CA1184976A - Porous passage means and method for particle analyzing systems - Google Patents

Porous passage means and method for particle analyzing systems

Info

Publication number
CA1184976A
CA1184976A CA000447782A CA447782A CA1184976A CA 1184976 A CA1184976 A CA 1184976A CA 000447782 A CA000447782 A CA 000447782A CA 447782 A CA447782 A CA 447782A CA 1184976 A CA1184976 A CA 1184976A
Authority
CA
Canada
Prior art keywords
passage
particle
fluid
particles
sensing zone
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired
Application number
CA000447782A
Other languages
French (fr)
Inventor
Robert H. Berg
Richard F. Karuhn
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Particle Data Inc
Original Assignee
Particle Data Inc
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Priority claimed from US05/907,010 external-priority patent/US4290011A/en
Application filed by Particle Data Inc filed Critical Particle Data Inc
Priority claimed from CA000373830A external-priority patent/CA1165393A/en
Priority claimed from US06/264,199 external-priority patent/US4434398A/en
Application granted granted Critical
Publication of CA1184976A publication Critical patent/CA1184976A/en
Expired legal-status Critical Current

Links

Landscapes

  • Sampling And Sample Adjustment (AREA)

Abstract

ABSTRACT
A method of and means for controlling orientation of particles through a sensing zone in a particle analyzing system, which facilitates particle shape determination, comprises laminar flow orientation of the particles in a stream moving through an elongate straight passage coaxially aligned with an elongate sensing zone longer than the longest particle to be sensed and analyzed.
The particles are carried through the sensing zone in an isokinetic laminar flow sheath of fluid.

Description

SPECIFICATION
.
This invention is concerned with improvements for particle analysis systems, and is more particularly concerned with a method of and means for facilitating the controlling of orientation of particles for passing through the sensing zone of the particle ana].yzing system.
Substantial advances have been made in isok.inetic sampling and controlled particle orientation for particle analysi.s techniques, both those involving photic sensing zone and those involving electrolytic sensing zones.
Considerable attention has been given to attain improved fidelity of particle dimension-related signals caused by particle passage through a given sensing zone. An example o~ an impoxtant advance in this direction is found in Robert H. Berg, U.S. Patent No. 4,001,678, entitled "~isplacement Metering With Independent Ancillary Flow".
Therein is taught how to attain improved fidelity of particle dimension response in particle sensing or counting apparatus by so-called hydrodynamic focusing in a sensing orifice in one of a pair of tubes immersed in a bath of particle-free electrolyte and utilizing independently contro].led coaxial flows, substantially accurately proportioned between ~ilamentary and sheathing ~lows, mainiaining accuracy in particle suspension metering and therefore particle concen-tratlon measurement. In that patent an apparatus and methodare disclosed especially useful in association with particle sensing counting and analyzing instruments of the kind a~allable from the assignee of the present application, Particle Data, Inc., under the trademarks "Electroæone", ~0 "CELLOSCOPE" and "ELZOME". Such apparatus operates on the principle o~ passing a sample of electrol~te with entra.ined '7~

particles through an orifice providing a properly constrictæ
path for an electrical current. Sensing of particles flowing through the orifice is effected by modulation of the electrical current by the particles, such modulation being amplified and suitably recorded, analy2ed, visually ~bserved on an oscilloscope, and the like. The measurement of particle lengths by this particle sensing method was initially reported by David R. Kominz in "Correlations of Length and Volumen Measurements in Myofibril Suspensions", Biophysical Journal, Vol. II, 1971, pp. 47-65. However, in spite of the substantial improvements attained according to the teachlngs of the aforesaid patent, there has still been some problem in achieving accurate particle length and shape determinations.
We have discovered a practical, simple and efficient method of and means for solving that problem, and for improving sheathed particle flow in general in particle analysis systems.
To this end, the present invention provides a method of controlling the presentation of particles in fluid suspension to a sensing zone to facilitate particle parameter determination in a particle analysis system of a type responsive to electrical signals generated by particles passing through the sensing zone, and comprising, ` 25 transporting the particles through an elongate passage and presenting the particles from a downstream end of the passage to said sensing zone, supplying particle-containing fluid to an entrance into said passage r supplying sheathing fluid to the outside of a porous wall throuqh which said passage extends, and efecting a differential pressure causing a particle-containing fluid stream to traverse said ~9L9~
_3~
passage ~rom said entrance to said downstream end and causing movement of said sheathin~ fluid through said porous wa]ls into sheathing relation to said particle-containing fluid stream.
For practice of the method, the present invention provides apparatus for controllinq the presentation of particles in fluid suspension to a sensing zone to facilitate particle parameter determination in a particle analysis system of a type responsive to electrical signals generated by particles passing through the sensing zone, comprising means defining an elongate passage for trans-porting the particles in suspension therethrough for presentation at the downstream end of the passage to said sensing zone, said passage means comprisin~ a porous wall, means for supplying particle containing fluid to an entrance into said passage and for supplying sheathing fluid to said porous wall outwardly relative to said passage, and means for effecting differential pressure for causing a particle-containing stream to traverse said passage from said entrance to said downstream end and for causing movement of said sheathing fluid through said porous wall into sheath.ing relation to said particle-containing stream.
Other objects, features and advantages of the invention will be readily apparent from the following description of representative embodiments thereof, taken in conjunction with the accompanving drawinqs, although variations and modifications ma,v be effected without departing from the spirit and SCoPe of the novel concepts embodied in the disclosure, and in which:
FIG. 1 is a schematic illustration o a particle analysis system of the electric curren~ mo~ulation pulse generation method, embodying principles oE the present invention.
FIG. 2 is a schematic adaptation for photic zone detection of particles in the practice of the present invention.
FIG. 3 is a fragmental vertical sectional detail view showing a represen~ative form of apparatus providing cooperative particle orientation and sensin~ zone passages for accurate particle shape determination according to the principles of the present invention.
~ IG. ~ is a schematic illustration showing the relationship of rod like particle traversing through the sensing zone of the apparatus of FIG.S. l, 2 and 7 relative to pulse curve observable on an oscilloscope~
FIG. 5 schematicallv illustrates a pulse curve generated bv a generally spherical particle as observed on an oscilloscope.
FIG. 6 schematically illustrates a pulse curve by a relatively flattened or disk-shaped particle as observed on an oscilloscope.
FIG. 7 illustrates a modified embodiment of the particle orientation and sensing zone passages within the principles of the present invention.
By wav of example, the principles of the present invention may be em~odied in displacement metering apparatus 5 (FIGS. l and 3j embodying significant improvements over the disclosure in the aforesaid U.,S. Patent 4~001,67g. To any extent necessary disclosure of that patent is incorporated herein by re:Eerence.
The apparatus 5 is especially ada~ted Eor use in a '7~

sensing system 6, often referred to as particle counter, where accurate isokinetic sample meterin~ is essential.
Particle-entraining fluid such as liquid electrolyte may be supplied for analysis from a suitable particle suspension source such, for example, as ma~ be contained in a supply chamber 7 in a container or beaker 8 or fro~ any other source through a conduit 9. From the supply chamher 7 the particle entraining liquid is transported ln a laminar flow stream through an elongate, preferably straight particle aligning first passage 10 of sufficient length to cause stable orientation of particles longitudinally in the direction of flow in that passage. In a convenient con-struction the passage 10 is adapted to extend through a plug member 11 coupled into a tubular lower end fitting extension 12 of a preferably test tube-like container 13 defining a double walled chamber 14 with a larger diameter tubular container 15. Mounted adjacently above the down-stream end of the passage 10 is an orifice plug member 16 providing a second elongate straight sensing zone passage 17 of greater length than the longest particle to be analyzeda The passage 17 has its upstream end in spaced coaxial alignment with the passage 10 and its downstream end discharging into an elongate chamber 18 within the container 13. Although the plug member 11 may be formed ~5 from glass, using usual glass fabricating techniques, the : orifice member 1~ is preferably made from a material in which the passage 17 can be held to substantially accurate diameter throughout its sensing zone length, a solid polymeric material such as Delrin having been found suit-able for the purpose. Such a material can readily be drilled to form the passage 17 in the small multi-micron diameter appropriate for the desired particle analysis.
While the containers 13 and 15 may be formed in an integral one piece arrangement, they are preferably two separate generally telescopically related hollow parts to facilitate separation and cleaning. Leading upwardly from the chamber 18 is a passage 19 provided by a vertical member 20 supported in any desirable manner~ At their upper ends the containers 13 and 15 are secured to the lower end portion of the member 20, preferably detachably for cleaning purposes. A tapered Eitting terminal 21 on the lower end of the member 20 may receive a complementarily shaped head 22 at the upper end of the container 13, such as in a standard glass joint. A fluid tight coupling of the tubular container 15 with the inner container 13 may be by means of an O-ring 23 adjacent to the lower end of the member 15 engaging in an annular shoulder groove 23a on the container 13, and and O-ring 24 adjacent the upper end of the member 15 engaging an annular shoulder 25 on the member 13. Means comprising one or more resilient bands 26 engage anchoring hooks 27 and 28 on respectively the lower end of the member 20 and the upper end of the member 15 and draw the members together whereby to maintain the assembly in operatively tight but separable connection.
At its upper end, the passage member 2Q has a valve 29 which controls connection of the passage 19 and the chamber 18 with a suitable vacuum source by way of a relatively small diameter vertical suction tube 30 having at its lower end a suction port 31 axially aligned in adjacent spaced relation to the downstream or exit end of the passage 17. Leading off from the member 20 adjacently below where the upper end of the tube 30 is secured, is a 7~

branch duct 32 leading to means ~or supplying fluid to and for effecting displacement of fluid in the chamber 18. A
line 33 communicates a source of fluid through a passage branch 34 extending from the upper portion of the me~ber 15 to cornmunicate with the chamber 14. The various connecting joi~ts and couplinqs of the system are cons-tructecl to be unyielding to pressure differences as high as desired in use, and the entire internal circuit of passageways and chambers is fluid filled. A pin hole 30a in the upper end of the tube 30 provides a bleed-off for any entrapped air in that area. A branch 15a on the member 15 at the upper end of the chamber 14 may serve to bleed air from that area. If preferred, and especially for handling of heavier particles, orientation of the apparatus just described may be inverted so that the passage 10 delivers downwardly to the passage 17. In such a rearrangement the air pocket bleed-offs will have to be reoriented.
Sensing of particles flowing through the sensing zone passage 17 is effected by modulation of an electrical current by the particles, generating pulses which are amplified and suitably recorded, totalized, visuallv observed on an oscilloscope, and the like. For this purpose, an electrode 35 is located in suitable operative relation to the chamber 18 such as in the adjacent portion of the passa~e 19 so as to be effective at the downstream or discharge end of the passage 17. An electrode 37 is located in the chamber 14 to be effective at the u~stream or entry end of passage 17. This provides for electronic connection with the appropriate analyzing instrumentalities of the system 6 represented schematically as including an amplifier 38 with which is connected an oscilloscope 39 for visual observation of pulses generated by particles tr~versing the sensing zone passage 17. From the amplifier 38 the pulses are received in means 38a for digitizing the pulse height, and means 38b for digitizing pulse length~
From the digitizing means 38a and 38b the pulse siqnals pass to a data accumulator and processln~ analyzer 38c for data accumulation and processing. Connected with the analyzer 38c are suitable means 38d such as a counter, computer, or the like, to provide a display record.
Representative hydraulic operating and flushing circuitry for the apparatus 5 comprises a vacuum gauge shown in this lnstance as a U-shaped metering siphon or manometer 40 which may be on the order of that described in Berg U.S. Patent 3,481,202, and is operatively connected at its upper end to ~he branch duct 32. Leading from that connection is a hydraulic line 41 having therein a three-way valve 42 and communicating with a hydraulic line 43 having a three-way valve 44 at one side of the connection of the line 43 with the line 41 and a flow regulating valve 45 at the other side of the connection of the line 43 with the line 41. At its opposite ends, the line 43 is connected in circuit with a diluent supply controlling and venting valve 47 by way of a loop circuit 48 connected at an intermediate point by a branch 49 with the line 43 adjacent to the valve 44 and by means of an opposite intermediate branch 50 with the line 43 adjacent to the valve 45. At one side of the loop circuit 48 as divided by connection with the line 43, communication by means of a branch 51 is effected with the diluent and vent valve 47. In the other half of the loop circuit 48 a flow regulating valve 52 is located adjacent to the branch 50 and a two-way valve S3 is located in the loop on the other side of branch line 54 which communicates with the loop between the valves 52 and 53 and leads to a three-way valve 55 for controlled communication with the duct 33 which is connected to the sheathing flow supply branch 34 leading to the chamber 14 of the apparatus. A hydraulic line 57 leads from a vacuum source through the three-way valve 29 to the vacuum end of the member 20 and the tuhe 30. A braneh hydraulic conneeting line 58 is connected in communication with the bleed-off branch 15a leadincl from the member 15. A two-way valve 59 is in control of the line 58. A common control ~0 is desirably provided for ~he valves 29, 42 and 55. A common eontrol 61 is desirably provided for the valves 44, 53 and 59. The valve 47 may have an independent eontrol. Each of the regulating valves 45 and 52 may be independently adjustable for regulating flow through its associated hydraulic line.
In an operating cycle of the apparatus 5, particles passing through ~he sensing zone passage 17 are analyzed for a number of eharaeteristics such as shape, mass or partiele unit volume, num~er of particles per unit volume of carrier liquid, and particle length. For some kinds of particles length is a critical characteristic. For example, it may be desirable to determine what percentage of partieles in an isokinetic sample are of a pa ticular ~5 length and/or shape~ Determination as to the concentration of particles having identifiable length in an isokinetic sample may be desired, as for example, asbestos particles when testing for environmental contamination.
We have discovered that much improved analytical results are obtained by having the passage 10 of sufficient length, considered with regard to the flow velocity o~ the '7~

filamentary stream in which the particles in an isokinetic sampling are transported, to orient the particles longitu-dinally in the passage. The filamentary .stream of longitudinally oriented particles is then transferred a limited distance from the downstream end of the orienta-tion passage lO into the sensincJ æone passa-~e 17 across a subchamber 64 where the filamentary stream is enveloped in a laminar flow sheath of particle free fluid. To enhance laminar sheathing of the filamentary stream of particles the plug member ll has a conical sharp edged tip portion 65 extending into and to a substantial extent through the subchamber 64 toward the upstream end of the passage 17. Entry into the passage 17 is preferablv through a funnel like entrance 67 the surface of which is desirably sl.ightly arched to a smooth inner end transition into the straight sensing zone part o-f the passage 17.
For isokinetic sampling, the apparatus 5 is conditioned to effect a low pressure differential in the chamber lg relative to the supply chamber 7 and the sheathing flu.id chamber 14 so that a predetermined volume of particle carrying electrolvte will be drawn from the supply chamber 7 through the orientation passage 10 at sufficient velocity and electrolyte entrainment to attain the desired longitudinal separation and lengthwise orientation of the particles transported in filamentarv stream through the passage lO. Integrity of the filamen-tary particle stream i.s maintained in the transition interval between the downstream end of the passage 10 and the upstream end of the passage 17, aided by enveloping the filamentarv stream isokinetically in a laminar non-turbulent flow sheath of clear ~l.uid in the chamber ~4 J'h,~ 'd L~9 7~;

supplied from the chamber 1~ hy way of ports 6~ in the wall of the member 13. As each particle traverses the length of the passage 17, the pulse signal generated by it is amplified, analyzed, variously discriminated and recorded in the sensing system 6, such as ~or number per unit volume of isokinetic sample, relative or proportional sizes, shapes, len~th and the like.
Waste particles leaving the exit end of the passage 17 are efficiently collected and dra~ off in isokinetic manner into the suction catcher conduit tube 30 through the suction port 31 which is desirably defined by a flared funnel like mouth 71 Suction attained by connection of the suction or catcher tube 30 with vacuum source by opening the valve 29 not only draws into the port 31 the waste particle stream leaving the passage 17, but also ambient fluid in the chamber 18 which sheaths the waste particles in a flush-flow stream and substantially prevents migration of any particles therefrom in the interval between the passage 17 exit and the suction port 31. This prevents spent particles from circulating in that area, and avoids modulation aberrations from possible turbulence in the chamber 18, assuring achieve~ent of a high degree of accuracy in the sensing zone analysis.
In operation, assuming that the supply chamber 7 has a fill of electrolyte carrying particles to be analyzed, and the remainder of the system is prepared for isokinetic samplingJ the valve control 60 is actuated to open the valves under its control, namely the valves 29, 42 and 55, and the valve control 61 is actuated to close the valves 44, 53 and 59 under its control, and the valve ~7 is actuated to connect a diluent :input line 62 throu~h ;7 the branch 51 with the loop circuit 48. Since the suction tube 30 is now connected with vacuum source, isokinetic sampling proceeds at a controlled rate and as long as desired to complete the analysis. When it is desired to fill and flush the system, the valves 29, 42 and 55 are controlled by the controller 60 to be in the open position, the valves 44, 53 and 59 controlled by the controller 61 are actuated to be in the open position, and the valve 47 is in the diluent connecting position.
For draining the system, all of the valves 29, 42 and 55 and the valves 44, 53 and 59 are open, and the valve 47 is actuated into the vent position, venting through a line 53.
For back flushing, the valve control 60 is operated : 15 to close the valves 29, 42 and 55, the valve control 61 is operated to open the valves 44, 53 and 59, and the valve 47 is operated to open the system to diluent input through the line 62. Should it be desired to clean out the diluent supply lines 33, 54 and the upstream portion of the passage 17, the valve controller 60 may ~e operated to close the valve 42 and open the valves 29 and 55 while the valves 44, 53 and 59 remain closed, and the valve 47 is opened to the vent side 63 and closed to the diluent input side 62.
Instead of electrical current modul.ation or electrolytic zone sensing of particles in the sensing zone passage 17, other types of sensors may be employed such as a sonic zone sensox wherein a particle is detected by reflection of an ultrasonic beam in a liquid medium r or other types of devices operative to generate pulses which vary in amplitude according to a particular para-meter. ~y way of example, a photic zone sensor 75 ~Fig. 2) '76 may be located in cooperation with the sensing zone orifice member 16 of displacement metering apparatus 5'.
For this purpose the member 16' is transparent so that particles travelling through the sensing zone passage 17' will be illuminated by a beam of ]ight from a lens assembly 77 in front of a light source 78 with a light trap 79 having a black llght absorbent surface disposecl in the path of the beam on the opposite side oE the member 16'. Light reflected from particles passiny through the sensing zone passage 17' is transmitted through a lens assembly 80 to the face of a photomultiplier tube 81 which applies signals to a pre-amp and gain control circuit 82.
A light trap 83 is disposed opposite the sensing zone 17~
on the axis of the lens assembly 80 and the photomultiplier 81, to provide a dark background. This type of sensor may also be used with the light source disposed opposite the llyht sensing means, and with pulses being thereby generated in respect to particles blocking the light.
Such a photic zone sensor is described, for example, in Berg et al U.S. Patent 3,345,502.
In the modification of Fig. 7, the apparatus 5" is a simplified version of the apparatus 5 which has already been described. For determining the shape of some types of particles it may not be necessary to provide a clear fluid sheathing of the laminar flow particle-carrying stream in transition between the particle orienting first passage and the second sensing zone passage. Accordingly, all of the structure involving the tubular container 15 and the sheathing flow supply chamber 14 of the apparatus 5 of Figs. 1 and 3 can be eliminated, while the remainder of the apparatus and the sensing system 6 may remain the ~ 7 same. In this modified arranyement an elongate combined orientation passage and sensing zone passaye member 84 which has a tapered end portion 85 fits snugly in a com-plernentary tapered coaxial bore 87 in a base end portion 88 of the modified tubular member 13'. Axi~lly within the member 84 is a first, particle orienting pasSaCJe 10' into which leads a preferably smoothly contoured bellmouth entrance 89 at the free end of the member 84. The arrange-ment is such that particle containinq suspension is drawn from a source which mav be supplied in a chamber such as the chamber 7 in a beaker ~ demonstrated in Fig. 3. The orientation passage 10' is dimensioned both in cross sectional flow area and in length to assure stable orientation of the particles longitudinally in the ~assage as the particles are transported in a laminar flow stream of the elec~rolytic fluid in which the particles are carried~ According to well known hydraulic principles, the velocity of a stream in laminar flow through a passage is greater at the center of the passage due to the drag of the passage walls on the perimeter of the stream.
~ccordingly as the stream is caused to traverse the orientation passage 10' the particles are caused to assume a stable longitudinal orientation in the stream.
From the first particle orientation in the passage 10' the particle pass immediately into a second elongate straight sensing zone passage 17" of greater length than the longest particle to be analyzed, such second passage being,in effect,a continuation of the passage 10' and having its upstream or entrance coaxially aligned with the downstream end of the first passage 10'. ~lthougll the electrode 37' may be oriented relat.ive to the member ~l ln 9t7~

the manner of the electrode 37 in Fig. 3, in this instance, the elec~rode 37', corresponding to the electrode 37 in Figs. 1 and 3, is shown as mounted in the member 84 at the entrance into the senslng zone passage 17" and is properly shaped for the intended purpose. Leading from the electrode 37' i5 an insulated electrical lead wire 90 unaffected by immersion in the particle suspension electro-lyte into which the member 84 extends in use. It will be understood that the cooperatiny electrode will correspond to the electrode 35 in Figs. 1 and 3. Similarly as described in connection with the sensing zone passage 17 in Figs. 1 and 3, the particles flowing through the sensing zone passage 17' effect modulation of an electrical current, thus generating pulses which are amplified and suitably recorded, totalized, visually observed and the like in the same manner as described in connection with Figs. 1 and 3. If additional sheathing of the filamentary stream in a laminar flow sheath of particle free fluid is desired, at least that portion of the member 84 upstream from the electrode 37' may be made of a suitable porous material such that as the stream is caused to traverse the coaxial passages 10' and 17'l, electrolyte free and clear of particles may be drawn throuqh the porous filter wall of the member 84 into the passage 10'. It will thus be apparent that a particular advantage of ~he porous filter wall structure of the member 84 is that the particle free sheathing electrolyte may be derived from a common reservoir 91 containing particles 92 suspended in the electrolyte 93 in which member 84, at least to the extent of the porous filter portion thereo, is immersed for receivlny particle-carryin~ electrolyte throuyh the entrance 89, and is adapted for simultaneously receiving particle-free electrolyte through the porous filter wall to provide a sheath of particle-free electrclyte for the particle carrying stream travellin(~ through the passage.
Isokinetic action is effected similarly as in Figs. 1 and 3 by suction applied through the suction and catcher tube 30 which has its entrance port in alignment with the e~it from the passage 17" in substantially the same orientation and for the same purpose as already described hereinbefore.
Substantial accuracy as to particle length as well as shape discrimination are attained not only for recording but also for instantaneous visual observation hy way of unique pulse patterns on the screen of the oscilloscope 39, during the smooth, sheathed passage of up to thousands of particles per minute through the sensing zone passage 17, 17' or 17". ~or example, Fig. 4 demonstrates the sharp, strong, particle length pulses observable on the oscilloscope 39 as linear, i.e., rod-like fiber-like, prolate spheroid, particles traverse the sensing zo~e passage 17, 17' or 17" seriatim. Illustratively, three particle positions A, B and C are shown. In position A, as the particle passes the entrance into the sensing zone, progress of the particle is observable as an ascendina substantially diagonal pulse line or ramp 95 which travels upwardly a substantially straight line, the ramp time rQpresenting the len~th of the particle. In position B, the particle is completely within the detection zone in the passage 17 whereupon the pulse shape or curve flattens off as shown at 97, the amplitude of which represents the volume of the particle. Then as the particle exits from the passage 17, 17' or 17" as illustrated bv the position '7~

~ 17-C, the pulse signal ramps in a substantially straight line diagonally downwardly as indicated at 98, which ramp time also representing the length of the particle.
Where particles in shapes other than linear pass S through the sensing zone passage 17, 17' or 17" the pulse shapes observed on the oscilloscope will differ from the Fig. 4 straight line angular pulse ramps of the linear particles. Hence, during isokinetic sampling in the apparatus 5, 5' or 5", involving diverse particles, linear particles can be discriminated from non-linear. For example, as depicted in Fig. 5, generally spherical, i.e., orthospheroid, ball-like, particles will be observed on the oscilloscope to produce a pulse shape of rather squared off form rising substantially vertically at the entry end, then flattening at the top while the particle is fully in the sensing zone, and then dropping off sub-stantially vertically at the departure or exit end wilh only slight transition curvatures at top and bottom of the vertical legs~
Fig. 6 demonstrates pulse shape observable when a particle of oblate spheroid shape, i.e~ r flake, disk of any of various relative thicknesses, or similar shape, traverses the sensing zone passage. As such a particle enters the sensing zone the oscilloscope pulse shape display will show a generally flat S or ogee slanting upward curve to a relatively flat horizontal top while the particle is fully in the sensing zone and then dropping off with a flat S or ogee curve as the particle leaves the sensing zone.
As to any of the particle identifying pulse shapes as represented in Figs. 4, 5 and 6, particle volume may also be discriminated by the pulse height. Thus the orthospheroid particles may show substantially greater pulse height than extreme prolate spheroid or extreme oblate spheroid particles, although within each of those categories there may be variations in particle volume.
Thus a substantial range of analytical results can be obtained not only in discrimination as to categories of particles but also as to determination of dimensional parameters within categories, where desirable.
It will be understood that variations and modifica-tions may be effected without departing from the spirit and scope of the novel concepts of this invention.

Claims (14)

The embodiments of the invention in which an exclusive property or privilege is claimed are defined as follows:
1. Apparatus for controlling the presentation of particles in fluid suspension to a sensing zone to facilitate particle parameter determination in a particle analysis system of a type responsive to electrical signals generated by particles passing through the sensing zone, comprising: means defining an elongate passage for transporting the particles in suspension therethrough for sensing zone presentation at a downstream end of the passage; said passage means comprising a porous wall;
means for supplying particle-containing fluid to an entrance into said passage, and for supplying sheathing fluid to said porous wall outwardly relative to said passage; and means for effecting differential pressure for causing a particle-containing stream to traverse said passage from said entrance to said downstream end and for causing movement of said sheathing fluid through said porous wall into sheathing relation to said particle-containing stream.
2. Apparatus according to claim 1, wherein said sensing zone and said elongate passage defining means comprise coaxially aligned portions of a member, and an electrode located at the downstream end of said elongate passage, said electrode comprising an element of said particle analysis system.
3. Apparatus according to claim 2, wherein said electrode comprises a ring embedded in and concentric with said passage.
4. Apparatus according to claim 1, wherein said porous wall comprises a filter so that said passage means may be immersed in a reservoir containing particle-carrying electrolyte for not only supplying particle containing fluid to said entrance, but also particle-free sheathing fluid through said porous wall.
5. Apparatus according to claim 1, wherein said means defining an elongate passage comprises an elongate member having a downstream end portion of substantially conical shape for substantially fluid tight engagement with a complementary surface of an associated member.
6. For use in apparatus for controlling the presentation of particles in fluid suspension caused to move by differential pressure through a sensing zone to facilitate particle parameter determination in a particle analysis system of a type response to electrical signals generated by particles passing through the sensing zone;
means defining an elongate passage for transporting the particles in suspension therethrough for sensing zone presentation at a downstream end of the passage; said passage means comprising a porous wall about said passage and adapted for receiving particle-containing fluid through an entrance into said passage from a source communicating with said entrance t and said porous wall being adapted to be exposed to sheathing fluid on the outside of said wall so that the sheathing fluid from the outside of said wall can pass through the porous wall into said passage in response to the differential pressure which is adapted to cause a particle-containing stream derived from said source to traverse said passage from said entrance to said downstream end and through said sensing zone and also to cause movement of the sheathing fluid through the porous wall into sheathing relation to the particle-containing stream in the passage.
7. Means according to claim 6, wherein the sensing zone and said elongate passage defining means comprise coaxially aligned portions of a member, and an electrode located at the downstream end of said elongate passage and comprising an element of the particle analysis system.
8. Means according to claim 6, wherein said electrode comprises a ring embedded in said member coaxially aligned with said passage.
9. Means according to claim 6, wherein said porous wall comprises a filter so that said means can be immersed in particle-containing electrolyte for providing both the particle-containing fluid in the passage and particle-free sheathing fluid through said wall into said passage.
10. Means according to claim 6, comprising a member having said porous wall and provided with a substantially conical surface adapted to interfit in substantial fluid tight connection with a complementary surface of an associated member.
11. A method of controlling the presentation of particles in fluid suspension to a sensing zone to facilitate particle parameter determination in a particle analysis system of a type responsive to electrical signals generated by particles passing through the sensing zone, and comprising: supplying particle-containing fluid to an entrance into an elongate passage;
supplying sheathing fluid to the outside of a porous wall through which said passage extends; and effecting a differential pressure causing a particle-containing fluid stream to traverse said passage from said entrance to said downstream end and through said sensing zone, and causing moving of said sheathing fluid through said porous wall into sheathing relation to said particle-containing fluid stream, and thereby presenting the particles in the sheathed stream to said sensing zone.
12. A method according to claim 11, which comprises causing the sheathed particle-containing stream to travel uninterruptedly from said downstream end of said passage into and through said sensing zone past an electrode which is part of said particle analysis system.
13. A method according to claim 11, which comprises filtering the sheathing fluid through said wall so that the sheathing fluid enters said passage through said wall in particle free condition.
14. A method according to claim 11, wherein said passage and porous wall are part of a member, and immersing said member in a reservoir providing a common supply of the particle-containing fluid and sheathing fluid and filtering particles from the sheathing fluid on passing through said porous wall into said passage.
CA000447782A 1978-05-18 1981-03-25 Porous passage means and method for particle analyzing systems Expired CA1184976A (en)

Applications Claiming Priority (3)

Application Number Priority Date Filing Date Title
US05/907,010 US4290011A (en) 1978-05-18 1978-05-18 Particle length and volume comeasurement with controlled orientation
CA000373830A CA1165393A (en) 1981-03-25 1981-03-25 Particle length and volume comeasurement with controlled orientation
US06/264,199 US4434398A (en) 1978-05-18 1981-05-15 Porous passage means and method for particle analyzing systems

Related Parent Applications (1)

Application Number Title Priority Date Filing Date
CA000373830A Division CA1165393A (en) 1978-05-18 1981-03-25 Particle length and volume comeasurement with controlled orientation

Publications (1)

Publication Number Publication Date
CA1184976A true CA1184976A (en) 1985-04-02

Family

ID=27167011

Family Applications (1)

Application Number Title Priority Date Filing Date
CA000447782A Expired CA1184976A (en) 1978-05-18 1981-03-25 Porous passage means and method for particle analyzing systems

Country Status (1)

Country Link
CA (1) CA1184976A (en)

Similar Documents

Publication Publication Date Title
US4395676A (en) Focused aperture module
CA1256825A (en) Method and apparatus for sorting particles
EP0131287A1 (en) Apparatus and method for regulating sheath fluid flow in a hydrodynamically focused fluid flow system
US4290011A (en) Particle length and volume comeasurement with controlled orientation
US4165484A (en) Particle counting apparatus utilizing various fluid resistors to maintain proper pressure differentials
US5266495A (en) Method and apparatus for controlled instrumentation of particles with a filter device
Fuchs Sampling of aerosols
US4434398A (en) Porous passage means and method for particle analyzing systems
EP0029662A1 (en) Automated method for cell volume determination
JPH01287442A (en) Flow rate control method and apparatus
EP0515658A1 (en) Aspiration method for hematology analyzing apparatus
JP3294285B2 (en) Instrumentation processing method and apparatus for particles using a filter
US3979669A (en) Particle analyzing system
US5293219A (en) Fiber length analyzer
CA1184976A (en) Porous passage means and method for particle analyzing systems
US3398079A (en) Electrochemical apparatus
CA1165393A (en) Particle length and volume comeasurement with controlled orientation
US4491786A (en) Transducer for measuring particles suspended in a fluid
US4140966A (en) Particle analyzing apparatus and fluid circulating system therefor
US3554037A (en) Continuous flow pipeline sampling orifice arrangement
US4206650A (en) Device for introducing samples into fluid analyzer
US3163699A (en) Sampling apparatus for flame photometer
US4226532A (en) Device for granulometric analysis of particles in fluids
US4863868A (en) Apparatus for detecting the presence of micro organism in liquid
CA1090424A (en) Aperture module for use in particle testing apparatus

Legal Events

Date Code Title Description
MKEX Expiry