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Volume 8, Issue 6, Pages 72-81 (December 2003)


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Article Outline

The Fiftieth Anniversary of the Coulter principle

Introduction

Act I

Act II

Act III

Summary

Epilogue

Acknowledgment

References

Copyright

The Fiftieth Anniversary of the Coulter principle 

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Introduced in the mid-1950s, the Coulter Principle became the foundation of an industry responding to the need for automated cell-counting instruments. The industry developed in three acts, as Wallace H. Coulter and his brother Joseph R. Coulter, Jr., developed the simple idea of passing cells through a sensing aperture. In Act I, Wallace's desire to automate the routine erythrocyte count led to a simple idea, the definition of the Coulter Principle, its patenting, its acceptance by the National Institutes of Health, and its description at a national conference. In Act II, the Coulter brothers addressed the practicalities of a commercial instrument and of a business organization to support its manufacture and sale. In Act III, a broad research effort developed regarding volumetric errors originating in functional characteristics of the sensing aperture, and the brothers' growing organization found solutions permitting introduction of increasingly automated hematology analyzers. Today the industry thrives, with several participants.

Introduction 

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“You can't patent a hole.” With that opinion, several attorneys dismissed Wallace H. Coulter's hopes of patenting his method for automating the erythrocyte count.1 For each specimen, a technician spent some 30 tedious minutes at a microscope counting the red cells in a standard chamber, the result being only rarely repeatable. Automating such counts had tantalized Wallace (Fig. 1) since he had read Moldavan's 1934 note proposing photoelectric counting of cells in a suspension as it flowed through a capillary tube mounted on a microscope.2 Over a decade had elapsed before Wallace discovered a better method, and a second decade was to pass before he was prepared to announce it.


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Figure 1. Wallace H. Coulter encountered the routine erythrocyte count during his visits to hospitals for General Electric X-Ray Corporation and began experiments toward automating it after returning to Chicago in 1946. In 1947, he discovered one form of the Coulter Principle.


Act I 

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After gathering technical experience elsewhere, Wallace returned to Chicago in 1946 and was soon joined in his quest by his brother, Joseph R. Coulter, Jr. (Fig. 2). As he later reminisced about their work in a basement laboratory:3 “The approach originally was to count blood cells going down a capillary tube, passing through a light beam, like counting people going down a corridor, but we weren't getting very good signals. We asked the question, ‘Is there some way, besides modulating a light beam, to generate electrical pulses by the passage of a cell?’ Although we didn't know it at the time, blood cells are insulators—so we arrived at a solution by modulating an electric current instead of a light beam.”


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Figure 2. Joseph R. Coulter, Jr., after his Army service, joined his brother Wallace in a small basement laboratory and helped solve many difficulties while incorporating the Coulter Principle into a practical automated instrument. In 1958, he helped found Coulter Electronics, Inc.


In a characteristically simple solution, by 1947 Wallace had reduced the capillary tube to its minimum length:1 “When we started we didn't have much money, so we made an aperture by making a small hole with a hot needle in a piece of cellophane from a cigarette package. It didn't hold up long, but we were able to count some cells.” Held onto the end of a glass tube by a rubber band, the punctured cellophane separated two electrodes connected to a source of electric current while cells suspended in ionic medium were passed through it simultaneously with the current. A cell's displacement of liquid equal to its own volume within the aperture was proportionally signaled by a voltage pulse between the electrodes passing the current through the aperture.

The brothers had found electrical contrasts between cells and the suspending medium that were some 10 times the ones obtained photoelectrically, the resultant voltage pulses readily permitting an accurate count of the cells in the volume of cell suspension passing through the aperture. This discovery had prompted Wallace's unexpectedly prolonged search for an attorney willing to prepare a patent application. Finally, in 1948, he was introduced to Irving Silverman who recognized the new method's significant potential, and in August 1949, a patent application was filed.

But the patent examiner also doubted that a hole could be patented. Fortunately, he also surmised that if an application were to include examples other than an axial current and sensing path through an aperture, a patent might be obtained on the principle of sensing particles in a constricted current path.1 An analogous path transverse to the aperture suspension flow was described, as well as apertures having non-circular cross sections. An insulated needle sweeping past particles in a stationary suspension was another example, a particle's presence being signaled by a pulse in the current between the moving needle and a second electrode contacting the conductive suspending medium. The new Coulter Principle being thus defined, the seminal patent was issued 50 years ago on October 20, 1953, with the preferred embodiment being a pinpoint aperture formed in the lower wall of a test tube.4

Meanwhile, the Coulter brothers had continued development, with emphasis on automation where feasible. With volunteer help from Walter Hogg, Joseph's friend from Army days, the brothers assembled an experimental instrument under contract to the Office of Naval Research: a mechanical metering system moved a controlled volume of cell suspension through the aperture while an interface unit provided it an electric current and sensed resultant signal pulses via a voltage amplifier having an adjustable threshold. Signal pulses above threshold triggered a pulse counter (Berkeley Scientific Model 410; Beckman Instrument, [then] Richmond, CA) mounted atop the interface unit. Repeated runs of a sample at successively increasing thresholds permitted manual recording of a cumulative distribution of cell size. The need to detect partial occlusion of the aperture soon became evident, so an oscilloscope was added to allow simultaneous monitoring of the signal pulses and the threshold setting.

Experience also emphasized the need to meter a precise volume of cell suspension through the aperture. Together, the Coulter brothers invented an elegant solution based on a mercury manometer (Fig. 3). As Joseph once remarked:5 “It was the manometer that made the counter work. It was simple, it was easy to control, and it kept working.” Combined with a microscope focused on the aperture, this metering system formed the basis of a sample stand that would remain essentially unchanged for over 30 years. In 1952, the first two instruments incorporating the new sample stand were built; the interface electronics and oscilloscope were integrated into a single compact console also including decade counters to accumulate the voltage pulses. In 1953, these prototypes went to the National Institutes of Health (NIH) for evaluation, and in May 1956, a patent application was filed on the manometer metering system.6


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Figure 3. Functional schematic of the Coulter sample stand, co-invented by the Coulter brothers.6 When stopcock F is opened, the mercury in the manometer reservoir R is drawn upward by a small vacuum pump connected to P, and the resulting pressure head causes movement of mercury column J after the stopcock is closed, drawing sample suspension E from the sample vessel through the hole in aperture wafer A into sample tube B. The aperture wafer and sample tube are made of dielectric materials having an electrical resistivity much greater than that of the suspending medium. Via connections H and I, electrodes C and D couple an electrical current through the aperture, and the resultant signal pulses to an amplifier and pulse counter (not shown). The volume of sample to be analyzed is determined by three control electrodes (K, L, M) penetrating the wall of the manometer tubing; when the flowing mercury causes electrical contact between K and L, the pulse counter starts, while mercury contact with M at a calibrated distance from L terminates it. Thus, cells are only counted in suspension flowing through the aperture at constant velocity, so permitting cell concentration to be determined as the count in the suspension volume equal to the volume of mercury between the electrodes L and M. The second stopcock G is only opened to fill or flush the sample tube with clean suspending media via O. The microscope for viewing the aperture is not shown. Adapted from Wallace's paper.7


The Coulter Principle was formally announced on October 3, 1956 in Wallace's sole technical paper:7 “In the new counter individual cells are caused to move through a small constricted electric current path in the suspending fluid and detection is based upon differences in electrical conductivity between the cell and the suspending fluid. The constricted current path is analogous to a light beam of small dimensions in an optical system. In passing thru the small current path in the fluid the individual blood cell changes the electrical resistance in the circuit, and causes a change in the voltage drop appearing across the current path. The electric current path of small dimensions and the flow of cell bearing fluid thru the path is provided for with a very simple structure. The boundary of the current path is the bore of a submerged orifice of small dimensions in the wall of an insulated vessel. ” In Figure 3, this submerged orifice is the central hole in aperture wafer A.

Shortly thereafter, the two NIH evaluations were published.8., 9. Both noted the improved accuracy, efficiency, and convenience of the Coulter method for counting erythrocytes. The journal issue containing one evaluation8 also contained the first advertisement for the new Coulter Counter®. The second evaluation9 attributed skewness in the size distribution to cell coincidence and presented a manual method for correcting the count for coincidence loss. It also included preliminary data on leukocyte counting.

The feasibility of automating significant hematological tasks had been demonstrated, but the work of commercialization yet lay ahead. Reliable mounting of the aperture had proven difficult.10 The mercury used in the manometer metering the suspension through the aperture was a concern, emphasizing an advantage of the mechanical system used in the experimental counter.11 The voltage source used to provide excitation current to the aperture produced unacceptable sensitivity to characteristics of both the aperture and the medium used to suspend cells.12 The need for precise sample dilutions had been recognized in the NIH studies, indicating the value of an automatic diluter.13 As Joseph later summarized a decade of preparation,5 “We knew there were problems, but we also knew we had something useful.” As another decade began, solutions to these problems would soon appear in the patents just cited.

Act II 

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The sensing aperture (the hole in wafer A, Fig. 3) was the heart of the Coulter Counter®, and it now received the brothers' first priority. For many potential applications, aperture diameters smaller than 100 μm would be required, with tight tolerances on both dimension and geometry. The poor repeatability of apertures made directly in the wall of sample tubes prompted experimentation with glass aperture wafers, formed as a cross section of a capillary tube. But cements used to mount the wafers failed, and the apertures were distorted by heat if fused to the sample tube. Ring jewels used as watch bearings were tried, with help from Hermann Foery (Swiss Jewel Company, [then] Locarno, Switzerland), who provided jewels that functioned as early low-noise apertures.1 A method for flame fusing the jewels to the sample tubes was developed5 through work with Sam Gutilla (then of Del Mar Scientific, Chicago, IL). The precision cylindrical hole in the jewels proved unaffected by fusing and provided a durable conduit for flow of both the electrical current and the sample suspension. By the end of 1958, a patent application could be filed on an interchangeable sample tube (B in Fig. 3) incorporating a fused ring jewel.10 The thickness of the jewel was chosen to provide an aperture length-to-diameter ratio of approximately 0.75 to minimize the particle coincidence noted in both the basic patent4 and a NIH study.9

By 1958, the Coulter brothers were ready to found Coulter Electronics, Inc., together with its sales organization, Coulter Sales Corporation. Two of the parent company's first full-time employees were long-time volunteers Joseph R. Coulter, Sr., and Walter Hogg. The Coulters' father had served as weekend secretary and accountant from the beginning, but now at age 68, he retired as a railroad telegrapher and began a second career working with his sons, only going into partial retirement in 1971. Walter would become the first employee to reach 20 years of service and the only employee to be named as an inventor on more U.S. patents than Wallace (95 and 82, respectively).

In hindsight, 1958 was a year of significant beginnings. Kilby demonstrated the first integrated circuit, an oscillator. Soon afterward, Noyce and Hoerni developed the planar process that enabled the microelectronics explosion. Townes and Schawlow described requirements for masers to function at optical frequencies, and within two years, Maiman demonstrated the first laser. All of these developments would play significant roles in the future of the new company.

At the beginning, replications of the prototypes,14 now known as the Model A Coulter Counter®, were assembled by Ernie Yasaka as Wallace could sell them. For industrial use,15 a stirrer was added to the sample stand (Fig. 4). Of immediate concern to the new company was a paper demonstrating a direct correlation between pulse amplitude and particle volume.16 By coupling a Coulter Counter® to a single-channel pulse-height analyzer (PHA) having dual variable pulse thresholds, Kubitschek had generated the first differential size distribution, thus highlighting two disadvantages of the Model A: First, its single threshold required generation of a cumulative size distribution via multiple sample runs at successively increasing thresholds,14., 16. requiring substantial time and calculation to manually produce a differential size distribution. The need for automated sizing was apparent. Second, the voltage source used to provide aperture current made pulse amplitudes sensitive to the dimensions of the particular aperture, the resistivity of the particular suspending medium, and temperature-induced variation in the latter,14., 15. all of which would thus complicate automation of accurate counting and sizing.


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Figure 4. The Model A Coulter Counter® with the industrial version of the sample stand (Fig. 3) shown at the right. The round black object at the upper right of the stand is the stirrer motor used to keep heavy industrial particles in suspension; the stirrer was not used on the stand for blood cell counting. The console contains, from left to right, the mechanical totalizer used for the slowly accumulating high-value digits, the three decade counters used for the rapidly accumulating low-value digits, and the oscilloscope display tube. Controls for the single threshold and the aperture current appear below the display tube.


Encouraged by favorable results on automated leukocyte counting,17 the company introduced an improved instrument18 in 1960, just as broad interest in accurate cell and particle sizing was emphasized.19 A current source for aperture excitation replaced the original voltage source, and a dual-threshold current-sensitive amplifier for sensing resultant particle pulses replaced the original single-threshold voltage amplifier.12 Consequently, the Model B Coulter Counter® was practically insensitive to the factors limiting the original counter, and with its thresholds interlocked to form a movable channel controlled by a sequencing four-second timer, it allowed an accessory Model H distribution plotter20 to automatically accumulate a 25-channel differential size distribution from 100-s sample runs.18 Development of the Model C Coulter Counter® was also advancing—the prototype included a 12-channel PHA. Not only did its more than 350 vacuum tubes contribute significantly to heating the company's facility, the resulting bulk also required disassembly for it to be moved. By 1961, when the company relocated from Chicago to Hialeah, Florida, a tabletop Model C was available to industry.21

During the 1960s, Model A and Model B counters proved useful for the counting and sizing of both erythrocytes and leukocytes17., 18., 22., 23., 24., 25., 26., 27., 28. (see reviews25., 27.) and were gaining application in microbiology16., 29., 30. and industrial particle analysis.31 Meanwhile, worries arose. In 1959, a competitive instrument based on the Coulter Principle was described.32 In 1960, the skewed distributions seen in the NIH study9 were confirmed.23 The cumbersome diluter13 provoked a customer to design his own22 and a better Coulter design.33 In 1962, the length-to-diameter ratio of the sensing aperture was reported to affect sizing resolution.34 A future competitor patented a derivative form of the Coulter Principle,35 and a principal of Coulter Sales Corporation patented a derivative sample tube on his own,36 later leaving to become another competitor.37 Further, early efforts at platelet counting encountered unexpected interference, apparently from small particles not seen by phase microscopy.38 Lushbaugh et al. raised the sizing ante by coupling a 100-channel PHA to a Model A Coulter Counter®,39., 40. and soon, several groups were coupling purpose-built Coulter particle sensors to commercial PHAs29., 41., 42., 43., 44., 45., 46., 47., 48. providing as many as 512 channels.29 The increasing availability and sophistication of volumetric tools increasingly made artifacts apparent in size distributions for a variety of cells and particles. In Wallace's snapshot phrasing,1 “Challenges are good, and we sure had our share of good.”

Act III 

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The sensing aperture (the hole in wafer A, Fig. 3) was the heart of the Coulter Principle, and designing a Coulter Counter® to automatically compensate for its functional characteristics now became the main priority. One of the NIH studies9 had noted the aperture's sensitive volume being about three times that of the geometric aperture, a consequence of the electric field established by the excitation current throughout the volumes of suspending medium in the sample vessel and sample tube (Fig. 3). Cells (or particles) interacted with this electric field as they were carried through the sensing aperture by the analogous hydrodynamic field produced by the metering system. For both aperture fields, the significant particle interactions occurred in a sensitive volume containing the sensing aperture and extending semi-elliptically outward from its entry and exit orifices approximately three or four aperture diameters.

Thus, by displacing volumes of the conductive suspending medium equal to its own, each cell distorted the electric field throughout its extent—but most significantly while passing through the sensing aperture.49 As a result, the volume of the cell was compared to that of the aperture. A change in the electrical resistance of the aperture, typically of about 1 part in 50,000, and the accompanying small change in ionic current through the aperture, produced the signal pulses that enabled counting and sizing of the cells. Accurate counting and repeatable sizing thus required extremely smooth suspension flow through the aperture.

Unlike the ionic current flow, due to the suspending medium's mass and viscosity, suspension flow was influenced by both inertia and a boundary layer at the surface of the sensing aperture, respectively. Consequently, these reacted to the microgeometry of the aperture and its two orifices,50 producing a kinetic flow field that was asymmetric about the midpoint of the aperture axis. The toroidal recirculating flow pattern at the aperture's exit orifice carried particles back into the aperture's sensitive volume, thereby generating secondary pulses that erroneously contributed to the particle count. For example, Walter Hogg found that the phantom particles encountered in an early platelet study38 were erythrocytes recirculating into the sensitive volume, their secondary pulses causing them to also be counted as platelets. Auxiliary flow sweeping the particles away from the exit orifice prevented both particle recursion and secondary pulses.51

It was always expected that coincident passage of cells through the aperture's sensitive volume would reduce cell counts through masked particle pulses,4., 7. but count loss was statistically predictable from cell concentration in the suspension.9., 52., 53., 54., 55., 56., 57., 58., 59., 60. Thus, single-channel counts were automatically correctable by suitable circuitry,61 and a late version of the Model D Coulter Counter® introduced this approach. However, atypical pulses resulting from coincident particle passage also induced broadening in size distributions,45 and typical erythrocyte size distributions demonstrated skewness.39., 40., 41., 44., 62. The skewness, attributed in one of the NIH studies9 to coincidence, was soon found in size distributions for other cell types38 and particles.31., 63., 64. With improvements in volumetric accuracy, size distributions proved to be bimodal for erythrocytes.40., 41., 65. All such distribution artifacts reduced sizing resolution.

By the late 1960s, studies related to origins of volumetric artifacts were burgeoning,28., 30., 44., 45., 49., 65., 66., 67., 68., 69., 70., 71., 72., 73., 74., 75., 76., 77., 78. and several groups were building experimental systems based on the Coulter Principle.28., 29., 30., 41., 45., 46., 47., 73., 79. The troublesome sizing artifact arose when particles passed through the sensing aperture at different radial distances from its axis.65 At low effective particle concentrations, apertures having lengths several times their diameter were shown to improve sizing resolution,34., 41., 67., 80. as did an auxiliary flow surrounding a smaller suspension stream so as to hydrodynamically focus particles through the aperture near its axis.81., 82., 83., 84., 85. At typical particle concentrations, sampling signal pulses at aperture midpoint67 or selecting them according to duration79 substantially improved volumetric accuracy (see overviews65., 67., 78., 86., 87., 88.).

A very significant result of the investigation into aperture functional properties was the first cell sorter,48., 70., 89., 90., 91. invented and built to determine whether bimodal erythrocyte distributions40., 41. were fact or artifact. Fulwyler combined the Coulter Principle with inkjet technology, and used the result to sort cells from a single distribution mode. When the sorted cells were resized, the resulting distribution demonstrated the original bimodal form and, thereby, the artifactual nature of such distributions.

During this investigative explosion, models of the Coulter Counter® followed advances in electronics, the transistorized Model F being developed concurrently with the Model C, to replace the Model A. The sample stand was adapted to flow-through use92., 93. and the Model J distribution plotter replaced the Model H plotter. In the latter part of 1968, the first automated hematology analyzer,94 the seven-parameter Coulter Counter® Model S, was introduced.95., 96. Simultaneously, the transistorized Model T Coulter Counter® replaced the Model C for industrial applications. Based on integrated circuitry, the Z family of counters was released in 1970, and the Channelyzer® volume analyzer appeared in 1972, simultaneously with the industrial TA family, which unitized counter and 16-channel PHA circuitry. Soon after, instruments came to rely on microprocessors.

Wallace often commented,1 “If it's useful, people will buy it.” Sales had increased with each level of improvement, but there was unprecedented demand for the Model S Coulter Counter®. Although a solid foundation for an industry was now in place, volumetric artifacts originating in particle interactions with the fields in the vicinity of the aperture82., 83. still required solutions that neither increased particle coincidence nor reduced the effective particle concentration within the aperture. Characteristics of the artifactual pulses were sufficiently distinctive that these pulses could be automatically edited from the pulse-data stream by specialized circuitry, and numerous such pulse-editing circuits were developed.97., 98., 99., 100., 101., 102., 103., 104., 105., 106., 107. Some of these enabled the performance of the automated nine-parameter Model S-Plus and the S-Plus II two-part differential analyzers introduced in 1977 and 1980, respectively. Others were used in the Coulter STKR, with its fully automated walkaway sample handling system, or with the VCS flow-cell technology introduced in 1986 and 1987, respectively. This design philosophy continues in the current Coulter LH 700 Series (Fig. 5).


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Figure 5. The latest descendant of the Model A Coulter Counter®, the LH 750 analyzer, is a fully automated instrument that determines 26 reportable hematological parameters. When combined with the LH Slide Maker and the LH Slide Stainer to form the LH 755 Hematology System, it also automates preparation of microscope slides from selected whole-blood samples.


Summary 

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The hole that could not be patented inspired a principle that could. Originating in Wallace's desire to automate a tedious routine, the Coulter Principle provided a repeatable physical measurement of cell or particle volume when appropriately calibrated and, in turn, has inspired a broad range of automated instrumentation of increasing sophistication and complexity. The broad acceptance of instruments incorporating Wallace's Principle has prompted development of similar instruments by a number of companies. The Coulter Principle remains the method of choice for volume measurement of microscopic particles and has become incorporated in numerous standards in a variety of scientific fields.31 By the late-1980s there were some 50,000 Coulter Counters® in operation in the United States alone. Publications describing practical applications or theoretical design aspects now number in the thousands, and related patents now number in the hundreds.

When Beckman Instruments, Inc., acquired Coulter Corporation in late 1997, the Coulter brothers' company had grown to some 5000 employees, with revenues in the hundreds of millions of dollars annually.3., 108. Acceptance of their instruments enabled support of automation in other technical areas, most notably flow sorters and flow cytometers, which owe major debts to the Coulter sensing aperture and its apparent simplicity.86 Among other applications of laboratory automation the brothers supported was pattern-recognition microscopy,109 experience from which contributed to the Coulter LH Slide Maker (Fig. 5).

Wallace's basic patent4 defined his principle via two forms of sensing aperture, both in dielectric material. He preferred the axial excitation/sensing version due to its ease of manufacture and linear volume response. Interestingly, due to the electric double layer that forms on conductive materials exposed to an electric field in ionic media, this form can be made to work even if the aperture is formed in some conductive materials.110., 111. In addition to particle volume, the resulting signal pulses are responsive to the electrochemical properties of the particle, the material containing the sensing aperture, and the suspending media. The axial form also can function if the sensing aperture is made in a composite structure comprising Wallace's original aperture wafer between two conductive elements.87., 88. The resulting size distributions can have minimal artifact due to particles either recirculating at the aperture exit orifice or passing through the aperture away from its axis.112

The axial implementation of the Coulter Principle has by far received the greatest attention, but attempts to scale it downward in size encounter a limit due to thermal noise. In principle, the second form using excitation and sensing transverse to the suspension flow may offer the ability to sense smaller particles, but at expense of requiring a volume linearization based on the selected geometry of aperture and electrodes.35., 113., 114., 115.

Will Act IV cast the Coulter Principle in a role including one of these, or will it feature a totally new combination of emerging science and familiar technology?

Epilogue 

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While Wallace was still looking for the insight that led him to the Coulter Principle, his father wrote a poem for the brothers:1 Why not direct it, / It's within your control. / You can nourish and guide it, / You can reach your goal! / Make use of this gift, / Let it labor for good. / Your thoughts are your life; / Geniuses use them—you should!

This play in three acts suggests that both he and Joseph understood well their father's advice. Wallace saw few problems but many opportunities. He was widely recognized in the scientific community for his inventive insights. Joseph acknowledged problems but saw them as challenges. He implemented much, in both technical and business areas. Both men believed that science should serve humanity, and the two combined their complementary strengths to successfully initiate or foster numerous developments in today's scientific armamentarium. The tremendous humanitarian value of their efforts needs no comment.

Despite their many achievements, the Coulter brothers (Fig. 6) remained both modest and enthusiastic about innovative ideas. They were devoted to family, which to both included employees, and were dependable friends. Both were always ready to unselfishly share their time, experience, and knowledge. Both expected a self-reliant best effort but were supportive when a goal honestly pursued proved unreachable. When one of the author's well-intentioned efforts proved not only counterproductive but also costly, Wallace met an apology with, “People who don't try, don't make mistakes,” to which Joseph added, “Some things are more important than money.”


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Figure 6. Wallace (left) and Joseph Coulter in the mid 1990s. Wallace was born February 13, 1913 and died August 7, 1998. Joseph was born August 18, 1924 and died November 27, 1995. In life, both acted on a belief that science should serve humanity, and their legacy is the humanitarian value of their efforts.


It has been remarked that a person is fortunate to have one good teacher. Those who were privileged to work with the Coulter brothers had two. This brief retrospective is dedicated to the memory of these exceptional brothers who both enjoyed and encouraged the quest to do better.

Acknowledgements 

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Dawn W. Graham assisted with archival research and laboratory work.110 W. Gerry Graham made experimental prototypes.87., 110. The quotation from Wallace's paper7 is used with permission by the International Engineering Consortium (www.iec.org).

References 

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1.. 1. Coulter, W.H. Coulter Corporation. Private communication to the author. 1976–1997.

Free on-line access to the patents listed below is available at the U.S. Patent and Trademark Office: http://patft.uspto.gov/netahtml/srchnum.htm. Click in “Query” and type the desired patent number, then click “Search”. Full text will not be available for the older patents; for patent images, click on “Help”, then follow “How to access full-page images”.

2.. 2. Moldavan A. Photo-electric technique for the counting of microscopical cells. Science. 1934;80:188–189.

3.. 3. Law G. From basement to board room: inside Coulter Electronics. New Miami. 1989;1(April):31–35 52–53.

4.. 4. Coulter, W.H. Means for counting particles suspended in a fluid. U.S. Patent 2,656,508, filed August 27, 1949 and issued October 20, 1953.

5.. 5. Coulter, J.R., Jr. Coulter Corporation. Private communication to the author. 1983–1995.

6.. 6. Coulter, W.H.; Coulter, J.R., Jr. Fluid metering apparatus. U.S. Patent 2,869,078, filed May 9, 1956 and issued January 13, 1959.

7.. 7. Coulter WH. High speed automatic blood cell counter and cell size analyzer. Proc Natl Electron Conf. 1956. 12. Chicago: National Electronics Conference, Inc; 1957; pp 1034–1040.

8.. 8. Brecher G, Schneiderman M, Williams GZ. Evaluation of electronic red blood cell counter. Am J Clin Pathol. 1956;26:1439–1449. MEDLINE

9.. 9. Mattern CFT, Brackett FS, Olson BJ. Determination of number and size of particles by electrical gating: blood cells. J Appl Physiol. 1957;10:56–70.

10.. 10. Coulter, W.H.; Berg, R.H.; Heuschkel, F.L. Scanner element for particle analyzers. U.S. Patents 2,985,830 and 3,122,431; filed December 29, 1958 and issued May 23, 1961 and February 25, 1964, respectively.

11.. 11. Coulter, W.H.; Coulter, J.R., Jr. Fluid metering system and apparatus. U.S. Patent 3,015,775; filed January 9, 1959 and issued January 2, 1962.

12.. 12. Coulter, W.H.; Hogg, W.R.; Moran, J.P.; Claps, W.A. Particle analyzing device. U.S. Patent 3,259,842; filed August 19, 1959 and issued July 5, 1966.

13.. 13. Coulter, W.H.; Coulter, J.R., Jr.; Claps, W.A. Automatic diluting apparatus. U.S. Patent 3,138,294; filed November 17, 1960 and issued June 23, 1964.

14.. 14. Berg RH. Rapid volumetric particle size analysis via electronics. IRE Trans Indust Elect. 1957;PGIE6:46–52.

15.. 15. Berg RH. Electronic size analysis of subsieve particles by flowing through a small liquid resistor. Am Soc Testing Mat. 1958;Tech publ no. 234:245–249.

16.. 16. Kubitschek HE. Electronic counting and sizing of bacteria. Nature. 1958;182:234–235. MEDLINE | CrossRef

17.. 17. Akeroyd JH, Gibbs MB, Vivano S, Robinette RW. On counting leukocytes by electronic means. Am J Clin Pathol. 1959;31:188–192. MEDLINE

18.. 18. Brecher G, Jakobek EF, Schneiderman MA, Williams GZ, Schmidt PJ. Size distribution of erythrocytes. Ann N Y Acad Sci. 1962;99:242–261. MEDLINE | CrossRef

19.. 19. Kubitschek HE. Electronic measurement of particle size. Research. 1960;13:128–135.

20.. 20. Coulter, W.H.; Siegelman, A. Particle distribution plotting apparatus. U.S. Patent 3,331,950; filed February 27, 1961 and issued July 18, 1967.

21.. 21. Lines RW, Wood WM. Automatic counting and sizing of fine particles. Ceramics. 1965;16:27–30 (May) and 28–31 (June).

22.. 22. Magath TB, Berkson J. Electronic blood-cell counting. Am J Clin Pathol. 1960;34:203–213. MEDLINE

23.. 23. Ruhenstroth-Bauer G, Zang D. Automatische zählmethoden: das Coulter'sche partikelzählgerät (Automatic counting method: the Coulter particle counting instrument). Blut. 1960;6:446–462.

24.. 24. Nelson MG, Carville J. Blood cell counting: a comparison of the EEL and Coulter machines. Irish J Med Sci. 1962;6th series(no. 442):447–456.

25.. 25. Pruden EL, Winstead ME. Accuracy control of blood cell counts with the Coulter Counter. Am J Med Tech. 1964;30:1–35.

26.. 26.  Boroviczény CH,  G DEStandardization in haemotology III. Bibl Haemat. 1966;24:2–82. MEDLINE

27.. 27. Boroviczény CH, G DE. On the standardization of the blood cell counts. Bibl Haemat. 1966;24:2–30. MEDLINE

28.. 28. Gutman J, Hofmann G, Ruhenstroth-Bauer G. Exact methods for measuring the volume distribution of erythrocytes on the basis of the Coulter Principle. Bibl Haemat. 1966;24:42–51. MEDLINE

29.. 29. Harvey RJ, Marr AG. Measurement of size distributions of bacterial cells. J Bacteriol. 1966;92:805–811. MEDLINE

30.. 30. Kubitschek HE. Counting and sizing micro-organisms with the Coulter Counter. In:  Ribbons RW,  Norris JR editor. Methods in Microbiology. Vol. 1:London: Academic Press; 1969;p. 593–610.

31.. 31. Lines RW. The electrical sensing zone method (the Coulter Principle). In:  Knapp JZ,  Barber TA,  Lieberman A editor. Liquid- and Surface-Borne Particle Measurement Handbook. New York: Marcel Dekker; 1996;p. 113–154.

32.. 32. Oulie C. Telling av de röde blodlegemer ved deres elektriske motstand (Counting of red cells by their electrical resistance). Nordisk Medicin. 1959;62:1421–1425. MEDLINE

33.. 33. Coulter, W.H. Automatic diluting apparatus. U.S. Patent 3,138,290; filed August 31, 1962 and issued June 23, 1964.

34.. 34. Kubitschek HE. Loss of resolution in Coulter counters. Rev Sci Instr. 1962;33:576–577.

35.. 35. Imadate, H. Particle counting device including fluid conducting means breaking up particle clusters. U.S. Patent 3,390,326; filed November 14, 1962 and issued June 25, 1968.

36.. 36. Berg, R.H. Peripherally locked and sealed orifice disk and method. U.S. Patent 3,266,526; filed November 26, 1962 and issued August 16, 1966.

37.. 37. Berg RH. Sensing zone methods in fine particle size analysis. Materials Research & Standards. 1965;5:119–125.

38.. 38. Sipe CR, Cronkite EP. Studies on the application of the Coulter electronic counter in enumeration of platelets. Ann N Y Acad Sci. 1962;99:262–270. MEDLINE | CrossRef

39.. 39. Lushbaugh CC, Maddy JA, Basmann NJ. Electronic measurement of cellular volumes (I. Calibration of the apparatus). Blood. 1962;20:233–240. MEDLINE

40.. 40. Lushbaugh CC, Basmann NJ, Glascock B. Electronic measurement of cellular volumes (II. Frequency distribution of erythrocyte volumes). Blood. 1962;20:241–248 See also: Correspondence. Blood 1964, 23, 403–405. MEDLINE

41.. 41. Van Dilla MA, Basman NJ, Fulwyler MJ. Electronic cell sizing. Report LA-3132-MS. Los Alamos: Los Alamos Scientific Laboratory; 1964; pp 182–204.

42.. 42. Buckhold B, Adams RB, Gregg EC. Osmotic adaptation of mouse lymphoblasts. Biochim Biophys Acta. 1965;102:600–608. MEDLINE

43.. 43. Lushbaugh CC, Lushbaugh DB. Rapid electronic red blood cell sizing as an aid to clinical diagnosis. Southern Med J. 1965;58:1208–1212.

44.. 44. Van Dilla MA, Basman NJ, Fulwyler MJ. Electronic cell sizing. Report LA-3610-MS. Los Alamos: Los Alamos Scientific Laboratory; 1966;.

45.. 45. Adams RB, Voelker WH, Gregg EC. Electrical counting and sizing of mammalian cells in suspension: an experimental evaluation. Phys Med Biol. 1967;12:79–92. MEDLINE

46.. 46. Edwards VH, Wilke CR. Electronic sizing and counting of bacteria. Biotech Bioeng. 1967;9:559–574.

47.. 47. Anderson EC, Petersen DF. Cell growth and division, (II. Experimental studies of cell volume distributions in mammalian suspension cultures). Biophys J. 1967;7:353–364. MEDLINE | CrossRef

48.. 48. Van Dilla MA, Fulwyler MJ, Boone IU. Volume distribution and separation of normal human leucocytes. Proc Soc Exptl Biol Med. 1967;125:367–370.

49.. 49. Gregg EC, Steidley KD. Electrical counting and sizing of mammalian cells in suspension. Biophys J. 1965;5:393–405. MEDLINE | CrossRef

50.. 50. Graham, M.D.; Dunstan, H.J.; Arboleda, C.A. Through-flow in Coulter particle-sensing conduits. Submitted to Cytometry 2003.

51.. 51. Hogg, W.R. Aperture tube structure for particle study apparatus. U.S. Patent 3,299,354; filed July 5, 1962 and issued January 17, 1967.

52.. 52. Wales M, Wilson JN. Theory of coincidence in Coulter particle counters. Rev Sci Instr. 1961;32:1132–1136.

53.. 53. Wales M, Wilson JN. Coincidence in Coulter Counters. Rev Sci Instr. 1962;33:575–576.

54.. 54. Princen LH, Kwolek WF. Coincidence corrections for particle size determinations with the Coulter Counter. Rev Sci Instr. 1965;36:646–653.

55.. 55. Strackee J. Coincidence loss in bloodcounters. Med & Biol Engng. 1966;4:97–99.

56.. 56. Samyn JC, McGee JP. Count loss with the Coulter Counter. J Pharm Sci. 1965;54:1794–1799. CrossRef

57.. 57. Mercer WB. Calibration of Coulter Counters for particles ∼1 μ in diameter. Rev Sci Instr. 1966;37:1515–1520.

58.. 58. Princen LH. Improved determination of calibration and coincidence correction constants for Coulter Counters. Rev Sci Instr. 1966;37:1416–1418.

59.. 59. Edmundson IC. Coincidence error in Coulter Counter particle size analysis. Nature. 1966;212:1450–1452. CrossRef

60.. 60. Mazumdar M, Kussmaul KL. A study of the variability due to coincident passage in an electronic blood cell counter. Biometrics. 1967;23:671–684. CrossRef

61.. 61. Pontigny, J.A.; Collineau, C.J. Digitalized coincidence correction method and circuitry for particle analysis apparatus. U.S. Patent 3,626,164; filed June 16, 1969 and issued December 7, 1971.

62.. 62. Winter H, Sheard RP. The skewness of volume distribution curves of erythrocytes. Aust J Exp Biol Med Sci. 1965;43:687–698.

63.. 63. Matthews BA, Rhodes CT. The use of the Coulter Counter for investigating the coagulation kinetics of mixed monodisperse particulate systems. J Coll Interface Sci. 1968;28:71–81.

64.. 64. Matthews BA, Rhodes CT. Some observations on the use of the Coulter Counter Model B in coagulation studies. J Coll Interface Sci. 1970;32:339–348.

65.. 65. Shank BB, Adams RB, Steidley KD, Murphy JR. A physical explanation of the bimodal distribution obtained by electronic sizing of erythrocytes. J Lab Clin Med. 1969;74:630–641. MEDLINE

66.. 66. Weed RI, Bowdler AJ. The influence of hemoglobin concentration on the distribution pattern of the volumes of human erythrocytes. Blood. 1967;29:297–312. MEDLINE

67.. 67. Bull BS. On the distribution of red cell volumes. Blood. 1968;31:503–515. MEDLINE

68.. 68. Jacobi H, Hanstein A, Hanstein W, Künzer W. Erfahrungen mit einem elektronischen erythrocytenzählgerät bei zählungen und volumenverteilungskurven (Experience with an electronic erythrocyte counting instrument by counting and volume distribution). Klin Wschr. 1967;45:154–160. MEDLINE | CrossRef

69.. 69. Coopersmith A, Ingram M. Red cell volumes and erythropoiesis (I. Age:density:volume relationship of normocytes). Am J Physiol. 1968;215:1276–1283. MEDLINE

70.. 70. Fulwyler MJ, Glascock RB, Hiebert RD, Johnson NM. Device which separates minute particles according to electronically sensed volume. Rev Sci Instr. 1969;40:42–48.

71.. 71. Coopersmith A, Ingram M. Red cell volumes and erythropoiesis (II. Age:density:volume relationships of macrocytes). Am J Physiol. 1969;216:473–482. MEDLINE

72.. 72. Ur A, Lushbaugh CC. Some effects of electrical fields on red blood cells with remarks on electronic red cell sizing. Brit J Haemat. 1968;15:527–538. MEDLINE | CrossRef

73.. 73. Harvey RJ. Measurement of cell volumes by electric sensing zone instruments. In:  Prescott DM editors. Methods in Cell Physiology. Vol. III:New York: Academic Press; 1968;p. 1–23.

74.. 74. Grover NB, Naaman J, Ben-sasson S, Doljanski F. Electrical sizing of particles in suspensions I. Theory. Biophys J. 1969;9:1398–1414 See also: Errata, Biophys J. 1972, 12, 1117. MEDLINE | CrossRef

75.. 75. Grover NB, Naaman J, Ben-sasson S, Doljanski F, Nadav E. Electrical sizing of particles in suspensions (II. Experiments with rigid spheres). Biophys J. 1969;9:1415–1425 See also: Errata, Biophys J. 1972, 12, 1117. MEDLINE | CrossRef

76.. 76. Eckoff RK. A static investigation of the Coulter Principle of particle sizing. J Sci Instr. 1969;2(Series 2):973–977.

77.. 77. Hurley J. Sizing particles with a Coulter Counter. Biophys J. 1970;10:74–79. MEDLINE | CrossRef

78.. 78. Wilkins B, Frandolig JE, Fischer CL. An interpretation of red cell volume distributions measured by pulse height analysis. J Assoc Advan Med Instr. 1970;4:99–105.

79.. 79. Taylor WB. A versatile cell detector for cell volume measurements. Med & Biol Engng. 1970;8:281–290.

80.. 80. Harvey RJ. Effect of transducer length on volume measurement by electric sensing zone instruments. Rev Sci Instr. 1969;40:1111–1112.

81.. 81. Crosland-Taylor PJ. A device for counting small particles suspended in a fluid through a tube. Nature. 1953;171:37–38. MEDLINE | CrossRef

82.. 82. Spielman L, Goren SL. Improving resolution in Coulter counting by hydrodynamic focusing. J Colloid and Interface Sci. 1968;26:175–182.

83.. 83. Thom R, Hampe A, Sauerbrey G. Die elektronische volumenbestimmung von blutkörperchen und ihre fehlerquellen (Electronic blood-cell volume determination and its sources of error). Z ges Exp Med. 1969;151:331–349.

84.. 84. Thom R, Kachel V. Fortschritte für die elektronische größenbestimmung von blutkörperchen (Progress for the electronic size determination of blood corpuscles). Blut. 1970;21:48–50.

85.. 85. Kachel V, Metzger H, Ruhenstroth-Bauer G. Der einfluß der partikeldurchtrittsbahn auf die volumenverteilungskurven nach dem Coulter-Verfahren (The influence of the particle path on the volume distribution according to the Coulter Principle). Z ges Exp Med. 1970;153:331–347.

86.. 86. Leif RC. A proposal for an automatic multiparameter analyzer for cells (AMAC). In:  Wied GL,  Bahr G editor. Automated Cell Identification and Cell Sorting. New York: Academic Press; 1970;p. 131–159.

87.. 87. Graham, M.D. Method and apparatus for sensing and characterizing particles. U.S. Patent 6,111,398; filed July 3, 1997 and issued August 29, 2000.

88.. 88. Graham, M.D.; Dunstan, H.J.; Graham, G.; Britton, T.; Harfield, J.G.; King, J.S. Potential-sensing method and apparatus for sensing and characterizing particles by the Coulter Principle. U.S. Patent 6,175,227; filed July 1, 1998 and issued January 16, 2001.

89.. 89. Fulwyler MJ. Electronic separation of biological cells by volume. Science. 1965;150:910–911. MEDLINE

90.. 90. Fulwyler, M.J. Particle separator. U.S. Patent 3,380,584; filed June 4, 1965 and issued April 30, 1968.

91.. 91. Fulwyler MJ. Electronic cell sorting by volume. In:  Wied GL,  Bahr G editor. Automated Cell Identification and Cell Sorting. New York: Academic Press; 1970;p. 97–109.

92.. 92. Coulter, J.R., Jr. Flow-through sample apparatus for use with electrical particle study device. U.S. Patent 3,340,471; filed June 14, 1962 and issued September 5, 1967.

93.. 93. Coulter, J.R., Jr. Flow-through sample apparatus for use with electrical particle study device. U.S. Patent 3,340,470; filed September 23, 1964 and issued September 5, 1967.

94.. 94. Rothermel, W.F.; Klein, R.I. Automatic method and apparatus for obtaining different dilutions from blood or the like samples and processing the same by fluid handling and electronics to obtain certain nonelectric parameters. U.S. Patent 3,549,994; filed April 17, 1967 and issued December 22, 1970.

95.. 95. Brittin GM, Brecher G, Johnson CA. Evaluation of the Coulter Counter Model S. Am J Clin Pathol. 1969;52:679–689. MEDLINE

96.. 96. Pinkerton PH, Spence I, Olgivie JC, Ronald WA, Marchant P, Ray PK. An assessment of the Coulter Counter Model S. J Clin Pathol. 1970;23:68–76. MEDLINE | CrossRef

97.. 97. Collineau, C.J. Pulse count correction method and apparatus. U.S. Patent 3,737,633; filed May 7, 1971 and issued June 5, 1973.

98.. 98. Bergegére, P. Particle study apparatus having improved particle resolution means. U.S. Patent 3,790,883; filed May 9, 1972 and issued February 5, 1974.

99.. 99. Bader, H. Methods and apparatuses for correcting coincidence count errors in a particle analyzer having a sensing zone through which the particles flow. U.S. Patent 3,949,197; filed September 26, 1972 and issued April 6, 1976.

100.. 100. Hogg, W.R. Method and apparatus for generating error corrected signals. U.S. Patent 3,936,739; filed February 12, 1974 and issued February 3, 1976.

101.. 101. Hogg, W.R. Particle analyzer of the Coulter type including coincidence error correction circuitry. U.S. Patent 3,940,691; filed February 19, 1974 and issued February 24, 1976.

102.. 102. Coulter, W.H.; Hogg, W.R. Methods and apparatuses for correcting coincidence count inaccuracies in a Coulter type of particle analyzer. U.S. Patent 3,949,198; filed March 26, 1974 and issued April 6, 1976.

103.. 103. Campbell, S.K. Method and apparatus for providing primary coincidence correction during particle analysis. U.S. Patent 3,938,038; filed July 1, 1974 and issued February 10, 1976.

104.. 104. Coulter, W.H.; Hogg, W.R.; Doty, E.N.; Longman, M.D.; Campbell, S. Method and apparatus for providing primary coincidence correction during particle analysis utilizing time generation techniques. U.S. Patent 3,936,741; filed July 2, 1974 and issued February 3, 1976.

105.. 105. Hogg, W.R. Method and apparatus for correcting total particle volume error due to particle coincidence. U.S. Patent 3,987,391; filed December 2, 1974 and issued October 19, 1976.

106.. 106. Coulter, W.H.; Hogg, W.R.; Longman, M.D.; Campbell, S.; Doty, E.N. Method and apparatus for providing primary coincidence correction during particle analysis utilizing time generation techniques. U.S. Patent 4,009,443; filed April 3, 1975 and issued February 22, 1977.

107.. 107. Coulter, W.H.; Hogg, W.R. Particle analyzer of the Coulter type including coincidence error correction circuitry. U.S. Patent 3,968,429; filed July 9, 1975 and issued July 6, 1976.

108.. 108. Upbin B. What have you invented for me lately?. Forbes. 1996;December 16:330–332.

109.. 109. Graham MD. The diff4: a second-generation slide analyzer. In:  Duff MJB editors. Computing Structures for Image Processing. London: Academic Press; 1983;p. 179–194.

110.. 110. Graham D, Graham MD. Must a particle-sensing aperture be in insulating material? Abstract #4061, ISAC XX; Montpellier, France, 21–25 May 2000. Cytometry. 2000;(Suppl. 10):161; or Cytometry CD, Vol. 5, 2000, Purdue University Cytometry Laboratories.

111.. 111. Graham, M.D.; Dunstan, H.J. Apparatus incorporating a sensing conduit in conductive material and method of use thereof for sensing and characterizing particles. U.S. Patent 6,259,242; filed May 26, 1999 and issued July 10, 2001.

112.. 112. Graham MD. Field-amending conduits for particle sensing. Abstract #6199, ISAC XX; Montpellier, France, 21–25 May 2000. Cytometry. 2000;(Suppl. 10):165; or Cytometry CD, Vol. 5, 2000, Purdue University Cytometry Laboratories.

113.. 113. Newton, W.A.; Graham, M.D. Field focused particle sensing zone. U.S. Patent 4,420,720; filed June 29, 1981 and issued December 13, 1983.

114.. 114. Williams RA, Nisbet A, Dickin FJ, Taylor SE. Microelectrical tomography of flowing colloidal dispersions and dynamic interfaces. Chem Engng J. 1995;56:143–148.

115.. 115. Koch M, Evans AGR, Brunnschweiler A. Design and fabrication of a micromachined Coulter Counter. J Micromech Microeng. 1999;9:159–161.

Beckman Coulter, Inc. USA

Corresponding Author InformationCorrespondence: M. Don. Graham, Ph.D., Beckman Coulter, Inc., Kentucky Technical Facility, 115 Patton Court, Nicholasville, KY 40356; Phone or automatic Fax: +1.859.885.5007

PII: S1535-5535(03)00023-6

doi:10.1016/S1535-5535(03)00023-6


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