JPH0473740B2 - - Google Patents
Info
- Publication number
- JPH0473740B2 JPH0473740B2 JP12630286A JP12630286A JPH0473740B2 JP H0473740 B2 JPH0473740 B2 JP H0473740B2 JP 12630286 A JP12630286 A JP 12630286A JP 12630286 A JP12630286 A JP 12630286A JP H0473740 B2 JPH0473740 B2 JP H0473740B2
- Authority
- JP
- Japan
- Prior art keywords
- light
- test tube
- angle
- cell
- present
- 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
Links
- 238000000034 method Methods 0.000 claims description 8
- 239000007788 liquid Substances 0.000 claims description 7
- 238000005375 photometry Methods 0.000 claims description 2
- 230000003287 optical effect Effects 0.000 description 6
- 238000005259 measurement Methods 0.000 description 5
- 239000010419 fine particle Substances 0.000 description 2
- 230000003321 amplification Effects 0.000 description 1
- 238000000149 argon plasma sintering Methods 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 230000004907 flux Effects 0.000 description 1
- 230000001678 irradiating effect Effects 0.000 description 1
- 238000003199 nucleic acid amplification method Methods 0.000 description 1
- 239000005304 optical glass Substances 0.000 description 1
- 238000007740 vapor deposition Methods 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
- G01N21/47—Scattering, i.e. diffuse reflection
- G01N21/49—Scattering, i.e. diffuse reflection within a body or fluid
- G01N21/51—Scattering, i.e. diffuse reflection within a body or fluid inside a container, e.g. in an ampoule
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
- G01N21/47—Scattering, i.e. diffuse reflection
- G01N21/49—Scattering, i.e. diffuse reflection within a body or fluid
- G01N21/51—Scattering, i.e. diffuse reflection within a body or fluid inside a container, e.g. in an ampoule
- G01N2021/513—Cuvettes for scattering measurements
Landscapes
- Physics & Mathematics (AREA)
- Health & Medical Sciences (AREA)
- Life Sciences & Earth Sciences (AREA)
- Chemical & Material 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)
本発明は各種の液内に存在する微粒子の光によ
る散乱光度測定法に関するものである。DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to a method for measuring light scattering of fine particles present in various liquids.
(従来技術と問題点)
従来、散乱光度測定には第4図に示すような横
断面正方形状の角型光学セルを用い、このセル
の中に被測定液を入れて、角型光学セルの軸
線に対し直角方向の側部よりフイルター、スリ
ツトを介して一定光束の平行光を光源より
照射し、被測定液による散乱光を、角型光学セル
の正面から受光部により受光し、増巾部に
て増巾観測するものがある。この角型光学セル
は第5図に示すように入射光の乱反射が生じない
ため正確な測定が可能であるが、4面が光学ガラ
スで各面は蒸着接合されているため、1本当り
5000円と高価なものであり、従来使用されている
測定装置にはこの角型セルが最低10本必要であつ
て、これだけでも相当な価格を占めることになつ
ている。(Prior art and problems) Conventionally, a square optical cell with a square cross section as shown in Fig. 4 is used for scattering photometry, and the liquid to be measured is placed in the cell and the square optical cell is heated. A light source emits a constant beam of parallel light from the side perpendicular to the axis through a filter and slit, and the light scattered by the liquid to be measured is received by the light receiving part from the front of the rectangular optical cell. There are some things that can be observed with increased width. As shown in Figure 5, this rectangular optical cell allows for accurate measurements because it does not cause diffuse reflection of incident light, but since the four sides are made of optical glass and each side is bonded by vapor deposition, each
It is expensive at 5,000 yen, and conventional measuring devices require at least 10 of these square cells, which alone accounts for a considerable amount of price.
そこで、本発明者は上記角型光学セルに代え
て、通常の円筒状の試験管(丸型セル)を用いて
散乱光度の測定ができないものかと種々試してみ
たが、試験管を用いて従来の方式と同様に、試験
管の側面から一定光束の平行光を照射し、これ
を正面から観測すると第6図のように試験管の内
面において平行光が乱反射′し、被測定液
のみの散乱光は測定できないものであつた。な
お、この試験管においては透明液の場合でも、試
験管の内面における平行光の乱反射′があるの
で、この乱反射光が受光部に影響を与えると云
う問題があつた。 Therefore, the inventor of the present invention tried various ways to measure the scattered light intensity by using an ordinary cylindrical test tube (round cell) instead of the above-mentioned square optical cell. Similar to the above method, when a constant beam of parallel light is irradiated from the side of the test tube and observed from the front, the parallel light is diffusely reflected on the inner surface of the test tube as shown in Figure 6, and only the liquid to be measured is scattered. Light was something that could not be measured. In this test tube, even when the liquid is transparent, parallel light is diffusely reflected on the inner surface of the test tube, so there is a problem in that this diffusely reflected light affects the light receiving section.
(問題点を解決するための手段)
本発明は市販の安価な試験管(丸型セル)を用
いて、従来の角型光学セルと同様の受光測定がで
きるようにしたもので、第1〜第3図に示すよう
に一定光束の平行光の入射角を、試験管の軸
線に対し直角より一定角度α偏位させた側面位置
から照射することにより、該平行光の試験管内に
おける反射光′を軸線に対し直角より入射角と
等しく角度分だけ反対側に反らせ、これら入射光
′と反射光′の通過しない部分を正面から測
定するようにしたことを特徴とするものである。(Means for Solving the Problems) The present invention uses a commercially available inexpensive test tube (round cell) to perform the same light reception measurement as a conventional square optical cell. As shown in Fig. 3, by irradiating a test tube with a constant incident angle of parallel light from a side position that is deviated by a certain angle α from a right angle to the axis of the test tube, the reflected light of the parallel light inside the test tube is is curved in the opposite direction by an angle equal to the incident angle from a right angle to the axis, and the portion through which the incident light ' and the reflected light ' do not pass is measured from the front.
〔実施例)
本発明は第1図に示すように丸型セルである試
験管の側部上方の光源から絞りを介して試
験管の軸線に対し直角より一定角度α偏位させて
一定光束の平行光を照射し、この平行光の試験
管内における入射光′と反射光′を横切らない
部分を正面から受光部にて受光し、さらにこ
れを増巾部にて増巾して観測するものである。
すなわち、本発明方法の原理は第3図に示すよう
に試験管の軸線に対し直角より一定角度α偏位
させた側面上方位置から一定光束の平行光を照
射すると、この平行光の試験管内における反射光
′は入射光′の入射角αの2倍角下方へ向けて
反射し、正面からみた場合入射光と反射光のいず
れも通過しない部分(点模様部分)ができる。
本発明はこの部分の正面中心部分′を正面か
ら受光部にて受光し被測定液内の微粒子による
乱反射光を測定するものである。[Example] As shown in FIG. 1, the present invention emits a constant luminous flux from a light source above the side of a test tube, which is a round cell, through a diaphragm and deviating by a constant angle α from perpendicular to the axis of the test tube. A method in which parallel light is irradiated, the part of the parallel light inside the test tube that does not cross the incident light ′ and reflected light ′ is received from the front by the light receiving part, and this is further amplified by the amplification part and observed. be.
That is, the principle of the method of the present invention is that, as shown in FIG. The reflected light ' is reflected downward at an angle twice the incident angle α of the incident light ', and when viewed from the front, a portion (a dot pattern portion) through which neither the incident light nor the reflected light passes is created.
In the present invention, light is received from the front center part' of this part by a light receiving section, and the diffusely reflected light by the fine particles in the liquid to be measured is measured.
上記の入射光の角度αはあまり大きければ試験
管内へ入る光が少なくなるし、また、あまり小さ
くても試験管内で乱反射が生じ、これが受光部に
影響を与えるので、約45°程度が望ましいが、特
に限定するものではない。 If the angle α of the incident light is too large, less light will enter the test tube, and if it is too small, diffuse reflection will occur within the test tube, which will affect the light receiving section, so it is preferably about 45°. , is not particularly limited.
本発明方法は一例として第2図に示すような形
態において実施される。すなわち、試験管は平
面L型のセルホルダーの内側隅部に圧接する
ように添わせて立て、セルホルダーの直角状の外
面(側面)の一方に、斜め下方に向けて試験管の
中心に向かう光源を設け、他の外面(正面)の
所定位置(入射光と反射光が横切らない部分′)
に受光部を設けて測定すれば、試験管のセツト
が確実かつ容易で便利である。 The method of the present invention is carried out in the form shown in FIG. 2, by way of example. In other words, the test tube is placed in pressure contact with the inner corner of the flat L-shaped cell holder, and placed on one of the right-angled outer surfaces (side surfaces) of the cell holder, pointing diagonally downward toward the center of the test tube. Provide a light source at a predetermined position on the other external surface (front) (the part where the incident light and reflected light do not cross)
If a light-receiving section is provided in the test tube for measurement, setting the test tube is reliable, easy, and convenient.
なお、上記セルホルダーの光源と受光部
とは、試験管の直径に応じて適宜な手段にて
各々上下左右にスライドできるようにしておけ
ば、試験管の直径が変つても適応できるものとな
る。 In addition, if the light source and light receiving part of the cell holder are made to be able to slide vertically and horizontally using appropriate means depending on the diameter of the test tube, it will be adaptable even if the diameter of the test tube changes. .
(発明の効果)
本発明は上記のように、平行光の入射角を試験
管の軸線と直角とせず、一定角度α上下に傾ける
ことにより試験管内面における反射光を一定の方
向に反らして、平行光内において入射光と反射光
が通過しない部分を確保し、この部分を受光部と
することにより、市販の安価な試験管を用いても
従来の角型セルと同様の測光性能が得られる効果
がある。従つて本発明方法を採用する測定装置は
安価となり産業利用性の高いものである。(Effects of the Invention) As described above, the present invention does not make the incident angle of the parallel light perpendicular to the axis of the test tube, but tilts it up and down at a certain angle α to deflect the reflected light on the inner surface of the test tube in a certain direction. By securing a part within the parallel light where the incident light and reflected light do not pass through, and using this part as the light receiving part, it is possible to obtain the same photometric performance as a conventional square cell even using a commercially available inexpensive test tube. effective. Therefore, a measuring device employing the method of the present invention is inexpensive and has high industrial applicability.
第1図は本発明による測定形態を概略的に示し
た説明図、第2図は測定装置の一例を概略的に示
す斜視図、第3図は本発明方法の原理を示すもの
でイは平面図、ロは正面図、第4図は従来装置の
概略斜視図、第5図は従来の角型セルによる測定
原理を示すものでイは平面図、ロは正面図、第6
図は従来法において試験管を利用した場合の原理
を示すものでイは平面図、ロは正面図である。
1……試験管、2……平行光、3……反射光、
5……光源、7……受光部。
Fig. 1 is an explanatory diagram schematically showing a measurement form according to the present invention, Fig. 2 is a perspective view schematically showing an example of a measuring device, and Fig. 3 shows the principle of the method of the present invention, and A is a plane. Fig. 4 is a schematic perspective view of the conventional device, Fig. 5 shows the principle of measurement using a conventional square cell, A is a plan view, B is a front view, and Fig. 6 is a front view.
The figures show the principle of using test tubes in the conventional method, with A being a plan view and B being a front view. 1...test tube, 2...parallel light, 3...reflected light,
5...Light source, 7...Light receiving section.
Claims (1)
を該試験管の軸線に対し直角より一定角度偏位さ
せた側面位置から一定光束の平行光を、照射し、
該平行光の試験管内における反射光を横切らない
部分を正面から観測するようにした散乱光度測定
法。1. Put the liquid to be measured in a cylindrical test tube, and irradiate it with a constant beam of parallel light from a side position with the incident angle of the light deviated by a certain angle from the right angle to the axis of the test tube,
A scattering photometry method in which a portion of the parallel light in a test tube that does not cross the reflected light is observed from the front.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP12630286A JPS62282246A (en) | 1986-05-30 | 1986-05-30 | Method for measuring scattering luminous intensity |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP12630286A JPS62282246A (en) | 1986-05-30 | 1986-05-30 | Method for measuring scattering luminous intensity |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS62282246A JPS62282246A (en) | 1987-12-08 |
| JPH0473740B2 true JPH0473740B2 (en) | 1992-11-24 |
Family
ID=14931835
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP12630286A Granted JPS62282246A (en) | 1986-05-30 | 1986-05-30 | Method for measuring scattering luminous intensity |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS62282246A (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| EP2667180A4 (en) * | 2011-01-21 | 2014-06-25 | Hitachi High Tech Corp | AUTOMATIC ANALYSIS DEVICE |
| JP7187874B2 (en) * | 2018-08-02 | 2022-12-13 | 株式会社島津製作所 | light scattering detector |
| JP2024171553A (en) * | 2023-05-30 | 2024-12-12 | 株式会社島津製作所 | Liquid Injection Device |
-
1986
- 1986-05-30 JP JP12630286A patent/JPS62282246A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS62282246A (en) | 1987-12-08 |
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