JP2002277449A - Measuring apparatus for degree of dryness or wetness of two phase fluid - Google Patents
Measuring apparatus for degree of dryness or wetness of two phase fluidInfo
- Publication number
- JP2002277449A JP2002277449A JP2001073768A JP2001073768A JP2002277449A JP 2002277449 A JP2002277449 A JP 2002277449A JP 2001073768 A JP2001073768 A JP 2001073768A JP 2001073768 A JP2001073768 A JP 2001073768A JP 2002277449 A JP2002277449 A JP 2002277449A
- Authority
- JP
- Japan
- Prior art keywords
- dryness
- fluid
- liquid
- phase fluid
- wetness
- 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.)
- Pending
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N2291/00—Indexing codes associated with group G01N29/00
- G01N2291/02—Indexing codes associated with the analysed material
- G01N2291/028—Material parameters
- G01N2291/02845—Humidity, wetness
Abstract
Description
【0001】[0001]
【発明の属する技術分野】本発明は、蒸気と凝縮液とし
てのドレン、あるいは、冷媒ガスと冷媒液などの気液二
相流体が混合した流体の乾き度又は湿り度を測定する装
置に関する。例えば、蒸気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乾き度Xと言
う。乾き度がXの場合、湿り度は(1−X)で表され
る。各種ボイラや蒸気動力を利用する機器、乾燥設備な
どでは、熱管理のために蒸気の乾き度を測定する必要が
ある。これは蒸気中の水分の含有量によって例えば乾燥
状態が変化してしまうためである。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an apparatus for measuring the dryness or wetness of a fluid in which a vapor and a condensed liquid or a gas-liquid two-phase fluid such as a refrigerant gas and a refrigerant liquid are mixed. For example, the ratio of the mass occupied by dry saturated steam to the total mass per unit volume of steam is referred to as dryness X. When the dryness is X, the wetness is represented by (1-X). In various boilers, equipment using steam power, and drying equipment, it is necessary to measure the dryness of steam for heat management. This is because, for example, the dry state changes depending on the moisture content in the steam.
【0002】[0002]
【従来の技術】従来の蒸気の乾き度測定装置としては、
例えば、蒸気の等エンタルピ変化を利用して乾き度を測
定する、所謂絞り乾き度計がある。これは、ノズルに湿
り蒸気を通して測定容器内に噴射して断熱膨脹(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
力と測定容器内の圧力及び温度を検出することにより、
モリエール線図あるいは飽和蒸気表あるいは過熱蒸気表
を用いて乾き度を測定するものである。2. Description of the Related Art Conventional steam dryness measuring devices include:
For example, there is a so-called squeezing dryness meter that measures the dryness by using a change in enthalpy of steam. This is done by injecting wet steam through the nozzle into the measuring vessel, adiabatic expansion (equal enthalpy change) into superheated steam, and detecting the pressure upstream of the nozzle and the pressure and temperature in the measuring vessel,
The dryness is measured using a Moliere diagram, a saturated steam table or a superheated steam table.
【0003】[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、気相としての蒸気の乾き度を測定することはで
きるが、流体配管中に混在する層状の凝縮液としてのド
レンを考慮した、流体配管全体の乾き度を測定すること
ができない問題があった。The conventional dryness meter described above can measure the dryness of vapor as a gas phase, but takes into account the drainage as a layered condensate mixed in the fluid piping. However, there has been a problem that the dryness of the entire fluid pipe cannot be measured.
【0004】例えば実際の蒸気配管においては、気相と
しての蒸気の層の下部に、液相としてのドレンの層が混
在した状態となっている場合が多々ある。上記従来の絞
り乾き度計では、蒸気中に含まれる微細な水滴の量の多
少に基づいて変化する蒸気の乾き度を測定することはで
きるが、下層のドレンを考慮した配管全体の乾き度を測
定することができないのである。For example, in an actual steam pipe, there are many cases where a layer of a drain as a liquid phase is mixed below a layer of a vapor as a gas phase. With the above conventional dryness meter, it is possible to measure the dryness of steam that changes based on the amount of fine water droplets contained in the steam.However, the dryness of the entire pipe taking into account the lower layer drainage can be measured. It cannot be measured.
【0005】従って、本発明の課題は、流体配管中に混
在する層状の液体も含めた配管全体の流体の乾き度又は
湿り度を測定することができる、二相流体の乾き度又は
湿り度測定装置を提供することである。Accordingly, an object of the present invention is to measure the dryness or wetness of a two-phase fluid, which can measure the dryness or wetness of the entire fluid including the layered liquid mixed in the fluid piping. It is to provide a device.
【0006】[0006]
【課題を解決するための手段】請求項1に係る発明は、
気液二相流体の乾き度又は湿り度を測定するものにおい
て、気相流体の流下する配管に相対して取付けた超音波
送受信器と、気相流体中を通る超音波の伝搬時間から気
相流体の乾き度又は湿り度を検出する気相流体乾き度検
出手段と、流体配管中の層状の液相流体の液位から重量
を検出する液相流体液位重量検出手段を具備して、気相
流体乾き度検出手段での検出値に、液相流体液位重量検
出手段からの検出値を加味して、気液二相流体の乾き度
又は湿り度を演算算出することを特徴とするものであ
る。According to the first aspect of the present invention,
For measuring the dryness or wetness of a gas-liquid two-phase fluid, an ultrasonic transmitter / receiver installed opposite to the pipe through which the gas-phase fluid flows, and a gas phase based on the propagation time of the ultrasonic wave passing through the gas-phase fluid A gas phase fluid dryness detecting means for detecting the dryness or wetness of the fluid; and a liquid phase fluid level detecting means for detecting the weight from the liquid level of the layered liquid phase fluid in the fluid piping. The dryness or wetness of a gas-liquid two-phase fluid is calculated by taking into account the value detected by the liquid phase liquid level weight detection means to the value detected by the phase fluid dryness detection means. It is.
【0007】請求項2に係る発明は、請求項1に係る発
明を実施するのに好適な実施形態を特定するものであ
り、前記液相流体液位重量検出手段が、流体配管の底部
外面に取付けられた超音波送受信器と、当該超音波送受
信器から上方に向けて放射された超音波が液面で反射さ
れて戻ってくるまでの時間から流体配管内の液位を検出
する液位検出手段を具備して、当該液位検出手段で検出
された液位から流体配管内の気相流体と液相流体の単位
容積を算出して、液相流体の単位容積から重量を演算算
出することを特徴とするものである。The invention according to claim 2 specifies an embodiment suitable for carrying out the invention according to claim 1, wherein the liquid phase fluid level weight detecting means is provided on an outer surface of a bottom of a fluid pipe. Liquid level detection for detecting the liquid level in the fluid pipe from the attached ultrasonic transceiver and the time until the ultrasonic wave radiated upward from the ultrasonic transceiver is reflected by the liquid surface and returned. Means for calculating the unit volumes of the gas phase fluid and the liquid phase fluid in the fluid pipe from the liquid level detected by the liquid level detecting means, and calculating and calculating the weight from the unit volume of the liquid phase fluid. It is characterized by the following.
【0008】[0008]
【発明の実施の形態】気相流体乾き度検出手段で気相流
体の乾き度を検出し、液相流体液位重量検出手段で検出
した液位から流体配管内の液相と気相の単位容積を算出
して、気相の単位容積と乾き度から、気相流体中の気体
重量Sと液体重量Dを算出すると共に、液相の単位容積
から液相流体の重量D´を算出することによって、気液
二相流体の乾き度X=S/(S+D+D´)として流体
配管全体の乾き度又は湿り度を測定することができる。BEST MODE FOR CARRYING OUT THE INVENTION The dryness of a gas phase fluid is detected by a gas phase fluid dryness detecting means, and the unit of the liquid phase and the gas phase in the fluid pipe is measured from the liquid level detected by the liquid phase fluid level detecting means. Calculating the volume, calculating the gas weight S and the liquid weight D in the gas phase fluid from the unit volume and dryness of the gas phase, and calculating the weight D 'of the liquid phase fluid from the unit volume of the liquid phase Accordingly, the dryness or wetness of the entire fluid pipe can be measured as the dryness X = S / (S + D + D ′) of the gas-liquid two-phase fluid.
【0009】気相流体乾き度検出手段において、気相流
体の流下する配管に相対して取付けた超音波送受信器の
送信器から超音波信号を発信し、他方の受信器で受信す
る。流体中を通る超音波の伝搬時間Tは、超音波送受信
器間の距離をL、流体中の音速をCとすると、T=L/
Cであるので、これより、流体中の音速を求めることが
できる。また、流体中の音速は流体の乾き度によって変
化し、乾き度が低いほど音速は大きくなると言う関係が
ある。従って、この音速と乾き度の関係に基づいて、上
記の算出した音速から気相流体の乾き度又は湿り度を算
出することができる。In the gas-phase fluid dryness detecting means, an ultrasonic signal is transmitted from a transmitter of an ultrasonic transmitter / receiver attached to a pipe through which the gas-phase fluid flows, and received by the other receiver. The propagation time T of an ultrasonic wave passing through a fluid is represented by T = L / L, where L is the distance between the ultrasonic transceivers and C is the speed of sound in the fluid.
Since it is C, the sound velocity in the fluid can be obtained from this. Further, there is a relationship that the speed of sound in a fluid changes depending on the degree of dryness of the fluid, and the lower the degree of dryness, the higher the speed of sound. Therefore, based on the relationship between the sound speed and the dryness, the dryness or wetness of the gas phase fluid can be calculated from the calculated sound speed.
【0010】液相流体液位重量検出手段において、流体
配管の底部外面に取付けられた超音波送受信器の送信器
から上方に向けて放射された超音波が、液面で反射され
て受信器に戻ってくるまでの時間から流体配管内の液位
を検出する。この検出された液位から液相部と気相部の
面積を算出し流体配管の単位長さにおける液相と気相の
単位容積を算出することができる。また、算出した液相
の単位容積と比容積から液相流体の重量を算出すること
ができる。In the liquid-phase fluid level weight detecting means, the ultrasonic waves radiated upward from the transmitter of the ultrasonic transmitter / receiver attached to the bottom outer surface of the fluid pipe are reflected by the liquid surface and reflected to the receiver. The liquid level in the fluid pipe is detected from the time until it returns. The areas of the liquid phase portion and the gas phase portion are calculated from the detected liquid level, and the unit volumes of the liquid phase and the gas phase at the unit length of the fluid pipe can be calculated. Further, the weight of the liquid phase fluid can be calculated from the calculated unit volume and specific volume of the liquid phase.
【0011】[0011]
【実施例】本実施例においては、超音波を用いて、蒸気
とドレンの気液二相流体の乾き度を測定する例を説明す
る。図1において、被測定流体としての蒸気とドレンの
混合流体が左側から右側へ流下する蒸気配管1の途中
に、一対の超音波送信器2と受信器3を取り付ける。図
1は蒸気配管1の平面図であり、超音波送受信器2,3
は蒸気配管1のほぼ中央部に取り付ける。また、図2に
示すように、蒸気配管1の底部外面には、ドレンの液位
を検出するための一対の超音波送受信器4を取り付け
る。蒸気配管1の中では、上部に蒸気5が、下部にドレ
ン6が層状に流下し、更に蒸気5は乾き飽和蒸気と微細
な水滴が混合した所謂湿り蒸気状態のものである。EXAMPLE In this example, an example will be described in which the dryness of a gas-liquid two-phase fluid of steam and drain is measured using ultrasonic waves. In FIG. 1, a pair of ultrasonic transmitters 2 and a receiver 3 are attached in the middle of a steam pipe 1 in which a mixed fluid of steam and drain as a fluid to be measured flows down from left to right. FIG. 1 is a plan view of a steam pipe 1 and ultrasonic transceivers 2 and 3.
Is attached to almost the center of the steam pipe 1. As shown in FIG. 2, a pair of ultrasonic transceivers 4 for detecting the liquid level of the drain are attached to the outer surface of the bottom of the steam pipe 1. In the steam pipe 1, a steam 5 flows down in a layered manner at the upper part and a drain 6 flows down at a lower part, and the steam 5 is in a so-called wet steam state in which dry saturated steam and fine water droplets are mixed.
【0012】蒸気配管1には、内部の圧力を検出するた
めの圧力センサ7を取り付ける。超音波送受信器2,
3,4と圧力センサ7は、それぞれ図示しない演算制御
部に接続する。A pressure sensor 7 for detecting the internal pressure is attached to the steam pipe 1. Ultrasonic transceiver 2,
Each of the pressure sensors 3 and 4 and the pressure sensor 7 are connected to an arithmetic control unit (not shown).
【0013】気相流体乾き度検出手段としての超音波送
受信器2,3では、超音波の伝搬時間から蒸気5中の音
速を算出し、この算出した音速と圧力センサ7での圧力
値から蒸気5の乾き度X1を検出する。圧力が既知の場
合は、圧力センサ7は必ずしも必要ではない。The ultrasonic transmitters and receivers 2 and 3 as the gas-phase fluid dryness detecting means calculate the sound speed in the steam 5 from the propagation time of the ultrasonic wave, and calculate the steam speed from the calculated sound speed and the pressure value from the pressure sensor 7. A dryness X1 of 5 is detected. If the pressure is known, the pressure sensor 7 is not always necessary.
【0014】蒸気5中の音速と蒸気の乾き度X1には一
定の相関関係があり、音速が大きくなるほど乾き度X1
は低くなる。また、同一の音速であっても蒸気圧力が高
いほど乾き度X1は高くなる。従って、算出した音速と
検出された圧力から蒸気5の乾き度X1を検出すること
ができる。There is a certain correlation between the speed of sound in the steam 5 and the dryness X1 of the steam. As the speed of sound increases, the dryness X1 increases.
Will be lower. Even at the same sound speed, the higher the steam pressure, the higher the dryness X1. Therefore, the dryness X1 of the steam 5 can be detected from the calculated sound speed and the detected pressure.
【0015】次に、超音波送受信器4で、蒸気5とドレ
ン6の単位容積を検出する例を説明する。蒸気配管1の
底部外面に取り付けた超音波送受信器4を、図示しない
演算制御部に接続する。演算制御部には予め飽和蒸気及
び飽和水の比容積と蒸気圧力の関係を記憶しておく。Next, an example in which the ultrasonic transceiver 4 detects the unit volumes of the steam 5 and the drain 6 will be described. The ultrasonic transmitter / receiver 4 attached to the bottom outer surface of the steam pipe 1 is connected to an arithmetic control unit (not shown). The relation between the specific volume of the saturated steam and the saturated water and the steam pressure is stored in the arithmetic control unit in advance.
【0016】超音波送受信器4から、所定時間毎に蒸気
配管1の底部外面から上方に向けて超音波を放射し、ド
レン6の上液面で反射されて戻ってくるまでの時間から
蒸気配管1内の液位を検出し、検出した液位から所定管
径を有する蒸気配管1の蒸気部5の面積とドレン部6の
面積を算出し、算出した蒸気部5の面積とドレン部6の
面積から蒸気配管1の単位長さにおける蒸気5の単位容
積V1とドレン6の単位容積V2を算出する。The ultrasonic transmitter / receiver 4 emits an ultrasonic wave upward from the bottom outer surface of the steam pipe 1 every predetermined time, and is reflected from the upper liquid surface of the drain 6 and returned from the steam pipe 1. 1, the area of the steam section 5 and the area of the drain section 6 of the steam pipe 1 having a predetermined pipe diameter are calculated from the detected liquid level, and the calculated area of the steam section 5 and the area of the drain section 6 are calculated. The unit volume V1 of the steam 5 and the unit volume V2 of the drain 6 in the unit length of the steam pipe 1 are calculated from the area.
【0017】次に、蒸気5の容積V1と乾き度X1か
ら、蒸気5中の乾き飽和蒸気の重量Sと、蒸気5中に含
まれている微細な水滴状のドレンの重量Dを算出する。
即ち、X1=S/(S+D)で表され、X1が既に求ま
っており、同様に既知のV1におけるSとDの比率から
SとDを算出することができる。Next, from the volume V1 of the steam 5 and the dryness X1, the weight S of the dry saturated steam in the steam 5 and the weight D of the fine droplet-shaped drain contained in the steam 5 are calculated.
That is, X1 = S / (S + D), and X1 has already been obtained. Similarly, S and D can be calculated from the ratio of S and D in the known V1.
【0018】次に、算出したドレン6の単位容積V2
に、蒸気配管1内の圧力に基づく飽和水の比容積の逆数
を掛け合わせてドレン6の重量D´を算出して、蒸気5
とドレン6から成る二相流体の乾き度XをX=S/(S
+D+D´)として求めることができる。Next, the calculated unit volume V2 of the drain 6
Is multiplied by the reciprocal of the specific volume of the saturated water based on the pressure in the steam pipe 1 to calculate the weight D ′ of the drain 6,
X = S / (S
+ D + D ').
【0019】[0019]
【発明の効果】上記のように本発明によれば、気相流体
乾き度検出手段と液相流体液位重量検出手段とを具備し
て、それぞれの検出手段からの検出値から、流体配管中
に混在する層状の液体も含めた配管全体の流体の乾き度
又は湿り度を測定することができる。As described above, according to the present invention, a gas-phase fluid dryness detecting means and a liquid-phase fluid level weight detecting means are provided. It is possible to measure the dryness or wetness of the fluid in the entire pipe including the layered liquid mixed in the liquid.
【図1】本発明による二相流体の乾き度又は湿り度測定
装置の平面図。FIG. 1 is a plan view of an apparatus for measuring dryness or wetness of a two-phase fluid according to the present invention.
【図2】図1におけるA−A線断面図。FIG. 2 is a sectional view taken along line AA in FIG.
1 蒸気配管 2,3 超音波送受信器 4 超音波送受信器 5 蒸気部 6 ドレン部 7 圧力センサ DESCRIPTION OF SYMBOLS 1 Steam piping 2, 3 Ultrasonic transceiver 4 Ultrasonic transceiver 5 Steam section 6 Drain section 7 Pressure sensor
Claims (2)
するものにおいて、気相流体の流下する配管に相対して
取付けた超音波送受信器と、気相流体中を通る超音波の
伝搬時間から気相流体の乾き度又は湿り度を検出する気
相流体乾き度検出手段と、流体配管中の層状の液相流体
の液位から重量を検出する液相流体液位重量検出手段を
具備して、気相流体乾き度検出手段での検出値に、液相
流体液位重量検出手段からの検出値を加味して、気液二
相流体の乾き度又は湿り度を演算算出することを特徴と
する二相流体の乾き度又は湿り度測定装置。An apparatus for measuring the dryness or wetness of a gas-liquid two-phase fluid, comprising: an ultrasonic transmitter / receiver attached to a pipe through which a gas-phase fluid flows; Gas phase fluid dryness detecting means for detecting the dryness or wetness of the gaseous fluid from the propagation time, and liquid phase fluid level weight detecting means for detecting the weight from the level of the layered liquid phase fluid in the fluid piping. To calculate the dryness or wetness of a gas-liquid two-phase fluid by taking into account the value detected by the liquid-phase fluid liquid level weight detector in addition to the value detected by the gas-phase fluid dryness detector. An apparatus for measuring dryness or wetness of a two-phase fluid.
配管の底部外面に取付けられた超音波送受信器と、当該
超音波送受信器から上方に向けて放射された超音波が液
面で反射されて戻ってくるまでの時間から流体配管内の
液位を検出する液位検出手段を具備して、当該液位検出
手段で検出された液位から流体配管内の気相流体と液相
流体の単位容積を算出して、液相流体の単位容積から重
量を演算算出することを特徴とする請求項1に記載の二
相流体の乾き度又は湿り度測定装置。2. The liquid-phase fluid level weight detecting means includes: an ultrasonic transceiver mounted on an outer surface of a bottom of a fluid pipe; and an ultrasonic wave radiated upward from the ultrasonic transceiver at a liquid level. A liquid level detecting means for detecting a liquid level in the fluid pipe from a time until it is reflected and returned, and a gas phase fluid and a liquid phase in the fluid pipe based on the liquid level detected by the liquid level detecting means. The apparatus for measuring dryness or wetness of a two-phase fluid according to claim 1, wherein a unit volume of the fluid is calculated, and a weight is calculated from the unit volume of the liquid phase fluid.
Priority Applications (1)
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Publication number | Priority date | Publication date | Assignee | Title |
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JP2010517229A (en) * | 2007-01-26 | 2010-05-20 | ダイムラー・アクチェンゲゼルシャフト | Fuel cell system equipped with an ultrasonic detector |
CN104458904A (en) * | 2014-12-08 | 2015-03-25 | 北京航空航天大学 | Minor-caliber two-phase airflow detection device for filling up spacecraft propellants |
CN105181793A (en) * | 2015-05-14 | 2015-12-23 | 中国人民解放军国防科学技术大学 | Method for measurement of two-phase flow gas holdup based on ultrasonic two-frequency signal |
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JP2000121616A (en) * | 1998-10-15 | 2000-04-28 | Tlv Co Ltd | Fluid dryness measuring device |
JP2001027595A (en) * | 1999-07-15 | 2001-01-30 | Tlv Co Ltd | Steam dryness measuring apparatus |
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JP2000121616A (en) * | 1998-10-15 | 2000-04-28 | Tlv Co Ltd | Fluid dryness measuring device |
JP2001027595A (en) * | 1999-07-15 | 2001-01-30 | Tlv Co Ltd | Steam dryness measuring apparatus |
Cited By (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2010517229A (en) * | 2007-01-26 | 2010-05-20 | ダイムラー・アクチェンゲゼルシャフト | Fuel cell system equipped with an ultrasonic detector |
US9012048B2 (en) | 2007-01-26 | 2015-04-21 | Daimler Ag | Fuel cell system with ultrasonic detector |
CN104458904A (en) * | 2014-12-08 | 2015-03-25 | 北京航空航天大学 | Minor-caliber two-phase airflow detection device for filling up spacecraft propellants |
CN104458904B (en) * | 2014-12-08 | 2017-03-15 | 北京航空航天大学 | A kind of detection means of the pipe with small pipe diameter air-flow two phase flow for spacecraft propulsion agent filling |
CN105181793A (en) * | 2015-05-14 | 2015-12-23 | 中国人民解放军国防科学技术大学 | Method for measurement of two-phase flow gas holdup based on ultrasonic two-frequency signal |
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