JPH0652231B2 - Sedimentation type particle size distribution measuring device - Google Patents
Sedimentation type particle size distribution measuring deviceInfo
- Publication number
- JPH0652231B2 JPH0652231B2 JP61074719A JP7471986A JPH0652231B2 JP H0652231 B2 JPH0652231 B2 JP H0652231B2 JP 61074719 A JP61074719 A JP 61074719A JP 7471986 A JP7471986 A JP 7471986A JP H0652231 B2 JPH0652231 B2 JP H0652231B2
- Authority
- JP
- Japan
- Prior art keywords
- particle size
- size distribution
- measurement
- light
- absorbance
- 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 - Lifetime
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N15/00—Investigating characteristics of particles; Investigating permeability, pore-volume or surface-area of porous materials
- G01N15/04—Investigating sedimentation of particle suspensions
- G01N15/042—Investigating sedimentation of particle suspensions by centrifuging and investigating centrifugates
Landscapes
- Chemical & Material Sciences (AREA)
- Biochemistry (AREA)
- Physics & Mathematics (AREA)
- Health & Medical Sciences (AREA)
- Life Sciences & Earth Sciences (AREA)
- Analytical Chemistry (AREA)
- Dispersion Chemistry (AREA)
- General Health & Medical Sciences (AREA)
- General Physics & Mathematics (AREA)
- Immunology (AREA)
- Pathology (AREA)
- Optical Measuring Cells (AREA)
- Length Measuring Devices By Optical Means (AREA)
Description
【発明の詳細な説明】 イ.産業上の利用分野 本発明は、沈降式粒度分布測定、より詳しくは粒子形状
の依存性を除去する技術に関する。Detailed Description of the Invention a. BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to sedimentation type particle size distribution measurement, and more particularly to a technique for removing the dependency of particle shape.
ロ.従来技術 粉粒体の粒子径や粒度分布を沈降速度に基づいて測定す
る装置においては、 ただし、V:粒子径dを持つ粒子についての沈降速度、 l1:粒子密度 l2:媒液密度 n :媒液粘度 K :自然沈降法にあっては重力加速度、 また遠心沈降法にあっては遠心力、 なる、ストークスの式に基づいて決まる粒子径毎の沈降
速度の差を吸光度の時間的変化として検出することが行
なわれているが、このストークスの関係式は、測定対象
である粉粒体が球形であることを前提としたものであ
る。B. Prior Art In an apparatus for measuring the particle size and particle size distribution of powder and granular materials based on the sedimentation velocity, However, V: sedimentation velocity for particles having a particle diameter d, l 1 : particle density l 2 : medium liquid density n: medium liquid viscosity K: gravity acceleration in the natural sedimentation method, and centrifugal sedimentation method Is the centrifugal force, and the difference in the sedimentation velocity for each particle size, which is determined based on the Stokes equation, is detected as the change in absorbance over time. This is based on the assumption that the particles are spherical.
しかしながら、最近のファインセラミックスに使用され
るような粉粒体は、第7図に示したように粒子の姿勢毎
の投影面積のバラつきが極めて大きいため、このような
粒子に適用した場合には測定精度と再現性が極めて低下
する(第6図)という問題がある。However, the powder particles used in recent fine ceramics have a very large variation in the projected area depending on the posture of the particles as shown in FIG. There is a problem that accuracy and reproducibility are extremely lowered (Fig. 6).
ハ.目的 本発明はこのような問題に鑑みてなされたものであっ
て、その目的とするところは、異形粒子の粒度分布を高
い精度と再現性をもって測定することができる沈降式粒
度分布測定装置を提供することにある。C. OBJECT The present invention has been made in view of the above problems, and an object thereof is to provide a sedimentation type particle size distribution measuring apparatus capable of measuring the particle size distribution of irregularly shaped particles with high accuracy and reproducibility. To do.
ニ.発明の概要 すなわち、本発明が特徴とするところは吸光度検出の光
路を複数方向に設けた点にある。D. SUMMARY OF THE INVENTION That is, the feature of the present invention is that the optical paths for detecting absorbance are provided in a plurality of directions.
ホ.実施例 そこで、以下に本発明の詳細を図示した実施例に基づい
て説明する。E. Examples Therefore, details of the present invention will be described below based on illustrated examples.
第1、2図は、本発明の一実施例を示すものであって、
図中符号1は、図示しないモータに接続した回転軸2よ
り駆動される回転円板で、透過窓1aを穿設した部分に
測定セル3が径方向に向けて取付けられ、回転円板1面
に平行で測定セル3を通る光路Lに対して略45゜に斜
むけた平面鏡4、5が並設されている。1 and 2 show one embodiment of the present invention,
In the figure, reference numeral 1 is a rotary disk driven by a rotary shaft 2 connected to a motor (not shown). A measuring cell 3 is attached in a radial direction to a portion where a transmission window 1a is formed, and the rotary disk 1 surface Plane mirrors 4 and 5 which are parallel to the optical path L and are inclined at an angle of approximately 45 ° with respect to the optical path L passing through the measuring cell 3.
この窓1aに対向する部分の一方の側には、沈降方向を
横切る方向に移動可能にされた発光素子6が配設され、
また他方の側には回転円板1面に反射面を略45゜に向
けた2枚の平面鏡7a、7bからなる山形ミラー7が配
設され、平面鏡8を介して回転円板1上の平面鏡4、測
定セル3、平面鏡5、及び後述する受光素子9に至る光
路を結ぶように光学系が構成されている。9は、受光素
子で、発光素子6の移動に合せて回転円板1の平面鏡5
からの光と、山形ミラー7の一方の平面鏡7aからの反
射光を平面鏡10を介して受けるように構成されてい
る。13は、測定回路で、回転円板1上の測定セル3が
検出領域に到達したときに開くゲート12を介して受光
素子9から信号を受けるものである。On one side of the portion facing the window 1a, a light emitting element 6 that is movable in a direction transverse to the sinking direction is provided.
On the other side, a chevron-shaped mirror 7 composed of two plane mirrors 7a and 7b having a reflecting surface directed to about 45 ° on the surface of the rotating disc 1 is provided, and a plane mirror on the rotating disc 1 is provided via a plane mirror 8. 4, an optical system is configured to connect the optical paths to the measurement cell 3, the plane mirror 5, and the light receiving element 9 described later. Reference numeral 9 is a light receiving element, and the plane mirror 5 of the rotary disc 1 is moved in accordance with the movement of the light emitting element 6.
And the reflected light from one flat mirror 7a of the chevron-shaped mirror 7 are received via the flat mirror 10. A measuring circuit 13 receives a signal from the light receiving element 9 via the gate 12 that opens when the measuring cell 3 on the rotating disk 1 reaches the detection region.
この実施例において、球状の粉粒体を媒液に分散させて
なるサンプルを収容した測定セル3を回転円板1にセッ
トして装置を作動すると、測定セル3内の粉粒体は遠心
力を受けて粒径に比例した速度で沈降を開始する。In this example, when the measuring cell 3 containing a sample in which spherical particles are dispersed in a liquid medium is set on the rotary disc 1 and the apparatus is operated, the particles in the measuring cell 3 are subjected to centrifugal force. Then, the sedimentation is started at a rate proportional to the particle size.
このとき、第1領域、つまり図中点線により示した位置
に発光素子6と受光素子9を配置すると、発光素子6か
らの光は、測定セル3を通過して山形ミラー7、平面鏡
10で反射されて受光素子9に至る光路を通ることにな
る。このような状態で測定セル3が検出範囲に対向する
と、ゲート12が開いて回転円板1面に対して直角に入
射した光による吸光度が検出される。At this time, if the light emitting element 6 and the light receiving element 9 are arranged in the first region, that is, the position shown by the dotted line in the figure, the light from the light emitting element 6 passes through the measuring cell 3 and is reflected by the chevron mirror 7 and the plane mirror 10. Then, the light passes through the optical path to the light receiving element 9. When the measurement cell 3 faces the detection range in such a state, the gate 12 opens and the absorbance due to the light incident at right angles to the surface of the rotating disk 1 is detected.
つぎに、発光素子6及び受光素子9を図中実線により示
す第2領域に移動させると、発光素子6からの光は、回
転円板1面に対して直角に測定セル3に一度入射した
後、山形ミラー7の平面鏡7b、平面鏡8、回転円板1
上の平面鏡4に反射されて回転円板1面に平行に再び測
定セル3に入射して粉粒体により吸収される。測定セル
3から出た光は、平面鏡5により反射されて受光素子9
に入射して測定回路13において吸光度が測定される。
云うまでもなく、粉粒体の形状が球体であるから、第1
の測定結果と第2の測定結果の間には、光路長に基づく
変化分が生じるだけで、方向性に基づく変化はない。Next, when the light emitting element 6 and the light receiving element 9 are moved to the second region shown by the solid line in the figure, the light from the light emitting element 6 is incident on the measurement cell 3 once at a right angle to the surface of the rotating disk 1. , The plane mirror 7b of the chevron-shaped mirror 7, the plane mirror 8, the rotating disk 1
The light is reflected by the upper plane mirror 4, enters the measuring cell 3 again in parallel to the surface of the rotating disk 1, and is absorbed by the particles. The light emitted from the measuring cell 3 is reflected by the plane mirror 5 and received by the light receiving element 9
And the absorbance is measured in the measurement circuit 13.
Needless to say, since the shape of the powder and granules is spherical,
Between the measurement result of 1 and the second measurement result, there is only a change based on the optical path length, and there is no change based on the directionality.
他方、非球形粉粒体をサンプルにして測定を行なうと、
この粉粒体の各粒子は媒液中において全ゆる方向に面を
向けた状態で沈降を開始する。On the other hand, when a non-spherical powder is used as a sample for measurement,
Each particle of the powder and granular material starts to settle in the liquid medium with its surface facing in all directions.
このような状態で、第1領域での吸光度を検出すると、
この光は、粒子面を光路に直角に向けた粒子の数に応じ
た吸収を受けるため、ブラウン運動等による粒子姿勢の
影響を大きく受け、測定毎にその結果がバラつくことに
なる(第6図)。In this state, if the absorbance in the first region is detected,
This light is absorbed according to the number of particles with the particle surface oriented at right angles to the optical path, and is thus greatly affected by the particle posture due to Brownian motion, etc., and the result will vary from measurement to measurement (6th Figure).
つぎに、発光素子6及び受光素子9を第2領域に移動す
ると、発光素子6からの光は、回転円板1の直角方向か
ら測定セル3に入射してこの光線上の粒子P1〜P4を
一度照射し、回転円板1に投影した粒子面積に一致した
吸光を受けて測定セル3外に出る(第4図I)。この光
は、山形ミラー7、平面鏡8、4により反射されて回転
円板1面に平行な方向から再び測定セル3に入射して前
回の吸光に関与した粒子P1〜P4の他面側、つまり回
転板に垂直な面に投影した面積に一致する吸光を受けた
後(II)、受光素子9に入射する。これにより、測定回
路13は、同一粒子P1〜P4を両面から見た大きさに
対応する吸光度信号を受け、粉粒体の長径と短径を幾何
平均した値に基づく粒度分布値を出力することになり、
同一試料を多数回測定しても常に同一の粒度分布値を出
力することになる(第5図)。Next, when the light emitting element 6 and the light receiving element 9 are moved to the second region, the light from the light emitting element 6 is incident on the measurement cell 3 from the direction perpendicular to the rotating disk 1 and the particles P 1 to P on this light beam. 4 is irradiated once, receives the light absorption corresponding to the particle area projected on the rotating disk 1, and goes out of the measurement cell 3 (FIG. 4I). This light is reflected by the chevron mirrors 7 and the plane mirrors 8 and 4 and is incident on the measurement cell 3 again from the direction parallel to the surface of the rotating disk 1 and the other surface side of the particles P 1 to P 4 involved in the previous absorption. That is, after receiving the light absorption that matches the area projected on the plane perpendicular to the rotating plate (II), it is incident on the light receiving element 9. As a result, the measurement circuit 13 receives the absorbance signal corresponding to the size of the same particles P 1 to P 4 viewed from both sides, and outputs the particle size distribution value based on the value obtained by geometrically averaging the major axis and the minor axis of the granular material. Will be
Even if the same sample is measured many times, the same particle size distribution value is always output (Fig. 5).
なお、この実施例においては、測定セル3に一方向から
入射させる第1領域の測定光学系を設けているが、第2
領域だけを用いることによって球形、非球形のいかんに
関わりなく粒度分布を測定できることは明らかである。In this embodiment, the measurement optical system for the first region which is incident on the measurement cell 3 from one direction is provided.
It is clear that the particle size distribution can be measured by using only the region regardless of whether it is spherical or non-spherical.
また、この実施例においては、発光素子6及び受光素子
9を移動させて共用させているが、各領域に発光素子と
受光素子を独立させて配設しても同様の作用を奏する。Further, in this embodiment, the light emitting element 6 and the light receiving element 9 are moved and shared, but the same effect can be obtained even if the light emitting element and the light receiving element are separately arranged in each region.
第3図は、本発明の第2の実施例を示すものであって、
図中符号20、21は、沈降方向を横切る平面上におい
て測定セル3領域で交差する光路上に配置した発光素子
で、測定セル3を挟んで対向する位置に受光素子22、
23を配設するとともに、2つの受光素子22、23か
らの出力を加算回路24に入力することにより、粉粒体
の幾何平均粒度を求めるようにしたもので、この実施例
によれば、光学系を不要にして装置を簡素化することが
できる外に、各方向の吸光度を独立に把握して粉粒体の
形状をより正確に知ることが可能となる。FIG. 3 shows a second embodiment of the present invention,
Reference numerals 20 and 21 in the figure denote light emitting elements arranged on an optical path that intersects in the measurement cell 3 region on a plane that crosses the sedimentation direction.
23 is provided and the outputs from the two light receiving elements 22 and 23 are input to the adder circuit 24 to obtain the geometric average particle size of the granular material. According to this embodiment, In addition to not requiring a system and simplifying the apparatus, it is possible to grasp the absorbance in each direction independently and to know the shape of the granular material more accurately.
なお、上述した実施例においては2方向での吸光度を測
定しているが、吸光度を測定する方向の数を多くする
程、測定精度が向上することは云うまでもない。Although the absorbance is measured in two directions in the above-described embodiment, it goes without saying that the measurement accuracy improves as the number of directions in which the absorbance is measured increases.
また、上述の実施例においては、遠心力を作用させるも
のに例を採って説明したが、重力の作用を利用した自然
沈降式のものに対しても適用できることは明らかであ
る。Further, in the above-described embodiment, the example in which the centrifugal force is applied has been described, but it is obvious that the present invention can be applied to the natural sedimentation type that utilizes the action of gravity.
ヘ.効果 以上、説明したように本発明によれば、測定測定セルの
複数方向から吸光度を検出するようにしたので、粉粒体
の実際的な形状に対応した吸光度を検出することができ
て、非球形粉粒体であってもその姿勢差の影響を可及的
に小さくして幾何平均に基づく粒度分布を短時間で正確
に測定することができる。F. Effects As described above, according to the present invention, since the absorbance is detected from a plurality of directions of the measurement measurement cell, it is possible to detect the absorbance corresponding to the practical shape of the granular material. Even in the case of spherical powder particles, the influence of the posture difference can be minimized to accurately measure the particle size distribution based on the geometric mean in a short time.
【図面の簡単な説明】 第1、2図は、それぞれ本発明の一実施例を示す装置の
斜視図と構成図、第3図は本発明の他の実施例を示す構
成図、第4図は、同上装置の動作を示すための説明図、
第5図は、同上装置による測定結果の一例を示す粒度分
布図、第6図は、従来装置による測定結果を示す粒度分
布図、及び第7図(イ)〜(ハ)は、それぞれ異形粉粒
体の姿勢差による投影面積と、これに等価な球形サイズ
を示す説明図である。 1……回転円板、3……測定セル 6……発光素子、9……受光素子 20、21……発光素子 22、23……受光素子BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 and FIG. 2 are a perspective view and a structural view of an apparatus showing an embodiment of the present invention, respectively. FIG. 3 is a structural view showing another embodiment of the present invention, and FIG. Is an explanatory view for showing the operation of the above device,
FIG. 5 is a particle size distribution chart showing an example of the measurement result by the same apparatus, FIG. 6 is a particle size distribution chart showing the measurement result by the conventional apparatus, and FIGS. It is explanatory drawing which shows the projected area by the attitude | position difference of a particle, and the spherical size equivalent to this. 1 ... Rotating disk, 3 ... Measuring cell 6 ... Light emitting element, 9 ... Light receiving element 20, 21 ... Light emitting element 22, 23 ... Light receiving element
Claims (1)
するセルと、沈降方向を横切る同一面上の複数方向から
前記セルを通る複数の光路を設定し、前記光路上に前記
測定セルを挟むように発光手段と受光手段を設けてなる
吸光度測定手段と、該吸光度測定手段からの各方向の吸
光度検出信号を加算せしめる手段とを備えてなる沈降式
粒度分布測定装置。1. A cell containing a sample in which a granular material is dispersed in a liquid medium and a plurality of optical paths passing through the cell from a plurality of directions on the same plane crossing the sedimentation direction are set, and the measurement is performed on the optical path. A sedimentation-type particle size distribution measuring apparatus comprising: an absorbance measuring means, which is provided with a light emitting means and a light receiving means so as to sandwich a cell, and a means for adding the absorbance detection signals from the absorbance measuring means in each direction.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61074719A JPH0652231B2 (en) | 1986-03-31 | 1986-03-31 | Sedimentation type particle size distribution measuring device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61074719A JPH0652231B2 (en) | 1986-03-31 | 1986-03-31 | Sedimentation type particle size distribution measuring device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS62231138A JPS62231138A (en) | 1987-10-09 |
| JPH0652231B2 true JPH0652231B2 (en) | 1994-07-06 |
Family
ID=13555307
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP61074719A Expired - Lifetime JPH0652231B2 (en) | 1986-03-31 | 1986-03-31 | Sedimentation type particle size distribution measuring device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0652231B2 (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP5087486B2 (en) * | 2008-07-17 | 2012-12-05 | 株式会社堀場製作所 | Diffraction / scattering particle size distribution analyzer |
-
1986
- 1986-03-31 JP JP61074719A patent/JPH0652231B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS62231138A (en) | 1987-10-09 |
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