JPH0746075B2 - Particle size distribution measuring device - Google Patents
Particle size distribution measuring deviceInfo
- Publication number
- JPH0746075B2 JPH0746075B2 JP61076274A JP7627486A JPH0746075B2 JP H0746075 B2 JPH0746075 B2 JP H0746075B2 JP 61076274 A JP61076274 A JP 61076274A JP 7627486 A JP7627486 A JP 7627486A JP H0746075 B2 JPH0746075 B2 JP H0746075B2
- Authority
- JP
- Japan
- Prior art keywords
- particle size
- size distribution
- particles
- sedimentation
- particle
- 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
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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
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- Chemical & Material Sciences (AREA)
- Dispersion Chemistry (AREA)
- Physics & Mathematics (AREA)
- Health & Medical Sciences (AREA)
- Life Sciences & Earth Sciences (AREA)
- Analytical Chemistry (AREA)
- Biochemistry (AREA)
- General Health & Medical Sciences (AREA)
- General Physics & Mathematics (AREA)
- Immunology (AREA)
- Pathology (AREA)
- Length Measuring Devices By Optical Means (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〉 本発明は粒度分布測定装置に関し、更に詳しくは、沈降
法を用いた粒度分布測定装置に関する。TECHNICAL FIELD The present invention relates to a particle size distribution measuring device, and more particularly to a particle size distribution measuring device using a sedimentation method.
〈発明の背景〉 一般に、粒子の大きさを表現するうえで最も問題となる
のは、粒子の形状が複雑で、球や立方体,円板,角柱と
いうように規則的ではないということである。このこと
に起因して、粒度の測定法の原理の相違により、得られ
る粒子径の意味が違ってくる。<Background of the Invention> Generally, the biggest problem in expressing the size of a particle is that the shape of the particle is complicated and is not regular such as a sphere, a cube, a disk, or a prism. Due to this, the meaning of the obtained particle size differs due to the difference in the principle of the particle size measuring method.
沈降法を応用した粒度測定法では、後述するように、
「測定に用いられる任意の媒質中を沈降する測定対象粒
子と同一密度で同一の沈降速度を有する球の直径に等し
い粒子径」という定義に基づいた、ストークス径と称す
る粒子径を測定することになる。すなわち、沈降法によ
り測定された粒子径は、試料粒子の形状は球と仮定され
たものであり、この形状の相違については考慮されてい
ない。In the particle size measurement method applying the sedimentation method, as described later,
To measure the particle diameter called Stokes diameter based on the definition "particle diameter equal to the diameter of a sphere having the same density and the same settling velocity as the particles to be measured settling in an arbitrary medium used for measurement". Become. That is, in the particle size measured by the sedimentation method, the shape of the sample particles is assumed to be a sphere, and the difference in this shape is not taken into consideration.
一方、粒子の投影像を基に長径、短径、面積などを測定
する顕微鏡法や、粒子の最大幅と最大暑さかフィルタの
目開きより小さければ通過することを利用したフルイ分
け法、あるいは流れの方向に長軸を沿わせた状態で円筒
体相当径を測定する細孔通過法等の測定法では、粒度分
布測定結果は粒子の形状による影響を大きく受ける。On the other hand, a microscope method that measures the major axis, minor axis, area, etc. based on the projected image of particles, a screening method that uses passage if the maximum width and maximum temperature of particles are smaller than the opening of the filter, or flow In a measurement method such as a pore passing method in which the major axis diameter is measured with the long axis along the direction of, the particle size distribution measurement result is greatly affected by the particle shape.
従って、沈降法で得られた測定結果を他の原理で測定さ
れた結果と比較すると、一致しないという問題が生ず
る。Therefore, when the measurement result obtained by the sedimentation method is compared with the result measured by another principle, there is a problem that they do not match.
本発明はこのような問題を解決するためになされたもの
で、沈降法を測定原理としているにも係わらず、得られ
る粒度分布測定結果に粒子形状の相違を反映したものと
することができ、もって他の原理に基づく測定装置で得
られる測定結果とより一致した測定結果を得ることので
きる粒度分布測定装置の提供を目的としている。The present invention has been made to solve such a problem, and despite the sedimentation method as the measurement principle, it is possible to reflect the difference in particle shape in the obtained particle size distribution measurement result, Therefore, it is an object of the present invention to provide a particle size distribution measuring device that can obtain a measurement result that is more consistent with the measurement result obtained by a measuring device based on another principle.
〈発明の原理〉 沈降法による粒子径の測定に当っては、以下に示すスト
ークスの式(10)が用いられる。<Principle of the Invention> In measuring the particle size by the sedimentation method, the Stokes equation (10) shown below is used.
任意の媒質中に浮遊している1個の粒子の沈降運動につ
いて考えると、粒子は重力と、媒質から受ける浮力の差
によって重量方向に沈降運動を行うが、一方では、この
運動のために媒質から逆方向の抵抗力Rの作用を受け、
その運動方程式は次のように表わされる。Considering the sedimentation motion of a single particle suspended in an arbitrary medium, the particle undergoes a sedimentation motion in the weight direction due to the difference between gravity and the buoyancy received from the medium. Receives a resistance force R in the opposite direction from
The equation of motion is expressed as follows.
ここで、uは粒子の沈降速度(cm/s),tは時間(S),m
は粒子の質量(g),m′は質量mが受ける浮力(g),g
は重力の加速度(cm/s2),Rは流体の抵抗力,Cは抵抗係
数,Aは粒子の運動方向に直角な粒子の投影面積(c
m2),ρは流体の密度(g/cm3)である。 Where u is the sedimentation velocity of the particles (cm / s), t is the time (S), m
Is the mass of the particle (g), m'is the buoyancy (g), g
Is the acceleration of gravity (cm / s 2 ), R is the resistance force of the fluid, C is the resistance coefficient, and A is the projected area of the particle (c
m 2 ) and ρ are fluid densities (g / cm 3 ).
(1),(2)よりρpを粒子の密度(g/cm3)とする
と、 粒子を球形とすれば、その直径をDp(cm)とすると、 であるから、(3)式は、 と変形される。これより、 で表わされる。From (1) and (2), let ρ p be the particle density (g / cm 3 ). If the particles are spherical and their diameter is D p (cm), Therefore, equation (3) is Will be transformed. Than this, It is represented by.
粒度測定において対象とされるのは、粒子に作用する抵
抗力がストークスの抵抗則に従う範囲であって、この範
囲において抵抗係数Cは、μを流体の粘性係数(g/cm・
s)とすると、 なお、ここでReはレイノルズ数で、 で表わされる。The target in particle size measurement is the range in which the resistance force acting on the particles complies with Stokes's law of resistance. In this range, the resistance coefficient C is μ as the viscosity coefficient of fluid (g / cm ·
s), Here, Re is the Reynolds number, It is represented by.
(7),(8)から、 これが粒子の沈降に関するストークスの式で、沈降法に
よる粒度測定の基本式である。From (7) and (8), This is the Stokes equation for the sedimentation of particles, which is the basic equation for particle size measurement by the sedimentation method.
実際の粒度測定においては、粒子が時間tの間に距離h
を沈降したとすると、 u=h/t 11) として、(10),(11)から、 によって粒子径DPを算出する。In the actual particle size measurement, the particles are separated by the distance h during the time t.
Is settled, u = h / t 11), and from (10) and (11), The particle size D P is calculated by
ここで算出された粒子径DPは、以上の説明より明らかな
ように、前述した如く、「測定に用いられる任意の媒質
中を沈降する、測定対象粒子と同一密度で同一の沈降速
度を有する球の直径に等しい粒子径」ということにな
り、これをストークス径と称している。As is clear from the above description, the particle diameter D P calculated here is, as described above, “settling in any medium used for measurement, having the same density and the same sedimentation velocity as the particles to be measured. The particle diameter is equal to the diameter of the sphere ", which is called the Stokes diameter.
以上のことから明らかなように、ストークスの式によれ
ば、粒子を球形と仮定してその沈降運動を説明するもの
で、粒子形状の相違についての考慮がなされていない。
これを考慮に入れてより現実に即した粒度を求めるため
には(10)式における終末速度umを、測定すべき粒子の
実際の終末速度に置換してやる必要が生ずる。すなわ
ち、ストークスの式における終末速度をum、実際の速度
(あるいは補正後の終末速度)をumcとしたとき、 なる補正係数によってストークスの式における終末速度
umを補正することにより、沈降法による粒度の測定結果
をより実態に即した値とすることができる。As is clear from the above, according to the Stokes equation, the sedimentation motion is explained assuming that the particles are spherical, and the difference in particle shape is not taken into consideration.
Taking this into consideration, in order to obtain a more realistic particle size, it is necessary to replace the terminal velocity u m in equation (10) with the actual terminal velocity of the particles to be measured. That is, when the terminal velocity in the Stokes equation is u m and the actual velocity (or corrected terminal velocity) is u mc , The final velocity in the Stokes equation by
By correcting u m , it is possible to make the measurement result of the particle size by the sedimentation method more realistic.
上述の補正の仕方については、主に実験結果に基づいて
種々の提案がなされているが、例えばPettyjohnらは、
粒子の球形度Ψをパラメータとして、 を導いている。球形度Ψは、 で定義され、規則的形状の粒子を例にとると、立方体0.
806,正四面体0.671,円柱(直径と高さが等しい)0.877
等の値を採る。Regarding the above correction method, various proposals have been mainly made based on experimental results, but Pettyjohn et al.
With the sphericity Ψ of the particle as a parameter, Is leading. The sphericity Ψ is For example, a regular shaped particle is defined as a cube 0.
806, regular tetrahedron 0.671, cylinder (equal in diameter and height) 0.877
Take the values such as.
また、Heywoodは、非球形粒子の終末速度の計算を平均
等影径DHと、Heywoodの体積形状係数k′を用いて行っ
ている。すなわち、粒子体積を k′DH3 ……(16) で定義し、k′を実験的に求め得る場合についてその沈
降速度の算出法を示している。この方法では、 の右辺を計算してCRe2を算出し、球形粒子についてのRe
とCの既知の関係からReを求めて、更に、 と前述のk′の値から、実験により求められているlogR
e補正値を割り出して、先に求められているReを補正
し、その補正後のReを用いて(9)式における沈降法速
度uを計算する。Heywood also calculates the terminal velocity of non-spherical particles by using the average equi-shadow diameter D H and Heywood's volumetric shape factor k ′. That is, the particle volume is defined by k'D H3 (16), and the method of calculating the sedimentation velocity is shown when k'can be experimentally obtained. in this way, On the right side and by calculating calculates the CRe 2, Re of the spherical particles
Re is obtained from the known relationship between C and C, and And the logR obtained by experiment from the above k'value
The e correction value is calculated, the previously obtained Re is corrected, and the corrected method Re is used to calculate the sedimentation method velocity u in equation (9).
〈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> An example of the present invention will be described below with reference to the drawings.
第1図は本発明実施例の構成を示すブロック図である。FIG. 1 is a block diagram showing the configuration of the embodiment of the present invention.
この実施例は、光透過法を応用した遠心沈降式粒度分布
測定装置に本発明を適用した場合を示している。This example shows a case where the present invention is applied to a centrifugal sedimentation type particle size distribution measuring apparatus to which a light transmission method is applied.
測定すべき試粒粒子wは、媒溶液中に均一に分散させて
懸濁液の状態として試料セル1内に収容される。この試
料セル1は回転円盤2に固着され、モータ3によって回
転が与えられる。この回転による遠心力場において、粒
子の沈降が促進され、測定時間が短縮化される。The sample particles w to be measured are uniformly dispersed in the medium solution and are accommodated in the sample cell 1 as a suspension. The sample cell 1 is fixed to a rotating disc 2 and is rotated by a motor 3. In the centrifugal force field due to this rotation, the sedimentation of particles is promoted and the measurement time is shortened.
粒子の沈降による懸濁液の濃度変化は、回転円盤2の回
転中心から一定距離に設けられた光源4と受光素子5と
で構成された光学系によって測定される。すなわち、こ
の光学系の光軸中心に試料セル1が到来したときに、回
転位置検出器6からの出力信号によってスイッチ7を閉
じる。このスイッチ7の閉成時における受光素子5の出
力信号は、懸濁液の吸光度を表わす信号となって、懸濁
液濃度の検出値として増幅器8,A−D変換器9を介して
演算制御部10に採り込まれる。The change in the concentration of the suspension due to the settling of the particles is measured by an optical system composed of a light source 4 and a light receiving element 5 provided at a fixed distance from the center of rotation of the rotating disk 2. That is, when the sample cell 1 arrives at the center of the optical axis of this optical system, the switch 7 is closed by the output signal from the rotational position detector 6. The output signal of the light receiving element 5 when the switch 7 is closed becomes a signal representing the absorbance of the suspension, and is arithmetically controlled via the amplifier 8 and the AD converter 9 as the detection value of the suspension concentration. Adopted in Part 10.
演算制御部10は、CPU11,ROM12,RAM13等からなるマイク
ロコンピータを主体として構成されており、キーボード
14,CRT15およびプリンタ16のほかに、上述したモータ3
をCPU11からの指令に基づいて制御するインバータ17、
および、シリアルインターフェース24を介して解析演算
部23が接続されている。The arithmetic and control unit 10 is mainly composed of a micro computer composed of a CPU 11, a ROM 12, a RAM 13, etc.
In addition to the 14, CRT 15 and printer 16, the motor 3 described above
An inverter 17, which controls the CPU based on a command from the CPU 11,
Also, the analysis calculation unit 23 is connected via the serial interface 24.
解析演算部23(例えば、商品名;島津ボッシュロム画像
解析装置オムニコンFAS−II)は、顕微鏡21に装着され
たTVカメラ22からの撮像信号を画像データとして取り込
み、その画像データに基づいて試料粒子の球形度Ψを決
定することができる。すなわち、顕微鏡21の視野下に試
料粒子を置いてTVカメラ22によって撮像することによ
り、解析演算部23はその撮像信号から試料粒子の幾何学
的情報を得て粒子形状を認識するとともに、その認識結
果に基づいて試料粒子の球形度Ψを決定する。この球形
度Ψの決定は、試料粒子を試料セル1内に収容して遠心
沈降させる前に行われ、このようにして決定された球形
度Ψは、シリアルインターフェース22を介して演算制御
部10に供給される。The analysis / calculation unit 23 (for example, trade name; Shimadzu Bosch Lom image analysis device Omnicon FAS-II) takes in an image pickup signal from the TV camera 22 attached to the microscope 21 as image data, and based on the image data, The sphericity Ψ can be determined. That is, by placing the sample particles under the field of view of the microscope 21 and capturing the image with the TV camera 22, the analysis calculation section 23 obtains the geometric information of the sample particles from the image pickup signal and recognizes the particle shape, and the recognition thereof. The sphericity Ψ of the sample particle is determined based on the result. The determination of the sphericity Ψ is performed before the sample particles are accommodated in the sample cell 1 and subjected to centrifugal sedimentation, and the sphericity Ψ thus determined is sent to the arithmetic control unit 10 via the serial interface 22. Supplied.
ROM12には、試料セル1内の懸濁液の濃度の時系列的検
出値から、前述したストークスの式に基づいて試料粒子
の粒度分布を算出する測定プログラムが書き込まれてい
るが、ここで、ストークスの式における終末速度umに
は、例えば前述したPettyjohnらによる、(13),(1
4)式を用いた補正が加えられる。この(14)式におけ
る球形度Ψは、沈降測定前に前記した解析演算部23から
供給されたものを用いる。A measurement program for calculating the particle size distribution of the sample particles based on the above-described Stokes equation from the time-series detection value of the concentration of the suspension in the sample cell 1 is written in the ROM 12, but here, The terminal velocity u m in the Stokes equation is calculated by Pettyjohn et al. (13), (1
Correction using equation 4) is added. As the sphericity Ψ in the equation (14), the sphericity Ψ supplied from the above-described analysis calculation unit 23 before the sedimentation measurement is used.
これにより、求められた粒度分布は、試料粒子の形状が
考慮された値となる。As a result, the obtained particle size distribution takes into consideration the shape of the sample particles.
なお、その他の測定条件等は、CRT15との対話形式によ
ってキーボード14から入力しておく。また、大部分の粒
子が沈降すれば、測定を終了して測定条件および測定結
果がプリンタ16に打出される。Note that other measurement conditions and the like are input from the keyboard 14 in an interactive form with the CRT 15. If most of the particles settle down, the measurement is terminated and the measurement conditions and the measurement results are output to the printer 16.
また、終末速度umの補正は、Pettyjohnらの方法によら
ず、Heywoodの方法によってもよいし、更に、他の方法
を用いることもできる。Further, the correction of the terminal velocity u m may be performed by the Heywood method instead of the Pettyjohn et al. Method, or another method may be used.
更にまた、本発明は沈降法による粒度分布測定装置に普
遍的に適用し得るもので、遠心沈降法以外に自然沈降法
による測定装置にも適用するこができ、また、濃度検出
は光透過法に限られないことは勿論である。Furthermore, the present invention can be universally applied to a particle size distribution measuring device by a sedimentation method, and can be applied to a measuring device by a natural sedimentation method in addition to the centrifugal sedimentation method, and the concentration can be detected by a light transmission method. Of course, it is not limited to.
〈発明の効果〉 以上説明したように、本発明によれば、試料粒子を撮像
する撮像手段と、その撮像手段からの画像データを取り
込んで当該試料粒子の形状に係るデータを出力する画像
解析手段と、その画像解析手段からのデータを用いてス
トークスの式による粒度分布の算出過程で沈降速度の補
正を行う補正演算手段を設けて、ストークスの式におけ
る沈降の終末速度を補正して粒度を求めるよう構成した
ので、試料粒子の形状の相違を反映した、つまり粒子形
状の実態により即した粒度分布測定結果を直接的に得る
ことができる。その結果、本発明の沈降法を用いた粒度
分布測定装置による測定結果は、例えば顕微鏡法、フル
イ分け法、あるいは細孔通過法等の、粒子形状の影響を
受けやすい他の測定法による測定結果と直接比較するこ
とが可能となり、ひいては沈降法に基づく測定結果の特
殊性を緩和して、より普遍的なものとすることができ
る。<Effects of the Invention> As described above, according to the present invention, an image capturing unit for capturing an image of a sample particle, and an image analyzing unit for capturing image data from the image capturing unit and outputting data relating to the shape of the sample particle. And a correction calculation means for correcting the sedimentation velocity in the process of calculating the particle size distribution by the Stokes equation using the data from the image analysis means, and correcting the terminal velocity of sedimentation in the Stokes equation to obtain the particle size. With this configuration, it is possible to directly obtain the particle size distribution measurement result that reflects the difference in the shape of the sample particles, that is, more suitable for the actual state of the particle shape. As a result, the measurement result by the particle size distribution measuring apparatus using the sedimentation method of the present invention is, for example, the microscopic method, the screening method, or the pore passing method, and the measurement results by other measurement methods susceptible to the particle shape. It becomes possible to directly compare with, and it is possible to relax the peculiarity of the measurement result based on the sedimentation method and make it more universal.
また、逆に、他の方法によるデータに一致するよう、粒
子の形状に係るデータの入力値を決定することによっ
て、沈降法と他の方法との相関を求める等の応用に供す
ることもできる。On the contrary, by determining the input value of the data relating to the shape of the particles so as to match the data obtained by another method, it can be applied to applications such as obtaining the correlation between the sedimentation method and another method.
第1図は本発明実施例の構成を示すブロック図である。 1……試料セル 2……回転円盤 4……光源 5……受光素子 10……演算制御部 11……CPU 12……ROM 13……RAM 21……顕微鏡 22……TVカメラ 23……解析演算部 24……シリアルインターフェース FIG. 1 is a block diagram showing the configuration of the embodiment of the present invention. 1 …… Sample cell 2 …… Rotating disk 4 …… Light source 5 …… Light receiving element 10 …… Computer control unit 11 …… CPU 12 …… ROM 13 …… RAM 21 …… Microscope 22 …… TV camera 23 …… Analysis Arithmetic unit 24 …… Serial interface
Claims (1)
液を収容する試料容器と、その試料容器内で試料粒子が
沈降することによって生ずる上記懸濁液の濃度変化を検
出する検出手段と、その濃度変化の検出信号からストー
クスの式を用いて試料粒子の粒度分布を算出する算出手
段を有する装置において、試料粒子を撮像する撮像手段
と、その撮像手段からの画像データを取り込んで当該試
料粒子の形状に係るデータを出力する画像解析手段と、
その画像解析手段からのデータを用いて上記ストークス
の式による粒度分布の算出過程で沈降速度の補正を行う
補正演算手段を備えたことを特徴とする、粒度分布測定
装置。1. A sample container for holding a suspension in which sample particles are dispersed in a medium solution, and detection for detecting a change in the concentration of the suspension caused by sedimentation of the sample particles in the sample container. In the device having a means and a calculating means for calculating the particle size distribution of the sample particles by using the Stokes equation from the detection signal of the concentration change, an imaging means for imaging the sample particles and the image data from the imaging means are captured. Image analysis means for outputting data relating to the shape of the sample particles,
A particle size distribution measuring device comprising a correction calculation means for correcting the sedimentation velocity in the process of calculating the particle size distribution by the Stokes equation using the data from the image analysis means.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61076274A JPH0746075B2 (en) | 1986-03-31 | 1986-03-31 | Particle size distribution measuring device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61076274A JPH0746075B2 (en) | 1986-03-31 | 1986-03-31 | Particle size distribution measuring device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS62231140A JPS62231140A (en) | 1987-10-09 |
| JPH0746075B2 true JPH0746075B2 (en) | 1995-05-17 |
Family
ID=13600674
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP61076274A Expired - Lifetime JPH0746075B2 (en) | 1986-03-31 | 1986-03-31 | Particle size distribution measuring device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0746075B2 (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| KR100947716B1 (en) * | 2008-03-28 | 2010-03-16 | 광주과학기술원 | Detection method of bacterial contamination of bioethanol |
Families Citing this family (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP7303066B2 (en) * | 2019-08-26 | 2023-07-04 | 株式会社東芝 | Physical property measuring device |
| CN115165687B (en) * | 2022-07-14 | 2024-06-21 | 西北核技术研究所 | A device and method for testing the dry settling velocity of micron-sized solid particles |
| CN116429226B (en) * | 2023-05-24 | 2025-12-12 | 上海平奥供应链管理有限公司 | Methods, devices, and storage media for detecting the coal load capacity of railway freight cars |
| CN120084591B (en) * | 2025-02-27 | 2026-01-09 | 自然资源部第二海洋研究所 | Underwater biological particle parameter acquisition device and acquisition method based on image |
-
1986
- 1986-03-31 JP JP61076274A patent/JPH0746075B2/en not_active Expired - Lifetime
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| KR100947716B1 (en) * | 2008-03-28 | 2010-03-16 | 광주과학기술원 | Detection method of bacterial contamination of bioethanol |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS62231140A (en) | 1987-10-09 |
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