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JPS6154451B2 - - Google Patents
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JPS6154451B2 - - Google Patents

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Publication number
JPS6154451B2
JPS6154451B2 JP13166582A JP13166582A JPS6154451B2 JP S6154451 B2 JPS6154451 B2 JP S6154451B2 JP 13166582 A JP13166582 A JP 13166582A JP 13166582 A JP13166582 A JP 13166582A JP S6154451 B2 JPS6154451 B2 JP S6154451B2
Authority
JP
Japan
Prior art keywords
suction
air volume
equipment
dust collection
air
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
Application number
JP13166582A
Other languages
Japanese (ja)
Other versions
JPS5922622A (en
Inventor
Akira Tamei
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.)
Kanadevia Corp
Original Assignee
Hitachi Shipbuilding and Engineering 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
Application filed by Hitachi Shipbuilding and Engineering Co Ltd filed Critical Hitachi Shipbuilding and Engineering Co Ltd
Priority to JP13166582A priority Critical patent/JPS5922622A/en
Publication of JPS5922622A publication Critical patent/JPS5922622A/en
Publication of JPS6154451B2 publication Critical patent/JPS6154451B2/ja
Granted legal-status Critical Current

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Description

【発明の詳細な説明】[Detailed description of the invention]

本発明は例えば製鉄所や焼結設備などにおける
集塵設備の吸引風量制御方法に関する。 発塵、発煙の防止のため、それらに密閉フード
を設け集塵・集煙を図るのが望ましいが、フード
は設けていても、スペース上、構造上、作業上か
ら密閉できない場合が多い。また設備自体も密閉
構造ではなく、すきまが存在する場合が多い。こ
のように設備やフードにすきまが存在する場合粉
塵などがこれらにより外部に出ないようすきまで
の通過流速を十分高めた風量で吸引することが必
要である。フード開口部での流速は焼結設備での
1例では次の通りである。
The present invention relates to a method for controlling the suction air volume of dust collection equipment in, for example, steel works and sintering equipment. In order to prevent the generation of dust and smoke, it is desirable to install airtight hoods to collect dust and smoke, but even if hoods are installed, it is often impossible to seal them due to space, structure, and work considerations. Furthermore, the equipment itself is not a sealed structure and often has gaps. When there are gaps in equipment or hoods, it is necessary to suction air at a sufficiently high flow rate to prevent dust from escaping to the outside. The flow rate at the hood opening is as follows in one example in a sintering facility.

【表】 従来の集塵設備の1例を第1図に示す。図にお
いて、1はダストを発生する設備で、この設備1
の上部にはダストを吸引するためのフード2が設
けられている。フード2は、設備1の幅よりその
開口部を大きくされており、設備1および設備1
と該フード2のすきま3から所定の流速で大気を
吸引する働きをなす。フード2で吸引された外気
は発生ダストと共に集塵ダクト4を通して集塵機
5へ導入され、集塵機5でダストを除去された
後、集塵フアン入口ダンパ6および排風機7を経
て煙突8から大気中に放出される構成とされてい
る。係る構成の集塵設備において、設備1は、通
常各種の反応を起こしたり高温物を取扱つたりす
るが、それらは時間とともに変化していくため、
集塵されたガスの温度も時間とともに変化する。
このように吸引ガス条件が変化した場合、吸引ガ
ス量はどのように変化するかを第2図を用いて説
明する。 第2図において、曲線AおよびA′は排風機7
の実風量と圧力の関係を示した特性曲線であり、
Aはガス温度t1の場合、A′はガス温度t2の場合
で、t1>t2である。また曲線CおよびC′は、同様
にガス温度t1およびt2の場合の排風機7実風量と
動力の関係を示したものである。一方、設備の抵
抗は一般に下式で示される。 ΔP=k1・γ・v2 ……(1) ここに ΔP:抵 抗 k:係 数 γ:ガス比重 v:ガス流速 今、ガス温度がt℃のときのガス比重γは下式
で示される。 γ=k2・273/273+t ……(2) (1)、(2)式より下式が成立する。 ΔP=k1・k2・273/273+t・v2 ……(3) すなわち、一定断面の場合、ガス流速は実風量
に比例するからガス温度が上昇した場合には同一
実風量であると抵抗が小さくなる。ここで、図中
B,B′で示す曲線はガス温度t1およびt2における
抵抗曲線である。図からも明らかなように、ガス
温度が変化しても抵抗曲線B,B′と排風機性能曲
線A,A′との交点(運転点)P,Qにおいて排
風機通過実風量はほとんど変らない。また動力は
温度t1,t2に対して図中R.S点の如く、温度の低
下に伴ない増加する。ところで、集塵に関して
は、前述のフード2開口部の流速によつて集塵風
量が決定されるため、外気温度をt0℃とするとt0
℃における最適風量Q0が決定され、前述の温度
上昇にも拘らずこの風量を吸引する必要があり、
また逆にこの風量以上の量を引く必要はない。い
ま温度t1℃における排風機7の吸引実風量をQ1
すると温度t0℃における風量Q0′に換算すれば
Q0′は下式となる。 Q0′=Q1・273+t/273+t ……(4) 風量Q0′は上記の通り最適風量としてQ0である
べき故Q0=Q0′とすると、(4)式により、温度が上
昇してくれば吸引実風量も増加させ、温度が低下
してくれば吸引実風量を減少させることになる。 このように、従来の集塵設備によると、ガス温
度はプロセス状況に応じて変動するものであるに
も拘らず、予想最高温度に対応する風量をベース
にして排風機7が一定回転で運転され、何ら制御
がなされていなかつた。すなわち前述のように、
ガス温度が低下してくれば吸引実風量は少くてよ
いのに、吸引実風量を変化させていないため、第
2図のR,S点の如く大きな差が出て、低温時の
電力消費が大きかつたり、また排風機7の設計値
は通常余裕をもたせたものであるため、現実には
必要以上の電力消費をなす設備となつていた。こ
のように集塵設備の吸引風量が制御されていない
理由は、設備1とフード2のすきま3すなわち外
気吸引個所における吸引風量を正確に把握するこ
とが困難なためで、吸引個所が1個所の場合、集
塵機5後の排気の風量、温度を測定して大気吸引
量を算出することが出来るが、排気中のダストの
影響や温度の変動により正確な値が把握しにくい
し、また吸引個所が多数ある場合には、個々の吸
引個所での吸引風量を知るには吸引個所近くのダ
クト4内で計測することになるが、その場合ダス
ト量がさらに多くなりまたダクト4の直管部が十
分とれないため、計測護差が大きくなるほど正確
な値を把握しにくいことによる。また、フード2
内圧力など圧力計測によつてフード2での吸引量
を知る方法もあるが、これも、ダストの問題や吸
引による温度上昇によるドラフトや温度変動によ
る影響で、極めて不正確・不安定な計測とならざ
るをえなかつた。 本発明はこのような問題を解決することを目的
とし、設備からのダスト、煙の発生を防止するた
めにフード設備などの吸引部を設けた集塵設備に
おいて、吸引部の外気吸引個所近傍に外気と連通
する計測管を設け、この計測管を通過する大気の
流量もしくは流速を計測してその値を前記吸引個
所の集塵風量の代表値とし、この代表値が所定の
設定値になるように集塵設備の排風量を自動的に
調整する集塵設備の吸引風量制御方法を提供する
ことによつて、その目的を達成するものであり、
これにより吸引部の外気吸引個所における大気の
流量もしくは流速を正確に計測できて集塵設備を
ガス温度の変動に必要にして十分な排風量とする
ことができ、もつて電力消費も必要最小限におさ
えて省エネルギを図ることができるものである。 以下本発明の方法をその一実施例を示す図面に
基づいて詳細に説明する。第3図中、第1図と同
じ機器については同一番号を符した。図におい
て、9はフード2のすきま3すなわち外気吸引個
所近傍に設けられた外気と連通する小径のパイプ
状計測管で、この計測管9には、その内部を通過
する大気の流量もしくは流速を計測する風量もし
くは風速測定用機器10が設けられている。そし
て測定用機器10は、その測定風量が設定風量と
一致するように、排風機駆動用電動機11の速度
を調整する速度調整用機器12に電気的接続がな
され、前記排風機駆動用電動機11の回転数を制
御可能とされている。次に、フード2のすきま3
近傍に計測管9を設けた理由を述べる。前述した
ように吸引空気は設備1およびすきま3から吸引
されるのであるが、その吸引風量は内部圧力と外
気圧力の差圧によつて決される。したがつて、そ
の差圧が判明すればそのときのすきま3部通過流
速が算出でき、その流速とすきま3部面積の積と
しての流量が算出できる。またこれにより差圧を
吸引量の代表値とすることができる。しかしなが
ら、前述の通りフード2内圧力の計測は正確を期
し難いし、またすきま3部通過流速を直接測定す
ることも困難である。そこでフード2のすきま3
近傍に小径の計測管9を新たなすきまとして設け
ることによつて、その計測管9内の流速もしくは
流量を吸引量の代表値とすることができるのであ
る。このようなことから、計測管9内を通過する
流体は大気であり、温度も大気温であるため、極
めて正確な計測ができることになる。なお、図示
しなかつたが、間欠的に計測を行なう場合は、計
測管9入口にバルブを設け、通常は閉にして漏れ
量を減ずるようにすればよい。 係る構成で、実際の運転時には、排風機7の回
転数を種々に変化させ、必要にして十分なる集塵
状況にあるところで測定閉機器10の数値を読み
取つておく。そしてその数値を設定値にして排風
機駆動用電動機11の回転数制御を行なつてやれ
ば、過剰な排風による効力損失を防ぐことができ
る。 なお、上記実施例においては排風機7の電動機
11を回転数制御する方法としたが、流体継手や
入口ダンパ6制御など動力の低減に結びつく風量
制御手段であればいずれでもよい。 以上本発明方法によれば、フード設備などの吸
引部の外気吸引個所における大気の流量もしくは
流速を正確に計測できて集塵設備をガス温度の変
動に必要にして十分な排風量とすることができ、
もつて電力消費も必要最小限におさえ省エネルギ
を図ることができる。また本方法を採用すること
により、例えば集塵ダクトにダストによる破孔が
発生した場合、計測管の値が所定値に達しないた
め、その際は警報を出すようにしておけば、設備
の目視によるチエツクをしなくてもその破孔の発
生を知ることができ、省力化にも大きく役立ち得
る。
[Table] Figure 1 shows an example of conventional dust collection equipment. In the figure, 1 is equipment that generates dust;
A hood 2 for suctioning dust is provided on the top of the hood. The hood 2 has an opening larger than the width of the equipment 1, and the hood 2 has an opening larger than the width of the equipment 1.
The hood 2 functions to suck atmospheric air through the gap 3 at a predetermined flow rate. The outside air sucked in by the hood 2 is introduced into the dust collector 5 through the dust collection duct 4 along with the generated dust, and after the dust is removed by the dust collector 5, it passes through the dust collection fan inlet damper 6 and the exhaust fan 7, and enters the atmosphere from the chimney 8. It is configured to be released. In dust collection equipment with such a configuration, the equipment 1 usually causes various reactions or handles high-temperature materials, but these changes over time.
The temperature of the collected gas also changes over time.
How the amount of suction gas changes when the suction gas conditions change in this way will be explained using FIG. 2. In Figure 2, curves A and A' are the exhaust fan 7.
This is a characteristic curve showing the relationship between actual air volume and pressure.
A is for the gas temperature t 1 and A' is for the gas temperature t 2 , where t 1 >t 2 . Similarly, curves C and C' show the relationship between the actual air volume of the exhaust fan 7 and the power when the gas temperatures are t 1 and t 2 . On the other hand, the resistance of equipment is generally expressed by the following formula. ΔP=k 1・γ・v 2 …(1) where ΔP: resistance k: coefficient γ: gas specific gravity v: gas flow velocity Now, when the gas temperature is t°C, the gas specific gravity γ is expressed by the following formula. It can be done. γ= k2・273/273+t...(2) From equations (1) and (2), the following equation holds true. ΔP=k 1・k 2・273/273+t・v 2 ……(3) In other words, in the case of a constant cross section, the gas flow velocity is proportional to the actual air volume, so if the gas temperature rises, the resistance will increase if the actual air volume is the same. becomes smaller. Here, the curves indicated by B and B' in the figure are resistance curves at gas temperatures t1 and t2 . As is clear from the figure, even if the gas temperature changes, the actual air volume passing through the exhaust fan hardly changes at the intersections (operating points) P and Q between the resistance curves B and B' and the exhaust fan performance curves A and A'. . Further, the power increases as the temperature decreases, as shown at the RS point in the figure, for temperatures t 1 and t 2 . By the way, regarding dust collection, since the dust collection air volume is determined by the flow velocity at the opening of the hood 2 mentioned above, if the outside air temperature is t 0 °C, then t 0
The optimal air volume Q 0 at °C has been determined, and it is necessary to draw in this air volume despite the temperature rise mentioned above.
Conversely, there is no need to draw more than this amount of air. Now, if the actual air volume sucked by the exhaust fan 7 at the temperature t 1 °C is Q 1 , then convert it to the air volume Q 0 ' at the temperature t 0 °C.
Q 0 ′ becomes the following formula. Q 0 ′=Q 1・273+t 0 /273+t 1 ……(4) The air volume Q 0 ′ should be Q 0 as the optimal air volume as described above. Therefore, if Q 0 =Q 0 ′, then according to equation (4), the temperature If the temperature rises, the actual suction air volume will be increased, and if the temperature decreases, the suction actual air volume will be decreased. As described above, according to conventional dust collection equipment, although the gas temperature fluctuates depending on the process situation, the exhaust fan 7 is operated at a constant rotation based on the air volume corresponding to the expected maximum temperature. , there was no control whatsoever. In other words, as mentioned above,
If the gas temperature decreases, the actual suction air volume can be reduced, but since the actual suction air volume is not changed, there is a large difference as shown at points R and S in Figure 2, and the power consumption at low temperatures is reduced. Since the exhaust fan 7 is large in size and the design value of the exhaust fan 7 is usually set with a margin, the equipment actually consumes more power than necessary. The reason why the suction air volume of the dust collection equipment is not controlled is that it is difficult to accurately grasp the suction air volume at the gap 3 between the equipment 1 and the hood 2, that is, at the outside air suction point. In this case, it is possible to calculate the amount of atmospheric suction by measuring the air volume and temperature of the exhaust air after the dust collector 5, but it is difficult to obtain an accurate value due to the influence of dust in the exhaust and fluctuations in temperature, and the suction point is If there are many, the amount of air sucked at each suction point must be measured in the duct 4 near the suction point, but in that case, the amount of dust will be even larger, and the straight pipe section of the duct 4 may be insufficient. This is because the larger the measurement difference, the more difficult it is to obtain an accurate value. Also, food 2
There is also a method of determining the amount of suction in the hood 2 by measuring internal pressure and other pressures, but this also results in extremely inaccurate and unstable measurements due to dust problems, drafts due to temperature rise due to suction, and temperature fluctuations. I had no choice but to do so. The purpose of the present invention is to solve such problems, and in dust collection equipment equipped with a suction part such as a hood equipment in order to prevent the generation of dust and smoke from the equipment, a vacuum cleaner is installed near the outside air suction part of the suction part. A measurement pipe communicating with the outside air is provided, the flow rate or flow velocity of the air passing through this measurement pipe is measured, and the value is taken as a representative value of the dust collection air volume at the suction point, and this representative value is set as a predetermined set value. This objective is achieved by providing a suction air volume control method for dust collection equipment that automatically adjusts the exhaust air volume of dust collection equipment.
This makes it possible to accurately measure the flow rate or flow velocity of the atmosphere at the outside air suction point of the suction section, making it possible to use dust collection equipment to keep up with gas temperature fluctuations and to ensure sufficient exhaust air volume, while also minimizing power consumption. It is possible to save energy by keeping the amount of energy to a minimum. Hereinafter, the method of the present invention will be explained in detail based on the drawings showing one embodiment thereof. In FIG. 3, the same equipment as in FIG. 1 is designated by the same number. In the figure, reference numeral 9 denotes a small-diameter pipe-shaped measurement tube that communicates with the outside air and is installed in the gap 3 of the hood 2, that is, near the outside air suction point. A device 10 for measuring air volume or speed is provided. The measuring device 10 is electrically connected to a speed adjusting device 12 that adjusts the speed of the exhaust fan driving electric motor 11 so that the measured air volume matches the set air volume. The rotation speed can be controlled. Next, gap 3 of hood 2
The reason why the measurement tube 9 was provided nearby will be explained. As mentioned above, the suction air is suctioned from the equipment 1 and the gap 3, and the suction air volume is determined by the pressure difference between the internal pressure and the outside air pressure. Therefore, if the differential pressure is known, the flow rate passing through the three gaps can be calculated, and the flow rate as the product of the flow rate and the area of the three gaps can be calculated. Moreover, this allows the differential pressure to be used as a representative value of the suction amount. However, as described above, it is difficult to measure the pressure inside the hood 2 accurately, and it is also difficult to directly measure the flow rate passing through the three gaps. Therefore, gap 3 of hood 2
By providing a small-diameter measuring tube 9 nearby as a new gap, the flow velocity or flow rate inside the measuring tube 9 can be used as a representative value of the suction amount. For this reason, since the fluid passing through the measuring tube 9 is the atmosphere and the temperature is the atmospheric temperature, extremely accurate measurements can be made. Although not shown, if measurements are to be made intermittently, a valve may be provided at the inlet of the measurement tube 9 and normally closed to reduce the amount of leakage. With such a configuration, during actual operation, the rotational speed of the exhaust fan 7 is varied, and the numerical value of the measuring closed device 10 is read when the necessary and sufficient dust collection situation is achieved. Then, by controlling the rotational speed of the exhaust fan driving electric motor 11 using this numerical value as a set value, loss of effectiveness due to excessive exhaust air can be prevented. In the above embodiment, the rotation speed of the electric motor 11 of the exhaust fan 7 is controlled, but any air volume control means that can reduce power, such as a fluid coupling or control of the inlet damper 6, may be used. As described above, according to the method of the present invention, it is possible to accurately measure the flow rate or flow velocity of the atmosphere at the outside air suction point of the suction part of the hood equipment, etc., and to make it possible to ensure a sufficient exhaust air volume even when the dust collection equipment is necessary for fluctuations in gas temperature. I can,
As a result, power consumption can be kept to a necessary minimum and energy savings can be achieved. In addition, by adopting this method, for example, if a hole occurs due to dust in the dust collection duct, the value in the measurement pipe will not reach the predetermined value. It is possible to know the occurrence of a hole without having to check the hole, which can be of great help in saving labor.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は従来の集塵設備の概略構成図、第2図
は第1図の集塵設備における排風機の実風量と圧
力の関係および排風機の実風量と動力の関係をあ
らわす図、第3図は本発明に係る集塵設備の概略
構成図である。 1……設備、2……フード、3……すきま(外
気吸引個所)、9……計測管、10……風量もし
くは風速測定用機器。
Figure 1 is a schematic configuration diagram of a conventional dust collection equipment, Figure 2 is a diagram showing the relationship between the actual air volume and pressure of the exhaust fan and the relationship between the actual air volume and power of the exhaust fan in the dust collection equipment shown in Figure 1. FIG. 3 is a schematic diagram of the dust collection equipment according to the present invention. 1... Equipment, 2... Hood, 3... Gap (outside air suction point), 9... Measuring pipe, 10... Equipment for measuring air volume or wind speed.

Claims (1)

【特許請求の範囲】[Claims] 1 設備からのダスト、煙の発生を防止するため
にフード設備などの吸引部を設けた集塵設備にお
いて、吸引部の外気吸引個所近傍に外気と連通す
る計測管を設け、この計測管を通過する大気の流
量もしくは流速を計測してその値を前記吸引個所
の集塵風量の代表値とし、この代表値が所定の設
定値になるよう集塵設備の排風量を自動的に調整
することを特徴とする集塵設備の吸引風量制御方
法。
1 In dust collection equipment equipped with a suction part such as a hood equipment in order to prevent the generation of dust and smoke from the equipment, a measurement pipe communicating with the outside air is installed near the outside air suction point of the suction part, and the air passing through this measurement pipe is installed near the outside air suction point of the suction part. The method is to measure the flow rate or flow velocity of the atmospheric air, use that value as a representative value of the dust collection air volume at the suction point, and automatically adjust the exhaust air volume of the dust collection equipment so that this representative value becomes a predetermined set value. Features: A suction air volume control method for dust collection equipment.
JP13166582A 1982-07-27 1982-07-27 How to control the suction air volume of dust collection equipment Granted JPS5922622A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP13166582A JPS5922622A (en) 1982-07-27 1982-07-27 How to control the suction air volume of dust collection equipment

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP13166582A JPS5922622A (en) 1982-07-27 1982-07-27 How to control the suction air volume of dust collection equipment

Publications (2)

Publication Number Publication Date
JPS5922622A JPS5922622A (en) 1984-02-04
JPS6154451B2 true JPS6154451B2 (en) 1986-11-22

Family

ID=15063360

Family Applications (1)

Application Number Title Priority Date Filing Date
JP13166582A Granted JPS5922622A (en) 1982-07-27 1982-07-27 How to control the suction air volume of dust collection equipment

Country Status (1)

Country Link
JP (1) JPS5922622A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2004150190A (en) * 2002-10-31 2004-05-27 Takenaka Komuten Co Ltd Dust diffusion preventing system

Families Citing this family (2)

* Cited by examiner, † Cited by third party
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JPS61167420A (en) * 1985-01-21 1986-07-29 Satake Eng Co Ltd Bag filter device
JPS63315122A (en) * 1987-06-17 1988-12-22 Shintou Dasutokorekutaa Kk Dust collection process for combustion furnace

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2004150190A (en) * 2002-10-31 2004-05-27 Takenaka Komuten Co Ltd Dust diffusion preventing system

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