JPH04323540A - Particle size distribution measuring device - Google Patents

Particle size distribution measuring device

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Publication number
JPH04323540A
JPH04323540A JP3090835A JP9083591A JPH04323540A JP H04323540 A JPH04323540 A JP H04323540A JP 3090835 A JP3090835 A JP 3090835A JP 9083591 A JP9083591 A JP 9083591A JP H04323540 A JPH04323540 A JP H04323540A
Authority
JP
Japan
Prior art keywords
scattered light
particle size
light
size distribution
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.)
Granted
Application number
JP3090835A
Other languages
Japanese (ja)
Other versions
JPH07117483B2 (en
Inventor
Manabu Ohata
大畑 学
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.)
Nikkiso Co Ltd
Original Assignee
Nikkiso 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 Nikkiso Co Ltd filed Critical Nikkiso Co Ltd
Priority to JP3090835A priority Critical patent/JPH07117483B2/en
Publication of JPH04323540A publication Critical patent/JPH04323540A/en
Publication of JPH07117483B2 publication Critical patent/JPH07117483B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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  • Investigating Or Analysing Materials By Optical Means (AREA)

Abstract

PURPOSE:To provide a particle size distribution measuring device in which a scattered light measuring cell is so disposed to prevent lowering of scattered light due to particles of micro particle size. CONSTITUTION:A particle size distribution measuring device includes a laser light emission means 2, a scattered light measuring cell 4 disposed on the ongoing optical axis of laser light emitted from the laser light emission means 2, and a scattered light measuring means comprising a light collecting lens 5 for collecting scattered light and a detection light-receiving element 6 for measuring the intensity of the scattered light. The light emission face of the scattered light measuring cell 4 is so disposed to have an angle of inclination with respect to the ongoing optical axis of the laser light.

Description

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

【0001】0001

【産業上の利用分野】この発明は、粒度分布測定装置に
関する。さらに詳しくは、微小な粒径を有する粒子によ
る散乱光を効率よく透過させるように散乱光測定用セル
を配置した粒度分布測定装置に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a particle size distribution measuring device. More specifically, the present invention relates to a particle size distribution measuring device in which a scattered light measuring cell is arranged so as to efficiently transmit scattered light caused by particles having a minute particle size.

【0002】0002

【従来の技術と発明が解決しようとする課題】近年、セ
ラミックス原料、超伝導物質、磁性材料等の製造工程あ
るいは半導体の製造工程において、超微粒子が注目され
ており、光の波長よりも小さなサブミクロン粒子の粒径
を測定する必要性が高まっている。
[Prior Art and Problems to be Solved by the Invention] In recent years, ultrafine particles have attracted attention in the manufacturing process of ceramic raw materials, superconducting materials, magnetic materials, etc., or in the manufacturing process of semiconductors. There is an increasing need to measure the particle size of micron particles.

【0003】一般に、これらの微小粒子の径あるいは粒
度分布の測定には、光学的粒径分布測定装置が利用され
ている。前記光学的粒径分布測定装置は、散乱光測定用
セルに収納された被測定粒子群にレーザ光を照射するこ
とによって発生した散乱光を、光学レンズによって集光
し、レンズ焦点面に配置された検出用受光素子によって
測定された前記散乱光の強度分布から散乱光強度の散乱
角度に対する分布を求め、その解析から粒径分布を決定
する。この粒径分布は、散乱光の強度分布を測定するこ
とで、ミィーの散乱理論に基づき計算で求められるもの
である。
[0003] Generally, an optical particle size distribution measuring device is used to measure the diameter or particle size distribution of these microparticles. The optical particle size distribution measuring device collects scattered light generated by irradiating a group of particles to be measured housed in a scattered light measurement cell with a laser beam using an optical lens, and focuses the scattered light on the focal plane of the lens. The distribution of the scattered light intensity with respect to the scattering angle is determined from the intensity distribution of the scattered light measured by the detection light receiving element, and the particle size distribution is determined from the analysis. This particle size distribution is calculated based on Mie's scattering theory by measuring the intensity distribution of scattered light.

【0004】粒度分布測定装置で被測定粒子からの散乱
光の強度を測定する場合、測定に使用されるレーザ光の
波長よりも被測定粒子の粒径が十分に大きいときにはレ
ーザ光の入射光前方に小さな角度範囲に集中した散乱光
が生じる。しかしながら、被測定粒子の粒径が、前記レ
ーザ光に対して微小であるときには、レーザ光によって
散乱される散乱角度の範囲が大きく、それに伴って散乱
光測定用セルの出射面に対する前記散乱光の入射角も大
きなものとなる。そのため、散乱光測定用セル出射面の
内壁面における光反射率が高くなり、測定されるべき散
乱光の透過率が低下する。また、一般に被測定粒子の粒
径が前記レーザ光の波長以下であるときには、散乱光の
光量が急激に減少する。したがって、被測定粒子として
微小な粒径を有する粒子が存在している場合、検出用受
光素子で測定される前記微小な粒径を有する粒子による
散乱光が少ないので、検出用受光素子および粒度分布解
析系の回路で生じるノイズと比較してS/Nが悪く、正
確な散乱光強度を測定することができず、必然的に高精
度な粒度分布を測定することができない。
When measuring the intensity of scattered light from particles to be measured using a particle size distribution measuring device, if the particle size of the particles to be measured is sufficiently larger than the wavelength of the laser beam used for measurement, the intensity of the scattered light from the incident particle of the laser beam is measured. Scattered light concentrated in a small angular range occurs. However, when the particle size of the particles to be measured is small with respect to the laser beam, the range of scattering angles at which the laser beam is scattered is large, and accordingly, the scattered light is The angle of incidence also becomes large. Therefore, the light reflectance on the inner wall surface of the emission surface of the cell for measuring scattered light increases, and the transmittance of the scattered light to be measured decreases. Furthermore, generally when the particle size of the particles to be measured is less than the wavelength of the laser beam, the amount of scattered light decreases rapidly. Therefore, when particles having a minute particle size are present as particles to be measured, there is little scattered light due to the particles having the minute particle size measured by the detection light receiving element, so the detection light receiving element and the particle size distribution are The S/N ratio is poor compared to the noise generated in the circuit of the analysis system, making it impossible to accurately measure the scattered light intensity, and inevitably making it impossible to measure the particle size distribution with high precision.

【0005】一方、さまざまの粒子を取り扱う技術分野
においては、測定に使用されるレーザ光の波長に対して
微小な粒径を有する粒子の粒度分布を高い精度で測定す
ることが必要とされている。
On the other hand, in technical fields that handle various particles, it is necessary to measure with high precision the particle size distribution of particles whose diameter is minute compared to the wavelength of the laser light used for measurement. .

【0006】本発明は、前記事情に基ずいてなされたも
のである。すなわち、本発明の目的は、微小粒径の粒子
による散乱光の低減が防止できるように散乱光測定用セ
ルを配置した粒度分布測定装置を提供することにある。
The present invention has been made based on the above circumstances. That is, an object of the present invention is to provide a particle size distribution measuring device in which a scattered light measuring cell is arranged so as to prevent a reduction in scattered light due to particles having a micro particle size.

【0007】[0007]

【前記課題を解決するための手段】前記目的を達成する
ための請求項1に記載の本発明は、平行なレーザー光を
照射するレーザー光照射手段と、被測定粒子を分散させ
てなる懸濁液を収納する散乱光測定用セルと、被測定粒
子による散乱光の強度を測定するために、前記散乱光測
定用セルの前方に配置された検出用受光素子および前記
散乱光を前記検出用受光素子面上に集光させる集光レン
ズからなる散乱光測定手段とを供え、前記レーザ光照射
手段から照射されるレーザ光の進行光軸に対して、前記
散乱光測定用セルの出射面が傾斜するように配置されて
なることを特徴とする粒度分布測定装置。
[Means for Solving the Problems] The present invention as set forth in claim 1 to achieve the above object provides a laser beam irradiation means for irradiating parallel laser beams, and a suspension in which particles to be measured are dispersed. A scattered light measurement cell that stores a liquid, a detection light receiving element disposed in front of the scattered light measurement cell to measure the intensity of the scattered light by the particles to be measured, and a detection light receiving element that receives the scattered light. a scattered light measuring means consisting of a condensing lens for condensing the light onto the element surface, and the output surface of the scattered light measuring cell is inclined with respect to the traveling optical axis of the laser beam irradiated from the laser beam irradiating means. A particle size distribution measuring device characterized in that the particle size distribution measuring device is arranged so as to

【0008】[0008]

【作用】粒度分布測定装置を使用して粒度分布を測定す
る場合、被測定粒子の粒径が、測定に用いられるレーザ
の波長に対して十分に大きいときには、小さな角度範囲
に集中した散乱光が生じるが、粒径が前記波長に対して
微小であるときには、レーザ光によって散乱される散乱
角度の範囲が大きくなる。一般に、界面における光の透
過率(π)は、入射角(θw )、出射角(θg )、
前記界面までの光伝搬媒体の屈折率(n1 )および前
記界面を透過した後の光伝搬媒体の屈折率(n2)を用
いて次式のように表わされる。
[Operation] When measuring particle size distribution using a particle size distribution measuring device, if the particle size of the particles to be measured is sufficiently large compared to the wavelength of the laser used for measurement, scattered light will be concentrated in a small angular range. However, when the particle size is minute compared to the wavelength, the range of scattering angles scattered by the laser beam becomes large. Generally, the transmittance (π) of light at an interface is determined by the angle of incidence (θw), the angle of exit (θg),
It is expressed as follows using the refractive index (n1) of the light propagation medium up to the interface and the refractive index (n2) of the light propagation medium after passing through the interface.

【0009】     π=4 (n1/cosθw) (n2/co
sθg)/{(n1/cosθw)+( n2/cos
θg)}2   散乱光が散乱光測定用セルの出射面を透過する透過
率(πA )は、前記散乱光測定用セルの内部に収納さ
れた、被測定粒子を含有する試料液と散乱光測定用セル
出射面との界面における透過率(πB )および前記散
乱光測定用セル出射面と散乱光測定用セル外部の空気と
の界面における透過率(πC )によって、πA =π
B ・ πC で表わされる。この透過率(πA )に
よって散乱光の強度(I)が補正されるが、前記散乱角
度が大きくなって臨界角に近付くほど、反射する光量が
増大し、透過する光が減少する。
π=4 (n1/cosθw) (n2/co
sθg)/{(n1/cosθw)+(n2/cos
θg)}2 The transmittance (πA) at which the scattered light passes through the emission surface of the scattered light measurement cell is determined by the difference between the sample liquid containing the particles to be measured and the scattered light measurement cell stored inside the scattered light measurement cell. Based on the transmittance (πB) at the interface with the emission surface of the cell for measuring scattered light and the transmittance (πC) at the interface between the emission surface of the cell for scattered light measurement and the air outside the cell for scattered light measurement, πA = π
It is expressed as B・πC. The intensity (I) of the scattered light is corrected by this transmittance (πA), but as the scattering angle increases and approaches the critical angle, the amount of reflected light increases and the amount of transmitted light decreases.

【0010】本発明では散乱光測定用セルの出射面を、
照射されるレーザ光の進行光軸に対して傾斜させて配置
することによって、散乱角度の大きな散乱光も散乱光測
定用セルの出射面における入射角を小さなものにできる
ので、散乱光の低減を防止することが可能である。
In the present invention, the exit surface of the cell for measuring scattered light is
By arranging it at an angle with respect to the traveling optical axis of the irradiated laser beam, even if the scattered light has a large scattering angle, the incident angle at the emission surface of the scattered light measurement cell can be made small, reducing the amount of scattered light. It is possible to prevent this.

【0011】[0011]

【実施例】以下、図面を参照しながら本発明を詳細に説
明する。図1および図2は、それぞれ本発明の粒度分布
測定装置の一実施例を上方から見た平面概略図であり、
本発明の粒度分布測定装置は、図1および図2に示した
実施例に限定されるものではない。図1に示す本発明の
粒度分布測定装置1は、基本的に、レーザ光照射手段2
と、前記レーザ光照射手段2から照射されるレーザ光の
進行光軸上に配置された散乱光測定用セル4と、散乱光
を集光する集光レンズ5と、前記散乱光の強度を測定す
る検出用受光素子6とを具備し、散乱光測定用セル4が
、前記進行光軸とに対して出射面が傾斜角を有するよう
に配置されている。
DESCRIPTION OF THE PREFERRED EMBODIMENTS The present invention will be described in detail below with reference to the drawings. 1 and 2 are schematic plan views of an embodiment of the particle size distribution measuring device of the present invention viewed from above, respectively.
The particle size distribution measuring device of the present invention is not limited to the embodiments shown in FIGS. 1 and 2. The particle size distribution measuring device 1 of the present invention shown in FIG.
, a scattered light measuring cell 4 disposed on the traveling optical axis of the laser beam irradiated from the laser beam irradiation means 2, a condensing lens 5 for condensing the scattered light, and measuring the intensity of the scattered light. The scattered light measurement cell 4 is arranged such that its output surface has an inclination angle with respect to the traveling optical axis.

【0012】また、図2に示す本発明の粒度分布測定装
置1は、レーザ光照射手段2から照射されるレーザ光の
進行光軸に対して散乱光測定用セル4の出射面が傾斜角
を有するように配置されていると共に、前記出射面の法
線上に集光レンズ5と検出用受光素子6とからなる散乱
光測定系を具備している。
Furthermore, the particle size distribution measuring device 1 of the present invention shown in FIG. In addition, a scattered light measurement system including a condenser lens 5 and a detection light receiving element 6 is provided on the normal line of the exit surface.

【0013】(1)レーザ光照射手段 レーザ光照射手段2は、図示しないレーザ光源と、図示
しないレーザ光発振装置と、出力されたレーザを平行に
するコリメータ3とを備えてなる。前記レーザ光源およ
びレーザ光発振装置は従来から公知のものでよく、レー
ザ光発振装置で出力することのできるレーザ光として、
例えばHe−Neガスレーザによる632.8nmのレ
ーザ光、半導体レーザによる680〜780nmのレー
ザ光などを挙げることができる。コリメータ3は、図示
しない複数のレンズ群から構成され、前記レーザ光発信
装置により出力されたレーザ光のビーム径を調節すると
共にレーザビームを平行光束にする。
(1) Laser beam irradiation means The laser beam irradiation means 2 comprises a laser light source (not shown), a laser beam oscillation device (not shown), and a collimator 3 for collimating the output laser beam. The laser light source and the laser light oscillation device may be conventionally known ones, and the laser light that can be output by the laser light oscillation device includes:
For example, 632.8 nm laser light from a He-Ne gas laser, 680-780 nm laser light from a semiconductor laser, etc. can be used. The collimator 3 is composed of a plurality of lens groups (not shown), and adjusts the beam diameter of the laser beam output from the laser beam transmitting device, and converts the laser beam into a parallel beam.

【0014】(2)散乱光測定用セル 散乱光測定用セル4は、コリメータ3により平行光束に
されたレーザ光の光路中に配置され、媒体中に被測定粒
子を分散させてなる懸濁液が、図示しない貯留槽から、
図示しない配管を介して流入することができるフローセ
ルとして構成される。散乱光測定用セルを形成する素材
は特に限定されるものではなく、従来から公知のガラス
、例えばパイレックスガラス、石英ガラスなどを挙げる
ことができる。
(2) Scattered light measurement cell The scattered light measurement cell 4 is disposed in the optical path of the laser beam made into a parallel beam by the collimator 3, and is a suspension formed by dispersing particles to be measured in a medium. However, from a storage tank (not shown),
It is configured as a flow cell that can flow in through piping (not shown). The material forming the scattered light measurement cell is not particularly limited, and conventionally known glasses such as Pyrex glass and quartz glass can be used.

【0015】通常、散乱光測定用セルの形状は、互いに
並行になった、相対する3組の面で形成される6面体で
ある。本発明の散乱光測定用セルは、相対する3組の内
の1組であるレーザ光照射手段から出力されたレーザ光
の入射面と試料粒子によって散乱した散乱光の出射面と
が、レーザ光照射手段2から照射されるレーザ光の進行
光軸に対して、所定の傾斜角度を有している。前記所定
の傾斜角度は0°〜60°の範囲である。
[0015] Usually, the shape of the scattered light measurement cell is a hexahedron formed by three sets of opposing faces that are parallel to each other. In the scattered light measuring cell of the present invention, the incident surface of the laser beam outputted from the laser beam irradiation means, which is one of the three opposing pairs, and the exit surface of the scattered light scattered by the sample particles are arranged such that the laser beam It has a predetermined inclination angle with respect to the traveling optical axis of the laser beam irradiated from the irradiation means 2. The predetermined angle of inclination is in the range of 0° to 60°.

【0016】(3)散乱光測定系 散乱光測定系は、被測定粒子による散乱光の強度を測定
するために配置された検出用受光素子6および前記散乱
光を前記検出用受光素子6上に集光させる集光レンズ5
によって構成される。前記散乱光測定系は、集光レンズ
5によって集光された散乱光の中心光軸とレーザ光照射
手段2から照射されるレーザ光の進行光軸とが、散乱光
測定用セル出射面の傾斜方向に、0°〜90°の角度を
形成する範囲に配置され、好ましくは、前記進行光軸と
散乱光測定用セル出射面の法線とで形成される範囲内に
配置される。
(3) Scattered light measurement system The scattered light measurement system includes a detection light-receiving element 6 disposed to measure the intensity of scattered light by the particles to be measured, and a detection light-receiving element 6 that directs the scattered light onto the detection light-receiving element 6. Condensing lens 5 to condense light
Consisted of. In the scattered light measurement system, the central optical axis of the scattered light focused by the condensing lens 5 and the traveling optical axis of the laser light irradiated from the laser light irradiation means 2 are aligned with the inclination of the emission surface of the scattered light measurement cell. It is arranged in a range forming an angle of 0° to 90° with respect to the direction, preferably in a range formed by the traveling optical axis and the normal line of the emission surface of the scattered light measurement cell.

【0017】検出用受光素子6は、集光レンズ5に対し
て散乱光測定セル4とは反対側に配置される。前記検出
用受光素子6は、集光レンズ5によって集光された散乱
光の光軸に直交する方向に配列された、複数の受光面を
有する光電変換素子群(例えば、フォトダイオード等)
から形成されている。散乱光測定用セル4中の被測定粒
子により生じた散乱光の強度は、集光レンズ5により集
光された散乱光の光軸中心に対して対称である。よって
、前記検出用受光素子6は、集光レンズ5によって集光
された散乱光の中心光軸を受光する中心光電変換素子と
、前記中心光電変換素子から一方向に一列に配列された
他の光電変換素子群とで構成される。通常、半導体ウェ
ハ上に、検出用受光素子を半導体技術によって区分形成
した後、半導体ウェハを切断し、粒度分布測定装置の散
乱光強度測定用ディテクタとして使用する。
The detection light receiving element 6 is placed on the opposite side of the condensing lens 5 from the scattered light measurement cell 4. The detection light-receiving element 6 is a group of photoelectric conversion elements (for example, photodiodes, etc.) having a plurality of light-receiving surfaces arranged in a direction perpendicular to the optical axis of the scattered light collected by the condenser lens 5.
It is formed from. The intensity of the scattered light generated by the particles to be measured in the scattered light measurement cell 4 is symmetrical with respect to the optical axis center of the scattered light collected by the condenser lens 5. Therefore, the detection light receiving element 6 includes a central photoelectric conversion element that receives the central optical axis of the scattered light collected by the condensing lens 5, and other photoelectric conversion elements arranged in a line in one direction from the central photoelectric conversion element. It is composed of a group of photoelectric conversion elements. Normally, after light-receiving elements for detection are formed in sections on a semiconductor wafer using semiconductor technology, the semiconductor wafer is cut and used as a detector for measuring the intensity of scattered light in a particle size distribution measuring device.

【0018】(4)粒度分布解析系 粒度分布測定装置における粒度分布解析系は、何れも図
示しない、マルチプレクサ、増幅アンプ、A/D変換器
、演算制御装置、出力装置などで構成される。マルチプ
レクサは、検出用受光素子を構成する各光電変換素子群
から出力される電気信号を切り替えるスイッチである。 前記マルチプレクサから出力される検出信号は、増幅ア
ンプにより増幅され、A/D変換器でデジタル信号に変
換された後、演算制御装置に出力される。前記演算制御
装置は、測定された散乱光強度および散乱角を示すデー
タを、周知であるフラウンホーファ回折理論、ミィーの
散乱理論に基づき粒度分布を演算する。前記演算制御装
置で演算された粒度分布データを、例えばCRT、XY
プロッターなどの出力装置に出力する。
(4) Particle Size Distribution Analysis System The particle size distribution analysis system in the particle size distribution measuring apparatus is composed of a multiplexer, an amplifier, an A/D converter, an arithmetic control device, an output device, etc., all of which are not shown. The multiplexer is a switch that switches electrical signals output from each photoelectric conversion element group that constitutes the detection light receiving element. The detection signal output from the multiplexer is amplified by an amplifier, converted into a digital signal by an A/D converter, and then output to an arithmetic and control unit. The arithmetic and control device calculates a particle size distribution based on data indicating the measured scattered light intensity and scattering angle based on the well-known Fraunhofer diffraction theory and Mie's scattering theory. The particle size distribution data calculated by the arithmetic and control device is transferred to, for example, a CRT, XY
Output to an output device such as a plotter.

【0019】(5)粒度分布の測定方法次に本発明の粒
度分布測定装置1による粒度分布測定について説明する
。まず散乱光測定用セル4中に、被測定粒子を水中に懸
濁した試料液を充填する。次いで、レーザ光照射手段2
により発振されたレーザ光をコリメータ3で平行光束に
し、前記散乱光測定用セル4に照射する。
(5) Method for Measuring Particle Size Distribution Next, the measurement of particle size distribution using the particle size distribution measuring device 1 of the present invention will be explained. First, the scattered light measurement cell 4 is filled with a sample solution in which particles to be measured are suspended in water. Next, the laser beam irradiation means 2
A collimator 3 converts the laser beam oscillated into a parallel beam of light, and irradiates the scattered light measurement cell 4 with the collimated beam.

【0020】散乱光測定用セル4に照射されたレーザ光
は、散乱光測定用セル4中の懸濁している被測定粒子に
より散乱される。前記散乱光測定用セル4の出射面が、
レーザ照射手段2から照射されるレーザ光の進行光軸に
対して傾斜しているので、前記被測定粒子の粒径がレー
ザ光の波長に対して微小である場合でも、被測定粒子に
より散乱して生じた散乱光は減衰することなく、集光レ
ンズ5により収束されて検出用受光素子6に照射される
。検出用受光素子6においては、複数の光電変換素子が
、収束された散乱光の進行光軸に直交する方向に一列に
配列されているので、各光電変換素子から出力される電
気信号は散乱光強度を示し、また、光電変換素子の位置
により散乱角が判別される。
The laser light irradiated onto the scattered light measurement cell 4 is scattered by the particles to be measured suspended in the scattered light measurement cell 4. The emission surface of the scattered light measurement cell 4 is
Since it is inclined with respect to the traveling optical axis of the laser beam irradiated from the laser irradiation means 2, even if the particle size of the particle to be measured is minute compared to the wavelength of the laser beam, it will not be scattered by the particle to be measured. The generated scattered light is converged by the condenser lens 5 and irradiated onto the detection light receiving element 6 without being attenuated. In the detection light-receiving element 6, a plurality of photoelectric conversion elements are arranged in a line in a direction perpendicular to the traveling optical axis of the converged scattered light, so that the electrical signal output from each photoelectric conversion element is the same as the scattered light. In addition, the scattering angle is determined based on the position of the photoelectric conversion element.

【0021】検出用受光素子6における各光電変換素子
から出力された電気信号は、マルチプレクサを介して増
幅アンプで増幅され、次いでA/D変換器でデジタル信
号に変換される。さらに、演算制御部にて散乱光の強度
および散乱角からその粒子の粒度分布を演算し、計算さ
れた粒度分布は出力装置から出力される。
The electrical signals output from each photoelectric conversion element in the detection light receiving element 6 are amplified by an amplifier via a multiplexer, and then converted into a digital signal by an A/D converter. Further, the calculation control section calculates the particle size distribution of the particles from the intensity and scattering angle of the scattered light, and the calculated particle size distribution is output from the output device.

【0022】[0022]

【発明の効果】本発明の、レーザ光照射手段から照射さ
れるレーザ光の進行光軸に対して、出射面が傾斜するよ
うに散乱光測定用セルを配置してなる粒度分布測定装置
によると、レーザ光の波長に対して微小な粒径を有する
粒子によって生じた散乱光を効率よく透過させることが
できる。
According to the particle size distribution measuring device of the present invention, the scattered light measuring cell is arranged such that the emission surface is inclined with respect to the traveling optical axis of the laser beam irradiated from the laser beam irradiation means. , it is possible to efficiently transmit scattered light generated by particles having a particle size smaller than the wavelength of the laser beam.

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

【図1】本発明の粒度分布測定装置の一実施例を示す概
略図である。
FIG. 1 is a schematic diagram showing an embodiment of a particle size distribution measuring device of the present invention.

【図2】本発明の粒度分布測定装置の一実施例を示す概
略図である。
FIG. 2 is a schematic diagram showing an embodiment of the particle size distribution measuring device of the present invention.

【符号の説明】[Explanation of symbols]

1    粒度分布測定装置 2    レーザ光照射手段 3    コリメータ 4    散乱光測定用セル 5    集光レンズ 6    検出用受光素子 1 Particle size distribution measuring device 2 Laser light irradiation means 3 Collimator 4 Scattered light measurement cell 5 Condensing lens 6 Detection light receiving element

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】  平行なレーザー光を照射するレーザー
光照射手段と、被測定粒子を分散させてなる懸濁液を収
納する散乱光測定用セルと、被測定粒子による散乱光の
強度を測定するために、前記散乱光測定用セルの前方に
配置された検出用受光素子および前記散乱光を前記検出
用受光素子面上に集光させる集光レンズからなる散乱光
測定手段とを供え、前記レーザ光照射手段から照射され
るレーザ光の進行光軸に対して、前記散乱光測定用セル
の出射面が傾斜するように配置されてなることを特徴と
する粒度分布測定装置。
Claim 1: A laser beam irradiation means for irradiating parallel laser beams, a scattered light measurement cell containing a suspension obtained by dispersing particles to be measured, and a cell for measuring scattered light by the particles to be measured. Scattered light measuring means comprising a detection light receiving element disposed in front of the scattered light measuring cell and a condensing lens for condensing the scattered light onto the surface of the detection light receiving element, A particle size distribution measuring device characterized in that the emission surface of the scattered light measuring cell is arranged so as to be inclined with respect to the traveling optical axis of the laser beam irradiated from the light irradiating means.
JP3090835A 1991-04-22 1991-04-22 Particle size distribution measuring device Expired - Lifetime JPH07117483B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3090835A JPH07117483B2 (en) 1991-04-22 1991-04-22 Particle size distribution measuring device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3090835A JPH07117483B2 (en) 1991-04-22 1991-04-22 Particle size distribution measuring device

Publications (2)

Publication Number Publication Date
JPH04323540A true JPH04323540A (en) 1992-11-12
JPH07117483B2 JPH07117483B2 (en) 1995-12-18

Family

ID=14009647

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3090835A Expired - Lifetime JPH07117483B2 (en) 1991-04-22 1991-04-22 Particle size distribution measuring device

Country Status (1)

Country Link
JP (1) JPH07117483B2 (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2000105185A (en) * 1998-08-22 2000-04-11 Malvern Instruments Ltd Device and method for measuring distribution of particle size
JP2003329570A (en) * 2002-05-10 2003-11-19 Horiba Ltd Apparatus for measuring distribution of particle size

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61221633A (en) * 1985-03-27 1986-10-02 Toa Medical Electronics Co Ltd Flow cell and flow sight meter equipped with flow cell
JPH02212741A (en) * 1989-02-10 1990-08-23 Shimadzu Corp Particle size distribution measuring apparatus

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61221633A (en) * 1985-03-27 1986-10-02 Toa Medical Electronics Co Ltd Flow cell and flow sight meter equipped with flow cell
JPH02212741A (en) * 1989-02-10 1990-08-23 Shimadzu Corp Particle size distribution measuring apparatus

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2000105185A (en) * 1998-08-22 2000-04-11 Malvern Instruments Ltd Device and method for measuring distribution of particle size
JP2003329570A (en) * 2002-05-10 2003-11-19 Horiba Ltd Apparatus for measuring distribution of particle size

Also Published As

Publication number Publication date
JPH07117483B2 (en) 1995-12-18

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