Measurement cell and centrifugal sedimentation type particle size distribution measuring device using said measurement cell

Abstract

The present invention improves measuring accuracy in a particle-size distribution measuring device that performs particle-size distribution measurement with a line start method. This measurement cell 2 is used for the line start method of a centrifugal sedimentation-type particle-size distribution measuring device, and comprises: a cell body 21 that has, on one end thereof, an opening section 21H and contains a density gradient solution WDGS; and a cell cap 22 that closes the opening section 21H of the cell body 21 and has an internal flow passage R therein that holds a sample liquid WSS, wherein the sample liquid WSS is introduced into the density gradient solution WDGS from the internal flow passage R by applying centrifugal force.

Description

[Technical field]

[0001] The present invention relates to a centrifugal sedimentation type particle size distribution analyzer, and more particularly to a measurement cell used in the line start method of a centrifugal sedimentation type particle size distribution analyzer. [Background technology]

[0002] As shown in Non-Patent Document 1, a conventional centrifugal sedimentation type particle size distribution measuring device uses a line start method in which a sample suspension is supplied to a cell containing a density gradient solution, and the particles in the sample suspension are centrifuged in the density gradient solution.

[0003] Specifically, this particle size distribution measuring device uses a hollow disk-shaped cell, and is configured to contain a density gradient solution in the cell which rotates at a constant speed, and to inject a sample suspension from the center of the rotation.

[0004] However, since the sample suspension is injected from the outside into a rotating cell, there is a tendency for the timing of the sample suspension injection to vary, and there is also a large variation in the time it takes for the sample suspension to reach the density gradient solution in the cell, resulting in poor measurement accuracy. [Prior art documents] [Non-patent literature]

[0005] [Non-Patent Document 1] Stephen T. Fitzpatrick, "Particle Size Measurement by Frequency-Specific Centrifugal Sedimentation: Advantages and Disadvantages, Current Status, and Future Prospects" [Retrieved May 30, 2018], Internet (URL: https: / / www.nihon-rufuto.com / myadmin / rufuto_catalog / wp-content / uploads / 2017 / 06 / CPS-Polymer-News.pdf) Summary of the Invention [Problem to be solved by the invention]

[0006] The present invention has been made to solve the above problems, and has as its main object to improve the measurement accuracy in a particle size distribution measuring device that measures particle size distribution by the line start method. [Means for solving the problem]

[0007] That is, the measurement cell of the present invention is a measurement cell used in the line start method of a centrifugal sedimentation type particle size distribution measuring device, and is characterized in that it comprises a cell body having an opening formed at one end and containing a density gradient solution, which is a solution in which a density gradient is formed, and a cell cap that covers the opening of the cell body and has an internal flow path formed therein for holding sample liquid, and that the sample liquid is introduced from the internal flow path into the density gradient solution by application of centrifugal force.

[0008] In this case, the internal flow path formed in the cell cap holds the sample liquid, and the sample liquid is introduced from the internal flow path into the density gradient solution by applying centrifugal force, so that the timing when centrifugal force is applied to the measurement cell or the timing when the measurement cell is rotated at a predetermined rotation speed can be set as the measurement start timing of the line start method, thereby improving the measurement accuracy. In addition, since the sample liquid is held in the cell cap, the distance between the sample liquid and the density gradient solution can be reduced, and the variation in the time it takes for the sample liquid to reach the density gradient solution can also be reduced, which also improves the measurement accuracy.

[0009] Here, when the measurement cell is configured to be detachable from the device body, it is conceivable to reduce the size of the measurement cell in order to facilitate attachment and detachment. In this case, if the sample liquid is introduced from outside, it takes a long time for the sample liquid to reach the measurement cell, which can cause measurement errors, and the introduction mechanism for introducing the sample liquid from outside into the rotating measurement cell becomes complicated. On the other hand, in the present invention, the sample liquid is held in the cell cap of the measurement cell, and therefore the above-mentioned problems caused by making the measurement cell detachable from the main body of the device can be preferably solved.

[0010] In order to enable sample liquid to be retained in the internal flow path of the cell cap when the cell cap is attached to the cell body, it is desirable that the internal flow path has a sample inlet at one end and a sample outlet at the other end, and that when the cell cap is attached to the cell body, the sample inlet is located outside the cell body and the sample outlet is located inside the cell body.

[0011] In a specific embodiment of the internal flow path, the internal flow path preferably comprises a liquid reservoir for holding the sample liquid introduced from the sample inlet, and a main flow path portion communicating with the liquid reservoir and with the sample outlet, and the sample liquid held in the liquid reservoir flows into the main flow path portion by application of centrifugal force, and is introduced into the density gradient solution through the main flow path portion. Here, the liquid reservoir has an internal volume set according to the volume of the sample liquid. By providing a liquid reservoir in the internal flow path in this manner, the position at which a predetermined amount of sample liquid is held in the internal flow path becomes constant, and the reproducibility of particle size distribution measurement can be improved.

[0012] If the main flow path portion has a single diameter, the sample liquid will be introduced into the density gradient solution in clumps, and a streaming phenomenon may occur, which may cause problems such as making it difficult to measure the particle size distribution with high accuracy. In order to suitably solve this problem, it is desirable for the main flow path section to have a small diameter flow path section connected to the liquid reservoir section, and a large diameter flow path section that is provided downstream of the small diameter flow path section and communicates with the sample outlet port. With this configuration, the sample liquid from the small diameter flow path spreads in the large diameter flow path and is introduced into the density gradient solution from the sample outlet, which prevents the streaming phenomenon from occurring and improves measurement accuracy.

[0013] As a specific embodiment of the internal flow path, it is preferable that the internal flow path further includes an inlet flow path portion that communicates the sample inlet and the liquid reservoir portion, the inlet flow path portion being provided along the rotation axis direction of the measurement cell, and the main flow path portion being provided along the centrifugal force direction applied to the measurement cell. Here, since the main flow path portion is provided along the centrifugal force direction, the sample liquid can be made to flow quickly through the main flow path portion.

[0014] In order to reliably hold the sample liquid in the liquid reservoir before rotation of the measurement cell and to facilitate the flow of the sample liquid from the liquid reservoir to the main flow path portion during rotation, it is desirable that the main flow path portion be connected to an upper portion of the liquid reservoir, and that the liquid reservoir portion have an inclined surface with an upward gradient toward the main flow path portion on the side to which the main flow path portion is connected.

[0015] In order to facilitate processing of the liquid reservoir in the cell cap, it is desirable for the liquid reservoir to have a conical or partial conical shape tapering toward the bottom. With this configuration, when forming the liquid reservoir in the cell cap, a hole can be formed in the cell cap using a drill.

[0016] When the sample outlet of the internal flow path is in contact with the density gradient solution, the surface tension acting near the sample outlet may prevent the sample liquid introduced into the density gradient solution from spreading (dispersing). In order to suitably solve this problem, it is desirable that a space be formed between the cell cap and the density gradient solution when the cell cap is attached to the cell body. With this configuration, the sample liquid introduced into the density gradient solution can be reliably spread, and measurement accuracy can be improved.

[0017] It is preferable that the cell body and the cell cap are provided with a restricting mechanism that restricts the attachment orientation of the cell cap relative to the cell body. This configuration makes it possible to prevent the cell cap from being attached to the cell body in an incorrect orientation.

[0018] In addition, the centrifugal sedimentation type particle size distribution measuring device according to the present invention is characterized in that it comprises the above-mentioned measurement cell and a cell rotation mechanism that rotates the measurement cell so that a centrifugal force is applied to the measurement cell from the side of the smaller density gradient to the side of the larger density gradient.

[0019] The cell rotation mechanism may have a cell holder to which the cell is attached. In this case, it is preferable that the measurement cell is detachably attached to the cell holder. With this configuration, the only part that is removed from the device body is the cell, making the removal process easier and also making the subsequent cleaning process easier. In addition, the cell may be configured to be detachable from the device body by configuring the cell holder to be detachable from the device body.

[0020] It is preferable that the measuring cell and the cell holder are provided with a restricting mechanism for restricting the mounting orientation of the measuring cell with respect to the cell holder. With this configuration, it is possible to prevent the measurement cell from being attached to the cell holder in an incorrect orientation.

[0021] In addition, the measurement cell of the present invention is a measurement cell used in a centrifugal sedimentation type particle size distribution measuring device, and is characterized in that it has a storage space for storing a dispersion medium, and an internal flow path that communicates with the storage space and holds a sample liquid therein, and that the sample liquid is introduced from the internal flow path into the dispersion medium by the application of centrifugal force. With this measurement cell, an internal flow path connected to the storage space holds the sample liquid, and the sample liquid is introduced from the internal flow path into the dispersion medium by applying centrifugal force, so that the distance between the sample liquid and the dispersion medium can be reduced and the variability in the time it takes for the sample liquid to reach the dispersion medium can also be reduced, thereby improving the measurement accuracy. Effect of the Invention

[0022] According to the present invention as described above, it is possible to improve the measurement accuracy in a particle size distribution measuring device that performs particle size distribution measurement by the line start method. [Brief description of the drawings]

[0023] [Figure 1] 1 is a diagram showing a schematic configuration of a centrifugal sedimentation type particle size distribution measuring device according to one embodiment of the present invention. [Diagram 2] FIG. 2 is a plan view of a cell holder to which the cell of the embodiment is attached. [Diagram 3] 4 is a cross-sectional view showing a schematic state of the measurement cell of the embodiment with a cell cap removed from a cell body. FIG. [Figure 4] 4 is a cross-sectional view showing a schematic state in which a cell cap is attached to a cell body in the measurement cell of the embodiment. FIG. [Diagram 5] 2A to 2C are a plan view, a front view, and a cross-sectional view taken along line AA, showing the configuration of a cell cap according to the embodiment. [Figure 6] 1A and 1B are cross-sectional views showing the embodiment (1) at the stage of sample preparation and (2) before the start of rotation. [Figure 7] 10 is a cross-sectional view showing a state in which the sample liquid reaches a density gradient solution after rotation has started in the embodiment; FIG. [Figure 8] 13A and 13B are a plan view and a cross-sectional view taken along line AA, showing the configuration of a cell cap according to another embodiment. [Explanation of symbols]

[0024] 100 Centrifugal sedimentation type particle size distribution measuring device 2. Measurement cell 3. Cell rotation mechanism 31 Cell holder W SS ...Sample solution W DGS ...Density gradient solution 21H...Opening 21 Cell body R Internal flow passage 22 Cell Cap 2A: Sample inlet 2B: Sample outlet R1: Liquid reservoir R2...Main flow section R2a: Small diameter flow passage R2b: Large diameter flow passage R3: Inlet flow passage R1x...Slope S1...space DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

[0025] Hereinafter, a centrifugal sedimentation type particle size distribution measuring device according to one embodiment of the present invention will be described with reference to the drawings.

[0026] <1. Configuration of particle size distribution measuring device> The centrifugal sedimentation type particle size distribution measuring device 100 of this embodiment measures particle size distribution by the line start method. As shown in FIG. DGS and sample solution W SS The sample liquid W in this embodiment is provided with a measurement cell 2 that contains the sample liquid W, a cell rotation mechanism 3 that rotates the measurement cell 2, and a light irradiation unit 4 and a light detection unit 5 that are provided on either side of a rotational passage area of ​​the measurement cell 2 by the cell rotation mechanism 3. SS is the sample suspension in which the particles are dispersed.

[0027] The measurement cell 2 is, for example, a hollow rectangular cell having a roughly rectangular parallelepiped shape. The measurement cell 2 contains a density gradient solution W DGS This density gradient solution W DGS is formed, for example, by using a plurality of sucrose solutions having different concentrations, and is contained in a multi-layered manner so that the density gradually increases toward the bottom side of the measurement cell 2. In this embodiment, a reference cell 6 is also provided, and the reference cell 6 contains water.

[0028] The cell rotation mechanism 3 rotates the measurement cell 2 so that a centrifugal force is applied to the measurement cell 2 from the side with a smaller density gradient to the side with a larger density gradient.

[0029] Specifically, the cell rotation mechanism 3 has a cell holder 31 to which the measurement cell 2 and the reference cell 6 are detachably attached, and a rotation unit 32 that rotates the cell holder 31 .

[0030] As shown in FIG. 2, the cell holder 31 is, for example, disk-shaped, and the measurement cell 2 and the reference cell 6 are attached so as to sandwich the center of rotation. Here, the measurement cell 2 is attached so that the direction of the density gradient is along the radial direction of the cell holder 31. The cell holder 31 is also formed with an attachment recess 31a corresponding to the cell shape, and the cells 2 and 6 are attached by fitting them into the attachment recess 31a. Furthermore, a guide mechanism (not shown) is provided between the measurement cell 2 and the reference cell 6 and the attachment recess 31a. The guide mechanism is composed of a guide rail provided on one of the attachment recess 31a or the cells 2 and 6, and a guide groove provided on the other. The guide rail or guide groove provided on the cells 2 and 6 may be provided integrally with the cells 2 and 6, or may be provided on a member attached to the cells 2 and 6. The guide mechanism also functions as a restriction mechanism that restricts the attachment direction of the measurement cell 2 or the reference cell 6 with respect to the cell holder 31.

[0031] The measurement cell 2 and the reference cell 6 are configured to be detachable from the cell holder 31. By making the cells 2, 6 detachable from the cell holder 31, the cells 2, 6 can be detached from the device body. When the cells 2, 6 are removed from the device body, the opening and closing lid 13 is in an open state.

[0032] Further, a cover body 33 is provided on the upper surface of the cell holder 31 to prevent the measurement cell 2 and the reference cell 6 from being accidentally removed during rotation (see FIG. 1).

[0033] The measurement cell 2 is attached to the cell holder 31 so that the side with the higher density is on the outside in the radial direction. As a result, when the cell holder 31 rotates, a centrifugal force is applied to the measurement cell 2 from the side with the smaller density gradient to the side with the larger density gradient.

[0034] 1, the rotating unit 32 has a rotating shaft 321 connected to the center of the lower surface of the cell holder 31, and a motor 322 that rotates the rotating shaft 321. The rotation speed of the motor 322 is controlled by the control unit 10. The rotating shaft 321 may be formed integrally with the cell holder 31, or may be formed separately. The rotating shaft 321 may be formed of a single member, or may be formed by connecting a plurality of members.

[0035] The cell holder 31 is accommodated in a storage space 100S formed inside the particle size distribution measuring device 100. A rotation shaft 321 of the rotating part 32 penetrates a lower wall 11 that defines the storage space 100S. An upper wall 12 that defines the storage space 100S is formed by an opening / closing lid 13 that is opened and closed when the measurement cell 2 is attached and detached.

[0036] As shown in FIG. 1, the light irradiating unit 4 is provided below the rotational passage area (cell holder 31) of the cells 2, 6. The light irradiating unit 4 in this embodiment is provided below the lower wall 11 of the storage space 100S, and irradiates light toward the cells 2, 6 through a light-transmitting window 11W formed in the lower wall 11. Specifically, the light irradiating unit 4 has a light source 41, such as an LED, and a condenser lens 42 that condenses the light emitted from the light source 41. The light emitted by the light irradiating unit 4 passes through a light passage hole 31h formed in the cell holder 31 and is irradiated to the measurement cell 2 or the reference cell 6.

[0037] As shown in Fig. 1, the light detection unit 5 is provided above the rotational passage area (cell holder 31) of the cells 2, 6. The light detection unit 5 of this embodiment is provided above the upper wall 12 of the storage space 100S, and detects light transmitted through the cells 2, 6 through a light-transmitting window 12W formed in the upper wall 12. Specifically, the light detection unit 5 has a photodetector 51 and a condensing lens 52 that condenses the light detected by the photodetector 51. The light detected by the light detection unit 5 passes through the cells 2, 6 and a light passing hole 33h formed in the cover body 33, and is condensed by the condensing lens 52.

[0038] The light intensity signal obtained by the photodetector 51 is acquired by the particle size distribution calculation unit 15, and particle size distribution data is calculated by the particle size distribution calculation unit 15. Here, the particle size distribution calculation unit calculates the particle size distribution data using the light intensity signal and a rotation start signal acquired from the control unit 10. The particle size distribution data is displayed on a display by a display unit (not shown).

[0039] <2. Specific configuration of measuring cell 2> The measurement cell 2 of this embodiment is used in the line start method of the centrifugal sedimentation type particle size distribution measuring instrument 100, as described above.

[0040] Specifically, as shown in FIGS. 3 and 4, the measurement cell 2 has an opening 21H at one end, and a density gradient solution W DGS The opening 21H of the cell body 21 is closed, and the sample liquid W is placed inside the cell body 21. SS The sample liquid W is then centrifuged by applying a centrifugal force to the cell cap 22. SS The density gradient solution W flows from the internal flow channel R. DGS It is configured to be introduced into

[0041] The cell body 21 is made of a metal such as aluminum, and has light-transmitting windows W1 and W2 on opposing walls 21a and 21b that face each other. The opposing walls 21a and 21b face each other in a direction perpendicular to the centrifugal force direction. By making the cell body 21 out of a metal, it is possible to provide the cell body 21 with a strength sufficient to withstand centrifugal force and excellent chemical resistance.

[0042] The light-transmitting windows W1 and W2 are formed by providing a glass window member 211 in a through hole formed in the opposing walls 21a and 21b of the cell body 21. The window member 211 is made of glass, and therefore has excellent chemical resistance. The window member 211 is fixed in a liquid-tight manner in the through hole formed in the opposing walls 21a and 21b via a seal member 212 and a fixing member 213. Of the light-transmitting windows W1 and W2, the size of the light-transmitting window W2 on the light-exiting side is made larger than the light-transmitting window W1 on the light-entering side. This allows light to be emitted from the light-transmitting window W2 on the light-exiting side even if a rotational deviation (shake of the rotation axis) occurs due to the cell rotation mechanism 3.

[0043] The cell cap 22 is made of, for example, resin, and is inserted into the opening 21H of the cell body 21 to close the opening 21H, as shown in Figures 3, 4, and 5. Here, the cell cap 22 has an insertion portion 22a that is inserted into the opening 21H of the cell body 21, and a rear end portion 22b that is located outside the cell body 21.

[0044] The internal flow path R formed in the cell cap 22 has a sample inlet 2A formed at one end and a sample outlet 2B formed at the other end. When the cell cap 22 is attached to the cell body 21, the sample inlet 2A is located outside the cell body 21, and the sample outlet 2B is located inside the cell body 21. Specifically, the sample inlet 2A is provided on the upper surface of the rear end 22b, and the sample outlet 2B is provided on the tip surface 22x of the insertion part 22a. With this configuration, when the cell cap 22 is attached to the cell body 21, the sample liquid W flows from the sample inlet 2A to the internal flow path R. SS can be introduced.

[0045] The internal flow path R is connected to the sample inlet 2A. SS The sample liquid W held in the liquid reservoir R1 is then centrifuged to flow through the sample outlet 2B. SS flows into the main flow passage R2, and the density gradient solution W DGS will be introduced.

[0046] Here, the internal flow channel R further includes an introduction flow channel portion R3 that communicates with the sample introduction port 2A and the liquid reservoir portion R1. The introduction flow channel portion R3 is provided along the rotation axis direction of the measurement cell 2 (the up-down direction on the paper in Figs. 3 and 4), and the main flow channel portion R2 is provided along the direction of the centrifugal force applied to the measurement cell 2 (the rotation radial direction, from left to right on the paper in Figs. 3 and 4). That is, in this embodiment, the introduction flow channel portion R3 and the main flow channel portion R2 are perpendicular to each other. Note that the introduction flow channel portion R3 may be formed at an angle with respect to the main flow channel portion R2.

[0047] The main flow path section R2 has a small diameter flow path section R2a, which is an upstream flow path that communicates with the liquid reservoir section R2, and a large diameter flow path section R2b that is provided downstream of the small diameter flow path section R2a and communicates with the sample outlet 2B. The small diameter flow path section R2a is a straight flow path having the same diameter, and the large diameter flow path section R2b is a straight flow path having the same diameter but larger than the diameter of the small diameter flow path section R2a. The small diameter flow path section R2a and the large diameter flow path section R2b are provided coaxially.

[0048] The liquid reservoir R1 is formed at the tip (lower end) of the inlet flow channel R3, and a predetermined amount (for example, 10 μL) of sample liquid W SS The liquid reservoir R1 is connected to the inlet flow channel R3, and is thus an open space at the top. The liquid reservoir R1 is configured to temporarily store the sample liquid W introduced from the sample inlet 2A into the inlet flow channel R3. SS Stores all of the above.

[0049] The positional relationship between the reservoir R1 and the main flow path R2 is such that the main flow path R2 is connected to the upper portion of the reservoir R1. In other words, the main flow path R2 is connected to the introduction flow path R3, thereby communicating with the reservoir R1.

[0050] Here, the liquid reservoir R1 has an inclined surface R1x with an upward gradient toward the main flow path R2 on the side (diametrically outer side) to which the main flow path R2 is connected. SS The liquid reservoir R1 of the present embodiment is configured to have a conical or partial conical shape tapered toward the bottom, thereby providing the inclined surface R1x.

[0051] Furthermore, in this embodiment, in a state where the cell cap 22 is attached to the cell body 21, the cell cap 22 and the density gradient solution W DGS A space S1 is formed between the tip surface 22x of the cell cap 22 and the density gradient solution W contained in the cell body 21. DGS A space S1 is formed between the density gradient solution W contained in the cell body 21 and the water surface. DGS The water surface shape is maintained by the surface tension, and the density gradient solution W DGS does not flow to the cell cap 22 side, and the tip surface 22x of the cell cap 22 and the density gradient solution W DGS A space S1 between the water surface and the

[0052] 5, the cell cap 22 is formed with a lightening portion 221 to reduce its weight. Here, the lightening portion 221 is formed on both the left and right sides of the internal flow path R formed in the center of the insertion portion 22a of the cell cap 22. The lightening portion 221 in this embodiment is a through hole. The lightening portion 221 is an elongated hole formed over a predetermined range along the attachment direction of the cell cap 22.

[0053] The cell cap 22 is also formed with an air vent portion 222 for venting air when the cell cap 22 is attached to the cell body 21. The air vent portion 222 is a communication passage that opens to the tip surface 22x of the cell cap 22 and communicates with the through hole of the hollowed-out portion 221. When the cell cap 22 is attached to the cell body 21, the air inside the cell body 21 is discharged to the outside through the through hole of the hollowed-out portion 221 via the air vent portion 222.

[0054] Furthermore, protrusions 223 are formed on both the left and right side surfaces of the cell cap 22 to ensure close contact with the left and right inner side surfaces of the cell body 21 when the cell cap 22 is attached to the cell body 21. Here, a lightening hole 221 is formed on the inside of the side surface on which the protrusions 223 are formed, so that the side surface portion on which the protrusions 223 are formed elastically deforms inward, and the protrusions 223 elastically come into close contact with the left and right inner side surfaces of the cell body 21.

[0055] In addition, the cell body 21 and the cell cap 22 are provided with a restricting mechanism that restricts the attachment orientation of the cell cap 22 relative to the cell body 21. Specifically, the restricting mechanism is configured by the shape of the opening of the cell body 21 and the shape of the insertion part 22a that is inserted into the opening 21H of the cell cap 22. For example, at least one of the four radiused parts of the shape of the opening 21H of the cell body 21 is made different, and the four radiused parts 22R1, 22R2 of the insertion part 22a of the cell cap part 22 are also formed accordingly (see the front view of FIG. 5). This makes it possible to determine the orientation in which the cell cap 22 can be inserted into the cell body 21.

[0056] Next, the line start method using the above-mentioned measuring cell 2 will be briefly explained. Sample liquid W in measuring cell 2 SS When introducing the sample liquid W, as shown in FIG. 6(1), with the cell cap 22 attached to the cell body 21, the sample liquid W is introduced from the sample introduction port 2A. SS After the introduction, the sample liquid W SS The liquid is held in the liquid reservoir R1 through the introduction flow channel R3 (see FIG. 6(2)).

[0057] After the introduction, the sample introduction port 2A may be closed with a cover 23. By closing the sample introduction port 2A with the cover 23, the sample liquid W SS This prevents the evaporation of the density gradient solution W and also prevents air from forming in the internal flow channel R. DGS It is possible to prevent the liquid from leaking out to the internal flow path R side.

[0058] Then, when the measuring cell 2 is rotated, the sample liquid W SS is subjected to centrifugal force and moves from the liquid reservoir R1 toward the small diameter flow passage R2a of the main flow passage R2, as shown in FIG. 7(1). Then, the measurement cell 2 is rotated and particle size distribution measurement is started at the same time. In this embodiment, the timing when the measurement cell 2 starts to rotate corresponds to the timing when the particle size distribution measurement is started. Here, the sample liquid W SS Since the sample liquid is held in the liquid reservoir R1 through the inlet flow path R3, it is located away from the rotation center of the measurement cell 2 and is easily subjected to centrifugal force due to rotation, and is easily flowed into the main flow path R2. Note that in a device configuration in which the sample liquid is introduced from the rotation center, it is difficult for the sample liquid to be subjected to centrifugal force immediately after introduction, and there is a large variation before it is introduced into the density gradient solution.

[0059] Then, as shown in FIG. 7(2), the sample liquid W flows from the small-diameter flow passage R2a to the large-diameter flow passage R2b. SS As shown in FIG. 7(3), the density gradient solution W DGS This prevents the streaming phenomenon from occurring. DGS Since a space S1 is formed between the density gradient solution W DGS The sample solution W introduced into SS This can reliably widen the gap, thereby improving measurement accuracy.

[0060] <Effects of this embodiment> According to the centrifugal sedimentation type particle size distribution measuring device 100 of the present embodiment, the internal flow path R formed in the cell cap 22 is SS The sample liquid W is held in place and centrifugal force is applied. SSThe density gradient solution W flows from the internal flow channel R. DGS Since the sample liquid W is introduced into the cell cap 22, the timing when centrifugal force is applied to the measurement cell 2 or the timing when the measurement cell 2 is rotated at a predetermined rotation speed can be set as the measurement start timing in the line start method, and the measurement accuracy can be improved. SS Since the sample liquid W SS and density gradient solution W DGS The distance to the sample liquid W can be reduced. SS is density gradient solution W DGS The variation in the time it takes for the sample liquid W to reach the target temperature can be reduced, which also improves the measurement accuracy. SS Since the rotating measurement cell 2 holds the sample liquid W SS This makes it possible to eliminate the need for an introduction mechanism for introducing the

[0061] In this embodiment, the liquid reservoir R1 is provided in the internal flow path R, so that a predetermined amount of sample liquid W SS This makes it possible to keep the position at which the particle size distribution is held constant, thereby improving the reproducibility of particle size distribution measurement.

[0062] Furthermore, the main flow path portion R2 is connected to the upper portion of the liquid reservoir portion R1, and the liquid reservoir portion R1 has an inclined surface R1x with an upward gradient toward the main flow path portion R2 on the side to which the main flow path portion R2 is connected. Therefore, the sample liquid W is reliably stored in the liquid reservoir portion R1 before the measurement cell 2 is rotated. SS During rotation, the sample liquid W is transferred from the liquid reservoir R1 to the main flow path R2. SS It can make it easier to flow.

[0063] Here, by forming the liquid reservoir R1 in a conical or partial conical shape tapering toward the bottom, the liquid reservoir R1 can be easily processed in the cell cap 22.

[0064] Furthermore, in a state where the cell cap 22 is attached to the cell body 21, the cell cap 22 and the density gradient solution W DGSSince a space S1 is formed between the density gradient solution W DGS The streaming phenomenon caused by the contact of the density gradient solution W with the cell cap 22 is mitigated. DGS The sample solution W introduced into SS This can reliably widen the gap, thereby improving measurement accuracy.

[0065] <Other Modified Embodiments> The present invention is not limited to the above-described embodiment.

[0066] For example, in the above embodiment, the particle size distribution is measured by the line start method, but the particle size distribution can be measured by the uniform sedimentation method as well as the line start method. In this case, the measurement cell 2 contains a sample dispersion liquid in which particles are dispersed in a medium. In the uniform sedimentation method, the measurement start timing is the rotation start timing of the measurement cell containing the sample dispersion liquid.

[0067] In this case, the measurement cell has a storage space for storing a dispersion medium, and an internal flow path that communicates with the storage space and holds a sample liquid therein, and the sample liquid is introduced from the internal flow path into the dispersion medium by applying centrifugal force. Specifically, the measurement cell includes a cell body having an opening formed at one end and storing a dispersion medium, and a cell cap that closes the opening of the cell body and has an internal flow path formed therein for holding the sample liquid, and the sample liquid is introduced from the internal flow path into the dispersion medium by applying centrifugal force. The cell body and the cell cap can be configured in the same manner as in the above embodiment. With this measurement cell, the internal flow path that communicates with the storage space holds the sample liquid, and the sample liquid is introduced from the internal flow path into the dispersion medium by applying centrifugal force, so that the distance between the sample liquid and the dispersion medium can be reduced, and the variation in the time it takes for the sample liquid to reach the dispersion medium can also be reduced, which can also improve the measurement accuracy.

[0068] In addition, although the liquid reservoir R1 in the above embodiment has a conical or partial conical shape tapering toward the bottom, it may have various other shapes. For example, the liquid reservoir R1 may have a partial spherical shape, a polygonal prism shape, etc. Even in this case, it is preferable to have an inclined surface R1x with an upward gradient toward the main flow path R2.

[0069] Furthermore, the measurement cell in the above embodiment is a square cell having an outer shape of a rectangular parallelepiped, but it may have another shape.

[0070] In addition, the measurement cell 2 of another embodiment is a density gradient solution W that seeps out through the gap between the cell body 21 and the cell cap 22 by capillary action. DGS 8, a recess (specifically, a groove) G may be formed on the side surface of the insertion portion 22a of the cell cap 22 to prevent the density gradient solution W from leaking out. This recess G is preferably formed in a ring shape around the axis on the side surface of the insertion portion 22a. By forming such a recess G on the side surface of the insertion portion 22a and increasing the gap between the body 21, the density gradient solution W DGS This can stop seepage due to capillary action.

[0071] In addition, various modifications and combinations of the embodiments may be made as long as they do not go against the spirit of the present invention. [Industrial Applicability]

[0072] According to the present invention, it is possible to improve the measurement accuracy in a particle size distribution measuring device that performs particle size distribution measurement by the line start method.

Claims

1. A measurement cell used in the line start method of a centrifugal sedimentation type particle size distribution analyzer, A cell body having an opening at one end and accommodating a density gradient solution, which is a solution in which a density gradient is formed; a cell cap that closes the opening of the cell body and has an internal flow path formed therein for holding a sample liquid; A measurement cell in which the sample liquid is introduced from the internal flow path into the density gradient solution by application of centrifugal force.

2. The internal flow channel has a sample inlet at one end and a sample outlet at the other end, 2. The measurement cell according to claim 1, wherein, when the cell cap is attached to the cell body, the sample inlet is located outside the cell body, and the sample outlet is located inside the cell body.

3. the internal flow path includes a liquid reservoir portion that holds the sample liquid introduced from the sample inlet, and a main flow path portion that communicates with the liquid reservoir portion and with the sample outlet, 3. The measurement cell according to claim 2, wherein the sample liquid held in the liquid reservoir flows into the main flow path section when centrifugal force is applied, and is introduced into the density gradient solution through the main flow path section.

4. 4. The measurement cell according to claim 3, wherein the main flow path portion has a small diameter flow path portion communicating with the liquid reservoir portion, and a large diameter flow path portion provided downstream of the small diameter flow path portion and communicating with the sample outlet port.

5. the internal flow path further includes an inlet flow path section communicating between the sample inlet and the liquid reservoir section, the inlet flow path portion is provided along a rotation axis direction of the measurement cell, The measurement cell according to claim 3 or 4, wherein the main flow path portion is provided along a direction of centrifugal force acting on the measurement cell.

6. The main flow path portion is connected to an upper portion of the liquid reservoir portion, 6. The measurement cell according to claim 3, wherein the liquid reservoir has an inclined surface, on a side to which the main flow path section is connected, that slopes upward toward the main flow path section.

7. 7. The measurement cell according to claim 6, wherein the liquid reservoir has a conical or partial conical shape tapering toward a bottom.

8. The measurement cell according to claim 1 , wherein a space is formed between the cell cap and the density gradient solution when the cell cap is attached to the cell body.

9. The measurement cell according to claim 1 , wherein the cell body and the cell cap are provided with a restricting mechanism that restricts an attachment orientation of the cell cap relative to the cell body.

10. A measuring cell according to any one of claims 1 to 9; and a cell rotation mechanism that rotates the measurement cell so that centrifugal force is applied from the small density gradient to the large density gradient.

11. the cell rotation mechanism has a cell holder to which the measurement cell is attached; The measurement cell is configured to be detachable from the cell holder, 11. The centrifugal sedimentation type particle size distribution measuring device according to claim 10, wherein the measuring cell and the cell holder are provided with a restricting mechanism for restricting an attachment orientation of the measuring cell with respect to the cell holder.

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