JPH0820355B2 - Particle size measurement method - Google Patents
Particle size measurement methodInfo
- Publication number
- JPH0820355B2 JPH0820355B2 JP63297383A JP29738388A JPH0820355B2 JP H0820355 B2 JPH0820355 B2 JP H0820355B2 JP 63297383 A JP63297383 A JP 63297383A JP 29738388 A JP29738388 A JP 29738388A JP H0820355 B2 JPH0820355 B2 JP H0820355B2
- Authority
- JP
- Japan
- Prior art keywords
- particle size
- dispersion liquid
- formula
- powder
- transmittance
- 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 - Fee Related
Links
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- 238000000691 measurement method Methods 0.000 title claims 3
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- 239000000843 powder Substances 0.000 claims description 56
- 239000007788 liquid Substances 0.000 claims description 54
- 238000002834 transmittance Methods 0.000 claims description 41
- 238000005259 measurement Methods 0.000 claims description 34
- 238000000034 method Methods 0.000 claims description 32
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- PNEYBMLMFCGWSK-UHFFFAOYSA-N aluminium oxide Inorganic materials [O-2].[O-2].[O-2].[Al+3].[Al+3] PNEYBMLMFCGWSK-UHFFFAOYSA-N 0.000 description 2
- 230000005540 biological transmission Effects 0.000 description 2
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- 239000000084 colloidal system Substances 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
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- HBMJWWWQQXIZIP-UHFFFAOYSA-N silicon carbide Chemical compound [Si+]#[C-] HBMJWWWQQXIZIP-UHFFFAOYSA-N 0.000 description 1
- 229910010271 silicon carbide Inorganic materials 0.000 description 1
- 239000000377 silicon dioxide Substances 0.000 description 1
- HQVNEWCFYHHQES-UHFFFAOYSA-N silicon nitride Chemical compound N12[Si]34N5[Si]62N3[Si]51N64 HQVNEWCFYHHQES-UHFFFAOYSA-N 0.000 description 1
- GCLGEJMYGQKIIW-UHFFFAOYSA-H sodium hexametaphosphate Chemical compound [Na]OP1(=O)OP(=O)(O[Na])OP(=O)(O[Na])OP(=O)(O[Na])OP(=O)(O[Na])OP(=O)(O[Na])O1 GCLGEJMYGQKIIW-UHFFFAOYSA-H 0.000 description 1
- 235000019982 sodium hexametaphosphate Nutrition 0.000 description 1
- 239000012798 spherical particle Substances 0.000 description 1
- 239000001577 tetrasodium phosphonato phosphate Substances 0.000 description 1
- 238000000870 ultraviolet spectroscopy Methods 0.000 description 1
Landscapes
- Length Measuring Devices By Optical Means (AREA)
Description
【発明の詳細な説明】 [産業上の利用分野] 本発明は、セラミック製品の原料等として使用される
アルミナ、窒化ケイ素、炭化ケイ素等の粉体の粒径や、
ケイ砂、ホワイトアランダム等の粉体の粒径を測定する
方法に関する。DETAILED DESCRIPTION OF THE INVENTION [Industrial field of application] The present invention relates to the particle size of powders of alumina, silicon nitride, silicon carbide and the like used as raw materials for ceramic products,
The present invention relates to a method for measuring the particle size of powder such as silica sand and white alundum.
[従来の技術と発明が解決しようとする課題] 光透過を利用した粒径測定方法においては、透過率及
び吸光係数を知ることが必要である。Roseの研究(Ros
e,H,E.,″The Measurement of Particle Size in Vevy
Fine Powders″ Constable & Co. Ltd., London(195
4)をはじめ、吸光係数の測定に関する研究は数多くあ
るが、透過光の波長は積極的には変えられていない。特
にサブミクロン域の粒子の粒径特性の測定に確定された
方法はなく、粉体特性の理解を困難にしている。[Problems to be Solved by Conventional Techniques and Inventions] In a particle size measuring method using light transmission, it is necessary to know the transmittance and the extinction coefficient. Study of Rose (Ros
e, H, E., ″ The Measurement of Particle Size in Vevy
Fine Powders ″ Constable & Co. Ltd., London (195
There are many studies on the measurement of extinction coefficient, including 4), but the wavelength of transmitted light is not actively changed. In particular, there is no definite method for measuring the particle size characteristics of particles in the submicron range, which makes it difficult to understand the powder characteristics.
最近の光を用いるサブミクロン域粒径測定には、光回
折法、光散乱法、光子相関法等があるが、簡便とは言え
ず、計測に際しても未だ種々の問題が存在する。The recent submicron particle size measurement using light includes a light diffraction method, a light scattering method, a photon correlation method and the like, but it cannot be said to be simple and there are still various problems in measurement.
つまり、光回折法で測定できるのは数μm〜200μm
の範囲の粒径に限られ、粒子径分布関数とのカーブフィ
ッテイング法により代表粒子径及び分布指数が決定され
るが、濃度により多重回折現象が起り、みかけの粒子径
が小さく測定される欠点があった。In other words, the optical diffraction method can measure a few μm to 200 μm
The representative particle size and distribution index are determined by the curve fitting method with the particle size distribution function, but the multiple diffraction phenomenon occurs depending on the concentration, and the apparent particle size is small. was there.
光散乱法での測定粒径範囲は0.1μm〜数μmであ
り、粒子パラメータαの定義α=πD/λ(ここに、λは
光源波長であり、Dは粒径である。)より、微小粒子を
測定する場合は入射光波長を短くしなければならないた
め、He−Cdレーザー又はHe−Neレーザーの光源を必要と
し、光散乱現象の角度依存性による誤差も出るし、高価
でもある。また、温度依存性があるので、温度管理をし
ないと誤差が出る。The measured particle size range by the light scattering method is 0.1 μm to several μm, and the particle parameter α is defined as α = πD / λ (where λ is the light source wavelength and D is the particle size). Since the incident light wavelength must be shortened when measuring particles, a He—Cd laser or a He—Ne laser light source is required, and errors due to the angle dependence of the light scattering phenomenon occur, which is also expensive. In addition, since there is temperature dependence, an error will occur unless the temperature is controlled.
光子相関法では、粒度分布がガウス分布であることを
仮定したうえで計数処理をしているので、ガウス分布を
もたない粒子に対しては誤差が大である。また、測定装
置が高価である。In the photon correlation method, since the counting process is performed on the assumption that the particle size distribution is Gaussian distribution, the error is large for particles that do not have Gaussian distribution. In addition, the measuring device is expensive.
単分散粒子の粒径測定に関しては、粒子濃度によらな
いHellerらの方法(Pangonis,W.J.,Heller,S.,and Econ
omou,N.A.,J.Chem.Phys.,34,960(1961)やGuckerらの
方法(Gucker,F.T.,and Rowell,R.L.,Disc.Frad.Soc.,3
0,185(1960))があるが、装置及び条件的に実用的で
ない。Regarding the particle size measurement of monodisperse particles, the method of Heller et al. (Pangonis, WJ, Heller, S., and Econ, which does not depend on particle concentration, is used.
omou, NA, J.Chem.Phys., 34,960 (1961) and Gucker's method (Gucker, FT, and Rowell, RL, Disc.Frad.Soc., 3
0,185 (1960)), but it is not practical in terms of equipment and conditions.
また、粒子濃度により粒径を測定する方法には、Hell
erらの方法(Heller,W.,and Nakagaki,M.,J.chem.Phy
s.,31,1188(1959))、Innらの方法(La Mer.V.K.,In
n,E.C.Y.,and Wilson,I.B.,J.Colloid Sci., 18,888(1
963))、チンダル現象の最大値をとって粒径を評価す
るHotsらの方法等があるが、吸光係数の算出に問題があ
る。In addition, the method of measuring the particle size by particle concentration is Hell
er et al. (Heller, W., and Nakagaki, M., J.chem.Phy
s., 31,1188 (1959)), Inn et al.'s method (La Mer.VK, In
n, ECY, and Wilson, IB, J.Colloid Sci., 18,888 (1
963)) and the method of Hots et al., Which evaluates the particle size by taking the maximum value of the Tyndall phenomenon, but there is a problem in the calculation of the extinction coefficient.
本発明はこれに鑑み、安価でしかも簡単な操作により
正確な粒径測定ができる方法を提供することを目的とす
る。In view of this, an object of the present invention is to provide a method which is inexpensive and enables accurate particle size measurement by a simple operation.
[課題を解決するための手段] 本発明に係る粒径測定方法は、粒径0.1〜1μmのサ
ブミクロン域の粒子の粒径を200〜1100nmの特定波長光
を用いて測定する、光散乱現象を生じる領域における粒
径測定方法において、既知粒径の基準粉体について、こ
の粉体の分散液の特定波長光に対する透過率(T)を測
定して、分散液濃度(c[g/cm3])が下記式(イ)をM
ie理論からのずれが1%以内の範囲で満す濃度範囲内で
基準粉体の特定分散液濃度を決定し、前記特定分散液濃
度に調製した複数の既知粒径の基準粉体の分散液につい
て、前記特定波長光の透過率を測定して粒径(D)と吸
光係数(K)との関係を下記式(ロ)に示す直線で近似
し、この式(ロ)とLambert−Beerの式とにより分散液
の透過率(T)と粉体粒径(D)との関係を表わす下記
式(ハ)に示す実験式を求めておき、粒径測定対象粉体
の分散液について前記特定波長光の透過率を測定し、前
記の実験式から粒径を算出する。[Means for Solving the Problems] The particle size measuring method according to the present invention is a light scattering phenomenon in which the particle size of particles in the submicron region having a particle size of 0.1 to 1 μm is measured using light having a specific wavelength of 200 to 1100 nm. In the method for measuring the particle size in the region in which the particle size is generated, the transmittance (T) of the dispersion liquid of the powder for a reference powder having a known particle size is measured to obtain the dispersion liquid concentration (c [g / cm 3 ]) Is the formula (a) below
ie, the dispersion liquid of a plurality of reference powders having known particle diameters is determined by determining the concentration of the specific dispersion liquid of the reference powder within a concentration range satisfying the deviation from the theory within 1%. With respect to the specific wavelength, the relationship between the particle size (D) and the extinction coefficient (K) was approximated by a straight line represented by the following formula (B), and this formula (B) and Lambert-Beer's The empirical formula shown in the following formula (C), which represents the relationship between the transmittance (T) of the dispersion liquid and the powder particle size (D), is calculated in advance, and the above-mentioned specification is made for the dispersion liquid of the particle size measurement target powder. The transmittance of wavelength light is measured, and the particle size is calculated from the above empirical formula.
式(イ);logT=a・c (ここで、T=透過光強度/入射光強度、a
=定数。) 式(ロ);logK=αilogD+βi (ここで、αi,βi=定数、i=1,2。) 式(ハ);D=EXP{(βi−logZ)/(1−αi)} (ここで、Z=−ρlogT/1.5cl、 ρ=粒子密度、l=分散液中の光
路長さ。) ここで、前記の粒径(D)と吸光係数(K)との関係
を下記式(ニ)に近似し、この式(ニ)とLambert−Bee
rの式とにより下記式(ホ)に示す前記の透過率(T)
と粉体粒径(D)との関係を表わす前記実験式を求めて
もよい。Formula (a); logT = a · c (where T = transmitted light intensity / incident light intensity, a
= Constant. ) Equation (b); logK = α i logD + β i (where α i and β i = constant, i = 1,2.) Equation (c); D = EXP {(β i −logZ) / (1- α i )} (where Z = −ρlogT / 1.5cl, ρ = particle density, 1 = optical path length in the dispersion liquid) where the particle size (D) and the extinction coefficient (K) The relationship is approximated to the following equation (d), and this equation (d) and Lambert-Bee
The transmittance (T) shown in the following equation (e) by the equation of r
The empirical formula representing the relationship between the particle size and the powder particle size (D) may be obtained.
式(ニ);K=mD3 (ここで、m=定数) (ここで、Z=−ρlogT/1.5cl、 ρ=粒子密度、l=分散液中の光
路長さ。) また、前記粒径測定対象粉体の分散液について、この
粉体の分散液の特定波長光に対する透過率(T)を測定
して、分散液濃度(c[g/cm3])が前記式(イ)をMie
理論からのずれが1%以内の範囲で満す濃度範囲内で、
前記粒径測定対象粉体の特定分散液濃度を決定し、この
特定分散液濃度に調製した前記粒径測定対象粉体の分散
液について、前記特定波長光の透過率を測定して、前記
実験式から粒径を算出する方が望ましい。Formula (d); K = mD 3 (where m = constant) (Where, Z = −ρlogT / 1.5cl, ρ = particle density, 1 = optical path length in the dispersion liquid.) Further, for the dispersion liquid of the particle size measurement target, the dispersion liquid of the powder is specified. The transmittance (T) for the wavelength light is measured, and the dispersion liquid concentration (c [g / cm 3 ]) is calculated according to the above formula (a) by Mie.
Within the concentration range where the deviation from theory is within 1%,
The specific dispersion liquid concentration of the particle size measurement target powder is determined, and the transmittance of the specific wavelength light is measured for the dispersion liquid of the particle size measurement target powder prepared to have the specific dispersion liquid concentration, and the experiment is performed. It is desirable to calculate the particle size from the formula.
さらに、800nm以上の長波長光を使用する方が望まし
い。Furthermore, it is desirable to use long wavelength light of 800 nm or longer.
[作用] 本発明の粒径測定方法では、粒径0.1〜1μmのサブ
ミクロン域の粒子の粒径を200〜1100nmの特定波長光を
用いて測定するという光散乱現象を生じる領域における
粒径測定方法において、分散液の透過率と粒径との関係
を示す実験式を求めるに際し、まず、既知粒径の基準粉
体について、この分散液の特定波長光に対する透過率
(T)を分散液濃度(c)とが、Mie理論からのずれが
1%以内の範囲で式(イ)を満すか否か、即ち、logT−
c曲線の直線性を確認して、このような条件を満す濃度
範囲内で特定分散液濃度を決定する。そのため、既知粒
径の基準粉体の特定分散液濃度が、特定波長光に対して
多重散乱を生じない範囲内に設定され、よって、その後
の実験式を求める段階において、Lambert−Beerの式を
適用することができる。また、この直線性を確認すると
いう簡易な方法により、多重散乱を生じない範囲内で特
定分散液濃度をできるだけ高く設定して、前記実験式を
求める段階における透過率の測定感度を上げることも容
易である。なお、Mie理論からのずれが1%より大きい
と、多重散乱により高い測定精度が得られない。[Operation] In the particle size measuring method of the present invention, particle size measurement in a region where a light scattering phenomenon occurs, in which the particle size of particles in the submicron range of 0.1 to 1 μm is measured using light of a specific wavelength of 200 to 1100 nm. In determining the empirical formula showing the relationship between the transmittance of the dispersion liquid and the particle size, the transmittance (T) of the dispersion liquid with respect to the specific wavelength light is first determined for the reference powder having a known particle size. Whether or not (c) satisfies expression (a) within a range of deviation from Mie theory of 1% or less, that is, logT-
The linearity of the c-curve is confirmed, and the specific dispersion liquid concentration is determined within the concentration range that satisfies such conditions. Therefore, the specific dispersion liquid concentration of the reference powder having a known particle diameter is set within a range that does not cause multiple scattering with respect to the specific wavelength light, and therefore, in the subsequent step of obtaining the empirical formula, the Lambert-Beer formula is used. Can be applied. Also, by a simple method of confirming this linearity, it is easy to increase the sensitivity of measurement of transmittance in the step of obtaining the empirical formula by setting the concentration of the specific dispersion as high as possible within the range where multiple scattering does not occur. Is. If the deviation from the Mie theory is larger than 1%, high measurement accuracy cannot be obtained due to multiple scattering.
そして、以上により、上記特定分散液濃度に調製した
複数の既知粒径の基準粉体分散液を用いて特定波長光の
透過率を測定すると、粒径と吸光係数との間に、式
(ロ)に示す誤差の小さな直線の近似式が成立する。Then, as described above, when the transmittance of the specific wavelength light is measured using the reference powder dispersion liquid having a plurality of known particle diameters adjusted to the specific dispersion liquid concentration, the formula ( The linear approximation formula with small error shown in) is established.
これにより、従来、良好な実験式が得られなかったサ
ブミクロン域において、粒径と吸光係数との間に式
(ハ)で表わされる高精度で簡易な実験式が得られる。As a result, in the submicron region where a good empirical formula has not been obtained conventionally, a highly accurate and simple empirical formula represented by the formula (C) between the particle diameter and the absorption coefficient can be obtained.
そして、この実験式を用いて、粒径測定対称粉体の分
散液について、前記特定波長光の透過率を測定して粒径
を算出するので、簡易にしかも高精度に粒径を求めるこ
とができる。Then, by using this empirical formula, the particle size is measured for the dispersion liquid of the particle size measuring symmetrical powder, and the particle size is calculated by measuring the transmittance of the specific wavelength light, so that the particle size can be obtained easily and with high accuracy. it can.
なお、以上において、粒径(D)と吸光係数(K)と
の関係を式(ニ)に近似すれば、透過率(T)と粒径
(D)との関係を示す式(ホ)がより簡単になり、よっ
て、さらに簡易な粒径測定が可能となる。In the above, if the relationship between the particle size (D) and the extinction coefficient (K) is approximated to the expression (D), the expression (E) indicating the relationship between the transmittance (T) and the particle size (D) is obtained. This simplifies the particle size measurement, and thus enables simpler particle size measurement.
また、粒径測定対象粉体の分散液について、その透過
率と濃度とが式(イ)をMie理論からのずれが1%以内
の範囲で満たすような濃度範囲内にその濃度を調製すれ
ば、前記の実験式から粒径を算出する際に用いる粒径測
定対象粉体の分散液が多重散乱を生じていないので、該
分散液の透過率の測定誤差が小さい。よって、粒径の測
定誤差が小さい。Further, if the dispersion and the concentration of the powder of the particle size measurement object are adjusted so that the transmittance and the concentration satisfy the equation (a) within the range of 1% from the Mie theory, the concentration is adjusted. Since the dispersion liquid of the particle diameter measurement target powder used when calculating the particle diameter from the above empirical formula does not cause multiple scattering, the measurement error of the transmittance of the dispersion liquid is small. Therefore, the measurement error of the particle size is small.
さらにこのとき、粒径測定対象粉体分散液の透過率の
測定感度を上げるために、多重散乱を生じない濃度範囲
内で特定分散液濃度をできるだけ高く設定することも容
易である。Further, at this time, in order to increase the measurement sensitivity of the transmittance of the powder dispersion for particle size measurement, it is easy to set the concentration of the specific dispersion as high as possible within the concentration range where multiple scattering does not occur.
なお、以上において、800nm以上の長波長光を使用す
れば、吸光係数と粒径との間の直線性がより良好にな
り、特に式(ニ)がより良好に成立するようになり、そ
の精度が非常に良好となる。また、長波長光であるほ
ど、より高い分散液濃度でも式(イ)が成立するため、
測定感度をより高くしやすい。In the above, if long-wavelength light of 800 nm or more is used, the linearity between the extinction coefficient and the particle size becomes better, and especially equation (d) becomes better, and its accuracy is improved. Will be very good. Further, the longer the wavelength of light, the higher the concentration of the dispersion liquid, the equation (a) holds,
It is easy to increase the measurement sensitivity.
[実施例] 第1図は、本発明の実施例に係る粒径測定方法に好適
に使用される分光光度計の光学系統図である。[Example] FIG. 1 is an optical system diagram of a spectrophotometer which is preferably used in a particle size measuring method according to an example of the present invention.
この分光光度計は、重水素ランプD2とハロゲンランプ
WIとの2光源を有する測定波長域200nm〜1100nmの紫外
可視分光光度計である。光源D2又はWIから出た光は、窓
板Wを通過し、光源集光ミラーM1で反射した後、入口ス
リットS1を通して回折格子Gに入射する。格子Gで回折
されて出口スリットS2を出た光は、迷光カットフィルタ
Fを通過してミラーM2に入射し、ハーフミラーM3により
試料側光束と対照側光束とに分けられ、ミラーM4,M5で
再び反射した後、窓板Wを通してそれぞれ試料室に入
る。試料室内において試料側セルSam.と対照側セルRef.
とをそれぞれ透過した光束は、レンズLで集光された
後、光検出器であるフォトダイオードP.D.に入射する。This spectrophotometer is equipped with a deuterium lamp D 2 and a halogen lamp.
It is an ultraviolet-visible spectrophotometer having a measurement wavelength range of 200 nm to 1100 nm and having two light sources of WI. The light emitted from the light source D 2 or WI passes through the window plate W, is reflected by the light source condensing mirror M 1 , and then enters the diffraction grating G through the entrance slit S 1 . The light diffracted by the grating G and exiting the exit slit S 2 passes through the stray light cut filter F, enters the mirror M 2, and is split by the half mirror M 3 into a sample-side light beam and a control-side light beam. After being reflected again at 4 and M 5 , they enter the sample chamber through the window plate W respectively. In the sample chamber, the sample cell Sam. And the control cell Ref.
The light fluxes that have respectively passed through and are condensed by the lens L and then enter the photodiode PD which is a photodetector.
この分光光度計を使用するに際し、粉体分散液を試料
側セルSam.としてセットする一方、分散媒のみを対照側
セルRef.としてセットする。このとき、粉体粒子が存在
しない場合に対するこの粒子が存在する場合の透過光の
減衰比すなわち透過率を測定することができる。When using this spectrophotometer, the powder dispersion is set as the sample side cell Sam., While only the dispersion medium is set as the control side cell Ref. At this time, it is possible to measure the attenuation ratio of the transmitted light, that is, the transmittance, when the powder particles are present as compared to when the powder particles are not present.
また、この分光光度計を使用して、分散液の濃度が多
重散乱を生じない範囲内にある既知粒径の粉体の分散液
について、単波長光での光透過に関するデータ取りを行
う。Also, using this spectrophotometer, data regarding light transmission with single wavelength light is obtained for a dispersion liquid of a powder having a known particle diameter, the dispersion liquid concentration of which is within a range where multiple scattering does not occur.
一般に、多重散乱を生じない稀薄濃度域で成立する単
分散系のLambert−Beerの法則は、次式(1)で示され
る。In general, the Lambert-Beer law of a monodisperse system that holds in a dilute concentration range where multiple scattering does not occur is represented by the following equation (1).
log(I0/I)=KAcl ……(1) I0:入射光強度、I:透過光強度、K:吸光係数、A:粒子
投影面積(1g当光束中)、c:粒子重量濃度、l:分散液中
の光路長さ。log (I 0 / I) = KAcl (1) I 0 : incident light intensity, I: transmitted light intensity, K: extinction coefficient, A: particle projected area (in 1g light flux), c: particle weight concentration, l: Optical path length in the dispersion.
ここで、透過率T=I/I0なので、式(1)は、次式
(9)となる。Here, since the transmittance T = I / I 0 , the equation (1) becomes the following equation (9).
logT=KAlc ……(9) 既知粒径の粉体の分散液についてその透過率Tを測定
すれば、式(9)より、吸光係数Kが得られる。logT = KAlc (9) If the transmittance T of a powder dispersion having a known particle size is measured, the extinction coefficient K can be obtained from the equation (9).
データ取りに使用する粉体としては、例えば単分散球
形粒子であるシリカ(SiO2)粒子やポリスチレンラテッ
クス粒子を使用することができる。ここでは、、ポリス
チレンラテックス粒子について、その結果を第2図に示
す。ポリスチレンラテックス粒子は0.061μm〜1.696μ
mの粒径のもの(11種類)を使用する。As the powder used for data collection, for example, silica (SiO 2 ) particles which are monodisperse spherical particles and polystyrene latex particles can be used. Here, the results of polystyrene latex particles are shown in FIG. Polystyrene latex particles are 0.061μm ~ 1.696μ
Use a particle size of m (11 types).
両対数グラフに描かれた吸光係数(K)−粒径(D)
曲線は、粒径(D)が大きくなるほど吸光係数Kが増大
し、極大値を示した後に振動域に入るという傾向を示
す。そして、波長λ=900nm〜1100nmの条件下におい
て、吸光係数Kが粒径Dの3乗にほぼ比例する。また、
粒径Dが小さくなるにつれて振動域から減衰域に入る
が、このとき、波長λが長い領域では吸光係数Kが直線
的にしかも互いに平行に、各波長ごとに減衰する。Extinction coefficient (K) -particle size (D) drawn on a log-log graph
The curve shows a tendency that as the particle size (D) increases, the absorption coefficient K increases and reaches a maximum value and then enters the vibration range. Under the condition of wavelength λ = 900 nm to 1100 nm, the absorption coefficient K is almost proportional to the cube of the particle size D. Also,
As the particle diameter D becomes smaller, it enters the vibration range to the attenuation range. At this time, in the region where the wavelength λ is long, the absorption coefficient K is attenuated linearly and parallel to each other for each wavelength.
第2図に示される粒径0.1μm〜1.0μmの範囲の吸光
係数Kの減衰域において、吸光係数Kと粒径Dとの関係
は2つの直線で近似できる。すなわち、定数αi,βiを
用いて吸光係数Kを式(2)で表わすことができる。In the attenuation region of the extinction coefficient K in the range of the particle size of 0.1 μm to 1.0 μm shown in FIG. 2, the relationship between the extinction coefficient K and the particle size D can be approximated by two straight lines. That is, the extinction coefficient K can be expressed by the equation (2) using the constants α i and β i .
logK=αilogD+βi ……(2) (i=1,2) 一方、Lambert−Beerの法則(式(1))より、 log(I0/I)=1.5Kcl/ρD ……(3) ここに、 ρ:粒子密度、D:粒径。logK = α i logD + β i (2) (i = 1,2) On the other hand, from Lambert-Beer's law (equation (1)), log (I 0 /I)=1.5 Kcl / ρD (3) Here, ρ: particle density, D: particle size.
粒子は球形であり、式(2)(3)より次の実験式
(4)を得る。The particles are spherical, and the following empirical formula (4) is obtained from the formulas (2) and (3).
D=EXP{(βi−logZ)/(1−αi)} ……(4) ここに、Zは、 Z=ρlog(I0/I)/1.5cl ……(5) である。D = EXP {(β i −logZ) / (1−α i )} (4) Here, Z is Z = ρlog (I 0 /I)/1.5cl (5).
式(5)において、I0/I=1/Tなので、式(4)は透
過率Tと粒径Dの関係を示す実験式である。Since I 0 / I = 1 / T in formula (5), formula (4) is an empirical formula showing the relationship between the transmittance T and the particle size D.
次に、第2図中のデータのうち直線性が最も良好な波
長λ=1100nmのデータのみを抽出して第3図に示す。Next, of the data in FIG. 2, only the data with the wavelength λ = 1100 nm, which has the best linearity, is extracted and shown in FIG.
第3図に示すように、ポリスチレンラテックス粒子の
粒径0.1μm〜1.0μmの範囲の減衰域で吸光係数Kが粒
径Dの3乗に比例すると近似すれば、定数mを用いて吸
光係数Kを式(6)で表わすことができる。As shown in FIG. 3, if it is approximated that the extinction coefficient K is proportional to the cube of the particle diameter D in the attenuation region of the polystyrene latex particle diameter of 0.1 μm to 1.0 μm, the extinction coefficient K is calculated using the constant m. Can be expressed by equation (6).
K=mD3 ……(6) この式(6)をLambert−Beer式に代入し、ポリスチ
レンラテックス粒子の場合に定数mがほぼ1に等しいこ
とを考慮すると、 log(I0/I)=1.5clD2/ρ ……(7) となる。ここで、次式(8)を得る。K = mD 3 (6) By substituting this equation (6) into the Lambert-Beer equation and considering that the constant m is almost equal to 1 in the case of polystyrene latex particles, log (I 0 /I)=1.5 clD 2 / ρ (7) Here, the following equation (8) is obtained.
式(5)において、I0/I=1/Tなので、式(8)は透
過率Tと粒径Dの関係を示す実験式である。 Since I 0 / I = 1 / T in the formula (5), the formula (8) is an empirical formula showing the relationship between the transmittance T and the particle diameter D.
以上のようにして既知粒径の粉体の分散液について透
過率Tと粒径Dとの関係を表わす実験式を作成した後、
以下の粒径測定操作を実施する。After creating an empirical formula representing the relationship between the transmittance T and the particle size D for a dispersion liquid of powder having a known particle size as described above,
The following particle size measurement operation is performed.
まず、計量した粒径測定対象粉体を一定量の水中に投
入し、超音波分散及び手での攪拌により投入粉体を水中
に分散させて既知濃度の均一な原液を作成する。この原
液を希釈して例えば4種類の濃度の試料を作成する。第
4図に示すように、セル1〜4には、例えば20%、40
%、60%及び80%の標線までそれぞれ予め水を入れてお
く。そして、各セルに前記の原液を注ぎ入れて各セル内
の液量を100%とし、更に超音波分散と手攪拌とを施
す。分散媒として使用する水は、イオン交換樹脂による
脱イオン水を使用することが好ましい。ただし、分散媒
は水に限らず、粉体の種類に応じて適宜変更可能であ
る。必要な場合にはヘキサメタリン酸ソーダ等の分散剤
を使用しても良い。First, the measured powder to be measured for particle diameter is charged into a fixed amount of water, and the charged powder is dispersed in water by ultrasonic dispersion and manual stirring to prepare a uniform stock solution of known concentration. The stock solution is diluted to prepare samples of four kinds of concentrations, for example. As shown in FIG. 4, cells 1 to 4 have, for example, 20% and 40%.
Prefill water up to the%, 60% and 80% marked lines respectively. Then, the above stock solution is poured into each cell to make the liquid amount in each cell 100%, and ultrasonic dispersion and manual stirring are further performed. The water used as the dispersion medium is preferably deionized water with an ion exchange resin. However, the dispersion medium is not limited to water, and can be appropriately changed according to the type of powder. A dispersant such as sodium hexametaphosphate may be used if necessary.
セル1〜4を試料側セルSam.として分光光度計に順次
セットし、例えば1100nmの波長の光源を選択して、フォ
トダイオードP.D.で光の透過率Tを測定する。Cells 1 to 4 are sequentially set in the spectrophotometer as sample side cells Sam. A light source having a wavelength of 1100 nm, for example, is selected, and the light transmittance T of the photodiode PD is measured.
粒径測定感度を上げるためには粒子濃度が高いことが
望ましい。つまり、粒子が稀薄すぎると測定濃度が悪く
なる。逆に、粒子濃度が高過ぎても多重散乱が発生して
誤差を生ずる。したがって、透過率(logT)−粒子重量
濃度(c)のグラフが直線性を示すことを通して多重散
乱が起っていないことを確認しながら、多重散乱域に達
しない範囲内で粒子濃度をできるだけ高くする。A high particle concentration is desirable in order to increase the sensitivity of particle size measurement. That is, if the particles are too thin, the measured concentration will deteriorate. On the contrary, even if the particle concentration is too high, multiple scattering occurs and an error occurs. Therefore, while confirming that multiple scattering does not occur through the graph of transmittance (logT) -particle weight concentration (c) showing linearity, the particle concentration should be as high as possible within the range not reaching the multiple scattering region. To do.
粒径測定対象粉体の分散液濃度を、多重散乱を生じな
い範囲内においてできるだけ高くすれば、測定誤差を最
小限におさえることができる。The measurement error can be minimized by increasing the concentration of the dispersion liquid of the particle size measurement target powder within the range where multiple scattering does not occur.
第5図は、ポリスチレンラテックスのサブミクロン粒
子(粒径D=0.061μm)について、透過率Tと粒子重
量濃度cとの関係を示す図である。第6図及び第7図
は、それぞれ同粒子の粒径がD=0.208μmの場合及び
D=0.309μmの場合の同様の図である。これら3図と
同様の透過率−濃度のグラフを描いて、Mie理論からの
ずれを1%以内におさえる。FIG. 5 is a diagram showing the relationship between the transmittance T and the particle weight concentration c for submicron particles of polystyrene latex (particle diameter D = 0.061 μm). FIG. 6 and FIG. 7 are similar views when the particle size of the same particles is D = 0.208 μm and D = 0.309 μm, respectively. Draw a graph of transmittance-concentration similar to these three figures and keep the deviation from Mie theory within 1%.
なお、基準粉体の分散液濃度を、多重散乱を生じない
範囲に調製するときも、同様に透過率−濃度のグラフを
描いて、直線性を示す範囲にする。Even when the dispersion concentration of the reference powder is adjusted to a range that does not cause multiple scattering, a transmittance-concentration graph is drawn in the same manner so that the dispersion exhibits linearity.
基準粉体の分散液濃度を、多重散乱を生じない範囲内
においてできるだけ高くすれば、実際値に良く適合する
実験式を決定することができる。By setting the dispersion concentration of the reference powder as high as possible within the range where multiple scattering does not occur, it is possible to determine an empirical formula that is well suited to the actual value.
以上のようにして透過率Tを求めれば、実験式
(4)、(8)を用いて粒径Dを算出することができ
る。なお、サブミクロン域の実験式は粒径Dが1μmを
越えた範囲では成立たないので、式(4)、(8)の粒
径計算結果が1μmを越えた場合には、適宜の方法で求
めたミクロン域の粒径算出式を使用する。If the transmittance T is obtained as described above, the particle diameter D can be calculated using the empirical formulas (4) and (8). Since the empirical formula in the submicron range does not hold in the range where the particle size D exceeds 1 μm, when the particle size calculation results of the formulas (4) and (8) exceed 1 μm, an appropriate method is used. Use the calculated particle size in the micron range.
以上、本発明を実施例により説明してきたように、本
発明によって、0.1μm〜1.0μmのサブミクロン域の粒
径を簡単に測定できる。また、分散液の透過率と粉体粒
径との関係は、種々の粉体粒子についても一般性、共通
性を有する。As described above, according to the present invention, the particle size in the submicron range of 0.1 μm to 1.0 μm can be easily measured by the present invention. Further, the relationship between the transmittance of the dispersion liquid and the particle size of the powder has generality and commonality among various powder particles.
また、サブミクロン粒子については、粒度分布幅がシ
ャープであるから、本発明を適用して特に高精度で粒径
測定を実行することができる。ただし、粒径の異なるも
のが混合された場合であっても本発明の方法は適用可能
である。Further, since the particle size distribution width of submicron particles is sharp, the present invention can be applied to perform particle size measurement with particularly high accuracy. However, the method of the present invention can be applied even when particles having different particle sizes are mixed.
[発明の効果] 以上のように本願発明者は、サブミクロン域の粒径測
定において、分散液の透過率と粒径との関係を示す実験
式を求める際に、基準粉体の分散液濃度を多重散乱を生
じない範囲内に調製すれば、分散液の吸光係数が粒径に
対して直線性を示すことを見出した。本発明の粒径測定
方法は、この直線性を利用して前記実験式を求めるの
で、簡単で精度が固い実験式が得られ、よって、実験式
から算出される粒径の精度が高い。[Effects of the Invention] As described above, the inventor of the present invention determines the concentration of the dispersion liquid of the reference powder when determining the empirical formula showing the relationship between the transmittance and the particle size of the dispersion liquid in the measurement of the particle size in the submicron range. It was found that the absorption coefficient of the dispersion shows linearity with respect to the particle diameter when the is prepared within the range where multiple scattering does not occur. In the particle size measuring method of the present invention, since the empirical formula is obtained by utilizing this linearity, a simple and precise empirical formula can be obtained, and therefore the accuracy of the particle size calculated from the empirical formula is high.
このように、従来、0.1μm〜1.0μmのサブミクロン
域の粒径は、短波長光によらなければ測定し得ないとい
う常識があったが、本発明によれば、このサブミクロン
域の粒径を長波長光でも簡単に測定でき、安価でしかも
簡単な操作により正確な粒径測定ができる方法を提供す
ることができる。As described above, conventionally, it was common knowledge that the particle size in the submicron range of 0.1 μm to 1.0 μm could be measured only by using the short-wavelength light. It is possible to provide a method in which the diameter can be easily measured even with long-wavelength light, and the particle size can be accurately measured at a low cost by a simple operation.
なお、本発明により、求められる粒径の値は、粉体粒
子に光を当てた際、その背景にできる投影面積に相当す
る面積を有する円の直径であるため、粒子形状がとうで
あれ、この投影面積径を求めることができる。According to the present invention, the value of the particle diameter obtained is the diameter of a circle having an area corresponding to the projected area of the background when the powder particles are exposed to light, so that the particle shape is always This projected area diameter can be obtained.
第1図は、本発明の実施例に係る粒径測定方法に使用さ
れる分光光度計の光学系統図、 第2図は、ポリスチレンラテックス粒子の吸光係数Kと
粒径Dとの関係を示す図、 第3図は、第3図中のデータのうち波長λ=1100nmの場
合を抽出して示す図、 第4図は、粒径測定のために第1図の分光光度計に試料
側セルとしてセットすべき4種類の濃度のセルを作成す
る過程を示す工程図、 第5図は、ポリスチレンラテックスのサブミクロン粒子
について、透過率Tと粒子重量濃度cとの関係を示す
図、 第6図は、他の粒径のポリスチレンラテックス・サブミ
クロン粒子の前図と同様の図、 第7図は、更に他の粒径のポリスチレンラテックス・サ
ブミクロン粒子の第5図と同様の図である。 符号の説明 D2……重水素ランプ、F……フィルタ G……回折格子、L……レンズ M1〜M5……ミラー、P.D.……フォトダイオード Ref.……対照側セル、Sam……試料側セル S1,S2……スリット、W……窓板 WI……ハロゲンランプ D……粒径 K……吸光係数 T……透過率FIG. 1 is an optical system diagram of a spectrophotometer used in a particle size measuring method according to an embodiment of the present invention, and FIG. 2 is a diagram showing a relationship between an extinction coefficient K of polystyrene latex particles and a particle size D. , Fig. 3 is a diagram showing a case where the wavelength λ = 1100 nm is extracted from the data in Fig. 3, and Fig. 4 is a sample side cell in the spectrophotometer of Fig. 1 for particle size measurement. FIG. 5 is a process diagram showing a process of producing cells of four kinds of concentrations to be set, FIG. 5 is a diagram showing the relationship between the transmittance T and the particle weight concentration c for submicron particles of polystyrene latex, and FIG. FIG. 7 is a view similar to the previous figure of polystyrene latex submicron particles of other particle sizes, and FIG. 7 is a view similar to FIG. 5 of polystyrene latex submicron particles of other particle sizes. Explanation of symbols D 2 …… Deuterium lamp, F …… Filter G …… Diffraction grating, L …… Lens M 1 to M 5 …… Mirror, PD …… Photodiode Ref. …… Control side cell, Sam …… Sample side cell S 1 , S 2 …… Slit, W …… Window plate WI …… Halogen lamp D …… Particle size K …… Extinction coefficient T …… Transmittance
───────────────────────────────────────────────────── フロントページの続き (72)発明者 水野 光国 愛知県名古屋市東区芳野3丁目5番12号 (72)発明者 藪内 正次 大阪府大阪市旭区新森2丁目20番1号 (56)参考文献 特開 昭59−159051(JP,A) 特開 昭55−131749(JP,A) 特開 昭62−175644(JP,A) 特開 昭60−158337(JP,A) 実開 昭63−118549(JP,U) 粉体工学研究会編「粒度測定技術」P. 164,日刊工業新聞社(昭和50年8月20日 発行) ─────────────────────────────────────────────────── ─── Continuation of the front page (72) Inventor Mitsukuni Mizuno 3-5-12 Yoshino, Higashi-ku, Nagoya, Aichi Prefecture (72) Inventor Shoji Yabuuchi 2-20-1, Shinmori, Asahi-ku, Osaka-shi, Osaka ( 56) References JP 59-159051 (JP, A) JP 55-131749 (JP, A) JP 62-175644 (JP, A) JP 60-158337 (JP, A) Sho 63-118549 (JP, U) “Powder Engineering Research Group,” Particle Size Measurement Technology, P. 164, Nikkan Kogyo Shimbun (Published August 20, 1975)
Claims (5)
の粒径を200〜1100nmの特定波長光を用いて測定する、
光散乱現象を生じる領域における粒径測定方法におい
て、 既知粒径の基準粉体について、この粉体の分散液の特定
波長光に対する透過率(T)を測定して、分散液濃度
(c[g/cm3])が下記式(イ)をMie理論からのずれが
1%以内の範囲で満す濃度範囲内で、基準粉体の特定分
散液濃度を決定し、 前記特定分散液濃度に調製した複数の既知粒径の基準粉
体の分散液について、前記特定波長光の透過率を測定し
て粒径(D)と吸光係数(K)との関係を下記式(ロ)
に示す直線で近似し、この式(ロ)とLambert−Beerの
式とにより分散液の透過率(T)と粉体粒径(D)との
関係を表わす下記式(ハ)に示す実験式を求めておき、 粒径測定対象粉体の分散液について前記特定波長光の透
過率を測定し、前記の実験式から粒径を算出することを
特徴とする粒径測定方法。 式(イ);logT=a・c (ここで、T=透過光強度/入射光強度、a
=定数。) 式(ロ);logK=αilogD+βi (ここで、αi、βi=定数、i=1,2。) 式(ハ);D=EXP{(βi−logZ)/(1−αi)} (ここで、Z=−ρlogT/1.5cl、 ρ=粒子密度、l=分散液中の光
路長さ。)1. The particle size of particles in the submicron region having a particle size of 0.1 to 1 μm is measured using light having a specific wavelength of 200 to 1100 nm,
In a particle size measuring method in a region where a light scattering phenomenon occurs, the transmittance (T) of a dispersion liquid of this powder with respect to a specific wavelength light is measured for a reference powder having a known particle size to obtain a dispersion liquid concentration (c [g / cm 3 ]) determines the specific dispersion liquid concentration of the reference powder within a concentration range in which the deviation from the Mie theory satisfies the following formula (a) within 1% and is adjusted to the specific dispersion liquid concentration. With respect to the dispersion liquid of the plurality of reference powders having known particle diameters, the transmittance of the specific wavelength light was measured, and the relationship between the particle diameter (D) and the extinction coefficient (K) was calculated by the following formula (B).
Approximate with the straight line shown in, and the empirical formula shown in the following formula (C) that represents the relationship between the transmittance (T) of the dispersion liquid and the powder particle size (D) by this formula (B) and the Lambert-Beer formula The particle size measurement method is characterized in that the transmittance of the specific wavelength light is measured for the dispersion liquid of the particle size measurement target powder, and the particle size is calculated from the empirical formula. Formula (a); logT = a · c (where T = transmitted light intensity / incident light intensity, a
= Constant. ) Formula (b); logK = α i logD + β i (where α i , β i = constant, i = 1,2.) Formula (c); D = EXP {(β i −logZ) / (1- α i )} (where, Z = −ρlogT / 1.5cl, ρ = particle density, l = optical path length in the dispersion liquid.)
の粒径を200〜1100nmの特定波長光を用いて測定する光
散乱現象を生じる領域における粒径測定方法において、 粒径測定対象粉体の分散液について測定する特定波長光
の透過率からこの粉体の粒径を算出する際に用いる下記
式(ハ)に示す分散液の透過率(T)と粉体粒径(D)
との関係を表わす実験式を、 既知粒径の基準粉体について、この粉体の分散液の特定
波長光に対する透過率(T)を測定して、分散液濃度
(c[g/cm3])が下記式(イ)をMie理論からのずれが
1%以内の範囲で満す濃度範囲内で、基準粉体の特定分
散液濃度を決定し、 前記特定分散液濃度に調製した複数の既知粒径の基準粉
体の分散液について、前記特定波長光の透過率を測定し
て粒径(D)と吸光係数(K)との関係を下記式(ロ)
に示す直線で近似し、この式(ロ)とLambert−Beerの
式とにより求めることを特徴とする粒径測定方法。 式(イ);logT=a・c (ここで、T=透過光強度/入射光強度、a
=定数。) 式(ロ);logK=αilogD+βi (ここで、αi、βi=定数、i=1,2。) 式(ハ);D=EXP{(βi−logZ)/(1−αi)} (ここで、Z=−ρlogT/1.5cl、 ρ=粒子密度、l=分散液中の光
路長さ。)2. A particle size measuring method in a region in which a light scattering phenomenon occurs in which a particle size of submicron particles having a particle size of 0.1 to 1 μm is measured using light having a specific wavelength of 200 to 1100 nm. The dispersion liquid transmittance (T) and the powder particle diameter (D) shown in the following formula (C) used when calculating the particle diameter of this powder from the transmittance of the specific wavelength light measured for the body dispersion liquid
The empirical formula expressing the relationship with is calculated by measuring the transmittance (T) of a dispersion liquid of this powder with respect to light of a specific wavelength for a reference powder having a known particle size, and measuring the dispersion liquid concentration (c [g / cm 3 ] ) Determines the specific dispersion liquid concentration of the reference powder within a concentration range in which the deviation from the Mie theory satisfies the following formula (a) within 1%, and a plurality of known dispersion liquids prepared to have the specific dispersion liquid concentration are prepared. With respect to the dispersion liquid of the reference powder having a particle diameter, the transmittance of the specific wavelength light is measured, and the relationship between the particle diameter (D) and the extinction coefficient (K) is expressed by the following formula (B).
A method for measuring particle diameter, which is characterized by approximating with a straight line shown in, and obtaining by this formula (b) and the Lambert-Beer formula. Formula (a); logT = a · c (where T = transmitted light intensity / incident light intensity, a
= Constant. ) Formula (b); logK = α i logD + β i (where α i , β i = constant, i = 1,2.) Formula (c); D = EXP {(β i −logZ) / (1- α i )} (where, Z = −ρlogT / 1.5cl, ρ = particle density, l = optical path length in the dispersion liquid.)
係を下記式(ニ)に近似し、この式(ニ)とLambert−B
eerの式とにより下記式(ホ)に示す前記の透過率
(T)と粉体粒径(D)との関係を表わす前記実験式を
求めることを特徴とする請求項1又は2に記載の粒径測
定方法。 式(ニ);K=mD3 (ここで、m=定数) (ここで、Z=−ρlogT/1.5cl、 ρ=粒子密度、l=分散液中の光
路長さ。)3. The relationship between the particle diameter (D) and the extinction coefficient (K) is approximated to the following formula (d), and this formula (d) and Lambert-B
3. The empirical formula representing the relationship between the transmittance (T) and the powder particle size (D) shown in the following formula (e) is obtained from the equation of eer, and the empirical formula is obtained. Particle size measurement method. Formula (d); K = mD 3 (where m = constant) (Where Z = −ρlogT / 1.5cl, ρ = particle density, l = optical path length in the dispersion.)
この粉体の分散液の特定波長光に対する透過率(T)を
測定して、分散液濃度(c[g/cm3])が前記式(イ)
をMie理論からのずれが1%以内の範囲で満す濃度範囲
内で、前記粒径測定対象粉体の特定分散液濃度を決定
し、 この特定分散液濃度に調製した前記粒径測定対象粉体の
分散液について、前記特定波長光の透過率を測定して、
前記実験式から粒径を算出することを特徴とする請求項
1〜3のいずれか1項に記載の粒径測定方法。4. A dispersion liquid of the powder to be measured for particle size,
The transmittance (T) of the dispersion liquid of this powder for light of a specific wavelength was measured, and the dispersion liquid concentration (c [g / cm 3 ]) was calculated by the above formula (a).
Within the concentration range where the deviation from the Mie theory is within 1%, the specific dispersion liquid concentration of the particle size measurement target powder is determined, and the particle size measurement target powder adjusted to this specific dispersion liquid concentration is determined. For the body dispersion, measuring the transmittance of the specific wavelength light,
The particle size measuring method according to claim 1, wherein the particle size is calculated from the empirical formula.
徴とする請求項1〜4のいずれか1項に記載の粒径測定
方法。5. The particle size measuring method according to claim 1, wherein long-wavelength light of 800 nm or more is used.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63297383A JPH0820355B2 (en) | 1988-11-24 | 1988-11-24 | Particle size measurement method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63297383A JPH0820355B2 (en) | 1988-11-24 | 1988-11-24 | Particle size measurement method |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH02143140A JPH02143140A (en) | 1990-06-01 |
| JPH0820355B2 true JPH0820355B2 (en) | 1996-03-04 |
Family
ID=17845780
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| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP63297383A Expired - Fee Related JPH0820355B2 (en) | 1988-11-24 | 1988-11-24 | Particle size measurement method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0820355B2 (en) |
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| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP4132692B2 (en) * | 2001-02-20 | 2008-08-13 | 株式会社堀場製作所 | Particle size distribution measuring device |
| JP2011153856A (en) * | 2010-01-26 | 2011-08-11 | Toshiba Corp | Device and method for measurement of particle size using terahertz wave |
| WO2012137686A1 (en) * | 2011-04-01 | 2012-10-11 | 関西ペイント株式会社 | Particle size evaluation method and particle size evaluation device |
| JP6196610B2 (en) * | 2012-02-21 | 2017-09-13 | 株式会社明治 | Simple measurement method for 50% particle size of dairy foods |
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|---|---|---|---|---|
| JPS55131749A (en) * | 1979-03-31 | 1980-10-13 | Hokkaido Daigaku | Method of quantitatively measuring floating particle |
| JPS59159051A (en) * | 1983-02-28 | 1984-09-08 | Shimadzu Corp | Particle size distribution measuring device |
| DE3347162A1 (en) * | 1983-12-27 | 1985-07-04 | Behringwerke Ag, 3550 Marburg | PHOTOMETRIC METHOD FOR DETERMINING CONCENTRATION IN REACTIONS WHICH ARE GIVING OR USING SPREAD CENTERS |
| JPS62175644A (en) * | 1986-01-29 | 1987-08-01 | Shimadzu Corp | Suspension particle size measurement method and particle size measurement device |
| JPS63118549U (en) * | 1987-01-23 | 1988-08-01 |
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1988
- 1988-11-24 JP JP63297383A patent/JPH0820355B2/en not_active Expired - Fee Related
Non-Patent Citations (1)
| Title |
|---|
| 粉体工学研究会編「粒度測定技術」P.164,日刊工業新聞社(昭和50年8月20日発行) |
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| Publication number | Publication date |
|---|---|
| JPH02143140A (en) | 1990-06-01 |
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