JPS63279143A - Decanter type particle size distribution measuring apparatus - Google Patents
Decanter type particle size distribution measuring apparatusInfo
- Publication number
- JPS63279143A JPS63279143A JP11422587A JP11422587A JPS63279143A JP S63279143 A JPS63279143 A JP S63279143A JP 11422587 A JP11422587 A JP 11422587A JP 11422587 A JP11422587 A JP 11422587A JP S63279143 A JPS63279143 A JP S63279143A
- Authority
- JP
- Japan
- Prior art keywords
- cell
- measuring cell
- rotary disc
- particle size
- size distribution
- 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.)
- Pending
Links
- 239000002245 particle Substances 0.000 title claims description 19
- 238000001816 cooling Methods 0.000 claims abstract description 26
- 238000005259 measurement Methods 0.000 claims abstract description 26
- 239000000725 suspension Substances 0.000 claims abstract description 10
- 238000009423 ventilation Methods 0.000 claims description 12
- 238000004062 sedimentation Methods 0.000 claims description 7
- 239000000523 sample Substances 0.000 abstract 2
- 239000007788 liquid Substances 0.000 abstract 1
- 239000011236 particulate material Substances 0.000 abstract 1
- 238000007664 blowing Methods 0.000 description 3
- 230000000694 effects Effects 0.000 description 3
- 238000010586 diagram Methods 0.000 description 2
- 239000007791 liquid phase Substances 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 230000000630 rising effect Effects 0.000 description 2
- 230000005540 biological transmission Effects 0.000 description 1
- 238000004364 calculation method Methods 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 230000005484 gravity Effects 0.000 description 1
- 230000020169 heat generation Effects 0.000 description 1
- 230000001788 irregular Effects 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 230000002123 temporal effect Effects 0.000 description 1
Landscapes
- Optical Measuring Cells (AREA)
Abstract
Description
【発明の詳細な説明】
〈産業上の利用分野〉
本発明は液相による遠心沈降式の粒度分布測定装置に関
する。DETAILED DESCRIPTION OF THE INVENTION <Industrial Application Field> The present invention relates to a centrifugal sedimentation type particle size distribution measuring device using a liquid phase.
〈従来の技術とその問題点〉
遠心液相沈降法に基づく粒度分布測定装置においては、
一般に、試料粒体を媒液中に分散させて懸濁液を作り、
その懸濁液を測定セル内に封入して回転盤に装着する。<Conventional technology and its problems> In a particle size distribution measuring device based on centrifugal liquid phase sedimentation method,
Generally, sample particles are dispersed in a medium to create a suspension.
The suspension is sealed in a measurement cell and mounted on a rotating disk.
そして、回転盤の回転による遠心力場において粒子群を
沈降させ、光透過法等によって所定の沈降距離において
)懸濁液濃度を刻々と測定し、その経時的変化から試料
粒体の粒度分布を求める。Then, the particle group is sedimented in the centrifugal force field generated by the rotation of the rotary disk, and the suspension concentration is measured moment by moment (at a predetermined sedimentation distance) using a light transmission method, etc., and the particle size distribution of the sample particles is determined from the change over time. demand.
このような遠心沈降式粒度分布測定装置において、回転
盤を高速回転する場合、空気との摩擦によって測定セル
の温度が上昇する。測定セル全体が均一に温められるの
であればさほど問題とはならないが、回転盤の外側、つ
まり回転中心から遠い部分はど速度が速く、より温度上
昇量が大きいため、測定セルの両端で温度差が生じ、懸
濁液にゆるやかな対流が発生する。この対流により、媒
液に対して比重差の少ない試料や、小さな粒子は沈降速
度に大きな影古を受け、濃度変化に不規則な乱れを生じ
、得られた粒度分布は不正確なものとなる。In such a centrifugal sedimentation type particle size distribution measuring device, when the rotary disk is rotated at high speed, the temperature of the measurement cell increases due to friction with the air. This is not a big problem if the entire measurement cell is heated uniformly, but the outside of the rotary disk, that is, the part far from the center of rotation, has a faster speed and a larger temperature rise, so there is a temperature difference between both ends of the measurement cell. occurs, and a gentle convection occurs in the suspension. Due to this convection, samples with a small difference in specific gravity relative to the medium and small particles have a large effect on the sedimentation rate, causing irregular turbulence in concentration changes and making the obtained particle size distribution inaccurate. .
従来、このような現象を未然に防止するために、外気を
測定室に送り込んで測定セルの昇温をおさえていたが、
回転数が10.00Orpm程度にも達すると、このよ
うな送風だけでは不十分であった。Conventionally, in order to prevent such phenomena from occurring, outside air was pumped into the measurement chamber to suppress the temperature rise in the measurement cell.
When the rotational speed reached about 10.00 rpm, such air blowing alone was insufficient.
〈問題点を解決するための手段〉
本発明は、高速度の回転を与えても上述の対流が生じる
ことなく、常に正確な測定結果を得ることのできる遠心
沈降式粒度分布測定装置の提供を目的としており、その
特徴とするところは、実施例に対応する第1図、第2図
に示すように、回転盤2に装着されて回転している測定
セル1に冷気を吹き付け得る電子冷却装置11と、回転
盤20回転数に応じて電子冷却装置11への給電量を変
化させる冷却制御回路12と、電子冷却装置11の冷気
吐出口と測定セル1の回転軌跡との間に介在し、回転盤
2の回転中心軸Cから遠去かるほど冷気の通過量が大き
くなるような複数の開口部10a。<Means for Solving the Problems> The present invention provides a centrifugal sedimentation type particle size distribution measuring device that can always obtain accurate measurement results without causing the above-mentioned convection even when high-speed rotation is applied. As shown in FIGS. 1 and 2 corresponding to the embodiment, the electronic cooling device is capable of blowing cold air onto the rotating measurement cell 1 mounted on the rotary disk 2. 11, a cooling control circuit 12 that changes the amount of power supplied to the electronic cooling device 11 according to the rotation speed of the rotary disk 20, and a cooling control circuit 12 that is interposed between the cold air discharge port of the electronic cooling device 11 and the rotation locus of the measurement cell 1, A plurality of openings 10a such that the farther away from the rotation center axis C of the rotary disk 2, the larger the amount of cold air passing through the openings 10a.
l Q b、−、10nを有してなる通風制限体10を
備えたことにある。The present invention is provided with a ventilation restricting body 10 having l Q b, -, 10n.
〈作用〉
測定セル1の温度上昇量は、回転盤2の回転数によって
定まる空気との摩擦力に基づくから、この回転数に応じ
て電子冷却装置11への給電量を変化させることによっ
てその冷却力を制御すれば、測定セル1全体の温度は回
転数に拘らず上昇することがない。<Function> Since the amount of temperature rise in the measuring cell 1 is based on the frictional force with the air determined by the rotation speed of the rotary disk 2, the amount of power supplied to the electronic cooling device 11 can be changed in accordance with this rotation speed to cool it down. If the force is controlled, the temperature of the entire measuring cell 1 will not rise regardless of the rotation speed.
更に、通風制限体10の介在により、測定セル1内の温
度勾配が解消される。Furthermore, due to the intervention of the ventilation restrictor 10, temperature gradients within the measuring cell 1 are eliminated.
〈実施例〉 本発明の実施例を、以下、図面に基づいて説明する。<Example> Embodiments of the present invention will be described below based on the drawings.
第1図は本発明実施例の全体構成図で、第2図はその通
風制限体10の拡大斜視図である。FIG. 1 is an overall configuration diagram of an embodiment of the present invention, and FIG. 2 is an enlarged perspective view of a ventilation restricting body 10 thereof.
測定すべき試料粒体は、媒液中に均一に分散させて懸濁
液の状態として、透明部材で形成された測定セルi内に
封入される。この測定セル1は、モータ3によって回転
駆動される回転盤2に着脱自在に装着される。モータ3
は、マイクロコンピュータ8から供給される回転数設定
信号に基づいて、モータ制御器9からの出力によってそ
の回転数が制御されるよう構成されている。The sample particles to be measured are uniformly dispersed in a medium and placed in a suspension state in a measurement cell i formed of a transparent member. This measurement cell 1 is detachably attached to a rotary disk 2 that is rotationally driven by a motor 3. motor 3
is configured such that its rotation speed is controlled by an output from a motor controller 9 based on a rotation speed setting signal supplied from a microcomputer 8.
回転盤2の回転中心軸Cから半径方向所定距離の位置に
は、光源4と、この光源4に対向する受光素子5が配設
されており、回転盤2に装着された測定セル1は、その
回転によって光源4と受光素子5との間を横切るよう構
成されている。測定セル1の回転位置はフォトインクラ
ブタ(図示せず)等によって検出され、測定セル1が光
源4と受光素子5との間を横切った時点における受光素
子5の出力信号、すなわち測定セル1の透過光測定信号
が、懸濁液の濃度測定データとして、増幅器6.A−D
変換器7を介してマイクロコンピュータ8に刻々と採取
されるよう構成されている。A light source 4 and a light receiving element 5 facing the light source 4 are disposed at a position a predetermined distance in the radial direction from the rotation center axis C of the rotary disk 2, and the measurement cell 1 mounted on the rotary disk 2 is It is configured to cross between the light source 4 and the light receiving element 5 by its rotation. The rotational position of the measuring cell 1 is detected by a photo ink clubter (not shown) or the like, and the output signal of the light receiving element 5 at the time when the measuring cell 1 crosses between the light source 4 and the light receiving element 5, that is, the measuring cell 1 The transmitted light measurement signal is sent to the amplifier 6 as suspension concentration measurement data. A-D
It is configured so that the data is collected every moment by a microcomputer 8 via a converter 7.
マイクロコンピュータ8は、この濃度測定データの経時
的変化から、公知の算法によって試料粒体の粒度分布を
算出することができる。The microcomputer 8 can calculate the particle size distribution of the sample particles using a known calculation method based on the temporal changes in the concentration measurement data.
さて、回転盤2に近接して、電子冷却装置11が配設さ
れており、その冷気吐出口は回転中の測定セル1に冷気
を吹きつけることができるよう、回転盤2に対向してい
る。この電子冷却装置11は、ペルチェ素子、送風機お
よび熱交換器等によって構成された公知のもので、その
吐出口からの送風温度(室温に対する温度差)はペルチ
ェ素子に流す電流によって決定される。このペルチェ素
子に流す電流は冷却制御回路12から供給されている。Now, an electronic cooling device 11 is disposed close to the rotary disk 2, and its cold air outlet faces the rotary disk 2 so that cold air can be blown onto the rotating measurement cell 1. . The electronic cooling device 11 is a known device that includes a Peltier element, a blower, a heat exchanger, etc., and the temperature of the air blown from its discharge port (temperature difference with respect to room temperature) is determined by the current flowing through the Peltier element. The current flowing through this Peltier element is supplied from the cooling control circuit 12.
冷却制御回路12は、ルック−アップテーブル12aと
、そのルック−アンプテーブル12aからのデータをア
ナログ化するためのD−A変換器12b、およびそのD
−A変換器12bの出力に応じた電流を出力するパワー
アンプ等の電流制御器12cとからなっている。The cooling control circuit 12 includes a look-up table 12a, a D-A converter 12b for analogizing data from the look-up table 12a, and a D-A converter 12b for analogizing data from the look-up table 12a.
- A current controller 12c such as a power amplifier that outputs a current according to the output of the A converter 12b.
ルック−アップテーブル12aは、回転盤2の回転数を
引数とし、その各回転数における測定セル1の発熱に抗
して昇温を防止するために必要な冷却力を電子冷却装置
11から出力するのに要する電流のデータを記憶してお
り、前述したマイクロコンピュータ8からの回転数設定
信号を入力して対応する電流データを出力するよう構成
されている。回転数と所要電流との関係は一般に、−次
間数で表わすことができず、従ってこの関係はあらかじ
め実験的に求めてルック−アップテーブル12aに書き
込んでおく。The look-up table 12a takes the rotational speed of the rotary disk 2 as an argument, and outputs from the electronic cooling device 11 the cooling power necessary to resist the heat generation of the measurement cell 1 at each rotational speed and prevent the temperature from rising. It is configured to input the rotation speed setting signal from the microcomputer 8 mentioned above and output the corresponding current data. Generally, the relationship between the number of rotations and the required current cannot be expressed as a negative order number, so this relationship is determined experimentally in advance and written in the look-up table 12a.
電子冷却装置11の冷気吐出口と測定セル1との間には
、通風制限体10が配設されている。この通風制限体1
0は、第2図に示すように、平板材料に、互いに平行で
、かつ、それぞれ回転盤2の半径方向に直交する方向に
伸びるスリット様の複数の開口部10a、 10 b
、 −、f Onを形成してなっており、その各開口部
10a、10b。A ventilation restrictor 10 is disposed between the cold air outlet of the electronic cooling device 11 and the measurement cell 1 . This ventilation restricting body 1
0, as shown in FIG. 2, a plurality of slit-like openings 10a, 10b are provided in the flat plate material, parallel to each other and extending in directions perpendicular to the radial direction of the rotary disk 2.
, -, f On, each opening 10a, 10b thereof.
−1・、10nの幅は、回転盤2の回転中心軸Cから遠
去かるほど広い。従って、電子冷却装置11からの冷気
は、軸Cから遠去かるほど、つまり、外側はど多量にこ
の通風制限体10を通過して回転中の測定セル1に吹き
付けられる。The width of −1·, 10n becomes wider as the distance from the rotation center axis C of the rotary disk 2 increases. Therefore, the further away from the axis C, that is, the more the cold air from the electronic cooling device 11 passes through the ventilation restricting body 10 and is blown onto the rotating measuring cell 1.
以上の本発明実施例において、マイクロコンピュータ8
から任意の回転数設定信号を与えてモータ3を回転させ
ると、その回転数に応じた温度の冷気が回転中の測定セ
ル1に吹き付けられ、回転数の大小に拘らず常に測定セ
ル1の温度上昇が阻止される。また、測定セル1には、
回転中心から遠去かるほど、つまり空気との摩擦による
発熱量の多い箇所はど、多量の冷気が吹き付けられるこ
とになり、内部での温度勾配も生じない。In the above embodiments of the present invention, the microcomputer 8
When the motor 3 is rotated by giving an arbitrary rotational speed setting signal from Rising is prevented. In addition, in the measurement cell 1,
The further away from the center of rotation, in other words, the areas where more heat is generated due to friction with the air, the more cold air will be blown into the area, and no temperature gradient will occur inside.
なお、通風制限体10は以上の実施例に限定されること
なく、例えば第3図にその正面図を示すように、回転中
心軸Cを中心とする複数の円弧状の開口部30a、30
b、−−−,30nを形成してもよく、むしろこの場合
の方が測定セル1に対してより理想的な分布で冷気の吹
き付けが可能となる。あるいは、各開口部の幅をそれぞ
れ同一とし、その配置を、回転中心軸Cから遠去かるほ
ど密にすることによっても、同様の効果が得られる。Note that the ventilation restricting body 10 is not limited to the above-mentioned embodiments, and for example, as shown in the front view in FIG.
b, ---, 30n may be formed; rather, in this case, cold air can be blown onto the measuring cell 1 with a more ideal distribution. Alternatively, the same effect can be obtained by making the widths of the openings the same and making the arrangement denser as the distance from the rotation center axis C increases.
また、冷却制御回路12において、ルック−アップテー
ブル12aに代えて、D−A変換器12bの出力側に折
線近似関数発生回路を設けてもよいことは勿論である。Furthermore, in the cooling control circuit 12, it goes without saying that a broken line approximation function generation circuit may be provided on the output side of the DA converter 12b in place of the look-up table 12a.
〈発明の効果〉
以上説明したように、本発明によれば、回転中の測定セ
ルに冷気を吹き付け得る電子冷却装置を設け、この電子
冷却装置への給電量を、測定セルの回転数に応じて変化
させるとともに、電子冷却装置の冷気吐出口と回転中の
測定セルとの間には、回転中心軸から遠去かるほど冷気
の通過量が増大する通風制限体を設けたので、測定セル
はその回転数の大小に拘らず、常にその温度上昇が阻止
され、しかも、測定セルには発熱の大きい箇所はど多量
の冷気が吹き付けられるから、内部での温度勾配が生じ
にくい。その結果、測定セル内で懸濁液に対流が生じず
、常に正確な粒度分布測定結果を得ることができる。<Effects of the Invention> As explained above, according to the present invention, an electronic cooling device capable of blowing cold air onto a rotating measuring cell is provided, and the amount of power supplied to the electronic cooling device is controlled according to the rotational speed of the measuring cell. In addition, a ventilation restrictor was installed between the cold air discharge port of the electronic cooling device and the rotating measurement cell, so that the amount of cold air passing through increases as the distance from the rotation center axis increases. Regardless of the number of rotations, the temperature rise is always prevented, and since a large amount of cold air is blown onto the measurement cell at locations where a large amount of heat is generated, it is difficult for a temperature gradient to occur inside the measurement cell. As a result, no convection occurs in the suspension within the measurement cell, making it possible to always obtain accurate particle size distribution measurement results.
第1図は本発明実施例の全体構成図で、第2図はその通
風制限体10の拡大斜視図である。
第3図は本発明の他の実施例の通風制限体の正面図であ
る。
1・・・測定セル
2・・・回転盤
3・・・モータ
4・・・光源
5・・・受光素子
8・・・マイクロコンピュータ
9・・・モータ制御器
10・・・通風制限体
10a、10b、−−,10n−・−開口部11・・・
電子冷却装置
12・・・冷却制御回路
12a・・・ルック−アップテーブル
12b・・・D−A変換器
12c・・・電流制御器FIG. 1 is an overall configuration diagram of an embodiment of the present invention, and FIG. 2 is an enlarged perspective view of a ventilation restricting body 10 thereof. FIG. 3 is a front view of a ventilation restrictor according to another embodiment of the present invention. 1...Measuring cell 2...Rotary disk 3...Motor 4...Light source 5...Light receiving element 8...Microcomputer 9...Motor controller 10...Ventilation restricting body 10a, 10b, --, 10n--Opening portion 11...
Electronic cooling device 12...Cooling control circuit 12a...Look-up table 12b...DA converter 12c...Current controller
Claims (1)
に収容し、その測定セルを回転盤に装着して回転を与え
、その回転中心軸から所定距離の位置における上記測定
セル内の懸濁液の経時的濃度変化を測定することにより
、試料粒体の粒度分布を求める装置において、回転中の
上記測定セルに冷気を吹き付け得る電子冷却装置と、上
記回転盤の回転数に応じて上記電子冷却装置への給電量
を変化させる冷却制御回路と、上記電子冷却装置の冷気
吐出口と上記測定セルの回転軌跡との間に介在し、上記
回転中心軸から遠去かるほど上記冷気の通過量が大きく
なるような複数の開口部を有してなる通風制限体を備え
たことを特徴とする、遠心沈降式粒度分布測定装置。A suspension obtained by dispersing sample particles in a medium is housed in a measuring cell, and the measuring cell is mounted on a rotary disk to give it rotation, and the measuring cell is placed at a position a predetermined distance from the central axis of rotation. In this device, the particle size distribution of the sample particles is determined by measuring the concentration change over time of the suspension in the cell. A cooling control circuit that changes the amount of power supplied to the electronic cooling device accordingly, and a cooling control circuit that is interposed between the cold air discharge port of the electronic cooling device and the rotation locus of the measurement cell, and the circuit that changes the amount of power supplied to the electronic cooling device according to the A centrifugal sedimentation type particle size distribution measuring device characterized by comprising a ventilation restricting body having a plurality of openings that allow a large amount of cold air to pass through.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP11422587A JPS63279143A (en) | 1987-05-11 | 1987-05-11 | Decanter type particle size distribution measuring apparatus |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP11422587A JPS63279143A (en) | 1987-05-11 | 1987-05-11 | Decanter type particle size distribution measuring apparatus |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS63279143A true JPS63279143A (en) | 1988-11-16 |
Family
ID=14632369
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP11422587A Pending JPS63279143A (en) | 1987-05-11 | 1987-05-11 | Decanter type particle size distribution measuring apparatus |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS63279143A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2020090776A1 (en) * | 2018-10-31 | 2020-05-07 | 株式会社堀場製作所 | Centrifugal sedimentation type particle size distribution measuring device |
-
1987
- 1987-05-11 JP JP11422587A patent/JPS63279143A/en active Pending
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2020090776A1 (en) * | 2018-10-31 | 2020-05-07 | 株式会社堀場製作所 | Centrifugal sedimentation type particle size distribution measuring device |
JPWO2020090776A1 (en) * | 2018-10-31 | 2021-09-24 | 株式会社堀場製作所 | Centrifugal sedimentation type particle size distribution measuring device |
US11499905B2 (en) | 2018-10-31 | 2022-11-15 | Horiba, Ltd. | Centrifugal sedimentation type particle size distribution measuring device |
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