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JPH0355779B2 - - Google Patents
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JPH0355779B2 - - Google Patents

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Publication number
JPH0355779B2
JPH0355779B2 JP60184567A JP18456785A JPH0355779B2 JP H0355779 B2 JPH0355779 B2 JP H0355779B2 JP 60184567 A JP60184567 A JP 60184567A JP 18456785 A JP18456785 A JP 18456785A JP H0355779 B2 JPH0355779 B2 JP H0355779B2
Authority
JP
Japan
Prior art keywords
particle size
optical lens
light
output
laser beam
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
JP60184567A
Other languages
Japanese (ja)
Other versions
JPS6244645A (en
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 filed Critical
Priority to JP60184567A priority Critical patent/JPS6244645A/en
Publication of JPS6244645A publication Critical patent/JPS6244645A/en
Publication of JPH0355779B2 publication Critical patent/JPH0355779B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N15/00Investigating characteristics of particles; Investigating permeability, pore-volume or surface-area of porous materials
    • G01N15/02Investigating particle size or size distribution
    • G01N15/0205Investigating particle size or size distribution by optical means

Landscapes

  • Chemical & Material Sciences (AREA)
  • Dispersion Chemistry (AREA)
  • Physics & Mathematics (AREA)
  • Health & Medical Sciences (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Analytical Chemistry (AREA)
  • Biochemistry (AREA)
  • General Health & Medical Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • Immunology (AREA)
  • Pathology (AREA)
  • Investigating Or Analysing Materials By Optical Means (AREA)

Description

【発明の詳細な説明】 [産業上の利用分野] この発明はガスタービン、デイーゼルエンジ
ン、ボイラ等の燃焼室に液体燃料を供給する噴射
弁から噴霧粒子、あるいは噴霧乾燥法による粉体
製造過程における固体粒子の代表粒径を計測する
装置に関するものである。
[Detailed Description of the Invention] [Industrial Application Field] This invention is applicable to the production of spray particles from an injection valve that supplies liquid fuel to the combustion chamber of a gas turbine, diesel engine, boiler, etc., or in the process of producing powder by a spray drying method. The present invention relates to a device for measuring the representative particle size of solid particles.

[従来技術] 従来この種の装置においては、テレビカメラに
より噴霧された粒子を撮影し、画像処理を行つて
代表粒径を計測する装置や、1個づつの粒子から
の散乱光の特徴からその粒径を求め、代表粒径を
計測する装置があるが、これらはいずれも画像処
理による統計上のサンプリングを必要とし、その
統計上十分なサンプルを得るためには時間がかか
ると共に、たとえばデイーゼルエンジン用の燃料
噴射弁からの噴霧のようにきわめて短時間に終了
する場合や、過渡的な変化を伴う噴霧の計測は不
可能である。更に、個々の粒子ではなく、粒子群
の光回折現像を利用し、代表粒径を計測する装置
があるが、この装置を利用するにはあらかじめ計
算された多数の回折パターンを形成してフアイル
しておき、これら回折パターンのフアイル中から
測定パターンに最も近いものを探し出してパター
ン合せをする必要があるので、その作業及び解析
に多くの時間を要すると共に、回折パターンの検
出部及び解析部の構成が複雑で大型化し、高価と
なる問題点がある。
[Prior art] Conventionally, in this type of device, there is a device that photographs the sprayed particles with a television camera, performs image processing, and measures the representative particle size, and a device that measures the representative particle size based on the characteristics of the scattered light from each particle. There are devices that determine the particle size and measure the representative particle size, but all of these require statistical sampling using image processing, and it takes time to obtain statistically sufficient samples, and it is difficult to use, for example, in a diesel engine. It is impossible to measure sprays that end in an extremely short period of time, such as sprays from commercial fuel injection valves, or sprays that involve transient changes. Furthermore, there is a device that uses optical diffraction development of a group of particles rather than individual particles to measure the representative particle size. In addition, it is necessary to find the one closest to the measurement pattern from among these diffraction pattern files and match the pattern, which requires a lot of time and requires a lot of time to perform the work and analysis. However, there are problems in that it is complicated, large-sized, and expensive.

[発明が解決しようとする問題点] 本発明は前記した従来例における粒径の計測の
ために多くの時間を要するという問題点を解消す
ると共に、過渡的変化を伴う噴霧粒子の計測不可
の問題点及び装置の複雑で且つ大型化の問題点を
解決しようとするものである。
[Problems to be Solved by the Invention] The present invention solves the above-mentioned problem in the conventional example that it takes a lot of time to measure the particle size, and also solves the problem that it is impossible to measure spray particles that involve transient changes. This is an attempt to solve the problems of complicated and large-sized devices.

[問題点を解決するための手段] 本発明は前記問題点を解決する具体的手段とし
て、レーザ発振器と、レーザビームで照射した噴
霧粒子群から前方に散乱される光を集光する光学
レンズと、該光学レンズの焦点位置に配して2個
の同心円形状の光電素子と、それらの光電素子か
らの電流信号をそれぞれ増幅する対数増幅器と、
それら各増幅器からの出力差を出力する引算器
と、その出力をA/D変換するA/D変換器と、
A/D変換された出力から粒径を演算する演算器
と、該演算結果をデイジタル表示する表示器とか
らなる噴霧粒子の粒径計測装置を提供するもので
あつて、レーザビームを噴霧粒子群に照射し、噴
霧粒子群で散乱した光を集光し、光電素子により
受光して電流信号を取り出し、その電流信号に基
いて瞬時に演算しデジタル表示するものもである
から計測のための時間が著しく短縮されると共
に、装置自体も小型軽量化されるのである。
[Means for Solving the Problems] As a specific means for solving the above problems, the present invention provides a laser oscillator, an optical lens for condensing light scattered forward from a group of spray particles irradiated with a laser beam, and the like. , two concentric photoelectric elements disposed at the focal point of the optical lens, and a logarithmic amplifier that amplifies the current signals from the photoelectric elements, respectively;
A subtracter that outputs the output difference from each of the amplifiers, and an A/D converter that converts the output from A/D.
The present invention provides a particle size measuring device for atomized particles, which includes a calculation unit that calculates a particle size from an A/D converted output, and a display device that digitally displays the calculation result, and the device is configured to measure a particle size of atomized particles by directing a laser beam to a group of atomized particles. The light scattered by the spray particles is collected, the photoelectric element receives the light, extracts a current signal, and instantaneously calculates and digitally displays the current signal based on the current signal. This will significantly shorten the time required, and the device itself will also be made smaller and lighter.

[実施例] 次に本発明を図示の実施例に基き更に詳しく説
明すると、1はレーザ発振器であり、該レーザ発
振器から照射されるレーザビームはコリメータレ
ンズ2によりコリメートされて平行なレーザビー
ム3として被測定噴霧粒子群3に照射される。噴
霧粒子群3を通過又は散乱した光を集光するため
の光学レンズ5が前記コルメーターレンズ2から
適宜の間隔をもつて配設され、該光学レンズ5の
略焦点位置に例えばシリコンフオトデイテクタ等
からなる環状を呈した2個の光電変換素子6,7
が同心円状に配設してある。この場合に、2個の
光電変換素子6,7は前記光学レンズ5の焦点位
置を中心にして光学レンズ5と対面するように同
心円状に配設される。
[Embodiments] Next, the present invention will be explained in more detail based on the illustrated embodiments. 1 is a laser oscillator, and a laser beam emitted from the laser oscillator is collimated by a collimator lens 2 to form a parallel laser beam 3. The spray particle group 3 to be measured is irradiated. An optical lens 5 for condensing the light that has passed through or been scattered by the spray particle group 3 is disposed at an appropriate distance from the colmeter lens 2, and a silicon photodetector, for example, is installed approximately at the focal point of the optical lens 5. Two annular photoelectric conversion elements 6, 7 consisting of
are arranged in concentric circles. In this case, the two photoelectric conversion elements 6 and 7 are arranged concentrically so as to face the optical lens 5 with the focus position of the optical lens 5 as the center.

このように配設された光電変換素子6,7は光
を受けることによつて電流を発生すると共に光量
によつて電流が増減し、それを電流信号として取
出すことができる。この電流信号を夫々同一特性
を有する対数増幅器8,9により増幅して引算回
路10に入力させる。この引算回路10により前
記対数増幅器8,9から入力された電流信号を引
算して出力され、A/D変換器11により変換さ
れて演算器12に入力され、該演算器12で演算
された結果が表示器13によつてデジタル表示さ
れるようになつている。
The photoelectric conversion elements 6 and 7 arranged in this manner generate current by receiving light, and the current increases or decreases depending on the amount of light, which can be extracted as a current signal. This current signal is amplified by logarithmic amplifiers 8 and 9, each having the same characteristics, and is input to a subtraction circuit 10. This subtraction circuit 10 subtracts the current signals input from the logarithmic amplifiers 8 and 9 and outputs the result, which is converted by the A/D converter 11 and input to the arithmetic unit 12, where it is calculated. The results are digitally displayed on the display 13.

前記演算器12での代表粒径算出について説明
すると、まず平行なレーザビーム3を受けて粒子
群4から前方に散乱される光の強度分布は、個々
の粒子からの散乱光強度の重ね合せであり、個々
の粒子から散乱光強度の分布は理論的に計算され
る。粒子群による散乱光の強度分布を種々の粒径
分布に対して検討したところ、焦点上での光強度
Ioと散乱角θによる焦点面での光強度I(θ)と
の比は、代表粒径Dと光の波長λとの比(πD/
λ)θの関係において、 O<(πD/λ)θ<2.5 の範囲では第3図のグラフに示したように、ほぼ
一定の関係にあることが分つた。そこで、I
(θ)/Ioと(πD/λ)θとの関係は、実用上充
分な精度で lnI(θ)/Io=−β(πD/λθ)2 と表わせるので、所定の角度θ1とθ2における強度
の比から次式により計算される。
To explain the calculation of the representative particle size by the arithmetic unit 12, first, the intensity distribution of the light scattered forward from the particle group 4 after receiving the parallel laser beam 3 is the superposition of the scattered light intensities from the individual particles. The distribution of scattered light intensity from individual particles is calculated theoretically. When we investigated the intensity distribution of scattered light by particle groups for various particle size distributions, we found that the light intensity at the focal point
The ratio of Io to the light intensity I(θ) at the focal plane due to the scattering angle θ is the ratio of the representative particle diameter D to the light wavelength λ (πD/
As shown in the graph of FIG. 3, it was found that the relationship between λ) and θ is almost constant in the range of O<(πD/λ)θ<2.5. Therefore, I
The relationship between (θ)/Io and (πD/λ)θ can be expressed as lnI(θ)/Io=−β(πD/λθ) 2 with sufficient accuracy for practical purposes, so if the predetermined angles θ 1 and θ It is calculated from the ratio of the intensities at 2 using the following formula.

従つて、測定しようとする噴霧粒子群4にレー
ザビーム3を照射し、光学レンズ5を通して集光
された光の内、焦点位置に集光する光は光電変換
素子7により受光されて所定の電流が出力され、
所定の角度に散乱した光が焦点面におけるリング
状の位置、即ち光電変換素子6により受光され、
その光量によつて所定の電流が出力される。そし
てこれら両電流は夫々対数増幅器8,9を介して
引算回路10によりその差が出力され、該出力が
A/D変換され前記演算器12により上記式に基
いて直ちに演算され、その結果が速かに表示器1
3に表示されるのである。従つて、表示された数
値は噴霧粒子の径を示すのである。
Therefore, the laser beam 3 is irradiated onto the atomized particle group 4 to be measured, and among the light that is focused through the optical lens 5, the light that is focused at the focal position is received by the photoelectric conversion element 7 and is converted into a predetermined current. is output,
The light scattered at a predetermined angle is received at a ring-shaped position on the focal plane, that is, by the photoelectric conversion element 6,
A predetermined current is output depending on the amount of light. The difference between these two currents is outputted by a subtraction circuit 10 via logarithmic amplifiers 8 and 9, respectively, and the output is A/D converted and immediately calculated by the arithmetic unit 12 based on the above formula, and the result is Immediately display 1
It is displayed in 3. Therefore, the displayed value indicates the diameter of the atomized particles.

[発明の効果] 以上説明したように本発明に係る噴霧粒子径の
計測装置は、被計測噴霧粒子群にレーザビームを
照射し、噴霧粒子群を通過した光、即ち散乱光を
光学レンズで集光し、その焦点位置の面に環状の
2個の光電変換素子を配設し、両光電変換素子の
出力差に基き、演算器により所定の演算を行うこ
とで直ちに粒径が測定できるものであり、従来例
のように膨大なサンプリングのデータ等を全く必
要とせず、しかもデータとの照合作業もなく、瞬
時にして粒径が計測できるという優れた効果を奏
する。
[Effects of the Invention] As explained above, the spray particle diameter measuring device according to the present invention irradiates the spray particle group to be measured with a laser beam, and collects the light that has passed through the spray particle group, that is, the scattered light, with an optical lens. The particle size can be measured immediately by emitting light, placing two annular photoelectric conversion elements on the plane of its focal position, and performing a predetermined calculation using a calculator based on the output difference between the two photoelectric conversion elements. Unlike conventional methods, this method does not require a huge amount of sampling data at all, and also has the excellent effect of being able to measure particle diameters instantly without any data comparison work.

又、その構成においても、レーザ発振器、光学
レンズ、一対の環状光電変換素子以下対数増幅
器、引算回路、演算器及び表示器が一体的に組込
んで形成できるので、全体が小型コンパクト化さ
れるという優れた効果も奏する。
Also, in its configuration, the laser oscillator, optical lens, a pair of annular photoelectric conversion elements, a logarithmic amplifier, a subtraction circuit, an arithmetic unit, and a display can be integrated and formed, so the entire structure can be made smaller and more compact. It also has this excellent effect.

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

第1図は本発明に係る装置の略示的側面図、第
2図は同装置の主要部を略示的に示したブロツク
図、第3図は代表粒径と散乱光の強さとの関係を
示すグラフである。 1……レーザ発振器、2……コリメーターレン
ズ、3……平行ビーム、4……噴霧粒子群、5…
…光学レンズ、6,7……光電変換素子、8,9
……対数増幅器、10……引算回路、11……
A/D変換器、12……演算器、13……表示
器。
Fig. 1 is a schematic side view of the device according to the present invention, Fig. 2 is a block diagram schematically showing the main parts of the device, and Fig. 3 is the relationship between the representative particle size and the intensity of scattered light. This is a graph showing. 1... Laser oscillator, 2... Collimator lens, 3... Parallel beam, 4... Spray particle group, 5...
...Optical lens, 6, 7... Photoelectric conversion element, 8, 9
... Logarithmic amplifier, 10 ... Subtraction circuit, 11 ...
A/D converter, 12... arithmetic unit, 13... display device.

Claims (1)

【特許請求の範囲】 1 レーザ発振器と、レーザビームで照射した噴
霧粒子群から前方に散乱される光を集光する光学
レンズと、該光学レンズの焦点位置に配した2個
の同心円形状の光電素子と、それらの光電素子か
らの電流信号をそれぞれ増幅する対数増幅器と、
それらの各増幅器からの出力差を出力する引算器
と、その出力をA/D変換するA/D変換器と、
A/D変換された出力から粒径を演算する演算器
と、該演算結果をデイジタル表示する表示器とか
らなる噴霧粒子の粒径計測装置。 2 前記レーザ発振器のレーザビームをコリメー
トするコリメータレンズを設けたことを特徴とす
る前記1項記載の噴霧粒子の粒径計測装置。
[Claims] 1. A laser oscillator, an optical lens that condenses light scattered forward from a group of spray particles irradiated with a laser beam, and two concentric photoelectrons arranged at the focal point of the optical lens. a logarithmic amplifier that amplifies the current signals from the photoelectric elements and the photoelectric elements, respectively;
a subtracter that outputs the output difference from each of those amplifiers, and an A/D converter that converts the output from A/D,
A particle size measuring device for atomized particles, which includes a calculator that calculates the particle size from A/D converted output, and a display that digitally displays the calculation result. 2. The atomized particle size measuring device according to item 1 above, further comprising a collimator lens for collimating the laser beam of the laser oscillator.
JP60184567A 1985-08-22 1985-08-22 Measuring instrument for particle size of sprayed particles Granted JPS6244645A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP60184567A JPS6244645A (en) 1985-08-22 1985-08-22 Measuring instrument for particle size of sprayed particles

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP60184567A JPS6244645A (en) 1985-08-22 1985-08-22 Measuring instrument for particle size of sprayed particles

Publications (2)

Publication Number Publication Date
JPS6244645A JPS6244645A (en) 1987-02-26
JPH0355779B2 true JPH0355779B2 (en) 1991-08-26

Family

ID=16155465

Family Applications (1)

Application Number Title Priority Date Filing Date
JP60184567A Granted JPS6244645A (en) 1985-08-22 1985-08-22 Measuring instrument for particle size of sprayed particles

Country Status (1)

Country Link
JP (1) JPS6244645A (en)

Families Citing this family (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63223543A (en) * 1987-03-13 1988-09-19 Canon Inc Particle analysis device
JPH02210247A (en) * 1989-02-10 1990-08-21 Asahi Eng Co Ltd Measuring instrument for contamination degree of oil
JPH0643950B2 (en) * 1989-09-29 1994-06-08 株式会社島津製作所 Particle size distribution measuring device
DE69129260T2 (en) * 1990-11-03 1998-11-19 Horiba Ltd Device for measuring the particle size distribution
KR100489437B1 (en) * 2002-10-25 2005-05-16 한국원자력연구소 System and Method for measuring simultaneously both optical size and aerodynamic size for atmospheric aerosol particles

Also Published As

Publication number Publication date
JPS6244645A (en) 1987-02-26

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