enters the expansion turbine 5B, and expands again to 10 atmospheres. It reaches a state of +20°C and is led out to the pipe 60B. The pipe 60B merges with the above-mentioned 52B and 39, becomes the pipe 40, and reaches the thermal power plant of the demand destination. The expansion turbines 5A and 5B transmit the generated power to the air compressor 3 connected thereto, and supply part or most of the power necessary for compressing the raw material air. As described above, in order to solve the inconvenience that high boiling point organic substances normally contained in LNG are concentrated and precipitated during the vaporization process, the present invention focuses on pressurizing LNG in which the organic substances are concentrated, and makes effective use of this pressure. By doing so, we can reduce the power consumption of the compressor and
This method makes it possible to improve the liquefaction rate of air by making maximum use of the cold temperature of air.Comparing the unit consumption of liquid air produced by this method with that of the conventional method, it is as follows. The consumption at thermal power plants, which are the final demand for LNG, is now 80,000 Nm 3 /h at night.
It is assumed that the peak power consumption during the daytime is 150000Nm 3 /h. That is, in the embodiment shown in FIG.
Assuming that 80000Nm 3 /h of LNG constantly flows through pipe 26 for air liquefaction, while the amount of LNG flowing through pipe 54 is negligible at night and reaches 70000Nm 3 /h during the daytime peak hours, each The following table shows the power consumed by the equipment, the power generated by the expansion turbine of the method of the present invention, and the required power when the power generated by the turbine is used as the drive source for the compressor.
【表】
従つて液体空気48000Nm3/h製造時に於ける
電力原単位は従来法では
13700/48000=0.285kWH/Nm3
であるのに対し、実施例1によつた場合は
7000/48000=0.146kWH/Nm3
となる。即ち本発明方法により、電力原単位が従
来法に比して約半分になるという大きな経済的効
果が得られる。[Table] Therefore, the electricity consumption rate when manufacturing liquid air at 48000Nm 3 /h is 13700/48000 = 0.285kWH/Nm 3 in the conventional method, whereas in the case of Example 1 it is 7000/48000 = 0.146 kWH/ Nm3 . That is, the method of the present invention provides a great economical effect in that the power consumption rate is about half that of the conventional method.
第1図は本願発明の方法の一実施例を示す系統
図、第2図は他の実施例を示す系統図である。
2は冷却器、3は圧縮機、4は電動機、5,5
A,5Bは膨脹タービン、7は予冷器、8a及び
8bは吸着器、10は原料空気予冷用熱交換器、
12及び14はLNG蒸発器、16は熱交換器、
17は膨脹弁、18は気液分離器、21は液体空
気貯槽、29及び33は気液分離器、34は電動
機、35は真空ポンプ、37,37A,37Bは
膨脹タービン、38は圧縮機、41は火力発電
所、44及び45はポンプ、47は熱交換器、4
9,49A,49Bは加熱器、55はポンプ、5
7,57A,57Bは加熱器、62はポンプであ
る。
FIG. 1 is a system diagram showing one embodiment of the method of the present invention, and FIG. 2 is a system diagram showing another embodiment. 2 is a cooler, 3 is a compressor, 4 is an electric motor, 5,5
A and 5B are expansion turbines, 7 is a precooler, 8a and 8b are adsorbers, 10 is a heat exchanger for precooling raw air,
12 and 14 are LNG evaporators, 16 is a heat exchanger,
17 is an expansion valve, 18 is a gas-liquid separator, 21 is a liquid air storage tank, 29 and 33 are gas-liquid separators, 34 is an electric motor, 35 is a vacuum pump, 37, 37A, 37B is an expansion turbine, 38 is a compressor, 41 is a thermal power plant, 44 and 45 are pumps, 47 is a heat exchanger, 4
9, 49A, 49B are heaters, 55 is a pump, 5
7, 57A, 57B are heaters, and 62 is a pump.
Claims (1)
に於て、原料空気を圧縮機で圧縮し、かつ予備処
理した後、液化天然ガス蒸発器に導入し、蒸発量
以上供給される液化天然ガスにより冷却した上膨
張せしめ、生成液体空気を貯留すると共に分離低
温空気を、その寒冷を回収した後、前記圧縮機に
吸引される原料空気に合流せしめる工程と、前記
液化天然ガス蒸発器に蒸発量以上供給された液化
天然ガスの蒸発ガスを加圧して需要先に供給する
と共に余剰液を臨界圧以上に加圧し、かつ加温し
た後、膨張タービンに導入し前記蒸発天然ガス加
圧用の動力源として膨張せしめる工程とからなる
ことを特徴とする液化天然ガスを利用した空気液
化方法。 2 前記臨界圧以上に加圧され、かつ加温された
天然ガスが複数段からなる膨張タービンにより膨
張されることを特徴とする特許請求の範囲第1項
記載の液化天然ガスを利用した空気液化方法。 3 液化天然ガスを利用して空気を液化する方法
に於て、原料空気を圧縮機で圧縮し、かつ予備処
理した後、液化天然ガス蒸発器に導入し蒸発量以
上に供給される液化天然ガスにより冷却した上膨
張せしめ、生成液体空気を貯留すると共に、分離
低温空気をその寒冷を回収した後、前記圧縮機に
吸引される原料空気に合流せしめる工程と、前記
液化天然ガス蒸発器に蒸発量以上供給された液化
天然ガスの蒸発ガスを加圧して需要先に供給する
と共に余剰液を臨界圧以上に加圧し、かつ加温し
た後、膨張タービンに導入し、前記蒸発天然ガス
加圧用の動力源として膨張せしめる工程と、別途
供給液化天然ガスを臨界圧以上に加圧し、かつ加
温した後、膨張タービンに導入し前記原料空気加
圧用の動力源として膨張せしめて供給する工程と
からなることを特徴とする液化天然ガスを利用し
た空気液化方法。 4 前記臨界圧以上に加圧され、かつ加温された
別途供給の天然ガスが複数段からなる膨張タービ
ンにより膨張されることを特徴とする特許請求の
範囲第3項記載の液化天然ガスを利用した空気液
化方法。[Claims] 1. In a method of liquefying air using liquefied natural gas, raw air is compressed with a compressor, and after being pretreated, it is introduced into a liquefied natural gas evaporator and the A step of cooling and expanding the liquefied natural gas with the supplied liquefied natural gas, storing the generated liquefied air and collecting the separated low-temperature air, and then combining the liquefied natural gas with the raw material air sucked into the compressor. The evaporated gas of the liquefied natural gas that has been supplied to the gas evaporator in excess of the evaporation amount is pressurized and supplied to the consumer, and the excess liquid is pressurized to a critical pressure or higher, heated, and then introduced into an expansion turbine to absorb the evaporated natural gas. An air liquefaction method using liquefied natural gas, characterized by comprising a step of expanding the gas as a power source for pressurizing the gas. 2. Air liquefaction using liquefied natural gas according to claim 1, characterized in that the natural gas pressurized above the critical pressure and heated is expanded by an expansion turbine consisting of multiple stages. Method. 3 In a method of liquefying air using liquefied natural gas, raw air is compressed with a compressor, pre-treated, and then introduced into a liquefied natural gas evaporator to supply liquefied natural gas in excess of the evaporation amount. The liquefied natural gas is cooled and expanded by the liquefied natural gas evaporator. The evaporated gas of the liquefied natural gas supplied above is pressurized and supplied to the consumer, and the surplus liquid is pressurized to a critical pressure or higher and heated, and then introduced into an expansion turbine, which generates power for pressurizing the evaporated natural gas. and a step of pressurizing separately supplied liquefied natural gas to a critical pressure or higher, heating it, introducing it into an expansion turbine, and expanding and supplying it as a power source for pressurizing the raw material air. An air liquefaction method using liquefied natural gas characterized by: 4 Utilizing the liquefied natural gas according to claim 3, wherein the separately supplied natural gas pressurized to the critical pressure or higher and heated is expanded by an expansion turbine consisting of multiple stages. air liquefaction method.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP5449579A JPS55146372A (en) | 1979-05-02 | 1979-05-02 | Method of liquefying air by liquefied natural gas |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP5449579A JPS55146372A (en) | 1979-05-02 | 1979-05-02 | Method of liquefying air by liquefied natural gas |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS55146372A JPS55146372A (en) | 1980-11-14 |
JPS6337308B2 true JPS6337308B2 (en) | 1988-07-25 |
Family
ID=12972209
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP5449579A Granted JPS55146372A (en) | 1979-05-02 | 1979-05-02 | Method of liquefying air by liquefied natural gas |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS55146372A (en) |
Families Citing this family (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS59180271A (en) * | 1983-03-31 | 1984-10-13 | 中部電力株式会社 | Air liquefying method utilizing cold heat of liquefied natural gas |
JP6087196B2 (en) * | 2012-12-28 | 2017-03-01 | レール・リキード−ソシエテ・アノニム・プール・レテュード・エ・レクスプロワタシオン・デ・プロセデ・ジョルジュ・クロード | Low temperature compressed gas or liquefied gas manufacturing apparatus and manufacturing method |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5216479A (en) * | 1975-07-30 | 1977-02-07 | Nippon Sanso Kk | Process for production of liquid air using chilling of liquefied natur al gas |
-
1979
- 1979-05-02 JP JP5449579A patent/JPS55146372A/en active Granted
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5216479A (en) * | 1975-07-30 | 1977-02-07 | Nippon Sanso Kk | Process for production of liquid air using chilling of liquefied natur al gas |
Also Published As
Publication number | Publication date |
---|---|
JPS55146372A (en) | 1980-11-14 |
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