JPH0758213B2 - Pulverized coal flow rate measuring method and device - Google Patents
Pulverized coal flow rate measuring method and deviceInfo
- Publication number
- JPH0758213B2 JPH0758213B2 JP27776289A JP27776289A JPH0758213B2 JP H0758213 B2 JPH0758213 B2 JP H0758213B2 JP 27776289 A JP27776289 A JP 27776289A JP 27776289 A JP27776289 A JP 27776289A JP H0758213 B2 JPH0758213 B2 JP H0758213B2
- Authority
- JP
- Japan
- Prior art keywords
- pulverized coal
- flow rate
- correlation
- phase fluid
- densitometer
- 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
Links
- 239000003245 coal Substances 0.000 title claims description 55
- 238000000034 method Methods 0.000 title claims description 14
- 239000012530 fluid Substances 0.000 claims description 27
- 238000005259 measurement Methods 0.000 claims description 26
- 238000006243 chemical reaction Methods 0.000 claims description 24
- 238000011144 upstream manufacturing Methods 0.000 claims description 24
- 239000000843 powder Substances 0.000 claims description 18
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical compound [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 claims description 10
- UQSXHKLRYXJYBZ-UHFFFAOYSA-N Iron oxide Chemical compound [Fe]=O UQSXHKLRYXJYBZ-UHFFFAOYSA-N 0.000 claims description 8
- 229910052742 iron Inorganic materials 0.000 claims description 5
- JRPBQTZRNDNNOP-UHFFFAOYSA-N barium titanate Chemical compound [Ba+2].[Ba+2].[O-][Ti]([O-])([O-])[O-] JRPBQTZRNDNNOP-UHFFFAOYSA-N 0.000 claims description 4
- 229910002113 barium titanate Inorganic materials 0.000 claims description 4
- 238000001514 detection method Methods 0.000 description 6
- 239000002245 particle Substances 0.000 description 5
- 230000008878 coupling Effects 0.000 description 3
- 238000010168 coupling process Methods 0.000 description 3
- 238000005859 coupling reaction Methods 0.000 description 3
- 238000010586 diagram Methods 0.000 description 3
- 238000010248 power generation Methods 0.000 description 3
- 239000002994 raw material Substances 0.000 description 2
- 239000000126 substance Substances 0.000 description 2
- 229910000831 Steel Inorganic materials 0.000 description 1
- 239000000571 coke Substances 0.000 description 1
- 239000008187 granular material Substances 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 239000000203 mixture Substances 0.000 description 1
- 239000010959 steel Substances 0.000 description 1
Landscapes
- Measuring Volume Flow (AREA)
Description
【発明の詳細な説明】 〔産業上の利用分野〕 本発明は,配管を介して搬送される微粉炭と気体の二相
流体の流量を,濃度計と相関流速計により測定するに際
し,測定の信頼性を向上せしめた方法及び装置に関す
る. 〔従来の技術〕 粉体と気体の二相流体を配管を介して搬送するに際し,
その流量を測定する技術としては,特開昭58−190719号
に開示されるような相関式流量測定装置が公知である. この公知の装置は,第3図に示すように,二相流体を搬
送する配管1の一部分に,該配管内の流路に臨む濃度計
2と相関流速計3とを設けている. 前記濃度計2は,流路を挟んで設けられた幅の広い濃度
検出用電極4a,4bを有し,該電極4a,4b間を通過する粉体
による静電容量の増加分を検知し,これを電気信号に変
換して濃度信号ρを出力する. 前記相関流速計3は,流体の搬送方向Fに対して距離L
を置いて配置された上流側検知器5と下流側検知器6と
から成り,それぞれ流路を挟んで設けられた幅の狭い流
速検出用電極5a,5b並びに6a,6bを有する.この相関流速
計3を通過する粉体による静電容量の変化分は電気信号
に変換され,上流側検知器5により検知された上流側電
気信号U1と,下流側検知器6により検知された下流側電
気信号U2を出力する.第4図に示すように,前記の上流
側電気信号U1と下流側電気信号U2との間の相互相関係数
から両信号間の遅れ時間γを求めることができる.即
ち,これらの両信号U1及びU2は,所謂ゆらぎ信号として
遅れ時間γで伝わっているから,粉体の流速vは,前記
一対の検知器5,6の距離Lと,前記遅れ時間γから, v=L/γ として求められる. この際,前記粉体の濃度ρは,濃度に比例した静電容量
の変化として連続的に測定されるため,配管1の断面積
をDとすると,粉体の流量Qは, Q=v×ρ×D として求められる. このように,公知の装置では,相関法で求められた遅れ
時間γと,濃度信号ρを用いて二相流体中の粉体の流量
を演算により求めることができる. 〔発明が解決しようとする課題〕 前記公知の装置は,二相流体中の粉体の流量を測定する
ために提案されている多くの技術のうち,理論的実用的
に最も優れている. ところが,本発明者らは,この公知の装置を微粉炭の流
量測定のために実施する場合には,所期の目的を達し得
ないことを知見した. 即ち,前述のように,公知の装置において粉体の流速を
測定するためには,上流側検知器5と下流側検知器6に
おけるそれぞれの流速検出用電極5a,5b並びに6a,6bによ
り,通過する粉体の静電容量の変化を検知し,時間差と
して現れる上流側電気信号U1と下流側電気信号U2の所謂
ゆらぎ信号としての遅れ時間γを検出しなければならな
い. 然しながら,微粉炭の場合,比誘電率(真空の誘電率と
の比)が小さいため(一般的に比誘電率=2〜3といわ
れている),検知器5,6における前記静電容量の変化に
乏しく,電気信号U1及びU2に顕在的な波形を得ることが
できない.即ち,第5図示のように,電気信号U1及びU2
における波形のピークが極めて小さく,所謂ゆらぎ信号
としての時間差による前記遅れ時間γを検知することが
困難である. このため,微粉炭の流量を測定するためには前記公知の
装置は適当でなく,別途,新たな発明を期待しなければ
ならない. ところで,鉄鋼分野においては,高炉の羽口で燃焼でき
る微粉炭の量は120kg/T pigであるといわれているが,
適切な計器が存在しないため,分配器の分配精度内で操
業が行われている.その分配精度は3δ(δ:標準偏
差)約±40kg/T pigであるため,実際には前記120kg/T
pigよりも40kg/T pig低い80kg/T pigで操業がなされて
いる.従って,微粉炭の流量を測定し制御することが可
能になれば,現状よりも微粉炭を40kg/T pig多く装入す
ることができることになり,これに応じてコークス(28
円/kg)を微粉炭(8円/kg)に代えることにより,製鉄
原価を大幅に低減することが可能になる. また,電力分野においては,原子力発電には事故や立地
条件に問題があり,また,ガスによる火力発電には原料
供給に問題があるため,石炭による火力発電が望まれて
いる.然し,良質炭の資源は乏しくなりつつあるから,
豊富にある劣質炭を利用しなければならないところ,微
粉炭の流量測定が可能にならなければ実現困難である.
即ち,劣質炭を高温で燃焼するためには,空気と石炭の
流量比を正確に保つ必要があり,微粉炭と空気との高精
度の混合比を測定し制御しなければならないからであ
る. 〔課題を解決するための手段〕 本発明は,上述した公知の装置を改良することにより,
微粉炭の流量を正確に測定することができるようにした
方法及び装置を提供するものである. このため,本発明方法が手段として構成したところは,
微粉炭と気体の二相流体の流路に臨んで設けた濃度計と
相関流速計により該二相流体の流量を測定する方法であ
って:前記相関流速計よりも上流側の流路において,前
記二相流体中に微粉炭よりも比誘電率を大とした計測反
応促進剤を添加する点にある.この際,前記計測反応促
進剤は,前記濃度計よりも下流側かつ前記相関流速計よ
りも上流側の流路において添加することが好ましい. また,本発明装置が手段として構成したところは,微粉
炭と気体の二相流体の流路に臨んで設けられる濃度計及
び相関流速計と;前記濃度計よりも下流側かつ相関流速
計よりも上流側において二相流体中に微粉炭よりも比誘
電率を大とした計測反応促進剤を添加するための促進剤
供給装置と;を備えて成る点にある. 本発明方法又は装置において使用する計測反応促進剤
は,微粉炭よりも比誘電率が大なる物質から成る粉体で
あれば良いが,鉄,酸化鉄,チタン酸バリウムから選ば
れた粉体とすることが好ましい. 〔実施例〕 以下図面に基づいて本発明の1実施例を詳述する. 第1図において,配管11は,微粉炭12と気体13の二相流
体14を搬送するものであり,該配管11の内部に搬送方向
Fに搬送される流体14の流路15を形成する. 前記配管11には,流路15に臨んで濃度計16と相関流速計
17とを設け,前記搬送方向Fに対して,前記濃度計16よ
りも下流側でかつ前記相関流速計17よりも上流側の流路
15において,計測反応促進剤18の供給装置19を設けてい
る. 前記濃度計16は,上述した公知の装置と同様に,流路15
を挟んで設けられた幅の広い濃度検出用電極16a,16bを
有し,該電極16a,16bの間を通過する微粉炭12による静
電容量の増加分を検知し,これを電気信号に変換して濃
度信号ρを出力する.尚,この濃度計16は,配管11の所
定個所に介装されるカップリング構造のものとしておく
ことが好ましい. 前記相関流速計17は,上述した公知の装置と同様に,流
路15の搬送方向Fに対して距離Lを置いて配置された上
流側検知器20と下流側検知器21とから成り,それぞれ流
路15を挟んで設けられた幅の狭い流速検出用電極20a,20
b並びに21a,21bを有する.従って,この相関流速計17を
通過する微粉炭12による静電容量の変化分は電気信号に
変換され,上流側検知器20により検知された上流側電気
信号U1と,下流側検知器21により検知された上流側電気
信号U2を出力し,後述するような両信号間の遅れ時間γ
を示すことができる.尚,この相関流速計17も,配管11
の所定個所に介装されるカップリング構造のものとして
おくことが好ましい. 前記計測反応促進剤18の供給装置19は,ホッパー又はタ
ンク等の貯留体22に計測反応促進剤18を貯留せしめ,該
貯留体22より制御弁23を介して計測反応促進剤18を流路
15内に導く供給路24を備えている.計測反応促進剤18を
貯留体22から流路15内に供給するための駆動源として
は,二相流体14が流送されている流路15内の負圧を利用
して,制御弁23を開放したとき貯留体22内の計測反応促
進剤18が自動的に流路15内に吸引される構成とすること
ができる.或いは,貯留体22にポンプ等の駆動装置を接
続し,計測反応促進剤18を強制的に流路15内に供給させ
るように構成しても良い.尚,この促進剤供給装置19
も,配管11の所定個所に介装されるカップリング構造の
ものとしておくことが好ましい. 前記計測反応促進剤18は,微粉炭よりも比誘電率を大と
した物質から成る粒体又は粉体であれば良く,その材質
を特に限定するものではない.然しながら、本発明装置
を高炉における微粉炭供給設備に実施する場合において
は,高炉原料中に混入しても支障がないことや,比誘電
率が微粉炭よりも顕著に大きいことや,コスト面を勘案
すると,計測反応促進剤18を鉄及び/又は酸化鉄の粒体
又は粉体とすることが最も良い.その他,計測反応促進
剤18として,比較的低コストであり比誘電率の高いチタ
ン酸バリウムの粒体又は粉体を用いても良い.これらの
計測反応促進剤18の粒径は,搬送されている微粉炭12の
粒径とほぼ同程度のものが好ましい. 以上の構成において,前記制御弁23は,本発明により微
粉炭の流量を測定するに際し,その都度,一時的に所定
量だけ開放され,貯留体22内の計測反応促進剤18を必要
量だけ流路15内に供給する.供給された促進剤18は,流
路15内で流送される二相流体14に混合され,微粉炭12と
同速度で搬送方向Fに送られ,相関流速計17を通過す
る.この際,計測反応促進剤18は,微粉炭12よりも比誘
電率が大であるため,上流側検知器20及び下流側検知器
21の流速検出用電極20a,20b並びに21a,21bに大きな静電
容量の変化分として検出され,その結果,両検知器20及
び21により出力される上流側電気信号U1及び下流側電気
信号U2の波形は,第5図に示した従来の場合に比し大き
く顕在化し,第2図示のような波形を示すことになる.
このため,このような信号U1及びU2の所謂ゆらぎ信号と
しての遅れ時間γを求めることが容易となり,微粉炭12
の流速v(v=L/γ)を確実に求めることが可能にな
る. そこで,この流速vと,上述した濃度ρとを求めること
により,配管11の断面積D内における微粉炭12の流量Q
(Q=v×ρ×D)を演算により求めるものであること
は,上述した公知の装置と同様である. 尚,濃度計16を促進剤供給装置19よりも下流側に設置し
ても良いが,この場合は,指示された濃度の値ρが促進
剤18と微粉炭12の混合体の濃度を示すので,該値ρから
促進剤18を除くための補正演算をしなければならない.
これに対して,上記実施例のように,濃度計16を促進剤
供給装置19よりも上流側に設置しておくと,指示された
濃度の値ρは微粉炭12のみの濃度を示すので,補正の必
要がない. 〔発明の効果〕 本発明によれば,濃度計と相関流速計を用いた従来の二
相流体の流量測定方法及び/又は装置を,微粉炭と気体
の二相流体に適用するに際し,相関流速計の上流側にて
微粉炭よりも比誘電率を大とした計測反応促進剤を添加
するので,相関流速計による上流側電気信号と下流側電
気信号の所謂ゆらぎ信号の波形を顕在化し,両信号の時
間遅れを確実容易に検出し,以て,微粉炭の流速を的確
に検出することができる.このため,従来の相関流速計
では測定困難と考えられた微粉炭の流量を容易に測定す
ることが可能となり,微粉炭を利用した各種技術分野の
発展に貢献できるという効果がある.DETAILED DESCRIPTION OF THE INVENTION [Industrial field of application] The present invention relates to the measurement of the flow rate of a two-phase fluid of pulverized coal and gas conveyed through a pipe by a densitometer and a correlation anemometer. The present invention relates to a method and apparatus with improved reliability. [Prior Art] When transferring a two-phase fluid of powder and gas through a pipe,
As a technique for measuring the flow rate, a correlation type flow rate measuring device as disclosed in JP-A-58-190719 is known. As shown in FIG. 3, this known device is provided with a densitometer 2 and a correlation velocity meter 3 which face a flow path in the pipe, in a part of the pipe 1 which conveys a two-phase fluid. The densitometer 2 has wide concentration detecting electrodes 4a, 4b provided across a flow path, and detects an increase in capacitance due to powder passing between the electrodes 4a, 4b, This is converted into an electric signal and the concentration signal ρ is output. The correlation velocity meter 3 has a distance L with respect to the fluid transport direction F.
It is composed of an upstream side detector 5 and a downstream side detector 6 which are arranged side by side, and each has a narrow flow velocity detecting electrode 5a, 5b and 6a, 6b which are provided across the flow path. The amount of change in capacitance due to the powder passing through the correlation anemometer 3 is converted into an electric signal, and the upstream electric signal U1 detected by the upstream detector 5 and the downstream electric signal detected by the downstream detector 6 The side electric signal U2 is output. As shown in FIG. 4, the delay time γ between the upstream electric signal U1 and the downstream electric signal U2 can be obtained from the cross-correlation coefficient between the two signals. That is, since both of these signals U1 and U2 are transmitted as a so-called fluctuation signal with the delay time γ, the powder flow velocity v is calculated from the distance L between the pair of detectors 5 and 6 and the delay time γ. It is calculated as v = L / γ. At this time, the concentration ρ of the powder is continuously measured as a change in capacitance proportional to the concentration. Therefore, when the cross-sectional area of the pipe 1 is D, the flow rate Q of the powder is Q = v × It is calculated as ρ × D. Thus, in the known device, the flow rate of powder in the two-phase fluid can be calculated by using the delay time γ obtained by the correlation method and the concentration signal ρ. [Problems to be Solved by the Invention] The known device is theoretically most practically excellent among many techniques proposed for measuring the flow rate of powder in a two-phase fluid. However, the present inventors have found that when this known device is used for measuring the flow rate of pulverized coal, the intended purpose cannot be achieved. That is, as described above, in order to measure the flow velocity of the powder in the known device, the flow velocity detection electrodes 5a, 5b and 6a, 6b in the upstream side detector 5 and the downstream side detector 6 are used to pass the particles. It is necessary to detect the change in the electrostatic capacity of the powder, and detect the delay time γ as a so-called fluctuation signal of the upstream electric signal U1 and the downstream electric signal U2 that appear as a time difference. However, in the case of pulverized coal, the relative dielectric constant (ratio with the dielectric constant of vacuum) is small (generally said to be 2 to 3), so The change is scarce and no obvious waveform can be obtained for the electric signals U1 and U2. That is, as shown in FIG. 5, electrical signals U1 and U2
The peak of the waveform at is extremely small, and it is difficult to detect the delay time γ due to the time difference as a so-called fluctuation signal. Therefore, the above-mentioned known device is not suitable for measuring the flow rate of pulverized coal, and a new invention must be expected separately. By the way, in the steel field, the amount of pulverized coal that can be burned at the tuyere of a blast furnace is said to be 120 kg / T pig.
Since there is no suitable instrument, operation is performed within the distribution accuracy of the distributor. Since the distribution accuracy is 3δ (δ: standard deviation) about ± 40kg / T pig, the above 120kg / T is actually used.
It is operated at 80kg / T pig which is 40kg / T pig lower than pig. Therefore, if it becomes possible to measure and control the flow rate of pulverized coal, it will be possible to load more pulverized coal by 40 kg / T pig than at present, and the coke (28
By replacing pulverized coal (8 yen / kg) with pulverized coal (8 yen / kg), it is possible to significantly reduce the cost of iron making. In the electric power field, nuclear power generation has problems in accidents and location conditions, and gas power generation has problems in raw material supply, so coal power generation is desired. However, the resources of good quality coal are becoming scarce,
Where abundant inferior coal must be used, it is difficult to achieve it unless pulverized coal flow rate measurement is possible.
That is, in order to burn inferior coal at high temperature, it is necessary to keep the flow rate ratio of air and coal accurate, and it is necessary to measure and control the highly accurate mixing ratio of pulverized coal and air. [Means for Solving the Problems] The present invention is achieved by improving the above-mentioned known device.
It is intended to provide a method and an apparatus capable of accurately measuring the flow rate of pulverized coal. Therefore, the place where the method of the present invention is configured as means is as follows.
A method for measuring the flow rate of a two-phase fluid by a densitometer and a correlation velocimeter provided facing a two-phase fluid flow of pulverized coal and gas: in a flow channel upstream of the correlation velocimeter, The point is to add a measurement reaction accelerator having a relative dielectric constant larger than that of pulverized coal to the two-phase fluid. At this time, it is preferable that the measurement reaction accelerator is added in a flow path downstream of the concentration meter and upstream of the correlation anemometer. Further, the device of the present invention is configured as a means: a densitometer and a correlation anemometer which are provided so as to face a flow path of a pulverized coal and a gas two-phase fluid; On the upstream side, a two-phase fluid is provided with a promoter supply device for adding a measurement reaction promoter having a relative dielectric constant larger than that of pulverized coal; The measurement reaction accelerator used in the method or apparatus of the present invention may be a powder made of a substance having a relative dielectric constant larger than that of pulverized coal, but a powder selected from iron, iron oxide and barium titanate may be used. Preferably. Embodiment An embodiment of the present invention will be described in detail below with reference to the drawings. In FIG. 1, a pipe 11 conveys a two-phase fluid 14 of pulverized coal 12 and a gas 13, and forms a flow path 15 for the fluid 14 conveyed in a conveyance direction F inside the pipe 11. In the pipe 11, the densitometer 16 and the correlation velocity meter are provided facing the flow path 15.
And a flow path downstream of the concentration meter 16 and upstream of the correlation anemometer 17 with respect to the transport direction F.
In 15, a supply device 19 for the measurement reaction accelerator 18 is provided. The densitometer 16 has a flow path 15 similar to the known device described above.
It has electrodes for wide concentration detection 16a, 16b sandwiched between the electrodes, detects the increase in capacitance due to the pulverized coal 12 passing between the electrodes 16a, 16b, and converts this to an electric signal. And output the concentration signal ρ. In addition, it is preferable that the densitometer 16 has a coupling structure that is interposed at a predetermined position of the pipe 11. The correlation anemometer 17 is composed of an upstream side detector 20 and a downstream side detector 21 which are arranged at a distance L with respect to the transport direction F of the flow path 15, like the above-mentioned known device, Narrow flow velocity detection electrodes 20a, 20 provided across the flow path 15
It has b and 21a and 21b. Therefore, the amount of change in the electrostatic capacitance due to the pulverized coal 12 passing through the correlation anemometer 17 is converted into an electric signal and detected by the upstream electric signal U1 detected by the upstream detector 20 and the downstream detector 21. The upstream upstream electric signal U2 is output, and the delay time γ
Can be shown. The correlation velocity meter 17 is also connected to the pipe 11
It is preferable to have a coupling structure that is inserted at a predetermined position of. The supply device 19 for the measurement reaction accelerator 18 stores the measurement reaction accelerator 18 in a reservoir 22 such as a hopper or a tank, and the measurement reaction accelerator 18 is flown from the reservoir 22 via a control valve 23.
It is equipped with a supply path 24 that leads into the inside of the unit. As a drive source for supplying the measurement reaction promoter 18 from the reservoir 22 into the flow path 15, the negative pressure in the flow path 15 through which the two-phase fluid 14 is sent is used to control the control valve 23. The measurement reaction accelerator 18 in the reservoir 22 can be automatically sucked into the flow path 15 when opened. Alternatively, a driving device such as a pump may be connected to the reservoir 22 so that the measurement reaction accelerator 18 is forcibly supplied into the flow path 15. This accelerator supply device 19
Also, it is preferable to use a coupling structure that is installed at a predetermined position of the pipe 11. The measurement reaction accelerator 18 may be a granular material or a powder made of a substance having a relative dielectric constant larger than that of pulverized coal, and the material thereof is not particularly limited. However, when the device of the present invention is applied to a pulverized coal supply facility in a blast furnace, there is no problem even if it is mixed in the blast furnace raw material, the relative dielectric constant is significantly larger than that of the pulverized coal, and the cost is low. Considering this, it is best to use iron and / or iron oxide particles or powder as the measurement reaction accelerator 18. In addition, as the measurement reaction accelerator 18, particles or powder of barium titanate having a relatively low cost and a high relative dielectric constant may be used. The particle size of these measurement reaction accelerators 18 is preferably approximately the same as the particle size of the pulverized coal 12 being conveyed. In the above configuration, the control valve 23 is temporarily opened by a predetermined amount each time when measuring the flow rate of pulverized coal according to the present invention, and the measurement reaction accelerator 18 in the storage body 22 is caused to flow by the required amount. Supply into path 15. The supplied accelerator 18 is mixed with the two-phase fluid 14 sent in the flow path 15, sent in the conveying direction F at the same speed as the pulverized coal 12, and passes through the correlation velocity meter 17. At this time, since the measurement reaction accelerator 18 has a larger relative dielectric constant than the pulverized coal 12, the upstream side detector 20 and the downstream side detector 20
The flow velocity detection electrodes 20a, 20b and 21a, 21b of 21 are detected as a large change in capacitance, and as a result, the upstream electric signal U1 and the downstream electric signal U2 output by both detectors 20 and 21 are detected. The waveform is much more obvious than the conventional case shown in FIG. 5, and the waveform shown in FIG. 2 is shown.
Therefore, it becomes easy to obtain the delay time γ as a so-called fluctuation signal of such signals U1 and U2, and the pulverized coal 12
The flow velocity v (v = L / γ) can be reliably obtained. Therefore, by obtaining the flow velocity v and the above-mentioned concentration ρ, the flow rate Q of the pulverized coal 12 in the cross-sectional area D of the pipe 11 is obtained.
The fact that (Q = v × ρ × D) is calculated is the same as in the above-described known device. The densitometer 16 may be installed on the downstream side of the accelerator supply device 19, but in this case, the indicated concentration value ρ indicates the concentration of the mixture of the accelerator 18 and the pulverized coal 12. , A correction calculation must be performed to remove the accelerator 18 from the value ρ.
On the other hand, when the densitometer 16 is installed upstream of the accelerator supply device 19 as in the above embodiment, the indicated concentration value ρ indicates the concentration of the pulverized coal 12 only. There is no need for correction. [Advantage of the Invention] According to the present invention, when applying the conventional two-phase fluid flow rate measuring method and / or apparatus using a densitometer and a correlation velocity meter to a two-phase fluid of pulverized coal and gas, the correlation velocity On the upstream side of the meter, a measurement reaction accelerator with a relative dielectric constant larger than that of pulverized coal is added, so the so-called fluctuation signal waveform of the upstream side electrical signal and the downstream side electrical signal by the correlation anemometer is revealed and both The time delay of the signal can be detected reliably and easily, and thus the flow rate of the pulverized coal can be detected accurately. For this reason, it becomes possible to easily measure the flow rate of pulverized coal, which was considered difficult to measure by the conventional correlation anemometer, and there is an effect that it can contribute to the development of various technical fields using pulverized coal.
第1図は本発明の1実施例を示す断面図,第2図(1)(2)
は同実施例における相関流速計により出力される所謂ゆ
らぎ信号の波形図,第3図は従来例に係る二相流体の流
量測定装置を示す断面図,第4図(1)(2)は同従来例にお
ける相関流速計により出力される所謂ゆらぎ信号の理想
的な波形図,第5図(1)(2)は同従来例を微粉炭に実施し
た場合の相関流速計により出力される所謂ゆらぎ信号の
波形図である. 11……配管,12……微粉炭,13……気体,14……二相流体,
15……流路,16……濃度計,16a,16b……濃度検出用電極,
17……相関流速計,18……計測反応促進剤,19……促進剤
供給装置,20……上流側検知器,21……下流側検知器,20
a,20b,21a,21b……流速検出用電極.FIG. 1 is a sectional view showing an embodiment of the present invention, and FIGS. 2 (1) (2).
Is a waveform diagram of a so-called fluctuation signal output by the correlation anemometer in the same embodiment, FIG. 3 is a sectional view showing a two-phase fluid flow rate measuring device according to a conventional example, and FIGS. 4 (1) (2) are the same. An ideal waveform diagram of the so-called fluctuation signal output by the correlation velocity meter in the conventional example, Fig. 5 (1) and (2) are so-called fluctuations output by the correlation velocity meter when the conventional example is applied to pulverized coal. It is a waveform diagram of the signal. 11 …… Piping, 12 …… Pulverized coal, 13 …… Gas, 14 …… Two-phase fluid,
15 …… flow path, 16 …… densitometer, 16a, 16b …… concentration detection electrodes,
17 …… Correlation velocity meter, 18 …… Measurement reaction accelerator, 19 …… Accelerator supply device, 20 …… Upstream detector, 21 …… Downstream detector, 20
a, 20b, 21a, 21b ... Electrodes for flow velocity detection.
Claims (5)
けた濃度計と相関流速計により該二相流体の流量を測定
する方法であって:前記相関流速計(17)よりも上流側の
流路において,前記二相流体中に微粉炭よりも比誘電率
を大とした計測反応促進剤(18)を添加することを特徴と
する微粉炭の流量測定方法.1. A method for measuring the flow rate of a two-phase fluid by a densitometer and a correlation velocimeter provided facing a flow path of a two-phase fluid of pulverized coal and gas, comprising: from the correlation velocimeter (17). Also in the upstream flow path, a method for measuring the flow rate of pulverized coal, characterized in that a measurement reaction accelerator (18) having a larger relative dielectric constant than pulverized coal is added to the two-phase fluid.
けた濃度計と相関流速計により該二相流体の流量を測定
する方法であって:前記濃度計(16)よりも下流側かつ前
記相関流速計(17)よりも上流側の流路において,前記二
相流体中に微粉炭よりも比誘電率を大とした計測反応促
進剤(18)を添加することを特徴とする微粉炭の流量測定
方法.2. A method for measuring the flow rate of a two-phase fluid by a densitometer and a correlation velocity meter provided facing a flow path of a two-phase fluid of pulverized coal and gas, which is more than the densitometer (16). In the flow path on the downstream side and on the upstream side of the correlation anemometer (17), a measurement reaction accelerator (18) having a relative dielectric constant larger than that of pulverized coal is added to the two-phase fluid. How to measure the flow rate of pulverized coal.
チタン酸バリウムから選ばれた粉体であることを特徴と
する特許請求の範囲第1項又は第2項に記載の微粉炭の
流量測定方法.3. The measurement reaction accelerator (18) is iron, iron oxide,
The method for measuring the flow rate of pulverized coal according to claim 1 or 2, wherein the powder is a powder selected from barium titanate.
けられる濃度計及び相関流速計と;前記濃度計(16)より
も下流側かつ相関流速計(17)よりも上流側において二相
流体中に微粉炭よりも比誘電率を大とした計測反応促進
剤(18)を添加するための促進剤供給装置(19)と;を備え
て成ることを特徴とする微粉炭の流量測定装置.4. A densitometer and a correlation anemometer which are provided so as to face a flow path of a pulverized coal and a gas two-phase fluid; a downstream side of the densitometer (16) and an upstream side of the correlation anemometer (17). Of the pulverized coal, comprising: an accelerator supply device (19) for adding a measurement reaction accelerator (18) having a relative dielectric constant larger than that of the pulverized coal in the two-phase fluid. Flow rate measuring device.
チタン酸バリウムから選ばれた粉体であることを特徴と
する特許請求の範囲第4項に記載の微粉炭の流量測定装
置.5. The measurement reaction accelerator (18) is iron, iron oxide,
The pulverized coal flow rate measuring device according to claim 4, wherein the powder is selected from barium titanate.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP27776289A JPH0758213B2 (en) | 1989-10-24 | 1989-10-24 | Pulverized coal flow rate measuring method and device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP27776289A JPH0758213B2 (en) | 1989-10-24 | 1989-10-24 | Pulverized coal flow rate measuring method and device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH03138534A JPH03138534A (en) | 1991-06-12 |
| JPH0758213B2 true JPH0758213B2 (en) | 1995-06-21 |
Family
ID=17587982
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP27776289A Expired - Fee Related JPH0758213B2 (en) | 1989-10-24 | 1989-10-24 | Pulverized coal flow rate measuring method and device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0758213B2 (en) |
Families Citing this family (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| DE4406046C2 (en) * | 1994-02-24 | 1997-11-20 | Wagner Int | Device and method for measuring a powder mass flow |
| DE19947394A1 (en) * | 1999-10-01 | 2001-05-03 | Dynatechnik Messysteme Gmbh | Method and device for measuring bulk material flows |
| JP2006077267A (en) * | 2004-09-07 | 2006-03-23 | Nippon Steel Corp | Powder blowing equipment |
| CN100582682C (en) | 2007-06-27 | 2010-01-20 | 清华大学 | Device and method for measuring parameters of gas-solid two-phase flow in square pneumatic conveying pipeline |
| DE102017113453A1 (en) * | 2017-06-19 | 2018-12-20 | Krohne Ag | Flow sensor, method and flowmeter for determining velocities of phases of a multiphase medium |
| CN113800223A (en) * | 2021-10-11 | 2021-12-17 | 中国神华能源股份有限公司哈尔乌素露天煤矿 | Method, device and system for detecting coal conveying amount of belt conveyor |
-
1989
- 1989-10-24 JP JP27776289A patent/JPH0758213B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JPH03138534A (en) | 1991-06-12 |
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