A Coulter counterW. R. Hogg, W. Coulter; Apparatus and method for measuring a dividing particle size of a particulate system; United States Patent 3557352 Coulter counter is an apparatus for counting and sizing particles suspended in . The Coulter counter is the commercial term for the technique known as resistive pulse sensing or electrical zone sensing. The apparatus is based on the Coulter principle named after its inventor, Wallace H. Coulter.
A typical Coulter counter has one or more microchannels that separate two chambers containing electrolyte solutions. As fluid that contains particles or cells is drawn through the microchannels, each particle causes a brief change to the electrical resistance of the liquid. The counter detects these changes in the electrical resistance.
The Coulter principle relies on the fact that particles moving in an electric field cause measurable disturbances in that field. The magnitudes of these disturbances are proportional to the size of the particles in the field. Coulter identified several requirements necessary for practical application of this phenomenon:
If multiple particles pass through the constriction simultaneously, their impedance profiles will overlap, resulting in an artifact known as coincidence. The apparatus cannot differentiate between one large particle and multiple small overlapping particles, causing anomalies in the resulting data.
A variety of experimental devices have been designed based on the Coulter principle. A few of these devices have been commercialized, with the most well-known applications being in the medical industry, particularly in hematology to count and size the various cells that comprise whole blood. All implementations of the Coulter principle have compromises between sensitivity, noise shielding, solvent compatibility, speed of measurement, sample volume, dynamic range, and reliability of device manufacture.
Coulter was awarded US Patent 2,656,508, Means for Counting Particles Suspended in a Fluid. This Coulter counter is an analytical instrument which employs the Coulter principle for a specific task, most commonly counting cells. The most commercially successful application of the Coulter principle is in hematology, where it is used to obtain information about patients' blood cells. Coulter counters can also be used in the processing and manufacturing of paint, ceramics, glass, metals, and food. They are also routinely employed for quality control.
Cells, being poorly conductive particles, alter the effective cross-section of the conductive microchannel. If these particles are less conductive than the surrounding liquid medium, the electrical resistance across the channel increases, causing the electric current passing across the channel to briefly decrease. By monitoring such pulses in electric current, the number of particles for a given volume of fluid can be counted. The size of the electric current change is related to the size of the particle, enabling a particle size distribution to be measured, which can be correlated to mobility, surface charge, and concentration of the particles.
The amount and quality of data obtained varies greatly as a function of the signal processing circuitry in the Coulter counter. Amplifiers with lower noise thresholds and greater dynamic range can increase the sensitivity of the system, and digital pulse height analyzers with variable bin widths provide much higher resolution data as compared to analog analyzers with fixed bins. Combining a Coulter counter with a digital computer allows capture and analysis of many electrical pulse characteristics, while analog counters typically store a limited amount of information about each pulse.
As electric current detectors became more sensitive and less expensive, the Coulter counter became a common hospital laboratory instrument for quick and accurate analysis of complete blood counts (CBC). The CBC is used to determine the number or proportion of white and red blood cells in the body. Previously, this procedure involved preparing a peripheral blood smear and manually counting each type of cell under a microscope, a process that typically required a half-hour.
A Coulter counter played an important role in the development of the first cell sorter, and was involved in the early development of flow cytometry. Some flow cytometers continue to utilize the Coulter principle to provide information about cell size and count.
The aperture format is the most-used configuration in commercial Coulter counters, and is suited to testing samples for quality control. In this setup, a small aperture (hole) of specific size is created in a material such as a jewel disk (made of the same material as in watches). This disk is then embedded in the wall of a glass tube, which is then referred to as an aperture tube. The aperture tube is placed in a conducting liquid such that the aperture is completely submerged, and a pump at the top of the tube draws liquid through the aperture. Electrical current is passed through electrodes on either side of the aperture tube; because glass is an electrical insulator, all of this current flows through the aperture. After recording baseline data, the sample to be analyzed is slowly added to the conducting liquid and drawn through the aperture. Variations in conductivity, caused as sample particles pass through the aperture, are recorded as electrical pulses and analyzed to determine the characteristics of the particles and the sample as a whole.
The flow cell format is most commonly implemented in hematology instruments, and some flow cytometers. In this format, electrodes are embedded at either end of a flow channel and the electric field is applied across the channel. This arrangement allows for continuous sample analysis and can be combined with other instrumentation (when equipped with a sheath flow to keep particles centered in middle of the flow channel). This can permit additional measurements to be performed simultaneously, such as probing the particle with a laser. The major disadvantages of the flow cell format are that it is much more expensive to manufacture and is typically fixed to a single channel width, whereas the aperture format offers a wide variety of aperture sizes.
Microfluidic approaches have been used to apply the Coulter principle to lab-on-a-chip particle detection. These techniques allow much smaller pores (holes) to be fabricated than can easily be achieved using in the aperture format. These approaches, known by the generic phrase microfluidic resistive pulse sensing, have allowed the extension of the Coulter principle to the deep sub-micron range, allowing, for example, the direct detection of virus particles in fluid.J. J. Kasianowicz et al.. "Characterization of individual polynucleotide molecules using a membrane channel", P. Natl. Acad. Sci. USA 93,13770–13773 (1996)O. Saleh and L. L. Sohn, "An artificial nanopore for molecular sensing", Nano Lett. 3, 37–38 (2003)J.-L. Fraikin, T. Teesalu, C. M. McKenney, E. Ruoslahti and A. N. Cleland, "A high-throughput label-free nanoparticle analyzer," Nature Nanotechnology 6, 308–313 (2011)
Subsequent developments were able to extend the information obtained by using alternating current (AC) in order to probe the complex numbers electrical impedance of the cells rather their simply counting their number. The cell may then be approximately modelled as an insulating cell membrane surrounding the cell's cytoplasm, which is conductive. The thinness of the cell membrane creates an electrical capacitance between the cytoplasm and the electrolyte surrounding the cell. The electrical impedance may then be measured at different AC frequencies. At low frequencies (well below 1 MHz) the impedance is similar to the DC resistance. However, higher frequencies in the MHz range can be used to probe the thickness of the cell membrane (which determines its capacitance). At much higher frequencies (well above 10 MHz) the impedance of the membrane capacitance drops to the point where the larger contribution to the measured impedance is from the cytoplasm itself (the membrane is essentially "short circuit"). Thus, by using different frequencies, the apparatus can become sensitive to the internal structure and composition of the cells.
Experimental considerations
Coincidence
Particle path
Conductive particles
Porous particles
Direct current and alternating current
Applications
Hematology
Cell count and size
Particle characterization
See also
External links
|
|