JP3381122B2 - Steam dryness measuring device - Google Patents

Steam dryness measuring device

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Publication number
JP3381122B2
JP3381122B2 JP14122195A JP14122195A JP3381122B2 JP 3381122 B2 JP3381122 B2 JP 3381122B2 JP 14122195 A JP14122195 A JP 14122195A JP 14122195 A JP14122195 A JP 14122195A JP 3381122 B2 JP3381122 B2 JP 3381122B2
Authority
JP
Japan
Prior art keywords
steam
pressure
throttle mechanism
dryness
flow
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 - Fee Related
Application number
JP14122195A
Other languages
Japanese (ja)
Other versions
JPH08313425A (en
Inventor
正義 原田
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.)
Tlv Co Ltd
Original Assignee
Tlv Co 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
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Priority to JP14122195A priority Critical patent/JP3381122B2/en
Publication of JPH08313425A publication Critical patent/JPH08313425A/en
Application granted granted Critical
Publication of JP3381122B2 publication Critical patent/JP3381122B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Description

【発明の詳細な説明】 【0001】 【産業上の利用分野】本発明は蒸気配管を流れる蒸気の
乾き度を測定する装置に関する。各種ボイラや蒸気動力
を利用する機器では、蒸気中の水分の含有量、即ち蒸気
流の単位体積当りの全質量に対する乾き飽和蒸気の占め
る質量の割合を示す乾き度Xを知る必要がある。これは
水分の含有量によって蒸気のエンタルピが異なるためで
ある。 【0002】 【従来の技術】従来の蒸気乾き度測定装置としては絞り
乾き度計がある。これは、被測定湿り蒸気をノズルを通
して測定室内で断熱膨脹(等エンタルピ変化)させて過
熱蒸気とし、ノズルの上流側の圧力P1と測定室内の圧
力P2及び測定室内の温度Tを検出することにより、飽
和蒸気表及び過熱蒸気表を用いて、上流側蒸気の乾き度
X1をX1=(E6−E1)/(E3−E1)として算
出するものである。上式において、E1は圧力P1にお
ける飽和水のエンタルピ、E3は同じく圧力P1におけ
る飽和蒸気のエンタルピ、E6は圧力P2と温度Tにお
ける過熱蒸気のエンタルピである。 【0003】 【発明が解決しようとする課題】上記従来の絞り乾き度
計では、過熱蒸気を作らなければならないので、蒸気の
圧力が低い場合や蒸気の乾き度が小さい場合には測定で
きない問題があった。従って、本発明の技術的課題は、
測定可能な乾き度の範囲が広く、簡単に乾き度を測定で
きる蒸気乾き度測定装置を提供することである。 【0004】 【課題を解決するための手段】上記の技術的課題を解決
するために講じた本発明の技術的手段は、蒸気配管の途
中に設けた絞り機構と、絞り機構の上流側の蒸気流量を
計測する第1流量計と、絞り機構の下流側の蒸気流量を
計測する第2流量計と、絞り機構の上流側の圧力を検出
する第1圧力センサ―と、絞り機構の下流側の圧力を検
出する第2圧力センサ―と、第1及び第2流量計で計測
された流量値と第1及び第2圧力センサ―で検出された
圧力値に基づいて上流側蒸気の乾き度を算出する演算部
を具備する蒸気乾き度測定装置にある。 【0005】 【作用】上記の技術的手段の作用は下記の通りである。
上流側の湿り蒸気は絞り機構を通して下流側で断熱膨脹
し、飽和水の少なくとも一部が再蒸発する。この再蒸発
蒸気量により第1流量計と第2流量計で計測される蒸気
流量値が異なる。 【0006】第1流量計で計測される蒸気流量値W1
は、絞り機構の上流側湿り蒸気の乾き度をX1、絞り機
構の上流側の全熱量をQとし、第1圧力センサーで検出
した圧力値P1及び飽和蒸気表から、W1=Q/(E2
+E1/X1)で表すことができる。上式において、E
1は圧力P1における飽和水のエンタルピ、E2は同じ
く圧力P1における飽和蒸気の潜熱である。 【0007】また第2流量計で計測される蒸気流量値W
2は、絞り機構の上流側あるいは下流側の全流体流量を
W、絞り機構の下流側の全熱量をQ(等エンタルピ変化
であり絞り機構の上流側の全熱量に等しい)とし、第2
圧力センサーで検出した圧力値P2及び飽和蒸気表か
ら、W2=(Q−W・E4)/E5で表すことができ
る。上式において、E4は圧力P2における飽和水のエ
ンタルピ、E5は同じく圧力P2における飽和蒸気の
である。ここで、全流体流量Wは、W=W1X1で
表すことができる。 【0008】上記三式より、絞り機構の上流側蒸気の乾
き度X1は、X1=(W1・E1−W1・E4)/(W
2・E5−W1・E2)として算出することができる。
この関係式の内、W1とW2は第1流量計と第2流量計
で計測される。またE1とE2は第1圧力センサ―で検
出した圧力値に基づいて飽和蒸気表から読取ることがで
き、同様にE4とE5は第2圧力センサ―で検出した圧
力値に基づいて飽和蒸気表から読取ることができるので
演算部に記憶させておいたりあるいは入力することによ
り判明する。従って、この関係式を演算部で解くことに
より絞り機構の上流側蒸気の乾き度を算出することがで
きる。 【0009】上記は絞り機構の上流側蒸気の乾き度を算
出するものであるが、絞り機構の下流側蒸気の乾き度は
下記のように算出することができる。尚、上記記号と同
じ記号は同じ意味で用いるものとする。第2流量計で計
測される蒸気流量値W2は、絞り機構の下流側蒸気の乾
き度をX2とすると、W2=Q/(E5+E4/X2)
であり、第1流量計で計測される蒸気流量値W1は、W
1=(Q−W・E1)/E2であり、全流体流量Wは、
W=W2X2であるので、絞り機構の下流側蒸気の乾
き度X2は、X2=(W2・E4−W2・E1)/(W
1・E2−W2・E5)として算出することができる。 【0010】 【実施例】上記の技術的手段の具体例を示す実施例を説
明する(図1参照)。湿り蒸気を送給する蒸気配管1の
途中に絞り機構2を設ける。絞り機構2の上流側に、蒸
気流量を計測する第1流量計3を設置すると共に、圧力
を検出する第1圧力センサ―4と温度を検出する第1温
度センサ―5を取り付ける。また絞り機構2の下流側
に、蒸気流量を計測する第2流量計6を設置すると共
に、圧力を検出する第2圧力センサ―7と温度を検出す
る第2温度センサ―8を取り付ける。第1及び第2流量
計3,6と第1及び第2圧力センサ―4,7と第1及び
第2温度センサ―5,8を演算部9に接続する。 【0011】絞り機構2としては、ノズルやベンチュリ
やオリフィス等を用いることができる。また第1及び第
2流量計3,6としては、例えば容積式流量計等を用い
ることができるが、本実施例においては渦式流量計を用
いた例を示す。 【0012】渦式の第1及び第2流量計3,6は、蒸気
の容積流量に蒸気の比重量を乗じて質量流量を計測する
ものである。第1及び第2流量計3,6で計測された蒸
気流量値W1,W2が演算部9に送られる。また第1及
び第2圧力センサ―4,7によって検出された圧力値P
1,P2と、第1及び第2温度センサ―5,8で検出さ
れた温度値T1,T2が演算部9に送られる。 【0013】演算部9は、飽和蒸気表及び過熱蒸気表を
テ―ブルとして記憶し、また乾き度の算出式を記憶して
いる。演算部9での処理プロセスは、次の通りである。
先ず、絞り機構2の上流側の圧力値P1及び温度値T1
から上流側蒸気が過熱蒸気であるか否かを判断する。上
流側蒸気が過熱蒸気であれば、過熱蒸気表から上流側蒸
気の過熱度を算出する。 【0014】上流側蒸気が過熱蒸気でなければ、絞り機
構2の下流側の圧力P2及びT2から下流側蒸気が過熱
蒸気であるか否かを判断する。下流側蒸気が過熱蒸気で
あれば、上流側蒸気の乾き度を従来の関係式であるX1
=(E6−E1)/(E3−E1)に基づいて算出す
る。 【0015】過熱蒸気でなければ、上流側蒸気の乾き度
を本発明の関係式であるX1=(W1・E1−W1・E
4)/(W2・E5−W1・E2)に基づいて算出し、
下流側蒸気の乾き度を本発明の関係式であるX2=(W
2・E4−W2・E1)/(W1・E2−W2・E5)
に基づいて算出する。上三式において、E1は圧力P1
における飽和水のエンタルピ、E2は同じく圧力P1に
おける飽和蒸気の潜熱、E3は同じく圧力P1における
飽和蒸気のエンタルピ、E4は圧力P2における飽和水
のエンタルピ、E5は同じく圧力P2における飽和蒸気
潜熱、E6は圧力P2と温度Tにおける過熱蒸気のエ
ンタルピである。 【0016】 【発明の効果】本発明は下記の特有の効果を生じる。上
記のように本発明によれば、蒸気を過熱状態にせずに乾
き度を測定できるので、測定可能な乾き度の範囲が広く
なると共に、簡単に乾き度を測定できる。
Description: BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an apparatus for measuring the dryness of steam flowing through a steam pipe. In various boilers and equipment using steam power, it is necessary to know the dryness X indicating the content of moisture in the steam, that is, the ratio of the mass of the dry saturated steam to the total mass per unit volume of the steam flow. This is because the enthalpy of the steam varies depending on the water content. 2. Description of the Related Art As a conventional steam dryness measuring device, there is an aperture dryness meter. This is achieved by adiabatically expanding (equally changing the enthalpy) the wet steam to be measured in the measurement chamber through the nozzle to form superheated steam, and detecting the pressure P1 upstream of the nozzle, the pressure P2 in the measurement chamber, and the temperature T in the measurement chamber. Using the saturated steam table and the superheated steam table, the dryness X1 of the upstream steam is calculated as X1 = ( E6- E1) / ( E3- E1). In the above equation, E1 is the enthalpy of the saturated water at the pressure P1, E3 is the enthalpy of the saturated steam at the pressure P1, and E6 is the enthalpy of the superheated steam at the pressure P2 and the temperature T. [0003] In the above-mentioned conventional diaphragm dryness meter, superheated steam must be produced. Therefore, there is a problem that it cannot be measured when the steam pressure is low or when the steam dryness is small. there were. Therefore, the technical problem of the present invention is:
An object of the present invention is to provide a steam dryness measuring device that can measure the dryness easily with a wide range of measurable dryness. [0004] The technical means of the present invention taken to solve the above-mentioned technical problems includes a throttle mechanism provided in the middle of a steam pipe and a steam upstream of the throttle mechanism. A first flow meter for measuring the flow rate, a second flow meter for measuring the steam flow rate on the downstream side of the throttle mechanism, a first pressure sensor for detecting a pressure on the upstream side of the throttle mechanism, and a downstream side of the throttle mechanism. A second pressure sensor for detecting pressure, and a dryness of the upstream steam is calculated based on a flow value measured by the first and second flow meters and a pressure value detected by the first and second pressure sensors. In a steam dryness measuring apparatus provided with a calculation unit for performing the above. The operation of the above technical means is as follows.
The wet steam on the upstream side is adiabatically expanded on the downstream side through the throttle mechanism, and at least a part of the saturated water is re-evaporated. The steam flow rate value measured by the first flow meter and the second flow meter differs depending on the re-evaporated steam amount. [0006] The steam flow value W1 measured by the first flow meter
Is the dryness of the wet steam on the upstream side of the throttle mechanism as X1, the total amount of heat on the upstream side of the throttle mechanism as Q, and from the pressure value P1 detected by the first pressure sensor and the saturated steam table, W1 = Q / (E2
+ E1 / X1). In the above equation, E
1 is the enthalpy of the saturated water at the pressure P1, and E2 is the latent heat of the saturated steam at the pressure P1. The steam flow value W measured by the second flow meter
2 is the total fluid flow upstream or downstream of the throttle mechanism as W, the total heat quantity downstream of the throttle mechanism as Q (equal enthalpy change and equal to the total heat quantity upstream of the throttle mechanism),
From the pressure value P2 detected by the pressure sensor and the saturated steam table, it can be expressed as W2 = (Q−W · E4) / E5. In the above equation, E4 is the enthalpy of the saturated water at the pressure P2, and E5 is the latent steam saturation vapor at the pressure P2.
Heat . Here, the total fluid flow rate W can be represented by W = W1 / X1. From the above three equations, the dryness X1 of the steam on the upstream side of the throttle mechanism is X1 = (W1 · E1-W1 · E4) / (W
2 · E5−W1 · E2).
In this relational expression, W1 and W2 are measured by the first flow meter and the second flow meter. E1 and E2 can be read from the saturated steam table based on the pressure value detected by the first pressure sensor. Similarly, E4 and E5 can be read from the saturated steam table based on the pressure value detected by the second pressure sensor. Since it can be read, it can be determined by storing it in the arithmetic unit or inputting it. Therefore, the degree of dryness of the steam on the upstream side of the throttle mechanism can be calculated by solving this relational expression by the calculation unit. In the above description, the dryness of the steam on the upstream side of the throttle mechanism is calculated. The dryness of the steam on the downstream side of the throttle mechanism can be calculated as follows. The same symbols as those described above have the same meaning. The steam flow value W2 measured by the second flow meter is W2 = Q / (E5 + E4 / X2) where X2 is the dryness of the steam on the downstream side of the throttle mechanism.
And the steam flow value W1 measured by the first flow meter is W
1 = (Q−W · E1) / E2, and the total fluid flow rate W is
Since W = W2 / X2, the dryness X2 of the steam on the downstream side of the throttle mechanism is X2 = (W2 · E4−W2 · E1) / (W
1 · E2−W2 · E5). An embodiment showing a specific example of the above technical means will be described (see FIG. 1). A throttle mechanism 2 is provided in the middle of a steam pipe 1 for supplying wet steam. On the upstream side of the throttle mechanism 2, a first flow meter 3 for measuring a steam flow rate is installed, and a first pressure sensor 4 for detecting pressure and a first temperature sensor 5 for detecting temperature are attached. A second flow meter 6 for measuring a steam flow rate is installed downstream of the throttle mechanism 2, and a second pressure sensor 7 for detecting pressure and a second temperature sensor 8 for detecting temperature are attached. The first and second flow meters 3 and 6, the first and second pressure sensors 4 and 7, and the first and second temperature sensors -5 and 8 are connected to the calculation unit 9. As the throttle mechanism 2, a nozzle, a venturi, an orifice, or the like can be used. As the first and second flowmeters 3 and 6, for example, positive displacement flowmeters or the like can be used. In this embodiment, an example using a vortex flowmeter is shown. The first and second vortex type flow meters 3 and 6 measure the mass flow rate by multiplying the volume flow rate of the steam by the specific weight of the steam. The steam flow values W1 and W2 measured by the first and second flow meters 3 and 6 are sent to the calculation unit 9. Further, the pressure value P detected by the first and second pressure sensors-4, 7
1, P2 and the temperature values T1, T2 detected by the first and second temperature sensors -5, 8 are sent to the arithmetic unit 9. The calculation section 9 stores the saturated steam table and the superheated steam table as tables, and also stores the dryness calculation formula. The processing process in the arithmetic unit 9 is as follows.
First, the pressure value P1 and the temperature value T1 on the upstream side of the throttle mechanism 2 are set.
Then, it is determined whether or not the upstream steam is superheated steam. If the upstream steam is superheated steam, the degree of superheat of the upstream steam is calculated from the superheated steam table. If the upstream steam is not superheated steam, it is determined from the pressures P2 and T2 on the downstream side of the throttle mechanism 2 whether or not the downstream steam is superheated steam. If the downstream-side steam is superheated steam, the dryness of the upstream-side steam is calculated by a conventional relational expression X1.
= ( E6- E1) / ( E3- E1). If it is not superheated steam, the dryness of the upstream steam is calculated by the relational expression of the present invention, X1 = (W1 · E1−W1 · E).
4) Calculated based on / (W2 · E5−W1 · E2),
The dryness of the downstream steam is calculated as X2 = (W
2 ・ E4-W2 ・ E1) / (W1 ・ E2-W2 ・ E5)
Calculated based on In the above three equations, E1 is the pressure P1
, The enthalpy of saturated water at E2, the latent heat of saturated steam at pressure P1 , and E3 at latent pressure P1.
E4 is the enthalpy of the saturated water at the pressure P2, E5 is the latent heat of the saturated steam at the pressure P2, and E6 is the enthalpy of the superheated steam at the pressure P2 and the temperature T.
It is enthalpy . The present invention has the following specific effects. As described above, according to the present invention, the degree of dryness can be measured without overheating the steam, so that the range of measurable dryness is widened and the dryness can be easily measured.

【図面の簡単な説明】 【図1】図1は本発明の実施例の蒸気乾き度測定装置の
構成図である。 【符号の説明】 1 蒸気配管 2 絞り機構 3 第1流量計 4 第1圧力センサ― 5 第1温度センサ― 6 第2流量計 7 第2圧力センサ― 8 第2温度センサ― 9 演算部
BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a configuration diagram of a steam dryness measuring apparatus according to an embodiment of the present invention. [Description of Signs] 1 Steam pipe 2 Throttle mechanism 3 First flow meter 4 First pressure sensor 5 First temperature sensor 6 Second flow meter 7 Second pressure sensor 8 Second temperature sensor 9 Operation unit

Claims (1)

(57)【特許請求の範囲】 【請求項1】 蒸気配管の途中に設けた絞り機構と、絞
り機構の上流側の蒸気流量を計測する第1流量計と、絞
り機構の下流側の蒸気流量を計測する第2流量計と、絞
り機構の上流側の圧力を検出する第1圧力センサ―と、
絞り機構の下流側の圧力を検出する第2圧力センサ―
と、第1及び第2流量計で計測された流量値と第1及び
第2圧力センサ―で検出された圧力値に基づいて蒸気の
乾き度を算出する演算部を具備することを特徴とする蒸
気乾き度測定装置。
(57) [Claims 1] A throttle mechanism provided in the middle of a steam pipe, a first flow meter for measuring a steam flow rate upstream of the throttle mechanism, and a steam flow rate downstream of the throttle mechanism A second flow meter for measuring the pressure, a first pressure sensor for detecting the pressure on the upstream side of the throttle mechanism,
A second pressure sensor that detects the pressure downstream of the throttle mechanism
And a calculation unit for calculating the dryness of the steam based on the flow value measured by the first and second flow meters and the pressure value detected by the first and second pressure sensors. Steam dryness measuring device.
JP14122195A 1995-05-15 1995-05-15 Steam dryness measuring device Expired - Fee Related JP3381122B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP14122195A JP3381122B2 (en) 1995-05-15 1995-05-15 Steam dryness measuring device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP14122195A JP3381122B2 (en) 1995-05-15 1995-05-15 Steam dryness measuring device

Publications (2)

Publication Number Publication Date
JPH08313425A JPH08313425A (en) 1996-11-29
JP3381122B2 true JP3381122B2 (en) 2003-02-24

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ID=15286949

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Application Number Title Priority Date Filing Date
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Country Status (1)

Country Link
JP (1) JP3381122B2 (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN1094592C (en) * 2000-03-02 2002-11-20 郑金华 Automatic testing and control method of dryness fraction of boiler
JP5924809B2 (en) * 2012-03-07 2016-05-25 国立研究開発法人産業技術総合研究所 Wetness measuring method and wetness measuring device
JP6307390B2 (en) * 2014-09-10 2018-04-04 アズビル株式会社 Dryness measuring device and dryness measuring method

Also Published As

Publication number Publication date
JPH08313425A (en) 1996-11-29

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