JPH058367B2 - - Google Patents
Info
- Publication number
- JPH058367B2 JPH058367B2 JP20794783A JP20794783A JPH058367B2 JP H058367 B2 JPH058367 B2 JP H058367B2 JP 20794783 A JP20794783 A JP 20794783A JP 20794783 A JP20794783 A JP 20794783A JP H058367 B2 JPH058367 B2 JP H058367B2
- Authority
- JP
- Japan
- Prior art keywords
- flow rate
- powder
- pulverized coal
- granular material
- pressure
- 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 - Lifetime
Links
- 239000000843 powder Substances 0.000 claims description 32
- 239000008187 granular material Substances 0.000 claims description 30
- 238000000034 method Methods 0.000 claims description 11
- 230000005514 two-phase flow Effects 0.000 claims description 10
- 239000007789 gas Substances 0.000 claims description 8
- 239000012159 carrier gas Substances 0.000 claims description 3
- 238000000691 measurement method Methods 0.000 claims description 2
- 239000003245 coal Substances 0.000 description 26
- 238000005259 measurement Methods 0.000 description 7
- 238000002347 injection Methods 0.000 description 5
- 239000007924 injection Substances 0.000 description 5
- 238000001514 detection method Methods 0.000 description 4
- 239000012530 fluid Substances 0.000 description 4
- 238000002485 combustion reaction Methods 0.000 description 3
- 239000002245 particle Substances 0.000 description 3
- 230000005856 abnormality Effects 0.000 description 2
- 238000007664 blowing Methods 0.000 description 2
- 238000006243 chemical reaction Methods 0.000 description 2
- 239000000446 fuel Substances 0.000 description 2
- 230000010349 pulsation Effects 0.000 description 2
- 208000035874 Excoriation Diseases 0.000 description 1
- 238000005299 abrasion Methods 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 238000002474 experimental method Methods 0.000 description 1
- 238000002309 gasification Methods 0.000 description 1
- 230000005484 gravity Effects 0.000 description 1
- 230000002452 interceptive effect Effects 0.000 description 1
- 238000012545 processing Methods 0.000 description 1
- 238000011160 research Methods 0.000 description 1
- 239000007787 solid Substances 0.000 description 1
- 230000004580 weight loss Effects 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01F—MEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
- G01F1/00—Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow
- G01F1/74—Devices for measuring flow of a fluid or flow of a fluent solid material in suspension in another fluid
Landscapes
- Physics & Mathematics (AREA)
- Fluid Mechanics (AREA)
- General Physics & Mathematics (AREA)
- Measuring Volume Flow (AREA)
- Measurement Of Mechanical Vibrations Or Ultrasonic Waves (AREA)
Description
【発明の詳細な説明】
本発明は、各種粉粒体が気体中に分散されて流
れている状態、即ち固気2相流(以下単に2相流
ということがある)における粉粒体の流量測定方
法に関し、特に2相流の流れを阻害することな
く、該粉粒体の流量を正確且つ簡単に測定するこ
とのできる方法に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to the flow rate of powder and granular materials in a state in which various powder and granular materials are dispersed in a gas, that is, solid-gas two-phase flow (hereinafter sometimes simply referred to as two-phase flow). The present invention relates to a measuring method, and particularly to a method that can accurately and easily measure the flow rate of the powder without interfering with the flow of the two-phase flow.
粉粒体を貯蔵容器から他の場所へ輸送する方法
として気流輸送方式が汎用されている。この場合
の粉粒体流量の測定は、貯蔵容器に取付けた歪ゲ
ージによつて該容器内における粉粒体の減量を測
定し、単位時間当りの平均流量に演算して求めて
いるのが普通である。この為、例えば数分間程度
の短かい時間における粉粒体の流量変動を測定す
ることはできない。また例えば高炉への微粉炭吹
込みの様に、1個の貯蔵容器から30本前後の羽口
へ微粉炭を分配輸送する場合には、全体としての
吹込量は知ることができても個々の羽口から送給
される微粉炭量を把握することはできず、一部の
輸送管路で送給不良が生じてもその状況を正確に
把握することができない。その為個々の輸送管路
毎に粉粒体流量を測定することのできる様な技術
が開発されつつあり、例えば気流輸送管内の差圧
や静電容量から粉粒体流量を測定する方法、或は
2相流で輸送される粉粒体に超音波を投射して流
量を測定する超音波ドプラー方式等が提案されて
いる。しかしながらこれら公知の方法は測定精度
の点で問題があり、満足し得るものとは言い難
い。即ち固気2相流は、比重が著しく異なる固体
と気体の混成流である為、輸送管内の粉粒体濃度
は相当片寄つており、例えば水平配管中では上層
が薄く下層が濃くなるとか、更には粒子の寸法が
不均一である為各粒子の挙動が複雑で流動状況が
安定しないといつた固有の問題を有している。し
かも2相流の流路に流量検知部材を配置する方法
では、粉粒体の衝突による検知部材の摩耗を避け
ることができず、更に該検知部材により流れが阻
害されて管詰りを生じ易くなるという問題もあ
る。 An air flow transport method is commonly used as a method for transporting powder and granular materials from a storage container to another location. In this case, the flow rate of the powder or granule is usually measured by measuring the weight loss of the powder or granule in the storage container using a strain gauge attached to the container, and calculating the average flow rate per unit time. It is. For this reason, it is not possible to measure the fluctuation in the flow rate of powder or granular material over a short period of time, for example, several minutes. Furthermore, when pulverized coal is distributed and transported from one storage container to around 30 tuyeres, such as when pulverized coal is injected into a blast furnace, even if the total injection amount can be known, individual It is not possible to grasp the amount of pulverized coal fed from the tuyere, and even if a feeding failure occurs in some transport pipes, the situation cannot be accurately grasped. For this reason, technologies are being developed that can measure the flow rate of powder or granular material for each individual transport pipe, such as a method of measuring the flow rate of powder or granular material from the differential pressure or capacitance within the air flow transport pipe, or For example, an ultrasonic Doppler method has been proposed in which the flow rate is measured by projecting ultrasonic waves onto powder particles transported in a two-phase flow. However, these known methods have problems in measurement accuracy and cannot be said to be satisfactory. In other words, solid-gas two-phase flow is a mixed flow of solid and gas with significantly different specific gravity, so the concentration of powder in the transport pipe is quite uneven. For example, in a horizontal pipe, the upper layer is thinner and the lower layer is thicker, and However, because the particle size is non-uniform, the behavior of each particle is complicated and the flow condition is unstable, which is an inherent problem. Moreover, with the method of arranging the flow rate detection member in the two-phase flow channel, it is not possible to avoid wear of the detection member due to collisions of powder and granules, and furthermore, the flow is obstructed by the detection member, making it easy to cause pipe clogging. There is also the problem.
本発明者等はこの様な問題を解消し、固気2相
流で輸送される粉粒体の流量を正確に測定するこ
とができ、しかも輸送流体の流れを阻害せず且つ
検知部材の摩耗等の問題も生じない様な流量測定
法を確立しようとして種々研究を進めてきた。本
発明はこうした研究の結果完成されたものであつ
て、その構成は、固気2相流における粉粒体の流
量を測定する方法であつて、輸送配管内の圧力変
化を圧力振動として測定し、該圧力振動を周波数
分析に付して振動エネルギーの単位時間における
積分値を求め、予め求めておいた振動エネルギー
の単位時間における積分値と粉粒体流量の相関々
係より粉粒体の流量を承知するところに要旨を有
するものである。 The present inventors have solved these problems and are able to accurately measure the flow rate of powder and granular materials transported by solid-gas two-phase flow, without impeding the flow of the transport fluid and without causing wear on the detection member. Various studies have been carried out in an attempt to establish a flow rate measurement method that does not cause such problems. The present invention was completed as a result of such research, and its structure is a method for measuring the flow rate of powder and granular material in a solid-gas two-phase flow, and the present invention is a method for measuring the flow rate of powder and granular materials in a solid-gas two-phase flow, and the pressure change in the transportation pipe is measured as pressure vibration. , the pressure vibration is subjected to frequency analysis to obtain the integral value of the vibration energy per unit time, and the flow rate of the granular material is calculated from the correlation between the predetermined integral value of the vibration energy per unit time and the granular material flow rate. The gist lies in the fact that we are aware of the following.
以下実施例図面を参照しながら本発明の構成及
び作用効果を詳細に説明する。第1図は本発明を
高炉ブローパイプへの微粉炭吹込量の測定に利用
した場合の実験法を示す概略縦断面図であり、図
中1は高炉耐火壁、2は羽口、3はブローパイ
プ、4は微粉炭供給管を夫々示し、微粉炭供給管
4から空気等のキヤリヤガスと共に微粉炭Cを供
給しつつ、ブローパイプ3の図面右方から加熱空
気Hを吹込み、ブローパイプ3内で微粉炭Cを加
熱空気Hと混合し燃焼させて羽口2から高炉内へ
吹込む様に構成されている。本発明ではこのブロ
ーパイプ3の側壁及び/又は微粉炭供給管4の側
壁に、管内の圧力変化を経時的に検知してその変
化状況を圧力振動として検知する圧力振動検知器
5及び/又は6を設置し、微粉炭Cの吹込みによ
つて生じる圧力変化を連続的に検知すると共に、
該圧力振動を周波数分析に付して振動エネルギー
の単位時間における積分値として求める。例えば
第2図イ,ロ、第3図イ,ロ及び第4図イ,ロは
微粉炭吹込量を64Kg/時間、80Kg/時間及び100
Kg/時間に夫々設定した場合における、圧力変化
検知器5で検知される圧力振動及びこれを周波数
分析して得た振動エネルギー(図では出力電圧の
ボルト値を2乗した値を示している)の関係を夫
夫対比して示したものであり、各図イからも明ら
かな様に何れの吹込量の場合もブローパイプ3の
内圧は約±1mmH2O以内の範囲で脈動している。
そして該脈動の振幅は微粉炭流量が多くなるほど
増大している。従つてこの振幅の大小によつて微
粉炭流量を測定することも可能であると考えられ
るが、実際には微粉炭流量の変化による振幅の変
動量が極めて小さいので、これを流量測定に利用
することはできない。ところが上記脈動を周波数
分析に付すと、振動エネルギーは各図ロに示す通
りとなり、粉粒体流量の違いによる振動エネルギ
ーの差は歴然としたものになつてくる。但し各図
ロにおける振動エネルギーの最大値を比較しよう
すると、この値が極めて急峻な先端値で示される
為測定精度においてやや難点がある。そこで本発
明では、特定周波数域(好ましくは振動エネルギ
ーが最も高い値を示す領域:図示例では100〜300
Hz)における振動エネルギーの積分値を比較する
ことによつて測定精度の誤差を少なくし、この積
分値を微粉炭の流量に換算して求めようとするも
のである。ちなみに第5図は微粉炭流量を0〜
120Kg/時間の範囲に亘つて変化させ、夫夫につ
いて周波数0〜601Hzの範囲における振動エネル
ギー(2乗値)の積分値との相関々係を示したグ
ラフであり、微粉炭流量が約20Kg/時間を越える
条件のもとでは該流量と前記積分値の間には見事
な相関々係が存在することが分かる。尚この相
関々係を示す1次式は、輸送される粉粒体の種類
やキヤリヤガスの種類・流速等によつても若干変
わつてくるので、輸送条件に応じて予め流量と積
分値の関係を示す標準線を作成しておき、実際の
粉粒体輸送時に測定した振動エネルギーの積分値
を上記標準線に当てはめて換算することにより、
任意の時点における粉粒体流量を正確に知ること
ができる。 DESCRIPTION OF THE PREFERRED EMBODIMENTS The configuration and effects of the present invention will be described in detail below with reference to the drawings. Fig. 1 is a schematic vertical cross-sectional view showing an experimental method when the present invention is used to measure the amount of pulverized coal injected into a blast furnace blow pipe. Pipe 4 indicates a pulverized coal supply pipe, and while supplying pulverized coal C together with a carrier gas such as air from the pulverized coal supply pipe 4, heated air H is blown from the right side of the blow pipe 3 in the drawing. The pulverized coal C is mixed with heated air H, combusted, and blown into the blast furnace through the tuyeres 2. In the present invention, a pressure vibration detector 5 and/or 6 is provided on the side wall of the blow pipe 3 and/or the pulverized coal supply pipe 4 to detect pressure changes in the pipe over time and detect the change as pressure vibration. is installed to continuously detect pressure changes caused by the injection of pulverized coal C.
The pressure vibration is subjected to frequency analysis to obtain an integral value of vibration energy per unit time. For example, in Figure 2 A and B, Figure 3 A and B, and Figure 4 A and B, the amount of pulverized coal injected is 64Kg/hour, 80Kg/hour, and 100Kg/hour.
The pressure vibrations detected by the pressure change detector 5 and the vibration energy obtained by frequency analysis of the pressure vibrations when set to Kg/hour (the figure shows the value obtained by squaring the volt value of the output voltage) As is clear from each figure A, the internal pressure of the blow pipe 3 pulsates within a range of approximately ±1 mmH 2 O for any blowing amount.
The amplitude of the pulsation increases as the pulverized coal flow rate increases. Therefore, it is considered possible to measure the pulverized coal flow rate based on the magnitude of this amplitude, but in reality, the amount of variation in the amplitude due to changes in the pulverized coal flow rate is extremely small, so this is used to measure the flow rate. It is not possible. However, when the above-mentioned pulsation is subjected to frequency analysis, the vibration energy becomes as shown in each figure (b), and the difference in vibration energy due to the difference in the flow rate of the powder becomes obvious. However, when trying to compare the maximum value of vibration energy in each figure (b), this value is shown as an extremely steep tip value, so there is a slight difficulty in measurement accuracy. Therefore, in the present invention, a specific frequency range (preferably a region where the vibration energy shows the highest value: 100 to 300 in the illustrated example)
The purpose is to reduce errors in measurement accuracy by comparing the integral value of vibration energy at Hz), and convert this integral value to the flow rate of pulverized coal. By the way, Figure 5 shows the pulverized coal flow rate from 0 to
This is a graph showing the correlation between the vibration energy (squared value) and the integral value in the frequency range of 0 to 601 Hz for husband and husband when the pulverized coal flow rate is approximately 20 kg/hour. It can be seen that under conditions exceeding time, there is an excellent correlation between the flow rate and the integral value. Note that the linear equation showing this correlation varies slightly depending on the type of powder or granular material being transported, the type of carrier gas, the flow rate, etc., so the relationship between the flow rate and the integral value should be calculated in advance according to the transport conditions. By creating a standard line shown below, and converting it by applying the integral value of the vibration energy measured during actual transportation of powder and granular material to the above standard line,
It is possible to accurately know the flow rate of powder or granular material at any point in time.
尚上記の例では、微粉炭と加熱空気が混合し燃
焼するブローパイプ3内の圧力変化を検知する例
を示しており、この場合は燃焼によるガス化反応
によつて管内圧が相当高くなるので、微粉炭の流
量検知精度は極めて高いものとなる。しかしなが
らこの様な燃焼による昇圧等を利用しなくとも、
粉粒体自体の流体輸送時の圧力変化を基にして同
様に粉粒体流量を求めることも勿論可能である。
例えば第6図は前記第1図の微粉炭供給管4に設
けた圧力振動検知器6によつて圧力振動を検知
し、以下第5図の方法に準じて特定周波数範囲
(0〜60.1Hz)における振動エネルギー(2乗値)
の積分値と微粉炭流量の相関々係を示したもので
あり、やはり1次函数的な相関々係を有している
ことが理解される。尚この場合の1次直線の勾配
は第5図の例に比べて緩やかであり、それに伴つ
て測定精度はやや低くなるが、積分値の算出に先
立つて振動エネルギーの出力電圧ボルト値を2乗
から3乗或は4乗に大きくしてやれば、変化勾配
が大きくなつて測定精度を高めることができる。 In the above example, the pressure change inside the blow pipe 3 where pulverized coal and heated air are mixed and combusted is detected. In this case, the pressure inside the pipe becomes considerably high due to the gasification reaction caused by combustion. , the accuracy of detecting the flow rate of pulverized coal is extremely high. However, even without using this kind of pressure increase due to combustion,
Of course, it is also possible to similarly determine the flow rate of the powder or granule based on the pressure change during fluid transport of the powder or granule itself.
For example, in FIG. 6, pressure vibrations are detected by the pressure vibration detector 6 installed in the pulverized coal supply pipe 4 of FIG. Vibration energy (square value) at
It shows the correlation between the integral value of Note that the slope of the primary straight line in this case is gentler than in the example shown in Figure 5, and the measurement accuracy is accordingly slightly lower; however, before calculating the integral value, the output voltage volt value of the vibration energy is squared. By increasing the value to the third or fourth power, the gradient of change becomes larger and measurement accuracy can be improved.
この様に本発明であれば、測定部材を粉粒体輸
送管路の流体流路断面位置に設置するのではな
く、側壁部に設けて管路内圧力の変動によつて測
定する方法であるから、輸送流体の接触による測
定機器を摩耗させたり或は流れを阻害して管路の
閉塞等を引き起こす恐れがなく、粉粒体の流量を
正確に検知することができる。しかも高炉用燃料
として使用する微粉炭の様に多数の管路及び吹込
口から粉粒体を供給する場合でも、各輸送管路に
個別に圧力振動検知器を設けておくことによつて
各管路毎の粉粒体流量を正確に把握することがで
きるので、高炉操業状況のコントロール等を適確
に行なうことができると共に、部分的な吹込み異
常等が起こつた場合でもその異常発生箇所を即座
に知ることができる。又この様に多数の輸送管路
による粉粒体輸送量を併行的に管理する場合にあ
つては、圧力振動検知器は各輸送管路毎に取付け
る一方信号処理用(周波数分析及び振動エネルギ
ーから流量への変換等)の機器は1台で共用し、
一定時間毎にスキヤンしながら各管路の粉粒体輸
送量を測定する様にすれば、設備上の負担も著し
く軽減することができるので好ましい。更に上記
では高炉吹込用微粉炭の流量測定に利用する場合
を主体にして説明してきたが、本発明は勿論この
用途に限定される訳ではなく、各種燃焼設備にお
ける粉体燃料の流量測定や単なる粉粒体輸送配管
における各種粉粒体の流量測定に利用することも
できる。 As described above, according to the present invention, the measurement member is not installed at the cross-sectional position of the fluid flow path of the powder transport pipe, but is installed on the side wall, and the measurement is performed based on fluctuations in the pressure inside the pipe. Therefore, the flow rate of the powder or granular material can be accurately detected without the risk of abrasion of the measuring device due to contact with the transport fluid or obstruction of the flow, causing blockage of the pipe line. Furthermore, even when granular materials such as pulverized coal used as blast furnace fuel are supplied from multiple pipes and inlets, each pipe is equipped with an individual pressure vibration detector. Since it is possible to accurately grasp the flow rate of powder and granular material for each channel, it is possible to accurately control the operating status of the blast furnace, and even if a partial injection abnormality occurs, the location of the abnormality can be identified. You can know instantly. In addition, when managing the amount of powder and granular material transported through a large number of transport pipes in parallel, a pressure vibration detector is installed for each transport pipe, while a pressure vibration detector is installed for signal processing (frequency analysis and vibration energy analysis). (conversion to flow rate, etc.) is shared by one unit,
It is preferable to measure the amount of powder and granular material transported in each pipe while scanning at regular intervals, since this can significantly reduce the burden on equipment. Furthermore, although the above description has mainly focused on the case where the present invention is used for measuring the flow rate of pulverized coal for blast furnace injection, the present invention is of course not limited to this use, and can be used to measure the flow rate of pulverized fuel in various combustion equipment or simply It can also be used to measure the flow rate of various powders and granules in powder and granule transportation piping.
第1図は本発明を高炉ブローパイプにおける微
粉炭の吹込みに利用する場合の要部断面説明図、
第2〜4図イ,ロ図は微粉炭吹込時におけるブロ
ーパイプ内の圧力変動及び周波数分析で得た振動
エネルギーを示す図、第5,6図は微粉炭流量と
振動エネルギーの積分値の関係を示すグラフであ
る。
1……高炉耐火壁、2……羽口、3……ブロー
パイプ、4……微粉炭供給管、5,6……圧力振
動検知器。
FIG. 1 is an explanatory cross-sectional view of the main parts when the present invention is used for blowing pulverized coal into a blast furnace blow pipe;
Figures 2 to 4 A and B are diagrams showing pressure fluctuations in the blow pipe during pulverized coal injection and vibration energy obtained from frequency analysis, and Figures 5 and 6 are the relationship between the pulverized coal flow rate and the integral value of vibration energy. This is a graph showing. 1... Blast furnace refractory wall, 2... Tuyere, 3... Blow pipe, 4... Pulverized coal supply pipe, 5, 6... Pressure vibration detector.
Claims (1)
体の流量を測定する方法において、輸送配管内の
圧力変化を圧力振動として測定し、該圧力振動を
周波数分析に付して振動エネルギーの単位時間に
おける積分値を求め、予め求めておいた振動エネ
ルギーの単位時間における積分値と粉粒体流量の
相関々係より粉粒体の流量を承知することを特徴
とする固気2相流における粉粒体の流量測定方
法。1. In a method of measuring the flow rate of powder and granular material transported in a pipe together with a carrier gas, pressure changes in the transport pipe are measured as pressure vibrations, and the pressure vibrations are subjected to frequency analysis to calculate the integral of the vibration energy over a unit time. The flow rate of powder and granular material in a solid-gas two-phase flow is characterized by determining the flow rate of the powder and granular material from the correlation between the integral value of the vibration energy in unit time determined in advance and the flow rate of the powder and granular material. Flow measurement method.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP20794783A JPS60100018A (en) | 1983-11-04 | 1983-11-04 | Flow rate measurement of pulverized substance in gas- solid dual-phase flow |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP20794783A JPS60100018A (en) | 1983-11-04 | 1983-11-04 | Flow rate measurement of pulverized substance in gas- solid dual-phase flow |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS60100018A JPS60100018A (en) | 1985-06-03 |
| JPH058367B2 true JPH058367B2 (en) | 1993-02-02 |
Family
ID=16548169
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP20794783A Granted JPS60100018A (en) | 1983-11-04 | 1983-11-04 | Flow rate measurement of pulverized substance in gas- solid dual-phase flow |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS60100018A (en) |
-
1983
- 1983-11-04 JP JP20794783A patent/JPS60100018A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS60100018A (en) | 1985-06-03 |
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