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JPS648583B2 - - Google Patents
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JPS648583B2 - - Google Patents

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Publication number
JPS648583B2
JPS648583B2 JP57066143A JP6614382A JPS648583B2 JP S648583 B2 JPS648583 B2 JP S648583B2 JP 57066143 A JP57066143 A JP 57066143A JP 6614382 A JP6614382 A JP 6614382A JP S648583 B2 JPS648583 B2 JP S648583B2
Authority
JP
Japan
Prior art keywords
liquid
light
frequency
signal
receiving element
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
JP57066143A
Other languages
Japanese (ja)
Other versions
JPS58183960A (en
Inventor
Hisashi Sugimoto
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.)
Asahi Sunac Corp
Original Assignee
Asahi Okuma Industrial 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 Asahi Okuma Industrial Co Ltd filed Critical Asahi Okuma Industrial Co Ltd
Priority to JP57066143A priority Critical patent/JPS58183960A/en
Publication of JPS58183960A publication Critical patent/JPS58183960A/en
Publication of JPS648583B2 publication Critical patent/JPS648583B2/ja
Granted legal-status Critical Current

Links

Landscapes

  • Special Spraying Apparatus (AREA)
  • Application Of Or Painting With Fluid Materials (AREA)
  • Spray Control Apparatus (AREA)

Description

【発明の詳細な説明】 本発明は、液体塗料の無気噴霧のように、高圧
力に加圧した液体を小形のノズルから空気中に高
速度で噴出して微粒化させる無気噴霧における霧
化状態の監視方法、及びその監視方法に使用する
装置に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention is directed to the spraying of airless spraying, in which highly pressurized liquid is ejected into the air from a small nozzle at high speed to atomize it, such as airless spraying of liquid paint. The present invention relates to a method for monitoring the state of environmental change and a device used in the method.

従来、ノズルの先端にリツプ状の噴出孔を設け
て、高圧力に加圧した液体をこの噴出孔から薄膜
状と成して空気中に噴出して微粒化させる無気噴
霧において、噴出孔から噴出する薄膜状の液体の
一側に発光ダイオード等の発光素子を、他側にフ
オトトランジスタ等の受光素子を夫々設けて、発
光素子から発せられた光が噴出する薄膜状の液体
を透過して受光素子に受光されるようにし、その
受光量、即ち液体を透過する透過率の変化によつ
て液体の噴出状況を監視しようとする方法は公知
である。
Conventionally, in airless spraying, a lip-shaped ejection hole is provided at the tip of the nozzle, and the highly pressurized liquid is ejected into the air as a thin film and atomized into particles. A light emitting element such as a light emitting diode is provided on one side of the ejected thin film liquid, and a light receiving element such as a phototransistor is provided on the other side, so that the light emitted from the light emitting element is transmitted through the ejected thin film liquid. A method is known in which the liquid is ejected by a light-receiving element and the amount of light received, that is, changes in the transmittance through the liquid, is used to monitor the ejection status of the liquid.

しかしながら、このような監視方法では、ノズ
ルの詰まりなどの原因によつて液体の噴出が完全
に停止したとか、或いは噴出量が極端に減少した
といつたような、液体の噴出状態の著しい変化が
あつた場合にのみこれを検知し得るのであつて、
その液体の噴出状態の微妙な変化までも検知する
ことは不可能であつた。
However, with this monitoring method, there is no possibility of significant changes in the state of liquid ejection, such as when the ejection of liquid has completely stopped or the amount of ejection has drastically decreased due to a cause such as a clogged nozzle. This can only be detected if
It was impossible to detect even the slightest change in the state of the liquid being ejected.

ところで、ノズルから噴出する薄膜状の液体が
空気との衝突によつて微粒化する霧化状態は、そ
の液体の噴出圧力、粘度、流量等の僅かな変化に
よつて著しい影響を受けるものであつて、液体が
正常な霧化状態にあるか否かを監視するには、前
述した従来の監視方法では不十分であり、液体の
噴出状態の微妙な変化を検知して、霧化状態を常
に正しい状態に保つことができるような監視方法
の確立が望まれていた。
Incidentally, the atomization state in which a thin film of liquid ejected from a nozzle becomes atomized by collision with air is significantly affected by slight changes in the ejection pressure, viscosity, flow rate, etc. of the liquid. Therefore, the conventional monitoring methods described above are insufficient to monitor whether the liquid is in a normal atomization state. It has been desired to establish a monitoring method that can maintain correct conditions.

本発明は、このような噴出液体の微妙な変化を
検知することによつて霧化状態を監視しようとす
る新たな方法を提供することを目的とする。
An object of the present invention is to provide a new method for monitoring the atomization state by detecting such subtle changes in the ejected liquid.

以下、その成立過程について説明すると、第1
図のに示すように、高圧力に加圧されて、リツ
プ状を成す扁平な噴出孔を有するノズルNから高
速度で空気中に噴出する液体Lは、ノズルNから
噴出した直後の極く狭い帯域Aにおいてはほぼ平
滑な膜状を成し、引き続く帯域Bにおいては、空
気との衝突により高速度で波打ち状に振動して空
気中を進行し、霧化点Cにおいて微粒子に分裂し
て飛散する。これを平面的に見ると、第1図の
に示すように、平滑な帯域Aから波打ち帯域Bに
入ると、液膜の幅が急激に拡がり、その膜厚が著
しく減少して霧化点Cにおいて微粒化するのであ
るが、波打ち帯域Bにおける液膜の振動をみてみ
ると、平滑な帯域Aから霧化点Cに向かつて、か
つ帯域の中央から両側に向かつて、液膜の振動周
波数は次第に減少するとともに、その振幅が次第
に拡大してゆくことが実験的に確認されている。
そして、この波打ち帯域Bにおける液膜の振動周
波数が同一となる地点をプロツトしてゆくと、第
1図のに示すように、例えば3000Hzといつた
高周波数の帯域が平滑な帯域Aから波打ち帯域B
のほぼ中央に向かつて次第に幅を拡げつつ拡が
り、その外側に2500Hz、更にその外側に2000Hz
といつたように、同一周波数帯域がその周波数を
次第に低下させながら、花弁状のパターンを成し
て拡がつていき、ついには、液膜の両側縁では例
えば1000Hzという低い周波数で振動し、霧化点
Cにおいて分裂して空気中に飛散してゆくのであ
る。そして、このような液膜の振動周波数が同一
となる地点を結ぶことによつて描かれるパターン
は、噴出する液体の噴出圧力、粘度、流量等の極
く僅かな変化によつても変化し、このとき霧化状
態には著しい変化が現われることが実験的に確認
されている。そこで、この波打ち帯域Bの任意の
地点における液膜の振動周波数を検知し、その変
化が一定値以上となつた場合には、液体の噴出状
態に変化が起きていることを確認できる点に着目
し、具体的にはこの周波数を光学的に検知するこ
とにより、液体の噴出状態、ひいてはその霧化状
態を監視することでができるのである。
Below, we will explain the process of its establishment.
As shown in the figure, the liquid L is pressurized to high pressure and is ejected into the air at high speed from the nozzle N, which has a lip-shaped flat ejection hole. In zone A, it forms a nearly smooth film, and in subsequent zone B, it vibrates at high speed in a wavy manner due to collision with the air and travels through the air, and at the atomization point C, it splits into fine particles and scatters. do. Looking at this from a two-dimensional perspective, as shown in Figure 1, when moving from the smooth zone A to the wavy zone B, the width of the liquid film rapidly expands and the film thickness decreases significantly, causing the atomization point C. However, looking at the vibration of the liquid film in the undulating zone B, the vibration frequency of the liquid film is It has been experimentally confirmed that the amplitude gradually increases as the amplitude gradually decreases.
Then, when plotting the points where the vibration frequencies of the liquid film in the wavy band B are the same, as shown in Figure 1, the high frequency band, for example 3000 Hz, changes from the smooth band A to the wavy band. B
2500Hz on the outside, and 2000Hz on the outside.
As mentioned above, the frequency of the same frequency band gradually decreases and spreads out in a petal-like pattern, until the edges of the liquid film vibrate at a low frequency of, for example, 1000Hz, causing fog. At the transformation point C, it splits and scatters into the air. The pattern drawn by connecting points where the vibration frequency of the liquid film is the same changes even with extremely slight changes in the ejection pressure, viscosity, flow rate, etc. of the ejected liquid. It has been experimentally confirmed that there is a significant change in the atomization state at this time. Therefore, we focused on the point that it is possible to detect the vibration frequency of the liquid film at any point in this waving band B, and if the change exceeds a certain value, it can be confirmed that a change has occurred in the liquid ejection state. Specifically, by optically detecting this frequency, it is possible to monitor the ejection state of the liquid and, by extension, the atomization state.

以下、本発明の実施例を第2図に基づいて説明
する。
Hereinafter, embodiments of the present invention will be described based on FIG. 2.

図において、1は先端にリツプ状を成す扁平な
噴出孔2を備えたノズルであつて、高圧力に加圧
された液体Lがそのノズル1の噴出孔2から空気
中に高速度で噴出される。このとき、噴出孔2か
ら噴出した直後の液体Lは、前述したように、狭
い範囲において平滑な液膜を形成し、その後空気
との衝突によつて波打ち状に振動し、振動周波数
が低下するとともに振幅が拡大して、ついには微
粒子に分裂して空気中に飛散してゆく。又、ノズ
ル1の噴出孔2の両側には、この噴出孔2と同一
方向に細長い空気噴出孔3,4が形成されてい
て、これらの空気噴出孔3,4から噴出された加
圧空気がエアカーテン5,6となつて、噴出孔2
から噴出する液体Lの両側においてほぼ平行に形
成されるようになつている。一方のエアカーテン
5の外側には、発光ダイオード等の第1の発光素
子7が液体Lの噴出方向に対して、約45゜の角度
を成して設置されていて、この発光素子7から発
せられる光が、液体Lの波打ち帯域を透過するよ
うになつており、この透過光は、他方のエアカー
テン6の外側に前記発光素子7と光軸を等しくす
るように設置されたフオトトランジスタ等の受光
素子8によつて受光されるようになつている。又
第2の発光素子9は、受光素子8と同じ側に配設
されており、前記第1の発光素子7から発せられ
た光が液体Lを透過する点とほぼ同一の地点に向
けて光を発し、その液膜に当つて反射した光が受
光素子8に受光されるようになつている。又受光
素子8は増幅器10に接続され、この増幅器10
は比較装置11に接続され、これは更に出力装置
12に接続されている。
In the figure, 1 is a nozzle equipped with a lip-shaped flat ejection hole 2 at the tip, and liquid L pressurized to a high pressure is ejected into the air from the ejection hole 2 of the nozzle 1 at a high velocity. Ru. At this time, as described above, the liquid L immediately after being ejected from the ejection hole 2 forms a smooth liquid film in a narrow range, and then vibrates in a undulating manner due to collision with the air, and the vibration frequency decreases. At the same time, the amplitude increases, and eventually it breaks up into fine particles and scatters into the air. Further, elongated air ejection holes 3 and 4 are formed on both sides of the ejection hole 2 of the nozzle 1 in the same direction as the ejection hole 2, and the pressurized air ejected from these air ejection holes 3 and 4 is The air curtains 5 and 6 form the nozzle 2.
The liquid L is formed substantially parallel to each other on both sides of the liquid L jetted from the liquid L. On the outside of one air curtain 5, a first light emitting element 7 such as a light emitting diode is installed at an angle of approximately 45 degrees with respect to the direction in which the liquid L is ejected. The transmitted light is transmitted through the undulating band of the liquid L, and this transmitted light is transmitted through a phototransistor or the like installed outside the other air curtain 6 so that the optical axis is equal to that of the light emitting element 7. The light is received by the light receiving element 8. Further, the second light emitting element 9 is disposed on the same side as the light receiving element 8, and emits light toward approximately the same point where the light emitted from the first light emitting element 7 passes through the liquid L. is emitted, and the light that hits the liquid film and is reflected is received by the light receiving element 8. Further, the light receiving element 8 is connected to an amplifier 10, and this amplifier 10
is connected to a comparison device 11, which in turn is connected to an output device 12.

次に、本実施例の作用を説明すると、第1の発
光素子7から発せられた光は、波打ち帯域におけ
る液膜の所定地点を透過して受光素子8によつて
受光されるのであるが、その地点における液膜は
サインカーブを成すように波打ち状に振動するた
め、時間とともにその透過率が変化する。即ち、
液膜が透過光とほぼ直角になつた場合には、その
透過率は最大となつて受光量が最大になるのに対
し、液膜が透過光とほぼ平行若しくはそれに近い
小角度を成す場合には、その透過率が最小となつ
て受光量が最小となり、この受光量の変化の周期
は液膜の振動周波数と一致する。即ち、受光素子
8には、液膜の振動周波数と同一の周波数で変化
する光信号が入力され、この光信号は受光素子8
で電気信号に変換された後増幅器10で増幅され
て比較装置11に入力される。ところで、この噴
出液体Lの噴出圧力が低下したり、又液体Lが塗
料である場合には、その塗料の粘度を調節するヒ
ータの故障などによつて粘度が上昇したり、或い
はノズル1の噴出孔2に異物が詰まつて噴出流量
が減少したなどといつた異常が生じた場合には、
波打ち帯域における振動周波数の同一地点を結ん
でなるパターンが変化するため、発光素子7から
発せられた光が透過する地点の液膜の振動周波数
も変化ることとなる。この変化はそのまま受光素
子8で変換される電気信号の周波数の変化として
増幅器10に入力され、この増幅器10で増幅さ
れた後比較装置11に入力される。この電気信号
の周波数の変化が、予め比較装置11に入力され
ている周波数の許容範囲を越えたときには、比較
装置11から出力装置12に対して異常検知信号
が送出されて、この信号を受けた出力装置12
は、液体Lの噴射を停止したり、或いは警報装置
等を作動する。
Next, to explain the operation of this embodiment, the light emitted from the first light emitting element 7 is transmitted through a predetermined point of the liquid film in the waving band and is received by the light receiving element 8. Since the liquid film at that point vibrates in a wavy manner forming a sine curve, its transmittance changes over time. That is,
When the liquid film is almost perpendicular to the transmitted light, its transmittance is maximum and the amount of light received is maximum, whereas when the liquid film is almost parallel to the transmitted light or at a small angle close to it, When the transmittance becomes the minimum, the amount of light received becomes the minimum, and the period of change in the amount of light received coincides with the vibration frequency of the liquid film. That is, an optical signal that changes at the same frequency as the vibration frequency of the liquid film is input to the light receiving element 8, and this optical signal is input to the light receiving element 8.
After the signal is converted into an electrical signal, it is amplified by an amplifier 10 and input to a comparator 11. By the way, if the jetting pressure of this jetting liquid L decreases, or if the liquid L is a paint, the viscosity increases due to a failure of the heater that adjusts the viscosity of the paint, or the jetting of the nozzle 1 If an abnormality occurs such as a decrease in the jet flow rate due to foreign matter clogging the hole 2,
Since the pattern formed by connecting points with the same vibration frequency in the waving band changes, the vibration frequency of the liquid film at the point through which the light emitted from the light emitting element 7 is transmitted also changes. This change is directly input to the amplifier 10 as a change in the frequency of the electric signal converted by the light receiving element 8, and after being amplified by the amplifier 10, is input to the comparator 11. When the change in the frequency of this electrical signal exceeds the permissible frequency range inputted in advance to the comparison device 11, an abnormality detection signal is sent from the comparison device 11 to the output device 12, and this signal is received. Output device 12
stops the injection of liquid L or activates an alarm device or the like.

一方、第2の発光素子9から発せられた光は、
液膜の所定地点で反射して前記受光素子8で受光
されるようになつており、液膜の振動によつて反
射角度が変化するため、その反射方向が変化する
ことによつて受光素子8の受光量が変化する。こ
こに、受光量の変化の周期は液膜の振動周波数と
一致するから、第2の発光素子9からの反射光
も、前述した第1の発光素子7からの透過光と同
じように、液膜の振動周波数と同一の周波数で変
化する光信号として受光素子8に入力される。従
つて、液膜の振動周波数の変化は、第1の発光素
子7或いは第2の発光素子9から発せられる何れ
か一方の光を受光素子8で受光するようにすれば
検知できるのであるが、両者を併用して透過光と
反射光の両方を受光素子8で受光することによつ
て、より確実に検知することができる。又、第1
の受光素子7からの透過光と第2の発光素子9か
らの反射光を干渉させて、この干渉を利用するこ
とによつて一層明確な検知が可能となる。
On the other hand, the light emitted from the second light emitting element 9 is
The light is reflected at a predetermined point on the liquid film and is received by the light receiving element 8, and since the reflection angle changes due to the vibration of the liquid film, the light receiving element 8 receives the light by changing the direction of reflection. The amount of light received changes. Here, since the period of change in the amount of received light matches the vibration frequency of the liquid film, the reflected light from the second light emitting element 9 also changes from the liquid in the same way as the transmitted light from the first light emitting element 7 described above. The light is input to the light receiving element 8 as an optical signal that changes at the same frequency as the vibration frequency of the membrane. Therefore, changes in the vibration frequency of the liquid film can be detected by having the light receiving element 8 receive the light emitted from either the first light emitting element 7 or the second light emitting element 9. By using both in combination and receiving both transmitted light and reflected light at the light receiving element 8, more reliable detection can be achieved. Also, the first
By causing the transmitted light from the light receiving element 7 and the reflected light from the second light emitting element 9 to interfere with each other, and by utilizing this interference, clearer detection becomes possible.

尚、空気噴出孔3,4から噴出する加圧空気で
形成されるエアカーテン5,6は、発光素子7,
9及び受光素子8の発光面及び受光面に液体が付
着して、その性能が低下するのを防止するための
ものであつて、第3図に示すように、発光素子7
若しくは受光素子8を保護筒13内に収容し、そ
の一端に接続した加圧空気供給管14から供給さ
れる加圧空気を発光素子7若しくは受光素子8の
周りを通して保護筒13から噴出することによ
り、ノズル1から噴出する液体Lの微粒子が発光
素子7若しくは受光素子8に付着するのを防止す
るようにしてもよい。
Note that the air curtains 5 and 6 formed by pressurized air ejected from the air ejection holes 3 and 4 are connected to the light emitting elements 7,
As shown in FIG.
Alternatively, the light-receiving element 8 is housed in the protective cylinder 13, and pressurized air supplied from the pressurized air supply pipe 14 connected to one end of the protective cylinder 13 is passed around the light-emitting element 7 or the light-receiving element 8 and ejected from the protective cylinder 13. It may also be possible to prevent fine particles of the liquid L ejected from the nozzle 1 from adhering to the light emitting element 7 or the light receiving element 8.

又、受光素子8は、フオトトランジスタのよう
に、光を受光してこれを電気信号に変換するもの
だけに限らず、例えば、受光素子8を光フアイバ
として、発光素子7或いは9の透過光若しくは反
射光を光信号のままで遠隔地に送つて、遠隔地に
設けた光電変換装置によつて電気信号に変換する
ようにしても良い。
Furthermore, the light receiving element 8 is not limited to one that receives light and converts it into an electrical signal, such as a phototransistor. The reflected light may be sent to a remote location as an optical signal and converted into an electrical signal by a photoelectric conversion device provided at the remote location.

上記実施例によつて具体的に説明したように、
本発明の無気噴霧における霧化状態の監視方法
は、ノズルから噴出した直後の薄膜状の液体の所
定位置に光を照射し、該液体を透過し若しくは反
射した光を受光して前記液体の所定位置における
振動数に対応する周波数の信号に変換し、該信号
の周波数の変化によつて前記液体の霧化状態を監
視することを要旨とするものであつて、液体を透
過し若しくは反射する光の強さによつて、その液
体の噴出状態を検知するのではなく、噴出する液
体の空気との衝突による波打ち状の振動の変化
を、透過光若しくは反射光の光の周波数の変化と
して受光し、これを信号に変換して、その周波数
の変化によつて霧化状態の変化を監視するように
したものであるから、噴出液体の噴出圧力、粘
度、流量等の極く僅かな変化をも正確に検知する
ことが可能となり、これらの微妙な変化によつて
影響を受ける液体の霧化状態を正確に監視するこ
とができて、例えば粗大な粒子の発生を防止する
ことできる効果を奏する。
As specifically explained in the above embodiment,
The method for monitoring the atomization state in airless spraying of the present invention is to irradiate light onto a predetermined position of a thin film of liquid immediately after it has been ejected from a nozzle, and to receive the light that has passed through or reflected from the liquid. The gist is to convert the signal into a signal with a frequency corresponding to the frequency of vibration at a predetermined position, and monitor the atomization state of the liquid based on changes in the frequency of the signal, and to transmit or reflect the liquid. Rather than detecting the ejected state of the liquid based on the intensity of the light, the system detects changes in the wave-like vibrations caused by the collision of the ejected liquid with the air as changes in the frequency of transmitted or reflected light. However, this is converted into a signal and changes in the atomization state are monitored based on changes in the frequency, so extremely small changes in the ejection pressure, viscosity, flow rate, etc. of the ejected liquid can be monitored. This makes it possible to accurately detect the atomization state of the liquid, which is affected by these subtle changes, and has the effect of preventing the generation of coarse particles, for example. .

又、本発明の無気噴霧における霧化状態の監視
装置は、ノズルから噴出した直後の薄膜状の液体
を挾んで若しくは該液体の一側に発光素子と該発
光素子から発せられて前記液体を透過し若しくは
反射した光を受光して前記液体の振動数に対応す
る周波数の信号に変換する受光素子とを設置し、
かつ、前記信号の周波数が所定範囲外となつたと
きに異常検知信号を発する比較装置を前記受光素
子に接続したことを要旨とするものであつて、前
記噴出液体の振動の変化が所定範囲外になつた場
合に、これを直ちに信号として取り出すことがで
き、前記発明方法を確実に実施し得る効果を奏す
る。
Further, the atomization state monitoring device in airless spraying of the present invention sandwiches a thin film of liquid immediately after it has been ejected from a nozzle, or attaches a light emitting element to one side of the liquid and displays the liquid emitted from the light emitting element. a light receiving element that receives transmitted or reflected light and converts it into a signal with a frequency corresponding to the frequency of the liquid;
and a comparison device that emits an abnormality detection signal when the frequency of the signal is outside a predetermined range is connected to the light receiving element, and the device is characterized in that when a change in the vibration of the ejected liquid is outside the predetermined range. When this happens, this can be immediately taken out as a signal, which has the effect of ensuring that the method of the invention can be carried out reliably.

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

第1図は無気噴霧の概略を説明するための正面
図及び平面図である。第2図は本発明の一実施例
を示す正面図及びブロツク図である。第3図は本
発明の他の実施例を示す要部断面図である。 1:ノズル、5,6:エアカーテン、7:第1
の発光素子、8:受光素子、9:第2の発光素
子、11:比較装置、L:液体。
FIG. 1 is a front view and a plan view for explaining the outline of airless spraying. FIG. 2 is a front view and a block diagram showing one embodiment of the present invention. FIG. 3 is a sectional view of a main part showing another embodiment of the present invention. 1: Nozzle, 5, 6: Air curtain, 7: First
8: Light-receiving element, 9: Second light-emitting element, 11: Comparison device, L: Liquid.

Claims (1)

【特許請求の範囲】 1 ノズルから噴出した直後の薄膜状の液体の所
定位置に光を照射し、該液体を透過し若しくは反
射した光を受光して前記液体の所定位置における
振動数に対応する周波数の信号に変換し、該信号
の周波数の変化によつて前記液体の霧化状態を監
視することを特徴とする無気噴霧における霧化状
態の監視方法。 2 ノズルから噴出した直後の薄膜状の液体を挾
んで若しくは該液体の一側に発光素子と該発光素
子から発せられて前記液体を透過し若しくは反射
した光を受光して前記液体の振動数に対応する周
波数の信号に変換する受光素子とを設置し、か
つ、前記信号の周波数が所定範囲外となつたとき
に異常検知信号を発する比較装置を前記受光素子
に接続したことを特徴とする無気噴霧における霧
化状態の監視装置。 3 前記受光素子が光フアイバであることを特徴
とする特許請求の範囲第2項記載の無気噴霧にお
ける霧化状態の監視装置。
[Claims] 1. Light is irradiated onto a predetermined position of a thin film of liquid immediately after it has been ejected from a nozzle, and the light transmitted through or reflected from the liquid is received to correspond to the frequency of vibration at the predetermined position of the liquid. A method for monitoring an atomization state in airless spraying, comprising converting the signal into a frequency signal and monitoring the atomization state of the liquid based on changes in the frequency of the signal. 2 A light-emitting element is placed between a thin film of liquid immediately after it has been ejected from a nozzle or on one side of the liquid, and the light emitted from the light-emitting element and transmitted through or reflected from the liquid is received and adjusted to the frequency of the liquid. A light-receiving element that converts the signal into a signal of a corresponding frequency is installed, and a comparison device that emits an abnormality detection signal when the frequency of the signal falls outside a predetermined range is connected to the light-receiving element. A monitoring device for the atomization state in air atomization. 3. The atomization state monitoring device in airless spraying according to claim 2, wherein the light receiving element is an optical fiber.
JP57066143A 1982-04-20 1982-04-20 Method and apparatus for monitoring atomized state in airless spraying Granted JPS58183960A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57066143A JPS58183960A (en) 1982-04-20 1982-04-20 Method and apparatus for monitoring atomized state in airless spraying

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57066143A JPS58183960A (en) 1982-04-20 1982-04-20 Method and apparatus for monitoring atomized state in airless spraying

Publications (2)

Publication Number Publication Date
JPS58183960A JPS58183960A (en) 1983-10-27
JPS648583B2 true JPS648583B2 (en) 1989-02-14

Family

ID=13307337

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57066143A Granted JPS58183960A (en) 1982-04-20 1982-04-20 Method and apparatus for monitoring atomized state in airless spraying

Country Status (1)

Country Link
JP (1) JPS58183960A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62176567A (en) * 1986-01-28 1987-08-03 Honda Motor Co Ltd Automatic coating machine

Also Published As

Publication number Publication date
JPS58183960A (en) 1983-10-27

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