JPS5855321B2 - Cooling water control device for condenser in power generation plant - Google Patents
Cooling water control device for condenser in power generation plantInfo
- Publication number
- JPS5855321B2 JPS5855321B2 JP1293779A JP1293779A JPS5855321B2 JP S5855321 B2 JPS5855321 B2 JP S5855321B2 JP 1293779 A JP1293779 A JP 1293779A JP 1293779 A JP1293779 A JP 1293779A JP S5855321 B2 JPS5855321 B2 JP S5855321B2
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- Prior art keywords
- vacuum
- cooling water
- increase
- condenser
- flow rate
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Description
【発明の詳細な説明】
本発明は火力、原子力等の発電プラントにおける復水器
の冷却水制御装置に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a cooling water control device for a condenser in a power plant such as a thermal power plant or a nuclear power plant.
火力、原子力発電プラントにおけるタービンの熱効率は
ボイラから発生する蒸気条件や復水器真空度、給水温度
、給水加熱段数などの熱サイクル条件、およびタービン
本体の性能によって決められる。The thermal efficiency of a turbine in a thermal or nuclear power plant is determined by the steam conditions generated from the boiler, the condenser vacuum degree, the feed water temperature, the heat cycle conditions such as the number of feed water heating stages, and the performance of the turbine itself.
中でも復水器真空度はタービンの効率に大きな影響を与
えることが知られている。In particular, it is known that the degree of vacuum in the condenser has a large effect on the efficiency of the turbine.
火力、原子力発電プラントでは、ボイラから発生した蒸
気はタービンに送られ、タービン内において膨張し、か
つ仕事をしたのち復水器に排気される。In thermal and nuclear power plants, steam generated from a boiler is sent to a turbine, expands within the turbine, performs work, and is then exhausted to a condenser.
この復水器は蒸気タービンの排気を冷却凝縮して復水す
ると共に、高度の真空状態を作って排圧を低めることに
より蒸気タービン中の熱落差を犬にし、タービンの出力
および効率を増進させる装置である。This condenser cools and condenses the steam turbine exhaust gas and condenses it, creating a high vacuum state and lowering the exhaust pressure to reduce the heat drop in the steam turbine, increasing the output and efficiency of the turbine. It is a device.
ここに、復水器の真空度は復水器に排気される排気量、
排気温度、復水器冷却水の温度と冷却水量、復水器の形
状ならびに冷却面積等によって変化することは周知の如
くである。Here, the degree of vacuum of the condenser is the amount of exhaust gas exhausted to the condenser,
It is well known that the temperature varies depending on the exhaust temperature, the temperature and amount of cooling water in the condenser, the shape of the condenser, the cooling area, etc.
そして復水器の最適真空度はタービンがその負荷に応じ
た最大効率運転となるように決められる。The optimum degree of vacuum in the condenser is determined so that the turbine operates at maximum efficiency according to its load.
次に従来の復水器真空度制御について説明する。Next, conventional condenser vacuum control will be explained.
第1図は復水器の冷却水系統図、第2図は従来の復水器
真空度制御装置の回路を示すブロック図である。FIG. 1 is a cooling water system diagram of a condenser, and FIG. 2 is a block diagram showing a circuit of a conventional condenser vacuum degree control device.
第1図において、取水口1の冷却水は、調節電動機3A
、3Bにより開度調節される循環水ポンプ2A、2Bに
よって必要流量が復水器5の水室4A、4Bに送給され
、復水器5における冷却管群(図示せず)を実線矢印方
向に通過する間に蒸気タービン6の排気と熱交換される
。In Fig. 1, the cooling water of the water intake 1 is supplied to the regulating motor 3A.
, 3B, the required flow rate is supplied to the water chambers 4A, 4B of the condenser 5 by the circulating water pumps 2A, 2B, whose openings are adjusted by the circulating water pumps 2A, 2B, and the cooling pipes (not shown) in the condenser 5 are moved in the direction of the solid line arrow. While passing through the exhaust gas of the steam turbine 6, heat is exchanged with the exhaust gas of the steam turbine 6.
温められた冷却水は排水として排水ロアから排出される
。The heated cooling water is discharged from the drainage lower as wastewater.
このような復水器冷却水系統における復水器の真空度制
御は復水器の冷却水量を調節することにより行なわれ、
冷却水の流量制御は第2図の最適真空度制御装置で行な
われる。The degree of vacuum in the condenser in such a condenser cooling water system is controlled by adjusting the amount of cooling water in the condenser.
The flow rate of cooling water is controlled by the optimum vacuum degree control device shown in FIG.
ところで、最適真空度は前述のようにタービン6の負荷
率によって決まり、一方、復水器真空度は蒸気タービン
の排気量、排気温度、復水器の冷却水量、冷却水温度、
復水器の形状ならびに冷却面積で決定される。By the way, as mentioned above, the optimum degree of vacuum is determined by the load factor of the turbine 6, while the degree of vacuum of the condenser is determined by the exhaust volume of the steam turbine, the exhaust temperature, the amount of cooling water in the condenser, the temperature of the cooling water,
It is determined by the shape of the condenser and the cooling area.
したがって最適真空度を得るための冷却水流量は蒸気タ
ービンの負荷率(排気量)に比例した発電機負荷と冷却
水温度により決まる。Therefore, the flow rate of cooling water to obtain the optimum degree of vacuum is determined by the generator load, which is proportional to the load factor (displacement amount) of the steam turbine, and the cooling water temperature.
その他のファクターは一定であるので係数として扱う。Since the other factors are constant, they are treated as coefficients.
流量調節にあたっては、負荷値G1と冷却水入口温度検
出器8による冷却水温度T1とが流量設定回路11に入
力され、設定回路11において最適真空度を得るための
復水器流量設定値Q1が算出される。When adjusting the flow rate, the load value G1 and the cooling water temperature T1 measured by the cooling water inlet temperature detector 8 are input to the flow rate setting circuit 11, and the condenser flow rate setting value Q1 for obtaining the optimum degree of vacuum is set in the setting circuit 11. Calculated.
この流量設定値Q1は復水器流量検出器9A。This flow rate set value Q1 is the condenser flow rate detector 9A.
9Bにより検出された復水器流量Q2A、Q2Bと加算
器12A、12Bにおいてそれぞれ比較される。The condenser flow rates Q2A and Q2B detected by 9B are compared in adders 12A and 12B, respectively.
その偏差値は電動機駆動回路13A、13Bに与えられ
、この入力によって調節電動機3A。The deviation value is given to motor drive circuits 13A and 13B, and this input drives the regulating motor 3A.
3Bが駆動され、そして循環ポンプ2A、2Bの開度調
節が行なわれて所要の復水器流量を得る。3B is driven, and the opening degrees of circulation pumps 2A and 2B are adjusted to obtain the required condenser flow rate.
さて、以上の復水器真空度制御方式では、真空度を最適
値とするために復水器流量すなわち循環ポンプ流量を調
節しているが、循環水ポンプが冷却水をくみ上けるのに
要するポンプ動力は非常に大きく、したがって最適質空
度を得てタービン効率を増したとしても逆にポンプ駆動
損失が増し、結果的には発電プラントの逆電端損失は増
えてしまうこととなる問題があった。Now, in the condenser vacuum level control method described above, the condenser flow rate, that is, the circulation pump flow rate, is adjusted in order to maintain the vacuum level at an optimal value. The pump power is very large, so even if the optimal air quality is achieved and the turbine efficiency is increased, the pump driving loss will increase, and as a result, the reverse terminal loss of the power generation plant will increase. there were.
そこで本発明は、発電プラントの送電端における利得を
向上するために復水器冷却水の流量を自動調節し、エネ
ルギーの有効活用を図った復水器の冷却水制御装置を提
供することを目的とする。SUMMARY OF THE INVENTION Therefore, an object of the present invention is to provide a condenser cooling water control device that automatically adjusts the flow rate of condenser cooling water in order to improve the gain at the power transmission end of a power generation plant and effectively utilizes energy. shall be.
以下本発明を図示する実施例によって説明する。The present invention will be explained below with reference to illustrative embodiments.
第3図は本発明による冷却水制御装置の一例を示すブロ
ック図である。FIG. 3 is a block diagram showing an example of a cooling water control device according to the present invention.
14は定格真空度設定器で、蒸気タービン運転上の定格
真空度Vac1を設定するためのものである。Reference numeral 14 denotes a rated vacuum degree setting device, which is used to set the rated vacuum degree Vac1 for steam turbine operation.
15は最適真空度算出回路で、発電機負荷検出器10に
より検出された負荷値G1が蒸気タービン6の排気量に
比例した信号として入力され、発電機負荷率に応じた最
適真空度値■ac2を算出する。Reference numeral 15 denotes an optimum degree of vacuum calculation circuit, into which the load value G1 detected by the generator load detector 10 is input as a signal proportional to the displacement of the steam turbine 6, and the optimum degree of vacuum value ac2 is calculated according to the generator load factor. Calculate.
以上のようにして得られた定格真空度Vac1(設定値
)と最適真空度値Vac1は加算器16に入力され、加
算器16において両値Vac1とVa c 2の差値V
ac3が算出され、この差値Vac3は蒸気タービン出
力増加分算出回路17に入力される。The rated vacuum degree Vac1 (setting value) and the optimum vacuum degree value Vac1 obtained as above are input to the adder 16, and the adder 16 calculates the difference value V between both values Vac1 and Va c 2.
ac3 is calculated, and this difference value Vac3 is input to the steam turbine output increase calculation circuit 17.
タービン出力増加分算出回路17には発電機負荷値G1
も入力されており、最適真空度の状態にて蒸気タービン
を運転した場合の蒸気タービンの出力増加分を電力値で
算出しPlを得る。The turbine output increase calculation circuit 17 has a generator load value G1.
is also input, and the increase in output of the steam turbine when the steam turbine is operated at the optimum degree of vacuum is calculated as a power value to obtain Pl.
一方、復水器冷却水取水口1の入口温度T1は温度検出
器8によって検出され、この入口温度Iと真空度差Va
c3とは冷却水増加分算出回路18に入力される。On the other hand, the inlet temperature T1 of the condenser cooling water intake 1 is detected by the temperature detector 8, and the difference between this inlet temperature I and the degree of vacuum Va
c3 is input to the cooling water increase calculation circuit 18.
そして、ここで最適真空度制御を行うために流すべき定
格真空度状態における冷却水量増加分Q3が算出され、
Q3は循環水ポンプ動力増加分算出回路19に出力され
る。Then, an increase in the amount of cooling water Q3 in the rated vacuum state that should be flowed in order to perform optimal vacuum control is calculated.
Q3 is output to the circulating water pump power increase calculation circuit 19.
また、循環水ポンプ動力増加分算出回路19には循環水
ポンプの開度値ηとポンプ揚程Mも入力され、最適真空
度制御を行うことによって生じた循環水ポンプの動力増
加分を電力値P2として算出回路19から出力される。Further, the opening value η and the pump head M of the circulating water pump are also input to the circuit 19 for calculating the increased power of the circulating water pump, and the increased power of the circulating water pump caused by performing the optimum vacuum degree control is calculated as the power value P2. is output from the calculation circuit 19 as .
この循環水ポンプ動力増加分電力値P2と蒸気タービン
効率増加分電力値P、とは加算器20に入力されて両値
の電力差P3が求められ、冷却水流量増加分算出回路2
1に入力される。The circulating water pump power increase power value P2 and the steam turbine efficiency increase power value P are input to an adder 20 to determine the power difference P3 between the two values, and the cooling water flow rate increase calculation circuit 2
1 is input.
この算出回路21には循環水ポンプの開度値ηとポンプ
揚程Mも入力されており、算出回路21は電力差P3が
正極性、つまり、ポンプ動力増加分電力値P2が効率増
加分電力値P1よりも高レベルであるときのみ損失電力
差P3に比例した補正冷却水流量Q4を出力する。The opening value η and the pump head M of the circulating water pump are also input to this calculation circuit 21, and the calculation circuit 21 calculates that the power difference P3 is positive polarity, that is, the pump power increase power value P2 is the efficiency increase power value Only when the level is higher than P1, a corrected cooling water flow rate Q4 proportional to the power loss difference P3 is output.
一方、最適真空度値Vac2と入力温度T1は最適真空
度制御必要冷却水流量算出回路22に入力され、算出回
路22において最適真空度制御をするための必要冷却水
流量Q5が算出される。On the other hand, the optimum degree of vacuum value Vac2 and the input temperature T1 are input to the optimum vacuum degree control required cooling water flow rate calculation circuit 22, and the calculation circuit 22 calculates the necessary cooling water flow rate Q5 for optimum vacuum degree control.
そして、必要冷却水流量Q、から補正冷却水流量Q4が
差し引かれ、総合冷却水量設定値Q1が求められる。Then, the corrected cooling water flow rate Q4 is subtracted from the required cooling water flow rate Q, and the total cooling water amount setting value Q1 is determined.
このQ1以降の制御系は従来行なわれている循環水ポン
プの流量制御系と同様であるので省略する。The control system after Q1 is the same as the conventional flow rate control system of a circulating water pump, and will therefore be omitted.
ところで、復水器の定格真空度Vaclは蒸気タービン
運用上の制限値として復水器冷却水温度変動、およびタ
ービンの負荷率の平均値等により決められる。Incidentally, the rated vacuum degree Vacl of the condenser is determined as a limit value for steam turbine operation based on condenser cooling water temperature fluctuations, the average value of the turbine load factor, and the like.
一方、タービンの最適効率を得るための最適真空度は、
タービン負荷率(タービン排気量)、排気温度、復水器
冷却面積、復水器冷却水量(循環水ポンプ流量)および
その温度等によって決まることは先にも述べた通りであ
る。On the other hand, the optimum degree of vacuum to obtain the optimum efficiency of the turbine is
As mentioned above, it is determined by the turbine load factor (turbine displacement), exhaust temperature, condenser cooling area, condenser cooling water amount (circulating water pump flow rate), its temperature, etc.
この中で排気温度は、一般に、一定温度とされており、
また復水器5の冷却面積も固定値である。Among these, the exhaust temperature is generally considered to be a constant temperature,
Furthermore, the cooling area of the condenser 5 is also a fixed value.
さらにタービン負荷率すなわらタービン排気量は排気温
度が一定なので発電機負荷に比例した値となる。Furthermore, since the exhaust gas temperature is constant, the turbine load factor, ie, the turbine displacement, has a value proportional to the generator load.
したがって最適真空度Vac2を得る復水器冷却水流量
は発電機負荷と冷却水温度の変数とその他の固定係数に
よって求められることは明らかである。Therefore, it is clear that the condenser cooling water flow rate to obtain the optimum degree of vacuum Vac2 is determined by the generator load, cooling water temperature variables, and other fixed coefficients.
かくして、第3図の最適真空度算出回路15は発電機負
荷G1を入力として最適真空度Va C2を得、そして
このVac2が最適真空度制御必要冷却水流量算出回路
22に入力されて、最適真空度制御をするための冷却水
量すなわち循環水ポンプ流量Q、か得られる。In this way, the optimum degree of vacuum calculation circuit 15 in FIG. The amount of cooling water for temperature control, that is, the circulating water pump flow rate Q, can be obtained.
一方、定格真空度Vq c 1と最適真空度Vac2と
の差Vac3は蒸気タービン出力増加分算出回路17に
入力され最適真空度制御することによって蒸気タービン
の効率と定格真空度下における蒸気タービン効率差とそ
のときの発電機負荷G1に応じて効率向上による発電々
力の増加分P1が得られる。On the other hand, the difference Vac3 between the rated vacuum degree Vq c 1 and the optimum vacuum degree Vac2 is input to the steam turbine output increase calculation circuit 17, and by controlling the optimum vacuum degree, the difference between the efficiency of the steam turbine and the steam turbine efficiency under the rated vacuum degree is calculated. According to the generator load G1 at that time, an increase P1 in generated power due to efficiency improvement is obtained.
さらに真空差Vac3と冷却水温度T1は冷却水流量増
加分算出回路18に入力され、最適真空度制御するため
に流す冷却水量の定格真空度制御時からの増加分Q3が
算出され、このQ3は循環水ポンプ動力増加分算出回路
19に入力され、そのときの循環水ポンプの開度値ηと
揚程Mから増加流量Qを流すために必要な循環水ポンプ
の動力増加分P2が得られる。Furthermore, the vacuum difference Vac3 and the cooling water temperature T1 are input to the cooling water flow rate increase calculation circuit 18, and the increase Q3 of the cooling water flow rate from the rated vacuum level control to achieve the optimum vacuum level control is calculated. It is input to the circulating water pump power increase calculation circuit 19, and the circulating water pump power increase P2 required to flow the increased flow rate Q is obtained from the opening value η and head M of the circulating water pump at that time.
そして効率向上による利得電力P1とポンプ動力増加(
損失電力) P2との差P3が加算器20により得られ
、この電力差P3は冷却水流量増加分算出回路21に入
力され、そのときの循環水ポンプの開度価ηと揚程Mか
ら補正冷却水流量Q4が得られる。Then, gain power P1 and pump power increase due to efficiency improvement (
The difference P3 from P2 (power loss) is obtained by the adder 20, and this power difference P3 is input to the cooling water flow increase calculation circuit 21, and the corrected cooling is calculated from the opening value η and head M of the circulating water pump at that time. A water flow rate Q4 is obtained.
なお流量Q4は利得電力P1よりも損失電力P2の方が
高いときのみ信号を出力するものであり、利得電力P1
が損失電力P2より高いときには零となっている。Note that the flow rate Q4 outputs a signal only when the loss power P2 is higher than the gain power P1.
When is higher than the power loss P2, it becomes zero.
そして、最適真空度制御に必要な流量Q5から補正冷却
水流量を加算器23により差し引きQlを得て循環水ポ
ンプの流量設定とする。Then, the corrected cooling water flow rate is subtracted by the adder 23 from the flow rate Q5 necessary for optimum vacuum degree control to obtain Ql, which is used as the flow rate setting of the circulating water pump.
以上Q)実施例では蒸気タービン排気量を発電機負荷か
ら得ているが、タービンの蒸気排出点に流量検出器をお
き、負荷の代わりに蒸気流量を入力しても同等の効果を
得ることができる。Above Q) In the example, the steam turbine displacement is obtained from the generator load, but it is possible to obtain the same effect by placing a flow rate detector at the steam exhaust point of the turbine and inputting the steam flow rate instead of the load. can.
以上の通り本発明によれば、最適真空度制御を行うこと
によって得られるタービン熱効率の向上による出力増加
分(電力利得外)と、同最適真空度制御によって生ずる
循環水ポンプの動力増加分(電力損失分)とを比較し、
発電プラントの送電端出力が常に正の利得を生ずるよう
に循環ポンプの流量制御が行なわれることとなるので、
発電プラントの送電端における電力が最大効率で出力さ
れ、エネルギーの有効活用を戊しうるものである。As described above, according to the present invention, the output increase (outside of power gain) due to the improvement in turbine thermal efficiency obtained by performing optimal vacuum degree control and the power increase of the circulating water pump (power loss),
Since the flow rate of the circulation pump is controlled so that the power output of the power generation plant always produces a positive gain,
Electric power at the transmission end of the power generation plant is output with maximum efficiency, and energy can be used more effectively.
第1図は復水器の冷却水系統図、第2図は従来の復水器
最適真空度制御装置のブロック図、第3図は本発明によ
る復水器冷却水制御装置の一実施例を示すブロック図で
ある。
1・・・・・・取水口、2A、2B・・・・・・循環ポ
ンプ、3A、3B・・・・・・循環ポンプ調節用電動機
、4A。
4B・・・・・・復水器小室、5・・・・・・復水器、
6・・・・・・蒸気タービン、7・・・・・・排水口、
8・・・・・・冷却水入口温度検出器、9A、9B・・
・・・・復水器入口冷却水量検出器、10・・・・・・
発電機負荷検出器、11・・・・・・流量設定回路、1
2A、12B・・・・・・加算器、13A。
13B・・・・・・電動機駆動回路、140.198.
定格真空度設定器、15・・・・・・最適真空度算出回
路、16・・・・・・加算器、11・・・・・・タービ
ン出力増加分算出回路、18・・・・・・冷却水流量増
加分算出回路、19・・・・・・ポンプ動力増加分算出
回路、20・・・・・・冷却水流量増加分算出回路、2
1・・・・・・最適真空度制御用冷却水量算出回路、V
ac、・・・・・・定格真空度、Vac2・・・・・・
最適真空度、Vac3・・・・・・真空度差、Pl・・
・・・・利得電力、P2・・・・・・損失電力、P3・
・・・・・電力差、T、・・・・・冷却水取水口入口温
度、Q、〜Q5・・・・・・冷却水流量値。Fig. 1 is a condenser cooling water system diagram, Fig. 2 is a block diagram of a conventional condenser optimum vacuum level control device, and Fig. 3 is an embodiment of a condenser cooling water control device according to the present invention. FIG. 1...Water intake, 2A, 2B...Circulation pump, 3A, 3B...Circulation pump adjustment electric motor, 4A. 4B... Condenser chamber, 5... Condenser,
6...Steam turbine, 7...Drain port,
8...Cooling water inlet temperature detector, 9A, 9B...
...Condenser inlet cooling water amount detector, 10...
Generator load detector, 11...Flow rate setting circuit, 1
2A, 12B...Adder, 13A. 13B...Motor drive circuit, 140.198.
Rated vacuum degree setting device, 15... Optimal degree of vacuum calculation circuit, 16... Adder, 11... Turbine output increase calculation circuit, 18... Cooling water flow rate increase calculation circuit, 19... Pump power increase calculation circuit, 20... Cooling water flow rate increase calculation circuit, 2
1... Cooling water amount calculation circuit for optimal vacuum degree control, V
ac,... Rated vacuum degree, Vac2...
Optimal degree of vacuum, Vac3... Difference in degree of vacuum, Pl...
... Gain power, P2 ... Loss power, P3.
...Power difference, T, ...Cooling water intake inlet temperature, Q, ~Q5...Cooling water flow rate value.
Claims (1)
却水制御装置において、復水器の定格真空度を設定する
定格真空度設定器、タービンの排気量に比例した信号を
入力としてタービン運転上の最適な真空度を算出する最
適真空度算出回路、前記定格真空度と最適真空度との偏
差を求める加算器、求められた真空度偏差に基づいてタ
ービンの熱効率向上に伴なうタービン出力の増加分を算
出するタービン出力増加分算出回路、前記真空度偏差に
基づいて真空度調節に伴なう復水器冷却水の循環ポンプ
動力の増加分を算出するポンプ動力増加分算出回路、前
記タービン出力増加分とポンプ動力増加分との偏差を求
めポンプ動力増加分がタービン山分増加分より高いとき
のみ出力する加算器、その増加分偏差に基づいて補正す
べき冷却水流量の流量増加分を算出する冷却水流量増加
分算出回路、この補正冷却水流量増加分を最適真空度調
節に必要な冷却水流量力)ら差し引いて総合冷却水流量
調節信号を出力する加算器、を備えた発電プラントにお
ける復水器の冷却水制御装置。1 In a cooling water control system for a condenser in a thermal or nuclear power plant, the rated vacuum setting device sets the rated vacuum of the condenser, and a signal proportional to the turbine displacement is input to determine the optimum level for turbine operation. An optimum degree of vacuum calculation circuit that calculates the degree of vacuum, an adder that calculates the deviation between the rated degree of vacuum and the optimum degree of vacuum, and an increase in turbine output due to improvement in thermal efficiency of the turbine based on the obtained degree of vacuum deviation. A circuit for calculating an increase in turbine output; a circuit for calculating an increase in pump power for circulating condenser cooling water due to vacuum adjustment based on the vacuum degree deviation; An adder that calculates the deviation between the increase in pump power and the increase in pump power and outputs only when the increase in pump power is higher than the increase in turbine peak, and a cooling function that calculates the increase in cooling water flow rate to be corrected based on the increase deviation. Condensing water in a power generation plant equipped with a water flow rate increase calculation circuit, an adder that subtracts this corrected cooling water flow rate increase from the cooling water flow rate required for optimal vacuum adjustment and outputs a comprehensive cooling water flow rate adjustment signal. Cooling water control device for the vessel.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1293779A JPS5855321B2 (en) | 1979-02-07 | 1979-02-07 | Cooling water control device for condenser in power generation plant |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1293779A JPS5855321B2 (en) | 1979-02-07 | 1979-02-07 | Cooling water control device for condenser in power generation plant |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS55107009A JPS55107009A (en) | 1980-08-16 |
| JPS5855321B2 true JPS5855321B2 (en) | 1983-12-09 |
Family
ID=11819188
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP1293779A Expired JPS5855321B2 (en) | 1979-02-07 | 1979-02-07 | Cooling water control device for condenser in power generation plant |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5855321B2 (en) |
-
1979
- 1979-02-07 JP JP1293779A patent/JPS5855321B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS55107009A (en) | 1980-08-16 |
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