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JPS6228395B2 - - Google Patents
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JPS6228395B2 - - Google Patents

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Publication number
JPS6228395B2
JPS6228395B2 JP12110180A JP12110180A JPS6228395B2 JP S6228395 B2 JPS6228395 B2 JP S6228395B2 JP 12110180 A JP12110180 A JP 12110180A JP 12110180 A JP12110180 A JP 12110180A JP S6228395 B2 JPS6228395 B2 JP S6228395B2
Authority
JP
Japan
Prior art keywords
heat exchanger
flow rate
feed water
temperature
water heater
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
Application number
JP12110180A
Other languages
Japanese (ja)
Other versions
JPS5747199A (en
Inventor
Seiitsu Nikawara
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Hitachi Ltd
Original Assignee
Hitachi Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP12110180A priority Critical patent/JPS5747199A/en
Publication of JPS5747199A publication Critical patent/JPS5747199A/en
Publication of JPS6228395B2 publication Critical patent/JPS6228395B2/ja
Granted legal-status Critical Current

Links

Description

【発明の詳細な説明】 本発明は発電プラント等の熱サイクルで構成さ
れるプラントにおける熱交換器の異常を早期に検
出し、診断する熱交換器の診断装置に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a heat exchanger diagnostic device for early detecting and diagnosing an abnormality in a heat exchanger in a power generation plant or other plant configured with a thermal cycle.

本発明は火力発電プラントに例をとつて以下に
説明する。
The present invention will be explained below by taking a thermal power plant as an example.

従来、火力発電所におけるタービン,ボイラ,
発電機および各種補機については温度,圧力,流
量,水位,電圧,電流などのようなプラント状態
量が、機器として許容される制限値内にあるか否
かを常時監視し、制限値を逸脱した時、即警報を
発して異常を予告しているが、この警報制限値は
機器損傷を防止することを目的としているため、
制限値そのものにかなり余裕を与えており、この
ため警報が発せられてもかならずしも機器異常と
は限らない。
Traditionally, turbines, boilers,
For generators and various auxiliary equipment, plant state variables such as temperature, pressure, flow rate, water level, voltage, current, etc. are constantly monitored to see if they are within the limit values allowed for the equipment, and to check for deviations from the limit values. When this occurs, an immediate alarm is issued to warn of the abnormality, but this alarm limit value is intended to prevent equipment damage.
A considerable margin is given to the limit value itself, so even if an alarm is issued, it does not necessarily mean that the device is abnormal.

この様に従来の警報監視は異常状態に近づいて
いることに主眼をおいているため、正確に異常を
キヤツチすることがむずかしく、また異常の原因
分析をする機能に欠けているため、正確な異常の
内容を把握できず、このため、無用なプラント操
作を行う可能性があつた。例えば熱交換器の一例
である高圧給水加熱器及び低圧水加熱器について
みると、器内水位高(あるいは低)の警報が用意
されているだけで、加熱器チユーブの漏洩や性能
劣化などについて監視されていない。
In this way, conventional alarm monitoring focuses on approaching an abnormal state, which makes it difficult to accurately catch an abnormality, and lacks the ability to analyze the cause of an abnormality. Therefore, there was a possibility that unnecessary plant operations could be performed. For example, if we look at high-pressure feed water heaters and low-pressure water heaters, which are examples of heat exchangers, only alarms are provided for high (or low) water levels in the vessel, and monitoring is performed to check for leaks or performance deterioration in the heater tube. It has not been.

本発明の目的は熱力学の第2法則(一つの熱源
からの熱を温度の降下なく、また他になんら変化
を及ぼすことなく継続して仕事にかえる運動は不
可能である)を応用して熱交換器の各部の熱損失
を算出し、その熱損失の分布状況から異常を診断
することを特徴とする熱交換器の診断装置を提供
するにある。
The purpose of the present invention is to apply the second law of thermodynamics (it is impossible to continuously convert heat from one heat source into work without a drop in temperature or any other change). It is an object of the present invention to provide a diagnostic device for a heat exchanger, which is characterized in that it calculates the heat loss of each part of the heat exchanger and diagnoses an abnormality from the distribution of the heat loss.

本発明の熱交換器の診断装置は第10図に図示
されているが、これを説明する前に、第1図を用
いて火力発電プラントのスケルトンを説明する。
第1図において、ボイラ1で発生した蒸気は主蒸
気管18を通つて高圧タービン2に入り、ここで
蒸気の熱エネルギーの一部は発電機4をまわすた
めの回転機械エネルギーに変換される。高圧ター
ビン2で仕事をした蒸気は低温再熱蒸気管19を
通り、再熱器16で再び加熱され、高温再熱蒸気
管20を通つて再熱タービン3に導かれ、再び仕
事をする。再熱タービン3で仕事をした蒸気は排
気として復水器5に入り、海水等の冷却水(図示
せず)によつて冷却されて水に復する。この復水
は復水ポンプ6によりポンプアツプされ、復水熱
交換器7、空気抽出器8およびグランドコンデン
サ9の各熱交換器を通つて熱回収を行い、低圧給
水加熱器10,脱気器11で復水の温度を上げ、
ボイラ給水ポンプ12で昇圧された給水は高圧給
水加熱器13で更に給水の温度を上げて主給水管
21を通つてボイラ1に給水される。高圧給水加
熱器13,脱気器11および低圧給水加熱器10
はいずれもタービンの抽出で加熱されるものであ
り、これらもまた熱交換器である。またボイラは
燃料調整弁17でコントロールされた燃料が燃料
バーナ14を通り火炉内で燃焼する。給水はこの
燃焼による熱を受けて蒸気となり、過熱器15で
過熱されタービン2に送られる。このようなプラ
ントにおいて、プラントが正常な状態で運転され
ている場合の各部の状態量を示したのが第2図で
ある。第2図では、第1図で省略されたものも一
部示されている。例えば、3′,3″は夫々中圧タ
ービン、低圧タービン、21はドレンクーラ、2
2はドレンポンプ、23はブースタポンプ、24
は給水ポンプ用タービン、25は重油加熱器、2
6は空気加熱器、27はS.S.R(スチームシール
レギユレータである。第2図は500MWを発電し
ているプラントの正常状態を示したもので、ボイ
ラ,タービン,補機等の各部における温度(1
゜:℃),圧力(P:Kg/cm2),流量(G:Kg/
Hr)およびエンタルピ(H:Kcal/Kg)が示さ
れている。ここで示されている状態量はエンタル
ピを別にすれば容易に計測できるものである。以
上の如き火力発電プラントにおける熱交換器の代
表例として第2図の熱平衡線図に示す最終段の高
圧給水加熱器13について診断を行なう場合の本
発明の考え方について以下説明する。
The heat exchanger diagnostic device of the present invention is illustrated in FIG. 10, but before explaining this, the skeleton of a thermal power plant will be explained using FIG. 1.
In FIG. 1, steam generated in a boiler 1 passes through a main steam pipe 18 and enters a high-pressure turbine 2, where a portion of the thermal energy of the steam is converted into rotary mechanical energy for turning a generator 4. The steam that has done work in the high-pressure turbine 2 passes through a low-temperature reheat steam pipe 19, is heated again in a reheater 16, is led to a reheat turbine 3 through a high-temperature reheat steam pipe 20, and does work again. The steam that has done work in the reheat turbine 3 enters the condenser 5 as exhaust gas, is cooled by cooling water (not shown) such as seawater, and is returned to water. This condensate is pumped up by a condensate pump 6, passes through each heat exchanger of a condensate heat exchanger 7, an air extractor 8, and a gland condenser 9, and recovers heat. Raise the temperature of the condensate with
The feed water whose pressure has been increased by the boiler feed water pump 12 is further raised in temperature by the high pressure feed water heater 13 and is then supplied to the boiler 1 through the main water supply pipe 21. High pressure feed water heater 13, deaerator 11 and low pressure feed water heater 10
Both are heated by the extraction of the turbine and are also heat exchangers. Further, in the boiler, fuel controlled by a fuel regulating valve 17 passes through a fuel burner 14 and is burned in a furnace. The feed water receives heat from this combustion and becomes steam, which is superheated in the superheater 15 and sent to the turbine 2. FIG. 2 shows the state quantities of each part in such a plant when the plant is operating under normal conditions. In FIG. 2, some parts omitted in FIG. 1 are also shown. For example, 3' and 3'' are an intermediate pressure turbine and a low pressure turbine, respectively, 21 is a drain cooler, and 2
2 is a drain pump, 23 is a booster pump, 24
2 is a water pump turbine, 25 is a heavy oil heater, 2
6 is an air heater, and 27 is an SSR (steam seal regulator). Figure 2 shows the normal state of a plant generating 500 MW, and shows the temperature ( 1
°: °C), pressure (P: Kg/cm 2 ), flow rate (G: Kg/
Hr) and enthalpy (H: Kcal/Kg) are shown. The state quantities shown here can be easily measured apart from enthalpy. The concept of the present invention when diagnosing the final stage high-pressure feed water heater 13 shown in the heat balance diagram of FIG. 2 as a typical example of a heat exchanger in a thermal power plant as described above will be explained below.

本発明の一実施例を示す第10図において、ブ
ロツク101は正常状態でのエネルギー損失(△
Q)を求める回路であり、以下△Qを求める考え
方を説明する。
In FIG. 10, which shows an embodiment of the present invention, a block 101 represents energy loss (△
This circuit calculates Q), and the concept of calculating ΔQ will be explained below.

まず、第3図は第2図の最終段の高圧給水加熱
器13まわりの状態量をぬき出したものである。
すなわち第3図の給水加熱器13において、加熱
器の加熱蒸気の圧力は73.2Kg/cm2、温度363.5
℃であり、この蒸気のエンタルピを上記検出した
温度,圧力を用いて蒸気表から求めると
728.8Kcal/Kgとなる。加熱蒸気のドレンの圧
力は加熱器々内圧力とほぼ同じで69.6Kg/cm2、温
度は260.6℃であり、このドレンのエンタルピを
蒸気表から求めると271.6Kcal/Kgとなる。加熱
器への給水の温度は255.0℃で圧力は給水ポン
プ出口から押出されるため、ここでは289.9Kg/
cm2である。加熱器出口給水は温度285.2℃、圧
力はほぼ入口給水圧力に等しい。との所の給
水エンチルピは蒸気表からそれぞれ265.3Kcal/
Kg,299.7Kcal/Kgとなる。加熱器々内は圧力
69.6Kg/cm2で、内部は飽和水であるため温度は蒸
気表から求められ、284.1℃となる。
First, FIG. 3 shows the state quantities around the high-pressure feed water heater 13 at the final stage in FIG. 2.
That is, in the feed water heater 13 shown in Fig. 3, the pressure of the heating steam of the heater is 73.2 Kg/cm 2 and the temperature is 363.5.
℃, and the enthalpy of this steam is calculated from the steam table using the temperature and pressure detected above.
It becomes 728.8Kcal/Kg. The pressure of the heated steam drain is approximately the same as the pressure inside the heaters, 69.6 Kg/cm 2 , and the temperature is 260.6°C, and the enthalpy of this drain is found to be 271.6 Kcal/Kg from the steam table. The temperature of the water supplied to the heater is 255.0℃ and the pressure is pushed out from the water supply pump outlet, so here it is 289.9Kg/
cm2 . The temperature of the heater outlet water supply is 285.2°C, and the pressure is approximately equal to the inlet water supply pressure. The water enthylpi at the place is 265.3Kcal/each from the steam table.
Kg, 299.7Kcal/Kg. Pressure inside the heaters
Since the temperature is 69.6Kg/cm 2 and the interior is saturated water, the temperature can be found from the steam table and is 284.1℃.

このように第3図において各点で計測された圧
力,温度から蒸気表によりエンタルピ(あるいは
温度)が容易に求められるので、別に計測された
給水流量1612676Kg/Hrをもとに下記式により容
易に加熱蒸気の流量Gsが求められる。
In this way, the enthalpy (or temperature) can be easily determined from the steam table from the pressure and temperature measured at each point in Figure 3, so it can be easily calculated using the following formula based on the separately measured water supply flow rate of 1612676 Kg/Hr. The flow rate Gs of heating steam is determined.

加熱蒸気流量Gs=給水流量×(出口給水エンタルピ−入口給水エンタピ)/(加熱蒸気エンタルピ−ドレンエン
タルピ) =1612676×(299.7−265.3)/(728.8−271.6)=121339Kg/Hr
…(1) (1)式は公知のバランス式である。第4図は第3
図に示す給水加熱器における温度変化の様子を線
図で表わしたもので、図中の番号は第3図のそれ
に対応しており、給水加熱器内の水,蒸気の温度
分布が良くわかる。
Heating steam flow rate Gs = Feed water flow rate x (Outlet feed water enthalpy - Inlet feed water enthalpy) / (Heating steam enthalpy - Drain enthalpy) = 1612676 x (299.7 - 265.3) / (728.8 - 271.6) = 121339 Kg /Hr
...(1) Equation (1) is a known balance equation. Figure 4 is the third
This is a diagram showing the state of temperature change in the feed water heater shown in the figure.The numbers in the figure correspond to those in Figure 3, and the temperature distribution of water and steam in the feed water heater can be clearly understood.

一方、第3図における給水加熱器13まわりの
状態の別の見方をしたのが第5図である。すなわ
ち第3図において計測されたと同じ圧力,温度か
らそのエントロピを蒸気表から求めたものを第5
図の( )内に示してある。本発明は熱力学の第
2法則(一つの熱源からの熱を温度の降下なく、
また他になんら変化を及ぼすことなく継続して仕
事にかえる運動は不可能である)に着目したもの
であり、これは別の見方をすると、他のなんらの
変化を及ぼすことなく熱交換をすることは不可能
ということである。従つて第5図における給水加
熱器での熱交換においても、エネルギ損失なく熱
交換は出来ないことになる。
On the other hand, FIG. 5 shows a different view of the state around the feed water heater 13 in FIG. 3. In other words, the entropy obtained from the steam table from the same pressure and temperature as measured in Figure 3 is shown in Figure 5.
It is shown in parentheses in the figure. The present invention is based on the second law of thermodynamics, which allows heat from a single heat source to be
In addition, it is impossible to continuously convert movement into work without causing any other changes.) From another perspective, this focuses on the fact that heat exchange without causing any other changes is impossible. That is impossible. Therefore, even in the heat exchange using the feed water heater shown in FIG. 5, heat exchange cannot be performed without energy loss.

第10図のブロツク101の出力である給水加
熱器13の熱交換でのエネルギ損失△Qは下記式
で求めることができる。
The energy loss ΔQ in heat exchange of the feed water heater 13, which is the output of block 101 in FIG. 10, can be determined by the following formula.

エネルギ損失△Q={(Gs×Ts−Gw×Tw)} ×(to+273.16)/K(Kcal/KW
)…(2) ここで Gs:加熱蒸気流量(Kg/Hr) Gw:給水流量(Kg/Hr) Ts:加熱流体のエントロピ(Kcal/
Kg〓) Tw:給水のエントロピ(Kcal/〓) KW:発電機出力(KW) to:ベースとなる温度(第2図では復
水器出口給水温度33.1℃) (2)式をもとに第5図における給水加熱器13で
の熱交換によるエネルギ損失(△Q)を求めると
下記のようになる。
Energy loss △Q={(Gs×Ts−Gw×Tw)}×(to+273.16)/K W (Kcal/K W H
)…(2) Here, Gs: Heating steam flow rate (Kg/Hr) Gw: Feed water flow rate (Kg/Hr) Ts: Heating fluid entropy (Kcal/Hr)
Kg〓) Tw: Entropy of feed water (Kcal/〓) KW : Generator output ( KW ) to: Base temperature (in Fig. 2, the condenser outlet feed water temperature is 33.1°C) Based on equation (2) The energy loss (ΔQ) due to heat exchange in the feed water heater 13 in FIG. 5 is calculated as follows.

△Q={121339×(0.68898−1.5001) +1612676×(0.72837−0.6650)} ×(33.1+273.16)/500000 ≒2.31(Kcal/KWH) ……(3) ここで求めたエネルギ損失△Q=2.31Kcal/K
WHは給水加熱器13が正常な状態であつても、
熱交換動作において発生する損失エネルギであ
る。
△Q={121339×(0.68898-1.5001) + 1612676×(0.72837-0.6650)} Q=2.31Kcal/K
Even if the feed water heater 13 is in a normal state,
This is the energy loss that occurs during heat exchange operations.

第10図ブロツク101は各負荷(給水流量)
のときのエネルギ損失△Qを出力するものであ
る。ブロツク100の出力はエネルギ損失の基準
となるものであり、実際のエネルギ損失がこれと
相違すれば何らかの異常が発生したものと判断で
きる。これらの異常のうち、給水管に穴があき、
給水側(高圧)から蒸気あるいはドレン側(低
圧)に給水の漏えいが発生した場合、給水加熱器
出入口の温度特性が正常状態に対してどのように
変化するかを第7図に示した。
Block 101 in Figure 10 shows each load (water supply flow rate)
It outputs the energy loss ΔQ when . The output of block 100 serves as a reference for energy loss, and if the actual energy loss differs from this, it can be determined that some abnormality has occurred. Among these abnormalities, there is a hole in the water supply pipe;
Figure 7 shows how the temperature characteristics at the inlet and outlet of the feed water heater change compared to normal conditions when a leak of feed water occurs from the water supply side (high pressure) to the steam or drain side (low pressure).

第7図aは給水加熱器入口側給水管で漏えいが
発生した場合であり、第7図bは途中の給水管で
漏えいした場合、第7図cは出口側給水管で漏え
いが発生した場合のそれぞれにおいて、正常状態
(実線)からの変化を点線で示した。
Figure 7a shows a case where a leak occurs in the water supply pipe on the inlet side of the feed water heater, Figure 7b shows a case in which a leak occurs in an intermediate water supply pipe, and Figure 7c shows a case in which a leak occurs in an outlet side water supply pipe. In each case, the change from the normal state (solid line) is indicated by a dotted line.

ここで第7図cの場合を例にとつて、熱交換時
のエネルギ損失(△Q)を求めてみる。第3図に
示す状態において、給水加熱器出口部において
20000Kg/Hrの漏えいが発生するとドレン温度は
おおよそ264.1℃に上がるが、事前の温度が260.6
℃のため温度による検出は困難である。
Here, taking the case of FIG. 7c as an example, the energy loss (ΔQ) during heat exchange will be determined. In the state shown in Figure 3, at the outlet of the feed water heater
If a leak of 20000Kg/Hr occurs, the drain temperature will rise to approximately 264.1℃, but the pre-temperature is 260.6℃.
℃, making detection by temperature difficult.

(121339×260.6+20000×285.2
/(121339+20000)≒264.1℃) この時の状態値は第8図に示すようになる。こ
こでエンタルピ,エントルピは蒸気表から求めら
れ夫々( )内に示すような値となる。第8図の
ような状態において給水加熱器出口側給水管から
の漏えい水が20000Kg/Hrであることがわかつて
いるとして、熱交換時のエネルギ損失(△QLEA
)を第8図をもとに(2)式,(3)式の考え方により
計算すると次のようになる。
(121339×260.6+20000×285.2
/(121339+20000)≒264.1°C) The state values at this time are as shown in FIG. Here, enthalpy and entropy are obtained from the steam table and have the values shown in parentheses. Assuming that it is known that the leakage water from the water supply pipe on the outlet side of the feedwater heater is 20000Kg/Hr under the condition shown in Figure 8, the energy loss during heat exchange (△Q LEA
When K ) is calculated based on Figure 8 and using equations (2) and (3), the result is as follows.

△QLEAK={(1592676×0.72837−1612676 ×0.6650+(141339×0.69678 −121339×1.5001)}×(33.1+273.1
6)/500000 ≒2.50(Kcal/KWH) …(4) この△QLEAKは給水加熱器が正常状態で熱交換
している場合のエネルギ損失△Q(=2.31Kcal/
WH)に比べ相対的に大きくなつており、これ
は給水管からの漏えいによる損失分が増えたため
であり、異常傾向がよくわかる。
△Q LEAK = {(1592676×0.72837−1612676×0.6650+(141339×0.69678 −121339×1.5001)}×(33.1+273.1
6)/500000 ≒2.50 (Kcal/K W H) …(4) This △Q LEAK is the energy loss △Q (=2.31Kcal/
This is relatively large compared to K W H), and this is due to an increase in the loss due to leakage from the water supply pipes, and the abnormal trend can be clearly seen.

しかしここに示した△QLEAKは理論的に計算し
たものであり、実際問題としては、給水加熱器に
おける給水管からの漏えい量20000Kg/Hrを外部
で直接検出することがむずかしい。ちなみに、
20000Kg/Hrは、給水量の1.24%にしかあたらな
いため、計測誤差にかくれてしまい、測定器での
検出も困難である。このため漏えいが20000Kg/
Hrあつても給水加熱器まわりの計算される状態
量は第9図のようになる。
However, the ΔQ LEAK shown here is calculated theoretically, and as a practical matter, it is difficult to directly detect the leakage amount of 20,000 Kg/Hr from the water supply pipe in the feed water heater externally. By the way,
Since 20,000Kg/Hr corresponds to only 1.24% of the water supply amount, it is hidden by measurement errors and is difficult to detect with measuring instruments. As a result, leakage amounted to 20,000Kg/
Even if Hr exists, the calculated state quantities around the feed water heater will be as shown in Figure 9.

本発明では、漏えい量は検出できないが、ドレ
ン流量GDは検出可能であり、これは漏えい量を
も含む情報であることに着目した。ドレン流量G
Dは実測可能であるが、それ以外にも第9図にお
いて給水加熱器ドレンは流量調整弁100により
調整されていることから、この流量調整弁の開度
(Vp)、前後差圧(△P)から調整弁を通るドレ
ン流量(GD)を下記式により求めることも出来
る。
In the present invention, although the amount of leakage cannot be detected, the drain flow rate G D can be detected, and attention has been paid to the fact that this is information that includes the amount of leakage. Drain flow rate G
D can be measured, but in addition to that, the feedwater heater drain is regulated by the flow rate regulating valve 100 in Fig. 9, so the opening degree (Vp) of this flow rate regulating valve, the differential pressure across the front and back (△P ), the drain flow rate (G D ) passing through the regulating valve can also be determined by the following formula.

D=f(Vp,△P) …(5) ここで流量調整弁の開度(Vp)及び弁の前後
差圧△Pは容易に測定できる。
G D =f(Vp, △P)...(5) Here, the opening degree (Vp) of the flow rate adjustment valve and the differential pressure △P across the valve can be easily measured.

第9図においてドレン流量が上記(5)式から
125000Kg/Hrと検出された(実際には第8図の
ように121339+20000Kg/Hr)とした場合、この
時の熱交換時エネルギ損失(△QLEAK″)を求め
ると △QLEAK″={1612676×(0.72837−0.6650) +125000×(0.69678−1.5001)} ×(33.1+273.16/50000
0) ≒1.90(Kcal/KWH) …(6) 但し、(6)式は漏えい量が不明のため給水加熱器
の出口給水流量は入口と同じとしている。
In Figure 9, the drain flow rate is calculated from equation (5) above.
If 125000Kg/Hr is detected (actually 121339 + 20000Kg/Hr as shown in Figure 8), the energy loss during heat exchange (△Q LEAK ″) at this time is calculated as △Q LEAK ″ = {1612676× (0.72837−0.6650) +125000×(0.69678−1.5001)} ×(33.1+273.16/50000
0) ≒1.90 (Kcal/K W H) ...(6) However, since the leakage amount is unknown in equation (6), the feed water flow rate at the outlet of the feed water heater is assumed to be the same as the inlet.

第9図においてドレン流量は実際には 121339+20000=141339Kg/H あつたにもかかわらず、流量調整弁開度から求め
た流量が検出誤差により125000Kg/Hと少なく検
出されても、給水加熱器が正常な時のエネルギ損
失△Q(=2.31(Kcal/KWH)と比較し(6)式で
求められた△QLEAK″は大きく変化しており、正
常状態からはずれていることが容易に判定でき
る。ドレン流量が141339Kg/Hrの場合は△Qと
△QLEAK″はもつとその差が大きくなる。すなわ
ち(5),(6)式によりエネルギ損失を求める方法は(5)
式により求める流量に相当大きな誤差をもつてい
ても、わずかな流量変動を容易に判別でき、しか
も正常時でのドレン流量に対し、下記のように増
減の判定まですることができる。
In Figure 9, the drain flow rate is actually 121339 + 20000 = 141339 Kg/H, but even if the flow rate calculated from the flow rate adjustment valve opening is detected as low as 125000 Kg/H due to a detection error, the feed water heater is functioning properly. Compared to the energy loss △Q (= 2.31 (Kcal/K W H)) when If the drain flow rate is 141339Kg/Hr, the difference between △Q and △Q LEAK ″ becomes larger.In other words, the method for calculating energy loss using equations (5) and (6) is (5).
Even if there is a fairly large error in the flow rate determined by the equation, slight fluctuations in flow rate can be easily determined, and furthermore, it is possible to determine whether the drain flow rate has increased or decreased in relation to the normal drain flow rate as shown below.

△Q>△QLEAK″の時は漏えい発生(ドレン流
量増加)。
When △Q>△Q LEAK '', a leak occurs (drain flow rate increases).

△Q<△QLEAK″の時はドレン流量減少 ここでエネルギ損失の絶対値は特に意味を持つ
ものではない。なお、ドレン流量の計測は流量計
より行つてもよい。
When △Q<△Q LEAK '', the drain flow rate decreases. Here, the absolute value of energy loss has no particular meaning. Note that the drain flow rate may be measured using a flowmeter.

第10図の実施例102では求めたエネルギ損
失△QLEAK″と正常時のそれ(△Q)とを比較
し、その偏差により給水管からの漏えいの有無を
判定し、信号線l1にドレン流量増加、かつ漏えい
発生の旨を出力する。△Q−△QLEAK″<αのと
きは信号線l3に漏えい以外の何らかの異常発生の
旨出力し、|△Q−△QLEAK″|≦−αのときは
信号線l2に正常の旨出力する。信号線l1の出力は
タイマ103を介して漏えい発生の報知に使用さ
れる。
In Example 102 of FIG. 10, the obtained energy loss △Q LEAK ″ is compared with that in the normal state (△Q), the presence or absence of leakage from the water supply pipe is determined based on the deviation, and a drain is connected to the signal line l 1 . Outputs that the flow rate has increased and that leakage has occurred. If △Q-△Q LEAK ″<α, outputs to signal line l3 that some abnormality other than leakage has occurred, and |△Q-△Q LEAK ″|≦ -α, a message indicating normality is output to the signal line l2.The output of the signal line l1 is used to notify the occurrence of leakage via the timer 103.

なお給水加熱器の漏えいは急速に拡大して行く
のが普通であるため、(5),(6)式から求めた△QLE
AK″の変化率を求め、第10図の漏えい検出ロジ
ツクに d/dt(△QLEAK″)<−α′ による判定をもオア条件として加えることによ
り、検出を早くすることも出来る。
Since leakage from feed water heaters usually expands rapidly, △Q LE obtained from equations (5) and (6)
Detection can also be made faster by determining the rate of change in AK '' and adding a determination based on d/dt( ΔQLEAK '')<-α' as an OR condition to the leakage detection logic shown in FIG.

第10図の以上の回路により漏えい発生を検知
するが、本発明ではこれ以外の異常あるいは異常
発生の要因である性能劣化をも以下の考えにより
検知する。
Although the occurrence of leakage is detected by the above-mentioned circuit shown in FIG. 10, the present invention also detects other abnormalities or performance deterioration which is a factor of abnormality occurrence based on the following idea.

まず、本発明の実施例としてとりあげた給水加
熱器の性能はTD(ターミナル温度差),DC(ド
レン温度差)で代表される。従つてこのTD,DC
が正常状態でのそれと比較し著しく悪い(TD,
DCが正常値に比べ大きくなる)場合は性能劣化
が考えられる。性能劣化はチユーブにスケール附
着などで熱交換性能が低下したことを意味してお
り、この時にはTDが大きくなつたり、DCが大き
くなつたりあるいはTD,DCとも大きくなつたり
する形であらわれるので他の異常と区別して検知
できる。第6図に正常状態での給水加熱器の温度
特性を示す。第6図aに示すTDはターミナル温
度差,DCはドレン出口温度差を表わしている
が、その特性は給水加熱器の給水流量(負荷)に
対し、第6図b,cに示す通りの関係がある。従
つて、これらの関係を第10図ブロツク104,
107に記憶しておいて基準値となし、一方これ
らの実際値TDa,DCaを実測し、夫々ブロツク1
05,108において大小関係を比較する。そし
て、信号線l4又はl7に出力有りのときオア回路1
06を介して検出器異常を出力する。信号線l6
はl9に出力有りの時オア回路110を介して性能
劣化を出力する。
First, the performance of the feed water heater taken as an example of the present invention is represented by TD (terminal temperature difference) and DC (drain temperature difference). Therefore, this TD, DC
is significantly worse than that under normal conditions (TD,
(DC is larger than the normal value), performance deterioration may occur. Performance deterioration means that the heat exchange performance has deteriorated due to scale adhesion to the tube, etc. At this time, it appears in the form of increased TD, increased DC, or both increased TD and DC. Can be detected separately from abnormalities. Figure 6 shows the temperature characteristics of the feed water heater under normal conditions. In Figure 6a, TD represents the terminal temperature difference and DC represents the drain outlet temperature difference, but their characteristics are related to the feedwater flow rate (load) of the feedwater heater as shown in Figures 6b and c. There is. Therefore, these relationships can be expressed as blocks 104 and 104 in FIG.
107 and use them as reference values, and on the other hand, these actual values TDa and DCa are actually measured and respectively stored in block 1.
05, 108, the magnitude relationship is compared. Then, when the signal line l4 or l7 has an output, the OR circuit 1
Detector abnormality is output via 06. When there is an output on the signal line l6 or l9 , a performance degradation signal is outputted via the OR circuit 110.

また、第9図のドレン調整弁100の開度は負
荷(給水流量)によつてほぼ定まることからブロ
ツク111において弁100の開度の基準値Vp
を準備し、実測開度VPaとの差をブロツク112
で求める。この場合に、信号線l3とl10に共に出力
有りをアンド回路115で検知しこの状態の継続
をタイム113で確認したときにはドレン調整弁
100の異常と判断する。信号線l1とl12に出力有
りをアンド回路116で検知できた状態がタイマ
114で確認できるときにはドレン流量検出器異
常であり、この旨出力する。尚、信号線l2,l5
l8,l11の出力は正常時のものであり、オア回路1
09を介して正常の旨報知する。この第10図の
実施例において、オア回路106又はタイマ11
4の検出器異常の出力があるときにタイマ103
が漏えい検出しているときはタイマ103の出力
を阻止するのが良い。
Furthermore, since the opening degree of the drain regulating valve 100 shown in FIG.
Prepare the block 112 and check the difference with the actual opening VPa.
Find it with In this case, when the AND circuit 115 detects that there is an output on both signal lines l3 and l10 , and confirms that this state continues at time 113, it is determined that the drain regulating valve 100 is abnormal. When the timer 114 confirms that the AND circuit 116 detects that there is an output on the signal lines l1 and l12 , the drain flow rate detector is abnormal, and this fact is output. In addition, the signal lines l 2 , l 5 ,
The outputs of l 8 and l 11 are normal, and OR circuit 1
09 to notify that it is normal. In the embodiment of FIG. 10, the OR circuit 106 or the timer 11
Timer 103 when there is an output of 4 detector abnormality.
It is preferable to block the output of the timer 103 when a leak is being detected.

第10図は給水加熱器まわりの総合診断を示し
たが、ここで、α,β,γおよびδは検出誤差等
を考慮した判定のための裕度であり、給水加熱器
の運転状態によつて可変にしてもよい。勿論この
中の一部についての診断のみ行うことも出来る。
なお当然ながら本診断機能は計算機の中に組込む
ことが出来る。
Figure 10 shows a comprehensive diagnosis around the feed water heater, where α, β, γ, and δ are margins for judgment that take into account detection errors, etc., and depend on the operating status of the feed water heater. It may be made variable. Of course, it is also possible to diagnose only some of these.
Of course, this diagnostic function can be incorporated into a computer.

本発明は給水加熱器に限らず、第4,6,7図
に示すような熱サイクルを持つ熱交換器には同様
に適用できる。
The present invention is not limited to feed water heaters, but can be similarly applied to heat exchangers having thermal cycles as shown in FIGS. 4, 6, and 7.

尚、本発明を実施するに際し、給水流量の測定
に大きな誤差があると、診断はそれだけ影響を受
けるが、ある程度の誤差量は第10図における判
定値α,β,γ,δを調整することにより対処で
きる。さらに大きな測定誤差については別にリー
ズナブルチエツク(発電機出力との相関々係とか
主蒸気流量との関係などから誤差の程度を判定す
る)を行い、必要以上の誤差がある場合には測定
異常として処置し、診断処理を中断するのが良
い。勿論診断回路が異常になれば本発明は用をな
さなくなるので、自己診断機能を備え異常と判定
した場合は本発明の診断機能を中断させるのが良
い。
Furthermore, when carrying out the present invention, if there is a large error in the measurement of the water supply flow rate, the diagnosis will be affected accordingly, but the judgment values α, β, γ, and δ in FIG. This can be handled by For even larger measurement errors, a separate reasonable check (determining the extent of the error based on the correlation with the generator output, the relationship with the main steam flow rate, etc.) is performed, and if there is an error that is more than necessary, it is treated as a measurement abnormality. It is better to interrupt the diagnostic process. Of course, if the diagnostic circuit becomes abnormal, the present invention becomes useless, so it is preferable to provide a self-diagnosis function and interrupt the diagnostic function of the present invention when it is determined that there is an abnormality.

又、本発明の実施例としてとりあげた給水加熱
器の性能はTD(ターミナル温度差)、DC(ドレ
ン温度差)で代表される。従つてこのTD,DCが
正常状態でのそれと比較し著しく悪い(TD,DC
が正常値に比べ大きくなる)場合は性能劣化が考
えられる。性能劣化はチユーブにスケール附着な
どで熱交換性能が低下したことを意味しており、
この時にはTDが大きくなつたり、DCが大きくな
つたりあるいはTD,DCとも大きくなつたりする
形であらわれるので、他の異常と区別して検知で
きる。
Furthermore, the performance of the feed water heater taken up as an example of the present invention is represented by TD (terminal temperature difference) and DC (drain temperature difference). Therefore, this TD and DC are significantly worse than those under normal conditions (TD, DC
(becomes larger than the normal value), performance may be degraded. Performance deterioration means that heat exchange performance has decreased due to scale adhesion to the tube, etc.
At this time, it appears as TD becoming larger, DC increasing, or both TD and DC increasing, so it can be detected separately from other abnormalities.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は火力発電プラントの機能を示すスケル
トン図、第2図は火力プラントの熱平衡線図、第
3,5,8,9図は給水加熱器まわりの状態値を
示す状態線図、第4図は給水加熱器内の温度分布
図、第6,7図は給水加熱器の特性線図、第10
図は異常診断装置の診断アルゴリズムを示すフロ
ー図である。 1…ボイラ、2…高圧タービン、3…再熱ター
ビン、4…発電機、5…復水器、6…復水ポン
プ、7…復水熱交換器、8…空気抽出器、9…グ
ランドコンデンサ、10…低圧給水加熱器、11
…脱気器、12…ボイラ給水ポンプ、13…高圧
給水加熱器、14…燃料バーナ、15…過熱器、
16…再熱器、17…燃料調整弁、18…排蒸気
管、19…低温再熱蒸気管、20…高温再熱蒸気
管、21…主管水管。
Figure 1 is a skeleton diagram showing the functions of a thermal power plant, Figure 2 is a thermal balance diagram of a thermal power plant, Figures 3, 5, 8, and 9 are state diagrams showing state values around the feed water heater, and Figure 4 is a diagram showing the state values around the feed water heater. The figure is a temperature distribution diagram inside the feed water heater, Figures 6 and 7 are characteristic diagrams of the feed water heater, and Figure 10 is a temperature distribution diagram of the feed water heater.
The figure is a flow diagram showing the diagnostic algorithm of the abnormality diagnostic device. 1... Boiler, 2... High pressure turbine, 3... Reheat turbine, 4... Generator, 5... Condenser, 6... Condensate pump, 7... Condensate heat exchanger, 8... Air extractor, 9... Grand condenser , 10...Low pressure feed water heater, 11
... deaerator, 12 ... boiler feed water pump, 13 ... high pressure feed water heater, 14 ... fuel burner, 15 ... superheater,
16... Reheater, 17... Fuel adjustment valve, 18... Exhaust steam pipe, 19... Low temperature reheat steam pipe, 20... High temperature reheat steam pipe, 21... Main water pipe.

Claims (1)

【特許請求の範囲】 1 加熱材と被加熱材との間で間接接触で熱交換
を行なう熱交換器の異常を診断する熱交換器の診
断装置において、 加熱材と被加熱材とが正常に熱交換を行なつて
いるときに熱交換器で生じるエネルギー損失を求
める第1の手段、熱交換器から排出された加熱材
の流量を検知する第2の手段、該第2の手段の出
力と、加熱材と被加熱材の状態量とを用いて加熱
材,被加熱材の夫々が所定の点において所有する
エントロピを導出するとともに、エントロピを介
して加熱材から被加熱材への熱交換に伴なう熱損
失を求める第3の手段、該第3の手段の出力と前
記第1の手段の出力との比較により熱交換器の異
常を検出する第4の手段とから構成されることを
特徴とする熱交換器の診断装置。 2 第1項記載の熱交換器の診断装置において、
第2の手段は熱交換器から排出された加熱材の流
量を調整弁の開度とその前後差圧とを用いて排出
された加熱材の流量を求めることを特徴とする熱
交換器の診断装置。
[Scope of Claims] 1. A heat exchanger diagnostic device for diagnosing an abnormality in a heat exchanger that performs heat exchange through indirect contact between a heating material and a heated material, comprising: a first means for determining the energy loss occurring in the heat exchanger during heat exchange; a second means for detecting the flow rate of the heating material discharged from the heat exchanger; an output of the second means; , the entropy possessed by each of the heating material and the heated material at a predetermined point is derived using the state quantities of the heating material and the heated material, and the heat exchange from the heating material to the heated material is performed via the entropy. and a fourth means for detecting an abnormality in the heat exchanger by comparing the output of the third means and the output of the first means. Features of heat exchanger diagnostic equipment. 2 In the heat exchanger diagnostic device described in paragraph 1,
The second means is a diagnosis of a heat exchanger characterized in that the flow rate of the heating material discharged from the heat exchanger is determined by using the opening degree of a regulating valve and the differential pressure before and after the regulating valve. Device.
JP12110180A 1980-09-03 1980-09-03 Device and method for diagnosis of heat exchanger Granted JPS5747199A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP12110180A JPS5747199A (en) 1980-09-03 1980-09-03 Device and method for diagnosis of heat exchanger

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP12110180A JPS5747199A (en) 1980-09-03 1980-09-03 Device and method for diagnosis of heat exchanger

Publications (2)

Publication Number Publication Date
JPS5747199A JPS5747199A (en) 1982-03-17
JPS6228395B2 true JPS6228395B2 (en) 1987-06-19

Family

ID=14802894

Family Applications (1)

Application Number Title Priority Date Filing Date
JP12110180A Granted JPS5747199A (en) 1980-09-03 1980-09-03 Device and method for diagnosis of heat exchanger

Country Status (1)

Country Link
JP (1) JPS5747199A (en)

Families Citing this family (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6377537A (en) * 1986-09-19 1988-04-07 Jgc Corp Plant operation supporting device
US5429178A (en) * 1993-12-10 1995-07-04 Electric Power Research Institute, Inc. Dual tube fouling monitor and method
JP3831420B2 (en) * 1995-01-19 2006-10-11 三菱重工業株式会社 Heat absorption amount estimation device for heat transfer surface
JP3614640B2 (en) * 1998-02-10 2005-01-26 東京電力株式会社 Thermal efficiency diagnosis method and apparatus for thermal power plant
US6678628B2 (en) 2002-01-14 2004-01-13 William J. Ryan Apparatus and methods for monitoring and testing coolant recirculation systems
US20070104306A1 (en) * 2003-10-29 2007-05-10 The Tokyo Electric Power Company, Incorporated Thermal efficiency diagnosing system for nuclear power plant, thermal efficiency diagnosing program for nuclear power plant, and thermal efficiency diagnosing method for nuclear power plant
DE102004021423A1 (en) 2004-04-30 2005-12-01 Siemens Ag Method and device for determining the efficiency of a heat exchanger
JP6953924B2 (en) * 2017-09-06 2021-10-27 いすゞ自動車株式会社 Heat exchanger modeling system and methods

Also Published As

Publication number Publication date
JPS5747199A (en) 1982-03-17

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