WO2021235169A1 - Number based particle diameter distribution measurement method and measurement system - Google Patents

Number based particle diameter distribution measurement method and measurement system Download PDF

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WO2021235169A1
WO2021235169A1 PCT/JP2021/016368 JP2021016368W WO2021235169A1 WO 2021235169 A1 WO2021235169 A1 WO 2021235169A1 JP 2021016368 W JP2021016368 W JP 2021016368W WO 2021235169 A1 WO2021235169 A1 WO 2021235169A1
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particle size
fine particles
dispersion medium
size distribution
flow
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Japanese (ja)
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晴久 加藤
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国立研究開発法人産業技術総合研究所
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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N15/00Investigating characteristics of particles; Investigating permeability, pore-volume or surface-area of porous materials
    • G01N15/02Investigating particle size or size distribution

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  • the present invention relates to a number-based particle size distribution measurement method and measurement system for fine particles in a dispersion medium, and in particular, a number-based particle size distribution for particles having a wide particle size distribution from nanometer size to micrometer size. Regarding measuring methods and measuring systems.
  • the particle size distribution is measured from the particle size and the number concentration by using a classification method such as the FFF (Field Flow Fractionation) method.
  • FFF Field Flow Fractionation
  • Non-Patent Document 1 after size classification by the FFF method, the particle size and the light scattering intensity concentration are calculated by an online multi-angle scattering measuring device, and the light scattering intensity concentration is converted into a number concentration according to the theory of Mie scattering. It discloses that the particle size distribution based on the number is calculated.
  • the particle size distribution and number concentration of each fraction are calculated by a scanning electron microscope, and the results are reconstructed to obtain a number-based particle size distribution. The method of measurement is also disclosed. Further, a method of measuring the particle size distribution based on the number of particles by evaluating all of them with a scanning electron microscope is also disclosed.
  • Non-Patent Document 2 a Stop-flow mode particle tracking analysis (PTA) device is connected to the subsequent stage of the FFF method, and the particle size distribution and the number concentration are measured for each fraction. Discloses a method for obtaining a particle size distribution based on the number of particles by reconstructing. Further, Non-Patent Document 3 and Patent Document 1 disclose a number-based particle size measuring method by a flow field particle tracking (FPT) method.
  • FPT flow field particle tracking
  • the scattering theory of Rayleigh scattering or Mie scattering is applied if the refractive index of the particles is not known in the conversion from the measured light scattering intensity to the number concentration. It is not possible to calculate the particle size distribution based on the number.
  • the particle size distribution based on the number can be calculated even if the refractive index of the particles is unknown.
  • the particles are individually measured with a scanning electron microscope, rapid measurement is not possible.
  • the particle size distribution based on the number can be calculated quickly and easily, but in the FPT method in which the particle size is measured from the scattered light intensity from the particles, the scattered light intensity is the particle size.
  • the present invention has been made in view of the above circumstances, and quickly and easily measures the particle size distribution based on the number of particles having a distribution in a wide particle size range from nanometer size to micrometer size. It seeks to provide possible methods and measurement systems.
  • the particle size distribution measuring method irradiates fine particles that move brown in a dispersion medium with laser light, and images bright spots due to scattered light at predetermined time intervals. It is a method of measuring the particle size and the number of fine particles and measuring the particle size distribution based on the number of fine particles by forming a flow field in the dispersion medium for the fine particles diffusing in the dispersion medium.
  • a classification step of arranging particles in the dispersion medium according to the particle size and classifying the particles, and an imaging step of irradiating the dispersion medium containing the classified fine particles with the laser beam to obtain the image are included.
  • the dispersion medium Prior to the imaging step, the dispersion medium is divided so as to include the fine particles in a predetermined particle size range, and the number concentration is adjusted without changing the number of the fine particles in each of the divided dispersion media. It is characterized by including an adjustment step to be performed.
  • the moving locus of the bright spot of the image obtained by irradiating the fine particles that move brown in the dispersion medium with laser light and imaging the bright spot by the scattered light at predetermined time intervals. It is a system that measures the particle size and the number of the fine particles and measures the particle size distribution based on the number of the fine particles, and forms a flow field in the dispersion medium for the fine particles diffusing in the dispersion medium.
  • the classification device in which the fine particles are arranged in the dispersion medium according to the particle size and classified, and the dispersion medium containing the classified fine particles are guided from the classification device to a cell and irradiated with the laser beam.
  • the dispersion medium is divided between the classification device and the cell so as to include the fine particles in a predetermined particle size range, including an image pickup device for obtaining an image, and in each of the divided dispersion media. It is characterized by including a concentration adjusting device for adjusting the number concentration without changing the number of the fine particles.
  • an image can be obtained under conditions suitable for each of the divided dispersion media in the imaging with the imaging device, and the number of particles having a distribution in a wide particle size range from nanometer size to micrometer size.
  • the particle size distribution based on the standard can be measured quickly and easily.
  • the density adjusting device and the adjusting step performed here adjust the particle size range so that bright spots due to scattered light can be obtained for the fine particles imaged in the imaging step. It may be a feature. According to such a feature, it is not necessary to expand or switch the dynamic range of the image pickup apparatus in response to the scattered light intensity which is non-linear with respect to the particle size, and the measurement can be performed quickly and easily.
  • the number concentration may be adjusted by adding or separating the dispersion medium in each of the divided dispersion media. According to such a feature, the number concentration can be adjusted by a simple method, and the rapid measurement of the particle size distribution on the basis of the number can be simplified.
  • the flow field is obtained by adding a flow in a liquid feeding direction along the flow path and a flow in a direction substantially perpendicular to the flow field, and the fine particles are arranged so as to intersect the liquid feeding direction.
  • the flow field is obtained by applying a centrifugal force in a liquid feeding direction along a flow path and a direction substantially perpendicular to the flow field so as to intersect the fine particles in the liquid feeding direction. It may be characterized by arranging them. According to such a feature, the classification by the particle size in the classification device and the classification step performed here can be easily performed.
  • FIG. 1 It is a block diagram which shows an example of the apparatus composition used for the measuring method of the particle size distribution of this invention. It is explanatory drawing about the principle of flow FFF. It is explanatory drawing about the principle of centrifugal FFF.
  • the particle size distribution measurement system used in the particle size distribution evaluation method includes a classification device 1, a connection unit 2, and a flow field particle tracking (FPT:) by a flow field separation method (FFF: Field Flow Fractionation). It is equipped with a measuring device 3 and an arithmetic processing device 4 by the Flow particle Tracking method.
  • FPT flow field particle tracking
  • FFF Field Flow Fractionation
  • the classification device 1 includes an eluent introduction unit 11 for introducing a dispersion medium, and a sample introduction unit 12 for injecting a dispersion liquid in which fine particles that move in Brownian motion in the dispersion medium are dispersed in the dispersion medium into a flow path continuing from the eluent introduction unit. And an FFF device 13 for classifying fine particles according to particle size.
  • a flow FFF device 14 see FIG. 2
  • a centrifugal FFF device 15 see FIG. 3
  • the flow FFF device 14 has a liquid feeding direction along a flow path from the inflow port 16 to the outflow port 18, and is provided with a microfiltration membrane 19 provided on one side wall of the flow path.
  • the flow 50 in the direction substantially perpendicular to the liquid feeding direction by the dispersion medium 17 can be formed as a crossing force field. Due to the flow 50 orthogonal to the liquid feeding direction, the fine particles 51 once collected at one place on the surface of the microfiltration membrane 19 diffuse from the microfiltration membrane 19 toward the center of the flow path to the particle diameter. It is classified according to the difference in diffusion rate based on it.
  • the particles are arranged in a direction intersecting the liquid feeding direction so that the particle size becomes smaller as the particle size approaches the center of the flow path. Further, in the laminar flow along the liquid feeding direction, since there is a velocity gradient that increases from the outer periphery of the flow path toward the center, the particles are classified by proceeding in the flow path in order from the fine particles 51 having a small particle size near the center of the flow path. The fractionation of the fine particles 51 is facilitated.
  • the centrifugal FFF device 15 has a liquid feeding direction along a flow path from the inlet 16 to the outlet 18, and the flow path is substantially perpendicular to the liquid feeding direction by the dispersion medium 17.
  • Centrifugal force 52 is applied as a crossing force field.
  • such a centrifugal force 52 can be applied by using a flow path having a curvature that curves the liquid feeding direction. Due to this centrifugal force 52, the fine particles 51 once collected at one place on the surface of the outer peripheral wall 19'diffuse from the outer peripheral wall 19' toward the center of the flow path, and the diffusion velocity and mass based on the particle diameter. It is classified according to the difference.
  • the particles are arranged in a direction intersecting the liquid feeding direction so that the particle size becomes smaller as the particle size approaches the center of the flow path. Further, in the laminar flow along the liquid feeding direction, since there is a velocity gradient that increases from the outer periphery of the flow path toward the center, the particles are classified by proceeding in the flow path in order from the fine particles 51 having a small particle size near the center of the flow path. The fractionation of the fine particles 51 is facilitated.
  • the classification device 1 is a mechanism capable of classifying fine particles having a wide range of particle sizes by the particle size and guiding them to the connection portion 2 by the flow field separation method.
  • the flow field separation method a method such as heat, magnetic field, electric field, etc. that gives other energy as a crossing force field can be appropriately selected according to the fine particles.
  • the connecting portion 2 is a mechanism that divides the dispersion medium into a plurality of particles so as to contain fine particles classified so as to contain fine particles in a predetermined particle size range, and guides each of them to the measuring device 3 in the subsequent stage.
  • the dispersion can be divided as described above by partitioning the time and amount until the dispersion liquid is derived from the classification device 1 at a predetermined value.
  • it is a concentration adjusting device that controls the amount of the dispersion medium for each of the divided dispersion liquids without changing the number of fine particles and leads to the measuring device 3 described later. Thereby, the number concentration of the fine particles 51 can be adjusted so that the measurement by the measuring device 3 can be easily performed.
  • the fine particles 51 are tracked as bright spots on the image, so that the bright spots are sufficiently separated from each other so that the individual bright spots can be accurately discriminated by image analysis.
  • the number concentration may be increased so that the density of bright spots on the image is not sparse and the time efficiency of measurement is not reduced. Therefore, the dispersion is diluted or concentrated so that the number concentration of the fine particles 51 is within a desired range.
  • the connecting portion 2 for example, in the FFF device 13, the dispersion medium 17 on the side opposite to the collected side of the fine particles 51 (on the tip side in the diffusion direction) is removed to increase the number concentration of the fine particles 51.
  • a split that leads to the measuring device 3 in the subsequent stage, or a syringe pump or a diaphragm pump that dilutes the dispersion liquid by adding a dispersion medium 17 to reduce the concentration of the number of fine particles 51 can be used.
  • the configuration of the connecting portion 2 can be appropriately selected according to the characteristics of the dispersion liquid consisting of the fine particles 51 to be classified and the dispersion medium 17 as a fluid.
  • the divided dispersion may be guided to different flow paths. In this case, each of the divided dispersion liquids may be provided with an optical cell of the measuring device 3 described later for each flow path.
  • the measuring device 3 described later when measuring the particle size by the flow field particle tracking method, conditions suitable for the range of the particle size of the fine particles 51 contained in each of the divided dispersions can be set, and the particles can be set. Makes it easy to measure the diameter.
  • the measuring device 3 is a device that measures the particle size of each particle of the fine particles 51 by the flow field particle tracking method and counts the number of the particles.
  • the measuring device 3 includes an image pickup device 31 capable of capturing the scattered light from the fine particles 51 and recording a bright spot corresponding to a single particle as an image, and fine particles classified and having their number densities adjusted. It includes a transparent optical cell 32 through which a dispersion medium 17 including 51 is circulated, and a laser light source 33 for irradiating a laser beam toward the fine particles 51 in the optical cell 32.
  • the image pickup device 31 captures an image in which pixels corresponding to elements of an image pickup device (CCD: Charge Coupled Device, CMOS image sensor, etc.) having a predetermined resolution are arranged in two dimensions via an optical system such as a lens, and uses the image data as image data. Output.
  • the image pickup apparatus 31 executes shooting at a predetermined exposure time and a predetermined time interval ⁇ t to continuously generate a plurality of images.
  • the exposure time is shorter than the time interval ⁇ t. For example, when the frame rate is 30 fps, the time interval ⁇ t is about 33 ms, and the exposure time is 30 ms.
  • the exposure time may be controlled by controlling the shutter speed or by illuminating the laser light source 33 in a pulsed manner. Further, the measuring device 3 adjusts the imaging conditions according to each of the divided dispersion liquids.
  • the arithmetic processing unit 4 has a built-in computer that executes a predetermined program, executes predetermined data processing according to the program, and operates as various processing units.
  • the arithmetic processing device 4 reconstructs the data analyzed by the image analysis unit 41, the particle size / number concentration analysis unit 43, and the particle size / number concentration analysis unit 43 to calculate the particle size distribution. It operates as a unit 44 and a control unit 45.
  • the arithmetic processing unit 4 includes a non-volatile storage device (flash memory, hard disk drive, etc.) as the storage unit 42.
  • the image analysis unit 41 controls the image pickup device 31, causes the image pickup device 31 to perform imaging in a predetermined range of the optical cell 32, and acquires image data of a plurality of images continuously generated by the image pickup device 31.
  • the image analysis unit 41 may appropriately change the exposure time and detection sensitivity of each captured image in the image pickup device 31 according to the particle size of the fine particles 51 classified in the classification device 1.
  • the particle size of the fine particles derived from the FFF device 13 may be theoretically calculated or actually measured by a simple monitor to set the optimum imaging conditions.
  • the image analysis unit 41 identifies the movement locus of the bright spot on the image based on the acquired image data by the flow field separation method, and obtains the displacement of the fine particles 51 corresponding to the bright spot. Then, kB is the Boltzmann constant, T is the absolute temperature, ⁇ is the viscosity coefficient of the dispersion medium, d is the particle diameter, and the squared average value of the displacement of the fine particles 51 is proportional to kBT / 3 ⁇ d, so that the particle diameter is calculated. .. Further, the image analysis unit 41 counts the number of bright spots that have passed through the predetermined region together with the calculation of the particle size to obtain the number of fine particles 51. As described above, in the flow field separation method, the number of bright spots is counted while tracking the bright spots corresponding to the individual fine particles 51, so that the number can be counted regardless of the material forming the fine particles 51.
  • the image analysis unit 41 uses a known method (method disclosed in Patent Document 1, fluid simulation, etc.) to determine the flow velocity distribution of the dispersion medium 17 in the image pickup region in the optical cell 32 corresponding to the angle of view of the image pickup device 31. It is preferable to specify in advance, correct the displacement of the fine particles 51 based on the flow velocity distribution of the dispersion medium 17, and specify the average square displacement ⁇ MS of the fine particles 51 based on the corrected displacement. That is, by correcting the displacement of the fine particles 51 based on the flow velocity distribution, the displacement of the fine particles 51 due to the Brownian motion is obtained after excluding the influence of the flow field of the dispersion medium 17.
  • the flow velocity distribution may be assumed to be constant (that is, the size and orientation are constant) within the imaging region.
  • the image analysis unit 41 counts the number of fine particles 51 passing through a predetermined region in the optical cell.
  • the particle size distribution based on the number of particles can be calculated.
  • the range of the intensity of scattered light from fine particles can be narrowed in the particle size measurement by the flow field particle tracking method, and the particle size to be easily classified. It is possible to count the number of each.
  • the classification device 1 and the measuring device 3 are connected via the connecting portion 2, it is possible to guide the dispersion liquid having a number concentration suitable for measurement to the measuring device 3, and each of the classified and fractionated dispersion liquids. You can measure the particle size and the number concentration online. Therefore, the particle size distribution based on the number can be measured quickly.
  • the particle size distribution based on the number can be measured quickly and easily.
  • the number concentration of the fine particles 51 in a plurality of outflow time ranges is calculated, and by reconstructing these, the number reference in the dispersion liquid of the injected fine particles can be obtained.
  • the particle size distribution can be calculated.

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Abstract

Provided are a method capable of promptly and easily measuring a particle diameter distribution based on the number of particles having a distribution within a wide particle diameter range from a nanometer size to a micrometer size, and a measurement system. Provided are a measurement method comprising emitting a laser beam over microparticles undergoing Brownian motion in a dispersion medium, imaging bright spots due to scattered light at certain time intervals, and, from a movement trajectory of the bright spots in a thus obtained image, measuring the particle diameter and number of microparticles so as to measure a number based particle diameter distribution, and a measurement system therefor. Microparticles dispersed in a dispersion medium are provided with a flow field in the dispersion medium, arranged, and classified in the dispersion medium in accordance with the particle diameter, and a laser beam is emitted over the dispersion medium containing the classified microparticles to obtain an image. Prior to such imaging, the dispersion medium is divided so as to contain microparticles within a certain particle diameter range, and the number concentration is adjusted without changing the number of microparticles in each divided dispersion medium.

Description

個数基準粒子径分布計測方法及び計測システムNumber-based particle size distribution measurement method and measurement system
 本発明は、分散媒中の微小粒子における個数基準の粒子径の分布計測方法及び計測システムに関し、特に、ナノメートルサイズからマイクロメートルサイズの幅広い粒子径分布を有する粒子における個数基準の粒子径分布を計測する方法及び計測システムに関する。 The present invention relates to a number-based particle size distribution measurement method and measurement system for fine particles in a dispersion medium, and in particular, a number-based particle size distribution for particles having a wide particle size distribution from nanometer size to micrometer size. Regarding measuring methods and measuring systems.
 レーザ光による回折や散乱を利用する粒子径分布の計測方法において、粒子径分布を体積基準で計測することが一般的であるが、これを個数基準の粒子径分布に変換することも求められる。例えば、流動場分離(FFF:Field Flow Fractionation)法などの分級法を用い、粒子径と個数濃度とから粒子径分布を計測する。 In the method of measuring the particle size distribution using diffraction or scattering by laser light, it is common to measure the particle size distribution on a volume basis, but it is also required to convert this into a particle size distribution based on the number. For example, the particle size distribution is measured from the particle size and the number concentration by using a classification method such as the FFF (Field Flow Fractionation) method.
 例えば、非特許文献1では、FFF法でサイズ分級した後に、オンライン多角度散乱計測装置で粒子径と光散乱強度濃度を算出し、光散乱強度濃度をミー散乱の理論に従って個数濃度に変換し、個数基準の粒子径分布を算出することを開示している。また、オフライン法として、FFF法でサイズ分級した後に、各分画分の粒子径分布及び個数濃度を走査型電子顕微鏡にて算出し、それらの結果を再構成して個数基準の粒子径分布を計測する方法も開示されている。更に、走査型電子顕微鏡にて、全数評価して個数基準の粒子径分布を計測する方法も開示している。 For example, in Non-Patent Document 1, after size classification by the FFF method, the particle size and the light scattering intensity concentration are calculated by an online multi-angle scattering measuring device, and the light scattering intensity concentration is converted into a number concentration according to the theory of Mie scattering. It discloses that the particle size distribution based on the number is calculated. In addition, as an offline method, after size classification by the FFF method, the particle size distribution and number concentration of each fraction are calculated by a scanning electron microscope, and the results are reconstructed to obtain a number-based particle size distribution. The method of measurement is also disclosed. Further, a method of measuring the particle size distribution based on the number of particles by evaluating all of them with a scanning electron microscope is also disclosed.
 一方、非特許文献2では、FFF法の後段にStop-flowモードの粒子追跡分析(PTA:Particle Tracking Analysis)装置を接続し、各分画分ごとに粒子径分布と個数濃度を計測し、これを再構成して個数基準の粒子径分布を求める方法を開示している。更に、非特許文献3や特許文献1では、流れ場粒子追跡(FPT:Flow particle Tracking)法による個数基準の粒子径計測方法が開示されている。 On the other hand, in Non-Patent Document 2, a Stop-flow mode particle tracking analysis (PTA) device is connected to the subsequent stage of the FFF method, and the particle size distribution and the number concentration are measured for each fraction. Discloses a method for obtaining a particle size distribution based on the number of particles by reconstructing. Further, Non-Patent Document 3 and Patent Document 1 disclose a number-based particle size measuring method by a flow field particle tracking (FPT) method.
国際公開第2016/159131号パンフレットInternational Publication No. 2016/159131 Pamphlet
 上記したように、流動場分離(FFF)法と他の計測方法を組み合わせることで、個数基準の粒子径分布を評価することができる。一方、FFF法にオンライン多角度散乱計測装置を組み合わせた評価法では、計測された光散乱強度から個数濃度への変換において、粒子の屈折率がわからなければレイリー散乱やミー散乱の散乱理論を適用できず、個数基準の粒子径分布を算出できない。 As described above, by combining the flow field separation (FFF) method and other measurement methods, it is possible to evaluate the particle size distribution based on the number of particles. On the other hand, in the evaluation method that combines the FFF method with an online multi-angle scattering measuring device, the scattering theory of Rayleigh scattering or Mie scattering is applied if the refractive index of the particles is not known in the conversion from the measured light scattering intensity to the number concentration. It is not possible to calculate the particle size distribution based on the number.
 一方、走査型電子顕微鏡で計数する方法や、FFF法に走査型電子顕微鏡を組み合わせる方法では、粒子の屈折率が不明であっても個数基準の粒子径分布を算出できる。しかし、走査型電子顕微鏡で粒子を個々に計測するため、迅速な計測ができない。また、FFF法にFPT法を組み合わせることで、個数基準の粒子径分布を迅速且つ簡便に算出でき得るが、粒子からの散乱光強度から粒子径を計測するFPT法では、散乱光強度が粒子径に対して非線形に大きく変化し、広い粒子径範囲の分布を有する粒子では精確な計測ができない。 On the other hand, in the method of counting with a scanning electron microscope or the method of combining the scanning electron microscope with the FFF method, the particle size distribution based on the number can be calculated even if the refractive index of the particles is unknown. However, since the particles are individually measured with a scanning electron microscope, rapid measurement is not possible. Further, by combining the FFF method with the FPT method, the particle size distribution based on the number can be calculated quickly and easily, but in the FPT method in which the particle size is measured from the scattered light intensity from the particles, the scattered light intensity is the particle size. On the other hand, it changes greatly non-linearly, and accurate measurement cannot be performed with particles having a wide particle size range distribution.
 本発明は、上記したような実情を鑑みてなされたものであって、ナノメートルサイズからマイクロメートルサイズの広い粒子径範囲の分布を有する粒子の個数基準での粒子径分布を迅速且つ簡便に計測できる方法及び計測システムを提供しようとするものである。 The present invention has been made in view of the above circumstances, and quickly and easily measures the particle size distribution based on the number of particles having a distribution in a wide particle size range from nanometer size to micrometer size. It seeks to provide possible methods and measurement systems.
 本発明による粒子径分布計測方法は、分散媒中をブラウン運動する微小粒子にレーザ光を照射し散乱光による輝点を所定時間間隔で撮像して得られる画像の該輝点の移動軌跡から該微小粒子の粒子径及び個数を計測し個数基準の粒子径分布を計測する方法であって、前記分散媒中を拡散する前記微小粒子に対して前記分散媒中に流れ場を形成して前記微小粒子を粒子径に従って前記分散媒中に配列させて分級する分級ステップと、分級された前記微小粒子を含む前記分散媒に前記レーザ光を照射して前記画像を得る撮像ステップと、を含み、前記撮像ステップに先立って、所定の粒子径範囲の前記微小粒子を含むように前記分散媒を分割し、分割されたそれぞれの前記分散媒中の前記微小粒子の個数を変化させずに個数濃度を調整する調整ステップを含むことを特徴とする。 The particle size distribution measuring method according to the present invention irradiates fine particles that move brown in a dispersion medium with laser light, and images bright spots due to scattered light at predetermined time intervals. It is a method of measuring the particle size and the number of fine particles and measuring the particle size distribution based on the number of fine particles by forming a flow field in the dispersion medium for the fine particles diffusing in the dispersion medium. A classification step of arranging particles in the dispersion medium according to the particle size and classifying the particles, and an imaging step of irradiating the dispersion medium containing the classified fine particles with the laser beam to obtain the image are included. Prior to the imaging step, the dispersion medium is divided so as to include the fine particles in a predetermined particle size range, and the number concentration is adjusted without changing the number of the fine particles in each of the divided dispersion media. It is characterized by including an adjustment step to be performed.
 また、本発明による粒子径分布計測システムは、分散媒中をブラウン運動する微小粒子にレーザ光を照射し散乱光による輝点を所定時間間隔で撮像して得られる画像の該輝点の移動軌跡から該微小粒子の粒子径及び個数を計測し個数基準の粒子径分布を計測するシステムであって、前記分散媒中を拡散する前記微小粒子に対して前記分散媒中に流れ場を形成して前記微小粒子を粒子径に従って前記分散媒中に配列させて分級する分級装置と、分級された前記微小粒子を含む前記分散媒を前記分級装置からセルに導きこれに前記レーザ光を照射して前記画像を得る撮像装置と、を含み、前記分級装置と前記セルとの間に、所定の粒子径範囲の前記微小粒子を含むように前記分散媒を分割し、分割されたそれぞれの前記分散媒中の前記微小粒子の個数を変化させずに個数濃度を調整する濃度調整装置を含むことを特徴とする。 Further, in the particle size distribution measurement system according to the present invention, the moving locus of the bright spot of the image obtained by irradiating the fine particles that move brown in the dispersion medium with laser light and imaging the bright spot by the scattered light at predetermined time intervals. It is a system that measures the particle size and the number of the fine particles and measures the particle size distribution based on the number of the fine particles, and forms a flow field in the dispersion medium for the fine particles diffusing in the dispersion medium. The classification device in which the fine particles are arranged in the dispersion medium according to the particle size and classified, and the dispersion medium containing the classified fine particles are guided from the classification device to a cell and irradiated with the laser beam. The dispersion medium is divided between the classification device and the cell so as to include the fine particles in a predetermined particle size range, including an image pickup device for obtaining an image, and in each of the divided dispersion media. It is characterized by including a concentration adjusting device for adjusting the number concentration without changing the number of the fine particles.
 かかる特徴によれば、撮像装置での撮像において分割された分散媒のそれぞれに適した条件で画像を得ることができ、ナノメートルサイズからマイクロメートルサイズの広い粒子径範囲の分布を有する粒子の個数基準での粒子径分布を迅速且つ簡便に計測できる。 According to such a feature, an image can be obtained under conditions suitable for each of the divided dispersion media in the imaging with the imaging device, and the number of particles having a distribution in a wide particle size range from nanometer size to micrometer size. The particle size distribution based on the standard can be measured quickly and easily.
 上記した発明において、前記濃度調整装置及びここでなされる調整ステップは、前記撮像ステップにおいて撮像される前記微小粒子に対して散乱光による輝点を得られるように前記粒子径範囲を調整することを特徴としてもよい。かかる特徴によれば、粒子径に対して非線形となる散乱光強度に対応して撮像装置のダイナミックレンジを拡げる、又は、切り替えることを必要とさせず、計測を迅速且つ簡便にできるのである。 In the above-described invention, the density adjusting device and the adjusting step performed here adjust the particle size range so that bright spots due to scattered light can be obtained for the fine particles imaged in the imaging step. It may be a feature. According to such a feature, it is not necessary to expand or switch the dynamic range of the image pickup apparatus in response to the scattered light intensity which is non-linear with respect to the particle size, and the measurement can be performed quickly and easily.
 上記した発明において、前記個数濃度は、分割した前記分散媒のそれぞれにおいて前記分散媒を追加又は分離することで調整されることを特徴としてもよい。かかる特徴によれば、簡単な方法で個数濃度を調整できて、個数基準での粒子径分布の迅速な計測をより簡便にし得る。 In the above-mentioned invention, the number concentration may be adjusted by adding or separating the dispersion medium in each of the divided dispersion media. According to such a feature, the number concentration can be adjusted by a simple method, and the rapid measurement of the particle size distribution on the basis of the number can be simplified.
 上記した発明において、前記流れ場は、流路に沿った液送方向とこれに略直行する方向の流れを加えたものであり、前記微小粒子を前記液送方向に交差するように配列させることを特徴としてもよい。又は、上記した発明において、前記流れ場は、流路に沿った液送方向とこれに略直行する方向の遠心力を加えたものであり、前記微小粒子を前記液送方向に交差するように配列させることを特徴としてもよい。かかる特徴によれば、分級装置及びここでなされる分級ステップにおける粒子径での分級を簡便に行うことができる。 In the above-described invention, the flow field is obtained by adding a flow in a liquid feeding direction along the flow path and a flow in a direction substantially perpendicular to the flow field, and the fine particles are arranged so as to intersect the liquid feeding direction. May be a feature. Alternatively, in the above-described invention, the flow field is obtained by applying a centrifugal force in a liquid feeding direction along a flow path and a direction substantially perpendicular to the flow field so as to intersect the fine particles in the liquid feeding direction. It may be characterized by arranging them. According to such a feature, the classification by the particle size in the classification device and the classification step performed here can be easily performed.
本発明の粒子径分布の計測方法に使用される装置構成の一例を示すブロック図である。It is a block diagram which shows an example of the apparatus composition used for the measuring method of the particle size distribution of this invention. 流れFFFの原理についての説明図である。It is explanatory drawing about the principle of flow FFF. 遠心FFFの原理についての説明図である。It is explanatory drawing about the principle of centrifugal FFF.
 本発明の1つの実施形態について図1乃至図3を用いて説明する。 One embodiment of the present invention will be described with reference to FIGS. 1 to 3.
 図1に示すように、粒子径分布評価方法に使用される粒子径分布計測システムは、流動場分離法(FFF:Field Flow Fractionation)による分級装置1、接続部2、流れ場粒子追跡(FPT:Flow particle Tracking)法による測定装置3、演算処理装置4を備えている。 As shown in FIG. 1, the particle size distribution measurement system used in the particle size distribution evaluation method includes a classification device 1, a connection unit 2, and a flow field particle tracking (FPT:) by a flow field separation method (FFF: Field Flow Fractionation). It is equipped with a measuring device 3 and an arithmetic processing device 4 by the Flow particle Tracking method.
 分級装置1は分散媒を導入する溶離液導入部11と、分散媒中をブラウン運動する微小粒子を分散媒に分散させた分散液を溶離液導入部から続く流路に注入する試料導入部12と、微小粒子を粒子径毎に分級するFFF装置13とを含む。FFF装置13としては、流れFFF装置14(図2参照)または遠心FFF装置15(図3参照)を好適に使用し得る。 The classification device 1 includes an eluent introduction unit 11 for introducing a dispersion medium, and a sample introduction unit 12 for injecting a dispersion liquid in which fine particles that move in Brownian motion in the dispersion medium are dispersed in the dispersion medium into a flow path continuing from the eluent introduction unit. And an FFF device 13 for classifying fine particles according to particle size. As the FFF device 13, a flow FFF device 14 (see FIG. 2) or a centrifugal FFF device 15 (see FIG. 3) can be preferably used.
 図2に示すように、流れFFF装置14は、流入口16から流出口18に向かう流路に沿った液送方向を有し、流路の一方の側壁に設けられた精密ろ過膜19を設けることで分散媒17による液送方向に略直行する方向の流れ50を交叉力場として形成できる。この液送方向に直行する流れ50により、一旦、精密ろ過膜19の表面の1か所に集められた微小粒子51は、精密ろ過膜19から流路中心に向けて拡散してその粒子径に基づく拡散速度の違いによって分級される。具体的には、流路の中心に近づくにつれて粒子径を小さくするよう液送方向に交差する方向に配列される。さらに、液送方向に沿った層流においては流路外周から中心に向けて速くなる速度勾配があるため、流路の中心近くの粒子径の小さな微小粒子51から順に流路を進み、分級された微小粒子51の分画を容易にする。 As shown in FIG. 2, the flow FFF device 14 has a liquid feeding direction along a flow path from the inflow port 16 to the outflow port 18, and is provided with a microfiltration membrane 19 provided on one side wall of the flow path. As a result, the flow 50 in the direction substantially perpendicular to the liquid feeding direction by the dispersion medium 17 can be formed as a crossing force field. Due to the flow 50 orthogonal to the liquid feeding direction, the fine particles 51 once collected at one place on the surface of the microfiltration membrane 19 diffuse from the microfiltration membrane 19 toward the center of the flow path to the particle diameter. It is classified according to the difference in diffusion rate based on it. Specifically, the particles are arranged in a direction intersecting the liquid feeding direction so that the particle size becomes smaller as the particle size approaches the center of the flow path. Further, in the laminar flow along the liquid feeding direction, since there is a velocity gradient that increases from the outer periphery of the flow path toward the center, the particles are classified by proceeding in the flow path in order from the fine particles 51 having a small particle size near the center of the flow path. The fractionation of the fine particles 51 is facilitated.
 図3に示すように、遠心FFF装置15は、流入口16から流出口18に向かう流路に沿った液送方向を有し、流路には分散媒17による液送方向に略直行する方向の遠心力52を交叉力場として付与される。例えば、図示を省略するが、液送方向を湾曲させる曲率を持った流路とすることでこのような遠心力52を付与できる。この遠心力52により、一旦、外周壁19’の表面の1か所に集められた微小粒子51は、外周壁19’から流路中心に向けて拡散してその粒子径に基づく拡散速度及び質量の違いによって分級される。具体的には、流路の中心に近づくにつれて粒子径を小さくするよう液送方向に交差する方向に配列される。さらに、液送方向に沿った層流においては流路外周から中心に向けて速くなる速度勾配があるため、流路の中心近くの粒子径の小さな微小粒子51から順に流路を進み、分級された微小粒子51の分画を容易にする。 As shown in FIG. 3, the centrifugal FFF device 15 has a liquid feeding direction along a flow path from the inlet 16 to the outlet 18, and the flow path is substantially perpendicular to the liquid feeding direction by the dispersion medium 17. Centrifugal force 52 is applied as a crossing force field. For example, although not shown, such a centrifugal force 52 can be applied by using a flow path having a curvature that curves the liquid feeding direction. Due to this centrifugal force 52, the fine particles 51 once collected at one place on the surface of the outer peripheral wall 19'diffuse from the outer peripheral wall 19' toward the center of the flow path, and the diffusion velocity and mass based on the particle diameter. It is classified according to the difference. Specifically, the particles are arranged in a direction intersecting the liquid feeding direction so that the particle size becomes smaller as the particle size approaches the center of the flow path. Further, in the laminar flow along the liquid feeding direction, since there is a velocity gradient that increases from the outer periphery of the flow path toward the center, the particles are classified by proceeding in the flow path in order from the fine particles 51 having a small particle size near the center of the flow path. The fractionation of the fine particles 51 is facilitated.
 つまり、分級装置1は、流動場分離法によって広範囲の粒子径を有する微小粒子を粒子径で分級して接続部2へ導くことのできる機構である。なお、流動場分離法として、熱、磁場、電場など、他のエネルギーを交叉力場として与えるものを微小粒子に合わせて、適宜、選択し得る。 That is, the classification device 1 is a mechanism capable of classifying fine particles having a wide range of particle sizes by the particle size and guiding them to the connection portion 2 by the flow field separation method. As the flow field separation method, a method such as heat, magnetic field, electric field, etc. that gives other energy as a crossing force field can be appropriately selected according to the fine particles.
 接続部2は、所定の粒子径範囲の微小粒子を含むように分級された微小粒子を含むように分散媒を複数に分割し、それぞれを後段の測定装置3へ導く機構である。例えば、分級装置1から分散液を導出されるまでの時間や量を所定値とするところで仕切ることで上記したように分散を分割できる。また、分割されたそれぞれの分散液について微小粒子の個数を変化させずに分散媒の量を制御して、後述する測定装置3へ導く濃度調整装置である。これによって測定装置3での計測を容易に行い得るよう微小粒子51の個数濃度を調整することができる。ここで、後段の流れ場粒子追跡法においては、微小粒子51を画像上の輝点として追跡するので、この輝点の個々を画像解析にて精度よく判別できるように輝点同士を十分離間させるように個数濃度を低下させる。また、画像上の輝点の密度が疎となって測定の時間的効率を低下させないよう個数濃度を上昇させてもよい。そのために、微小粒子51の個数濃度を所望の範囲にするように分散液を希釈し又は濃縮するのである。 The connecting portion 2 is a mechanism that divides the dispersion medium into a plurality of particles so as to contain fine particles classified so as to contain fine particles in a predetermined particle size range, and guides each of them to the measuring device 3 in the subsequent stage. For example, the dispersion can be divided as described above by partitioning the time and amount until the dispersion liquid is derived from the classification device 1 at a predetermined value. Further, it is a concentration adjusting device that controls the amount of the dispersion medium for each of the divided dispersion liquids without changing the number of fine particles and leads to the measuring device 3 described later. Thereby, the number concentration of the fine particles 51 can be adjusted so that the measurement by the measuring device 3 can be easily performed. Here, in the flow field particle tracking method in the subsequent stage, the fine particles 51 are tracked as bright spots on the image, so that the bright spots are sufficiently separated from each other so that the individual bright spots can be accurately discriminated by image analysis. To reduce the number concentration. Further, the number density may be increased so that the density of bright spots on the image is not sparse and the time efficiency of measurement is not reduced. Therefore, the dispersion is diluted or concentrated so that the number concentration of the fine particles 51 is within a desired range.
 接続部2としては、例えば、FFF装置13において、微小粒子51の集められた側と反対側の(拡散する方向の先端側の)分散媒17を除去して微小粒子51の個数濃度を上昇させて後段の測定装置3へ導くスプリットや、分散媒17を追加して分散液を希釈させて微小粒子51の個数濃度を低下させるシリンジポンプやダイヤフラムポンプなどを用い得る。接続部2の構成は分級すべき微小粒子51及び分散媒17からなる分散液の流体としての特性に従い、適宜、選択し得る。なお、分割された分散液をそれぞれ異なる流路に導くようにしてもよい。この場合、分割された分散液のそれぞれを後述する測定装置3の光学セルをそれぞれの流路に対して設けることもできる。 As the connecting portion 2, for example, in the FFF device 13, the dispersion medium 17 on the side opposite to the collected side of the fine particles 51 (on the tip side in the diffusion direction) is removed to increase the number concentration of the fine particles 51. A split that leads to the measuring device 3 in the subsequent stage, or a syringe pump or a diaphragm pump that dilutes the dispersion liquid by adding a dispersion medium 17 to reduce the concentration of the number of fine particles 51 can be used. The configuration of the connecting portion 2 can be appropriately selected according to the characteristics of the dispersion liquid consisting of the fine particles 51 to be classified and the dispersion medium 17 as a fluid. The divided dispersion may be guided to different flow paths. In this case, each of the divided dispersion liquids may be provided with an optical cell of the measuring device 3 described later for each flow path.
 なお、分級した微小粒子51の群の粒子径の範囲を粒子径の差として2~3倍程度以内に抑えるよう分割することが好ましい。これによって、後述する測定装置3では、流れ場粒子追跡法によって粒子径を測定するにあたり、分割された分散液のそれぞれについて含まれる微小粒子51の粒子径の範囲に適した条件を設定でき、粒子径の測定を容易とする。 It is preferable to divide the group of the classified fine particles 51 so that the range of the particle size is suppressed within about 2 to 3 times as the difference in particle size. As a result, in the measuring device 3 described later, when measuring the particle size by the flow field particle tracking method, conditions suitable for the range of the particle size of the fine particles 51 contained in each of the divided dispersions can be set, and the particles can be set. Makes it easy to measure the diameter.
 測定装置3は、流れ場粒子追跡法によって微小粒子51の個々の粒子についての粒子径を計測し、その個数を計数する装置である。詳細には、測定装置3は、微小粒子51からの散乱光を撮像し、単一の粒子に対応する輝点を画像として記録できる撮像装置31と、分級されて個数濃度を調整された微小粒子51を含む分散媒17を流通させる透明な光学セル32と、光学セル32内の微小粒子51に向けてレーザ光を照射させるレーザ光源33とを含む。撮像装置31は、レンズなどの光学系を介して所定解像度の撮像素子(CCD:Charge Coupled Device、CMOSイメージセンサなど)の素子に対応する画素を2次元に配列させた画像を撮影し画像データとして出力する。撮像装置31は、所定の露出時間及び所定の時間間隔Δtで撮影を実行して、複数の画像を連続的に生成する。なお、露出時間は、時間間隔Δtより短い。例えば、フレームレートは30fpsの場合、時間間隔Δtは約33msであり、露出時間は30msとされる。なお、露出時間は、シャッタースピードを制御し、又は、レーザ光源33をパルス点灯し制御してもよい。また、測定装置3は、分割された分散液のそれぞれに合わせて撮像条件を調整される。 The measuring device 3 is a device that measures the particle size of each particle of the fine particles 51 by the flow field particle tracking method and counts the number of the particles. Specifically, the measuring device 3 includes an image pickup device 31 capable of capturing the scattered light from the fine particles 51 and recording a bright spot corresponding to a single particle as an image, and fine particles classified and having their number densities adjusted. It includes a transparent optical cell 32 through which a dispersion medium 17 including 51 is circulated, and a laser light source 33 for irradiating a laser beam toward the fine particles 51 in the optical cell 32. The image pickup device 31 captures an image in which pixels corresponding to elements of an image pickup device (CCD: Charge Coupled Device, CMOS image sensor, etc.) having a predetermined resolution are arranged in two dimensions via an optical system such as a lens, and uses the image data as image data. Output. The image pickup apparatus 31 executes shooting at a predetermined exposure time and a predetermined time interval Δt to continuously generate a plurality of images. The exposure time is shorter than the time interval Δt. For example, when the frame rate is 30 fps, the time interval Δt is about 33 ms, and the exposure time is 30 ms. The exposure time may be controlled by controlling the shutter speed or by illuminating the laser light source 33 in a pulsed manner. Further, the measuring device 3 adjusts the imaging conditions according to each of the divided dispersion liquids.
 演算処理装置4は、所定のプログラムを実行するコンピュータを内蔵し、プログラムに従って所定のデータ処理を実行し各種処理部として動作する。ここで演算処理装置4は、画像解析部41、粒子径・個数濃度解析部43、粒子径・個数濃度解析部43で解析されたデータを再構成して粒子径分布を算出する粒子径分布解析部44、および制御部45として動作する。また、演算処理装置4は、不揮発性の記憶装置(フラッシュメモリ、ハードディスクドライブなど)を記憶部42として備える。 The arithmetic processing unit 4 has a built-in computer that executes a predetermined program, executes predetermined data processing according to the program, and operates as various processing units. Here, the arithmetic processing device 4 reconstructs the data analyzed by the image analysis unit 41, the particle size / number concentration analysis unit 43, and the particle size / number concentration analysis unit 43 to calculate the particle size distribution. It operates as a unit 44 and a control unit 45. Further, the arithmetic processing unit 4 includes a non-volatile storage device (flash memory, hard disk drive, etc.) as the storage unit 42.
 画像解析部41は、撮像装置31を制御し、撮像装置31に、光学セル32の所定範囲の撮像を実行させ、撮像装置31によって連続的に生成された複数の画像の画像データを取得する。なお、画像解析部41は、撮像装置31における各撮像画像の露出時間や検出感度を分級装置1において分級された微小粒子51の粒子径に合わせて、適宜変更するようにさせてもよい。例えば、FFF装置13から導出される微小粒子の粒子径を理論的に算出し、または簡易モニターによって実測し、最適な撮像条件を設定するようにしてもよい。また、画像解析部41での輝点から微小粒子51の計数漏れを発生させないように、接続部2における分級する微小粒子51の粒子径の範囲を調節させるフィードバック信号を与えるようにしておくことが好ましい。 The image analysis unit 41 controls the image pickup device 31, causes the image pickup device 31 to perform imaging in a predetermined range of the optical cell 32, and acquires image data of a plurality of images continuously generated by the image pickup device 31. The image analysis unit 41 may appropriately change the exposure time and detection sensitivity of each captured image in the image pickup device 31 according to the particle size of the fine particles 51 classified in the classification device 1. For example, the particle size of the fine particles derived from the FFF device 13 may be theoretically calculated or actually measured by a simple monitor to set the optimum imaging conditions. Further, it is possible to give a feedback signal for adjusting the range of the particle size of the fine particles 51 to be classified in the connection unit 2 so that the counting omission of the fine particles 51 does not occur from the bright spot in the image analysis unit 41. preferable.
 画像解析部41では、流動場分離法によって、取得した画像データに基づいて画像上の輝点の移動軌跡を特定し、かかる輝点に対応する微小粒子51の変位を求める。そして、kBをボルツマン定数、Tを絶対温度、ηを分散媒の粘性係数、dを粒子径とし、微小粒子51の変位の2乗平均値がkBT/3πηdに比例することから粒子径を算出する。また、画像解析部41では、粒子径の算出と併せて所定の領域を通過した輝点の数を計数し微小粒子51の数とする。このように流動場分離法では、個々の微小粒子51にそれぞれ対応する輝点を追跡しながら輝点の数を計数するので、微小粒子51を形成する材料によらずにその数を計数できる。 The image analysis unit 41 identifies the movement locus of the bright spot on the image based on the acquired image data by the flow field separation method, and obtains the displacement of the fine particles 51 corresponding to the bright spot. Then, kB is the Boltzmann constant, T is the absolute temperature, η is the viscosity coefficient of the dispersion medium, d is the particle diameter, and the squared average value of the displacement of the fine particles 51 is proportional to kBT / 3πηd, so that the particle diameter is calculated. .. Further, the image analysis unit 41 counts the number of bright spots that have passed through the predetermined region together with the calculation of the particle size to obtain the number of fine particles 51. As described above, in the flow field separation method, the number of bright spots is counted while tracking the bright spots corresponding to the individual fine particles 51, so that the number can be counted regardless of the material forming the fine particles 51.
 なお、画像解析部41では、既知の方法(特許文献1の開示する方法や流体シミュレーションなど)で、撮像装置31の画角に対応する光学セル32内の撮像領域における分散媒17の流速分布を予め特定し、分散媒17の流速分布に基づいて微小粒子51の変位を補正して、補正後の変位に基づいて微小粒子51の平均二乗変位ΔMSを特定することが好ましい。すなわち流速分布に基づく微小粒子51の変位の補正を行うことで、分散媒17の流れ場の影響を除外した上でブラウン運動による微小粒子51の変位を得るのである。なお、流速分布は、撮像領域内で一定(つまり、大きさおよび向きが一定)と仮定してもよい。 The image analysis unit 41 uses a known method (method disclosed in Patent Document 1, fluid simulation, etc.) to determine the flow velocity distribution of the dispersion medium 17 in the image pickup region in the optical cell 32 corresponding to the angle of view of the image pickup device 31. It is preferable to specify in advance, correct the displacement of the fine particles 51 based on the flow velocity distribution of the dispersion medium 17, and specify the average square displacement ΔMS of the fine particles 51 based on the corrected displacement. That is, by correcting the displacement of the fine particles 51 based on the flow velocity distribution, the displacement of the fine particles 51 due to the Brownian motion is obtained after excluding the influence of the flow field of the dispersion medium 17. The flow velocity distribution may be assumed to be constant (that is, the size and orientation are constant) within the imaging region.
 さらに、画像解析部41では、光学セル内の所定領域を通過する微小粒子51の個数を計数する。 Further, the image analysis unit 41 counts the number of fine particles 51 passing through a predetermined region in the optical cell.
 上記した微小粒子の粒子径と個数を累積することで、試料導入部12に試料として注入された微小粒子51を分散させた分散液における個数基準の粒子径分布を算出することができる。 By accumulating the particle size and the number of the above-mentioned fine particles, it is possible to calculate the particle size distribution based on the number in the dispersion liquid in which the fine particles 51 injected as a sample are dispersed in the sample introduction unit 12.
 以上のように、本実施例によれば、個数基準の粒子径分布を算出することができる。特に、流動場分離法によって分級することで、流れ場粒子追跡法による粒子径の計測においては、微小粒子からの散乱光の強度の範囲を狭くすることができて、簡便に分級すべき粒子径毎の個数の計数をすることができる。 As described above, according to this embodiment, the particle size distribution based on the number of particles can be calculated. In particular, by classifying by the flow field separation method, the range of the intensity of scattered light from fine particles can be narrowed in the particle size measurement by the flow field particle tracking method, and the particle size to be easily classified. It is possible to count the number of each.
 また、接続部2を介して、分級装置1と測定装置3とを接続したので、測定装置3に計測に適した個数濃度の分散液を導くことができ、分級し分画された分散液毎にオンラインで粒子径と個数濃度を計測できる。そのため、迅速に個数基準の粒子径分布を計測できる。 Further, since the classification device 1 and the measuring device 3 are connected via the connecting portion 2, it is possible to guide the dispersion liquid having a number concentration suitable for measurement to the measuring device 3, and each of the classified and fractionated dispersion liquids. You can measure the particle size and the number concentration online. Therefore, the particle size distribution based on the number can be measured quickly.
 つまり、例えば、約10nm~3μmといった、ナノメートルサイズからマイクロメートルサイズの広い粒子径範囲の分布を有する微小粒子であっても、個数基準での粒子径分布を迅速且つ簡便に計測できる。 That is, even for fine particles having a wide particle size range from nanometer size to micrometer size, for example, about 10 nm to 3 μm, the particle size distribution based on the number can be measured quickly and easily.
 なお、光学セル32内の容積を勘案することで、複数の流出時間範囲における微小粒子51の個数濃度を算出し、これらを再構成することでも、注入された微小粒子の分散液における個数基準の粒子径分布を算出することができる。 In addition, by considering the volume in the optical cell 32, the number concentration of the fine particles 51 in a plurality of outflow time ranges is calculated, and by reconstructing these, the number reference in the dispersion liquid of the injected fine particles can be obtained. The particle size distribution can be calculated.
 以上、本発明の代表的な実施例を説明したが、本発明は必ずしもこれらに限定されるものではなく、当業者であれば、本発明の主旨又は添付した特許請求の範囲を逸脱することなく、種々の代替実施例及び改変例を見出すことができるであろう。 Although typical examples of the present invention have been described above, the present invention is not necessarily limited to these, and those skilled in the art will not deviate from the gist of the present invention or the scope of the attached claims. , Various alternative and modified examples will be found.
1     分級装置
2     接続部
3     測定装置
4     演算処理装置
12    試料導入部
13    FFF装置
14    流れFFF装置
15    遠心FFF装置
16    流入口
17    分散媒
18    流出口18
19    精密ろ過膜
31    撮像装置
32    光学セル
33    レーザ光源
41    画像解析部
42    記憶部
43    粒子径・個数濃度解析部
44    粒子径分布解析部
45    制御部
51    微小粒子

 
1 Classification device 2 Connection part 3 Measuring device 4 Arithmetic processing device 12 Sample introduction unit 13 FFF device 14 Flow FFF device 15 Centrifugal FFF device 16 Inflow port 17 Dispersion medium 18 Outlet 18
19 Microfiltration membrane 31 Imaging device 32 Optical cell 33 Laser light source 41 Image analysis unit 42 Storage unit 43 Particle size / number concentration analysis unit 44 Particle size distribution analysis unit 45 Control unit 51 Fine particles

Claims (10)

  1.  分散媒中をブラウン運動する微小粒子にレーザ光を照射し散乱光による輝点を所定時間間隔で撮像して得られる画像の該輝点の移動軌跡から該微小粒子の粒子径及び個数を計測し個数基準の粒子径分布を計測する方法であって、
     前記分散媒中を拡散する前記微小粒子に対して前記分散媒中に流れ場を形成して前記微小粒子を粒子径に従って前記分散媒中に配列させて分級する分級ステップと、
     分級された前記微小粒子を含む前記分散媒に前記レーザ光を照射して前記画像を得る撮像ステップと、を含み、
     前記撮像ステップに先立って、所定の粒子径範囲の前記微小粒子を含むように前記分散媒を分割し、分割されたそれぞれの前記分散媒中の前記微小粒子の個数を変化させずに個数濃度を調整する調整ステップを含むことを特徴とする粒子径分布計測方法。
    The particle size and number of the fine particles are measured from the movement locus of the bright spots in the image obtained by irradiating the fine particles that move in Brownian motion in the dispersion medium with laser light and imaging the bright spots due to the scattered light at predetermined time intervals. It is a method of measuring the particle size distribution based on the number of particles.
    A classification step of forming a flow field in the dispersion medium for the fine particles diffusing in the dispersion medium and arranging the fine particles in the dispersion medium according to the particle size to classify them.
    It comprises an imaging step of irradiating the dispersion medium containing the classified fine particles with the laser beam to obtain the image.
    Prior to the imaging step, the dispersion medium is divided so as to contain the fine particles in a predetermined particle size range, and the number concentration is adjusted without changing the number of the fine particles in each of the divided dispersion media. A particle size distribution measuring method comprising an adjustment step for adjustment.
  2.  前記調整ステップは、前記撮像ステップにおいて撮像される前記微小粒子に対して散乱光による輝点を得られるように前記粒子径範囲を調整することを特徴とする請求項1記載の粒子径分布計測方法。 The particle size distribution measuring method according to claim 1, wherein the adjustment step adjusts the particle size range so that a bright spot due to scattered light can be obtained for the fine particles imaged in the image pickup step. ..
  3.  前記個数濃度は、分割した前記分散媒のそれぞれにおいて前記分散媒を追加又は分離することで調整されることを特徴とする請求項1記載の粒子径分布計測方法。 The particle size distribution measuring method according to claim 1, wherein the number concentration is adjusted by adding or separating the dispersion medium in each of the divided dispersion media.
  4.  前記流れ場は、流路に沿った液送方向とこれに略直行する方向の流れを加えたものであり、前記微小粒子を前記液送方向に交差するように配列させることを特徴とする請求項1記載の粒子径分布計測方法。 The flow field is obtained by adding a flow in a liquid feeding direction along a flow path and a flow in a direction substantially orthogonal to the flow, and is characterized in that the fine particles are arranged so as to intersect the liquid feeding direction. Item 1. The particle size distribution measuring method according to Item 1.
  5.  前記流れ場は、流路に沿った液送方向とこれに略直行する方向の遠心力を加えたものであり、前記微小粒子を前記液送方向に交差するように配列させることを特徴とする請求項1記載の粒子径分布計測方法。 The flow field is obtained by applying a centrifugal force in a liquid feeding direction along a flow path and a direction substantially perpendicular to the flow direction, and is characterized in that the fine particles are arranged so as to intersect the liquid feeding direction. The particle size distribution measuring method according to claim 1.
  6.  分散媒中をブラウン運動する微小粒子にレーザ光を照射し散乱光による輝点を所定時間間隔で撮像して得られる画像の該輝点の移動軌跡から該微小粒子の粒子径及び個数を計測し個数基準の粒子径分布を計測するシステムであって、
     前記分散媒中を拡散する前記微小粒子に対して前記分散媒中に流れ場を形成して前記微小粒子を粒子径に従って前記分散媒中に配列させて分級する分級装置と、
     分級された前記微小粒子を含む前記分散媒を前記分級装置からセルに導きこれに前記レーザ光を照射して前記画像を得る撮像装置と、を含み、
     前記分級装置と前記セルとの間に、所定の粒子径範囲の前記微小粒子を含むように前記分散媒を分割し、分割されたそれぞれの前記分散媒中の前記微小粒子の個数を変化させずに個数濃度を調整する濃度調整装置を含むことを特徴とする粒子径分布計測システム。
    The particle size and number of the fine particles are measured from the movement locus of the bright spots in the image obtained by irradiating the fine particles that move in Brownian motion in the dispersion medium with laser light and imaging the bright spots due to the scattered light at predetermined time intervals. It is a system that measures the particle size distribution based on the number of particles.
    A classifying device that forms a flow field in the dispersion medium for the fine particles diffusing in the dispersion medium and arranges the fine particles in the dispersion medium according to the particle size to classify them.
    A device including an image pickup device that guides the dispersion medium containing the classified fine particles from the classifier to a cell and irradiates the cell with the laser beam to obtain the image.
    The dispersion medium is divided between the classifier and the cell so as to contain the fine particles in a predetermined particle size range, and the number of the fine particles in each of the divided dispersion media is not changed. A particle size distribution measuring system characterized by including a concentration adjusting device for adjusting the number concentration.
  7.  前記濃度調整装置は、前記撮像装置において撮像される前記微小粒子に対して散乱光による輝点を得られるように前記粒子径範囲を調整することを特徴とする請求項6記載の粒子径分布計測システム。 The particle size distribution measurement according to claim 6, wherein the density adjusting device adjusts the particle size range so that a bright spot due to scattered light can be obtained for the fine particles imaged by the image pickup device. system.
  8.  前記濃度調整装置において、前記個数濃度は、分割した前記分散媒のそれぞれにおいて前記分散媒を追加又は分離することで調整されることを特徴とする請求項6記載の粒子径分布計測システム。 The particle size distribution measuring system according to claim 6, wherein in the concentration adjusting device, the number concentration is adjusted by adding or separating the dispersion medium in each of the divided dispersion media.
  9.  前記分級装置において、前記流れ場は、流路に沿った液送方向とこれに略直行する方向の流れを加えたものであり、前記微小粒子を前記液送方向に交差するように配列させることを特徴とする請求項6記載の粒子径分布計測システム。 In the classification device, the flow field is obtained by adding a flow in a liquid feeding direction along the flow path and a flow in a direction substantially perpendicular to the flow field, and the fine particles are arranged so as to intersect the liquid feeding direction. 6. The particle size distribution measuring system according to claim 6.
  10.  前記分級装置において、前記流れ場は、流路に沿った液送方向とこれに略直行する方向の遠心力を加えたものであり、前記微小粒子を前記液送方向に交差するように配列させることを特徴とする請求項6記載の粒子径分布計測システム。

     
    In the classification device, the flow field is obtained by applying a centrifugal force in a liquid feeding direction along a flow path and a direction substantially perpendicular to the flow field, and the fine particles are arranged so as to intersect the liquid feeding direction. The particle size distribution measuring system according to claim 6, wherein the particle size distribution is measured.

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