JPH0126009B2 - - Google Patents
Info
- Publication number
- JPH0126009B2 JPH0126009B2 JP4615281A JP4615281A JPH0126009B2 JP H0126009 B2 JPH0126009 B2 JP H0126009B2 JP 4615281 A JP4615281 A JP 4615281A JP 4615281 A JP4615281 A JP 4615281A JP H0126009 B2 JPH0126009 B2 JP H0126009B2
- Authority
- JP
- Japan
- Prior art keywords
- solid particles
- transport line
- flow rate
- air
- line
- 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
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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
- G01F1/05—Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow by using mechanical effects
- G01F1/34—Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow by using mechanical effects by measuring pressure or differential pressure
Landscapes
- Physics & Mathematics (AREA)
- Fluid Mechanics (AREA)
- General Physics & Mathematics (AREA)
- 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、複数ラインでの搬送中の固体粒子
(粉流体)の流量測定装置に関するものである。DETAILED DESCRIPTION OF THE INVENTION [Industrial Field of Application] The present invention relates to an apparatus for measuring the flow rate of solid particles (fluid powder) being conveyed in multiple lines.
[従来の技術]
例えば、微粉炭等の固体粒子を空気輸送する場
合、この固体粒子の供給量を何んらかの手段で知
る必要があるが、従来、固体粒子の供給量を知る
手段として、固体粒子の供給点に秤量装置を設置
する手法と、インパクト流量計を設置する手法と
がある。[Prior Art] For example, when solid particles such as pulverized coal are transported by air, it is necessary to know the amount of solid particles supplied by some means. There are two methods: one is to install a weighing device at the solid particle supply point, and the other is to install an impact flow meter.
第1図は秤量装置の一例を示す構成図である。
この装置は、固体粒子を一時的に保持するホツパ
ー1と、輸送ライン(図示せず)に固体粒子を供
給する供給機2と、計量装置3とを含むものであ
り、計量装置3でホツパー1内に保持された固体
粒子の重量を計量し、計量した固体粒子を供給機
2から供給するものである。 FIG. 1 is a configuration diagram showing an example of a weighing device.
This device includes a hopper 1 that temporarily holds solid particles, a feeder 2 that supplies the solid particles to a transport line (not shown), and a metering device 3. The weight of the solid particles held within is measured, and the weighed solid particles are supplied from a feeder 2.
インパクト流量計は、固体粒子を自然落下させ
て板で受け、この際生じる衝撃力を利用して流量
を測定するものである。 An impact flow meter measures the flow rate by allowing solid particles to fall naturally and being received by a plate, and using the impact force generated at this time.
[発明が解決しようとする問題点]
前記従来の秤量装置を設置する場合は、全体装
置が相当大がかりとなりその設備費が高くなるう
えに、設置スペースも広いものを必要とする。ま
た、第2図に示すように、1台の秤量装置4から
多数の輸送ライン5に固体粒子を供給する場合、
全体の固体粒子の供給量は測定できても、各々の
ラインの固体粒子の流量は測定できないという問
題点がある。[Problems to be Solved by the Invention] When installing the conventional weighing device, the entire device becomes quite large-scale and the equipment cost increases, and a large installation space is also required. Furthermore, as shown in FIG. 2, when solid particles are supplied from one weighing device 4 to a large number of transportation lines 5,
There is a problem in that although the total amount of solid particles supplied can be measured, the flow rate of solid particles in each line cannot be measured.
また、インパクト流量計を使用した場合は輸送
ラインの途中に固体粒子を自然落下させる設備を
必要とする他、多くの付帯設備を必要とし、設備
費は高くまた設置面積も広くなる。 Furthermore, when an impact flow meter is used, it requires equipment to allow solid particles to fall naturally in the middle of a transportation line, and also requires many incidental equipment, resulting in high equipment costs and a large installation area.
ここにおいて、本発明は、複数の輸送ラインの
各々の流量測定が可能でしかも構成簡単にして設
備費が安価で、設置面積も少ない固体粒子の流量
測定装置を提供しようとするものである。 SUMMARY OF THE INVENTION It is an object of the present invention to provide a solid particle flow rate measuring device that is capable of measuring the flow rate of each of a plurality of transportation lines, has a simple configuration, has low equipment cost, and has a small installation area.
[問題点を解決するための手段]
本発明に係る固体粒子の流量測定装置は、空気
流により固体粒子を輸送する複数の輸送ラインに
おいて、各輸送ラインの固体粒子を含有する以前
の空気流の流速と、空気と固体粒子の混合流の定
常な一定管長部に発生圧力降下を測定し、これら
の測定値を順次共通演算器に送り、各輸送ライン
に流れる固体粒子の流量を演算することを特徴と
する。[Means for Solving the Problems] The solid particle flow rate measurement device according to the present invention measures the flow rate of the previous air flow containing solid particles in each transport line in a plurality of transport lines that transport solid particles by air flow. This method measures the flow velocity and the pressure drop that occurs over a steady, constant pipe length in a mixed flow of air and solid particles, and sends these measured values sequentially to a common calculator to calculate the flow rate of solid particles flowing in each transport line. Features.
[作用]
この発明においては、複数の輸送ラインの空気
流の流速と固気二相混合流の一定管長部の圧力降
下を各々測定し、これらの測定値を順次1つの演
算器で演算処理することにより、各輸送ラインに
流れる固体粒子の流量を簡単に測定する。[Operation] In this invention, the flow velocity of the air flow in a plurality of transportation lines and the pressure drop of a solid-gas two-phase mixed flow at a constant pipe length are each measured, and these measured values are sequentially processed by a single computing unit. This makes it easy to measure the flow rate of solid particles flowing through each transport line.
[実施例]
第3図は本発明に係る流量測定装置の一例を示
す構成ブロツク図である。図において、5は固体
粒子の複数輸送ラインで、一端は空気供給源(図
示せず)に結合されて空気が供給され、他端は固
体粒子の輸送先(図示せず)に結合され、その途
中のP点において固体粒子ホツパー1から固体粒
子が各輸送ライン5に供給されている。6は各輸
送ライン5の固体粒子の供給点Pより上流側に
各々設置され、各々の輸送ライン5の空気流速
Uaを測定する複数の気体流量計、7は各輸送ラ
イン5の固体粒子の供給点Pより下流側であつ
て、空気と固体粒子の混合流体が定常な区間(固
体粒子の運動が安定した区間)に各々設置された
複数の差圧計で、各ラインにおいて同一の或る一
定距離での混合流体の圧力損失△Pを測定する。
8は各流体流量計6からの空気流速測定信号と、
各差圧計7からの圧力損失測定信号とを入力し、
各々タイミング制御器9によつて一定時間ずつ時
分割して各ライン毎の気体流量計出力信号と差圧
計出力信号とをペアにして順次出力する走査切換
器であり、この走査切換器8からは各ライン毎の
両測定信号が順次時分割的に出力される。10は
これら空気流速測定信号と圧力損失測定信号とを
順次各ライン毎に受けとつてタイミング制御器9
によるタイミング制御のもとに下記のように両信
号の演算処理をする共通演算器である。[Embodiment] FIG. 3 is a configuration block diagram showing an example of a flow rate measuring device according to the present invention. In the figure, 5 is a solid particle transport line, one end of which is connected to an air supply source (not shown) to supply air, and the other end is connected to a solid particle transport destination (not shown). Solid particles are supplied from the solid particle hopper 1 to each transport line 5 at point P along the way. 6 is installed upstream of the solid particle supply point P of each transport line 5, and the air flow velocity of each transport line 5 is
A plurality of gas flowmeters 7 for measuring U a are located downstream of the solid particle supply point P of each transport line 5, in a section where the mixed fluid of air and solid particles is steady (the movement of the solid particles is stable). A plurality of differential pressure gauges installed in each section) measure the pressure loss ΔP of the mixed fluid at the same certain distance in each line.
8 is an air flow rate measurement signal from each fluid flow meter 6;
Input the pressure loss measurement signal from each differential pressure gauge 7,
It is a scan switch that sequentially outputs the gas flow meter output signal and the differential pressure gauge output signal for each line in a pair in a time-divided manner by a timing controller 9 for a fixed period of time. Both measurement signals for each line are sequentially output in a time-division manner. 10 is a timing controller 9 which sequentially receives these air flow velocity measurement signals and pressure loss measurement signals for each line.
This is a common arithmetic unit that performs arithmetic processing on both signals as described below under the timing control of
このように構成した装置において、共通演算器
10は各輸送ライン5の気体流量計6で検出する
空気流速信号Uaと差圧計7で検出する圧力変換
信号△Pとをタイミング制御器9を介して順次入
力し、(1)式で示される演算を行うことにより、各
輸送ライン5を流れる固体粒子の流量Gsを順次
演算する。 In the device configured in this manner, the common computing unit 10 transmits the air flow rate signal U a detected by the gas flow meter 6 of each transportation line 5 and the pressure conversion signal ΔP detected by the differential pressure gauge 7 via the timing controller 9. The flow rate G s of the solid particles flowing through each transport line 5 is sequentially calculated by inputting the data sequentially and performing the calculation shown in equation (1).
Gs=π・D2・g/4・K・Ua(△P−△Pa) ……(1)
この(1)式は以下のようにして導かれる。ただし
各信号は次のように定める。G s =π・D 2・g/4・K・U a (△P−△P a )...(1) This equation (1) is derived as follows. However, each signal is defined as follows.
G:流量 [Kg/s]
U:流速 [m/s]
γ:比重量 [Kg/m3]
x:輸送ライン5の距離 [m]
g:重力加速度 [m/s2]
D:輸送ライン5の内径 [m]
A:輸送ライン5の断面積 [m2]
θ:輸送ライン5の水平との傾き [度]
τ:管摩擦応力 [Kg/m2]
λ:管摩擦係数 [−]
φ:速度比(Us/Ua) [−]
P:圧力 [Kg/m2]
なお、各記号の添字aは空気を示し、sは固体
粒子を示す。G: Flow rate [Kg/s] U: Flow velocity [m/s] γ: Specific weight [Kg/m 3 ] x: Distance of transportation line 5 [m] g: Gravitational acceleration [m/s 2 ] D: Transportation line Inner diameter of 5 [m] A: Cross-sectional area of transportation line 5 [m 2 ] θ: Inclination of transportation line 5 with respect to horizontal [degrees] τ: Pipe friction stress [Kg/m 2 ] λ: Pipe friction coefficient [-] φ: Speed ratio (Us/Ua) [-] P: Pressure [Kg/ m2 ] Note that the subscript a of each symbol indicates air, and s indicates solid particles.
第4図に示すように水平と角度θだけ傾いた輸
送ライン5において、入口圧力P、出力圧力P+
dP/dxdxの流れの方向の微小長さdxに占める固気
二相流について運動量保存則を適用すると(2)式で
表わせる。 As shown in Fig. 4, in the transport line 5 inclined by an angle θ with respect to the horizontal, the inlet pressure P, the output pressure P+
Applying the law of conservation of momentum to the solid-gas two-phase flow that occupies the minute length dx in the flow direction of dP/dxdx, it can be expressed by equation (2).
1/g{d(Ga・Ua)/dx+d(Gs・Us)/dx}
=−AdP/dx−πDτ−γAsinθ……(2)
ここで左辺第1項は気体部分の運動量の変化、
第2項は固体粒子部分の運動量の変化を示し、右
辺第1項は圧力差、第2項は管摩擦、第3項は重
力による運動量の変化を示す。 1/g {d(G a・Ua)/dx+d(G s・U s )/dx}
=-AdP/dx-πDτ-γAsinθ...(2) Here, the first term on the left side is the change in momentum of the gas part,
The second term indicates the change in momentum of the solid particle portion, the first term on the right side indicates the pressure difference, the second term indicates the tube friction, and the third term indicates the change in momentum due to gravity.
空気輸送のように気体と固体粒子の混合比
Gs/Gaが小さい場合には、固体粒子の占める体
積は気体の体積に比べて無視でき、固気二相流の
比重量γは(3)式で表わせる。 Mixing ratio of gas and solid particles as in pneumatic transport
When G s /G a is small, the volume occupied by solid particles can be ignored compared to the volume of gas, and the specific weight γ of the solid-gas two-phase flow can be expressed by equation (3).
γ≒γa+Gs/AUs=γa+γs ……(3)
また、(2)式においては気体流と固体粒子流との
相加性があるので(4)式が成立する。 γ≒γ a +G s /AU s = γ a +γ s (3) Moreover, in equation (2), since there is additivity between the gas flow and the solid particle flow, equation (4) holds true.
dP=dPa+dPs
τ=τa+τs ……(4)
この(3)式、(4)式より気体流に対して(2)式は次の
ようになる。 dP=dP a +dP s τ=τ a +τ s ...(4) From equations (3) and (4), equation (2) for gas flow becomes as follows.
Ga/g・dUa/dx
=−AdPa/dx−πDτa−γaAsinθ ……(5)
同様に固体粒子流に対して(2)式は次のようにな
る。 G a /g・dU a /dx =−AdP a /dx−πDτa−γaAsinθ (5) Similarly, equation (2) for solid particle flow becomes as follows.
Gs/g・dUs/dx
=−AdPs/dx−πDτs−Gs/Ussinθ ……(6)
固体粒子流と気体流の速度が一定の場合には、
固体粒子流と管壁との管摩擦係数λsと管摩擦応力
τsとの間および気体流と管壁との管摩擦係数λaと
管摩擦応力τaとの間には各々次式の関係が成立す
る。 G s /g・dU s /dx = −AdP s /dx−πDτ s −G s /U s sinθ ……(6) When the speeds of the solid particle flow and the gas flow are constant,
The relationship between the pipe friction coefficient λ s between the solid particle flow and the pipe wall and the pipe friction stress τ s , and between the pipe friction coefficient λ a and the pipe friction stress τ a between the gas flow and the pipe wall are expressed by the following equations. A relationship is established.
したがつて、固体粒子流の速度が一定の場合、
すなわちdUs/dx=0の場合には(6)式は(7)式を使つ
て以下のように展開することができる。 Therefore, if the velocity of the solid particle stream is constant,
That is, when dU s /dx=0, equation (6) can be expanded as follows using equation (7).
−dPs/dx=1/A(πDτs+Gs/Ussinθ)
=1/A(λsGsUs/2gD+Gs/Ussinθ)
=Gs/A(λsUs/2gD+sinθ/Us)
この式を距離xについて積分すると
△Ps=Gs/A(λsUs2gD+sinθ/Us)x
=Gs4Ua/πD2g(λs/2D+gsinθ/U2/a)x…
…(8)
(8)式において
K=(λs/2D+gsinθ8/U2/a)x ……(9)
とすると(8)式は次式で表わせる。−dP s /dx=1/A(πDτ s +G s /U s sinθ) =1/A(λ s G s U s /2gD+G s /U s sinθ) =G s /A(λ s U s /2gD+sinθ /U s ) Integrating this equation with respect to distance x, △P s = G s /A (λ s U s 2gD + sinθ/U s )x = G s 4U a /πD 2 g (λ s /2D+gsinθ/U 2 / a ) x…
...(8) In equation (8), K=(λ s /2D+gsinθ8/U 2 / a )x ...(9) If equation (8) can be expressed as the following equation.
△Ps=Gs4UaK/πD2g ……(10)
同様に気体流の速度が一定の場合、すなわち
dUa/dx=0の場合にはは(5)式は(7)式を使つて展開
すると次のようになる。 △P s = G s 4U a K/πD 2 g ……(10) Similarly, when the velocity of the gas flow is constant, i.e.
When dU a /dx=0, equation (5) can be expanded using equation (7) as follows.
−dPa/dx=1/A(πDλaγaUa 28g+γaAsinθ)
△Pa=(λaγaUa 2/2gD+γasinθ)x ……(11)
したがつて気体流の距離x間の圧力損失△Pa
は気体流の流速Uaから演算で求めることができ
る。−dP a /dx=1/A(πDλ a γ a U a 2 8g+γ a Asinθ) △P a = (λ a γ a U a 2 /2gD+γ a sinθ)x ...(11) Therefore, the gas flow Pressure loss △P a between distance x
can be calculated from the flow velocity U a of the gas flow.
一方、固気二相流の距離x間の圧力損失△Pは △P=△Ps+△Pa ……(12) であるから、(10)式と(12)式から Gs=πD2g/4・K・Ua(△P−△Pa)……(1) と(1)式を導くことができる。 On the other hand, the pressure loss △P over the distance x in solid-gas two-phase flow is △P = △P s + △P a ...(12), so from equations (10) and (12), G s = πD 2 g/4・K・U a (△P−△P a )...Equations (1) and (1) can be derived.
この(1)式の係数のうち輸送ライン5の内径D、
重力加速度g等の値は予め共通演算器10に記憶
させておき、パラメータKは共通演算器10で気
体流量計6で測定する空気流速Uaによつて予じ
め設定された率で修正する。 Among the coefficients of this equation (1), the inner diameter D of the transportation line 5,
Values such as gravitational acceleration g are stored in advance in the common calculator 10, and the parameter K is corrected by the common calculator 10 at a preset rate based on the air flow velocity U a measured by the gas flow meter 6. .
[発明の効果]
本発明に係る固体粒子の流量測定装置は、各ラ
インにて固体粒子の供給点より上流側の空気流速
を測定するとともに、固体粒子の供給点より下流
側の空気と固体粒子との混合流体が定常な区間で
の混合流体の圧力損失を測定し、これらの測定値
を時分割的に1台の演算器で演算処理して順次各
ラインの固体粒子の流量を測定するようにしたも
ので、これを実現するための全体装置は、各ライ
ン毎の空気流量計と差圧計、及び1台の共通演算
器と走査切換器で構成でき、きわめて簡単な構成
となる。このことから従来の手法に比べ、設備費
が軽減できる他に、設置スペースを小さくできる
等の効果がある。[Effects of the Invention] The solid particle flow rate measuring device according to the present invention measures the air flow velocity upstream from the solid particle supply point in each line, and also measures the air flow rate downstream from the solid particle supply point in each line. The pressure drop of the mixed fluid is measured in a section where the mixed fluid is steady, and these measured values are processed in a time-division manner by a single computing unit to sequentially measure the flow rate of solid particles in each line. The overall device for realizing this is extremely simple, consisting of an air flow meter and a differential pressure meter for each line, and one common computing unit and scan switch. Therefore, compared to the conventional method, not only can equipment costs be reduced, but also the installation space can be reduced.
第1図は公知の秤量装置の一例を示す構成図、
第2図は1台の秤量装置から多数の輸送ラインに
固体粒子を供給する場合の構成図、第3図は本発
明に係る流量測定装置の実施例を示す構成ブロツ
ク図、第4図は上記実施例の原理を示す説明図で
ある。
5……輸送ライン、P……固体粒子供給点、6
……気体流量計、7……差圧計、8……走査切換
器、9……タイミング制御器、10……共通演算
器。
FIG. 1 is a configuration diagram showing an example of a known weighing device,
Fig. 2 is a block diagram of the case in which solid particles are supplied from one weighing device to a large number of transport lines, Fig. 3 is a block diagram of the structure showing an embodiment of the flow rate measuring device according to the present invention, and Fig. 4 is the above-described block diagram. It is an explanatory diagram showing the principle of an example. 5...Transportation line, P...Solid particle supply point, 6
...Gas flow meter, 7...Differential pressure gauge, 8...Scanning switch, 9...Timing controller, 10...Common computing unit.
Claims (1)
ン、各輸送ラインの輸送すべき固体粒子の供給点
より上流にて各輸送ラインに各々設置され各輸送
ラインの空気流の流速を測定する複数の空気流速
測定手段、前記固体粒子の供給点より下流側であ
つて空気と固体粒子の混合流体が定常な区間にて
各輸送ラインに各々設置され各輸送ラインの混合
流体の一定輸送距離間での圧力損失を測定する複
数の差圧測定手段、前記空気流速測定手段と差圧
測定手段からの両測定信号を入力しこれらの信号
を輸送ライン毎に時分割して順次出力する走査切
換手段、該走査切換手段から各輸送ライン毎の前
記両測定信号を順次受けとり該測定信号を演算処
理して各輸送ライン毎の前記固体粒子の流量を順
次求める共通の演算器、を具備した固体粒子の流
量測定装置。1 A plurality of transport lines connected to an air supply source at one end, a plurality of transport lines each installed in each transport line upstream of the supply point of the solid particles to be transported in each transport line and measuring the flow velocity of the air flow in each transport line. An air flow rate measuring means is installed in each transport line in a section downstream of the solid particle supply point and where the mixed fluid of air and solid particles is steady, and is installed on each transport line in a section where the mixed fluid of air and solid particles is constant, and measures a plurality of differential pressure measuring means for measuring pressure loss; a scanning switching means for inputting both measurement signals from the air flow rate measuring means and the differential pressure measuring means; and sequentially outputting these signals in time division for each transportation line; Flow rate measurement of solid particles, comprising: a common computing unit that sequentially receives both measurement signals for each transport line from a scanning switching means, performs arithmetic processing on the measurement signals, and sequentially obtains the flow rate of the solid particles for each transport line. Device.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4615281A JPS57182124A (en) | 1981-03-31 | 1981-03-31 | Flow rate measuring apparatus for solid particles |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4615281A JPS57182124A (en) | 1981-03-31 | 1981-03-31 | Flow rate measuring apparatus for solid particles |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS57182124A JPS57182124A (en) | 1982-11-09 |
| JPH0126009B2 true JPH0126009B2 (en) | 1989-05-22 |
Family
ID=12739004
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP4615281A Granted JPS57182124A (en) | 1981-03-31 | 1981-03-31 | Flow rate measuring apparatus for solid particles |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS57182124A (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS57207826A (en) * | 1981-06-17 | 1982-12-20 | Hideo Nagasaka | Measuring device for flow rate of pulverulent body |
| US4490077A (en) * | 1981-07-28 | 1984-12-25 | Nippon Kokan Kabushiki Kaisha | Apparatus for continuously measuring flow rate of fine material flowing through transport pipe |
| JPS601522A (en) * | 1983-06-17 | 1985-01-07 | Nippon Kokan Kk <Nkk> | Powder flow measurement method |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5032827A (en) * | 1973-07-23 | 1975-03-29 |
-
1981
- 1981-03-31 JP JP4615281A patent/JPS57182124A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS57182124A (en) | 1982-11-09 |
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