Device for counting particles

Abstract

A device for counting particles comprises a detector arranged to produce an electrical measurement signal in response to the passage of one or more particles, and a comparator arranged to compare the measurement signal with a threshold signal and to increment a counting value when the measurement signal exceeds the threshold signal, characterized in that it furthermore comprises a threshold-adjusting circuit that applies a lowpass filter to the measurement signal, and that is connected to the comparator in order to use the resulting signal as threshold signal.

Claims

1. A device for counting particles comprising a detector arranged to produce an electrical measurement signal in response to the passage of one or more particles, a comparator arranged to compare the measurement signal with a threshold signal and to increment a counting value when the measurement signal exceeds the threshold signal, wherein the comparator is mounted between at least two hysteresis resistors, and a threshold-adjusting circuit that applies a lowpass filter to the measurement signal, and that is connected to the comparator in order to use the resulting signal as threshold signal.

2. The device of claim 1, wherein the threshold-adjusting circuit comprises a resistor and a capacitor mounted in series, and the comparator being an operational amplifier in comparator mode one input of which receives the measurement signal, and the other input of which is connected to the threshold-adjusting circuit between the resistor and the capacitor.

3. The device of claim 1, furthermore comprising an analogue-digital converter for digitizing the measurement signal, and wherein the comparator and the threshold-adjusting circuit are produced in digital form.

4. The device of claim 3, wherein the threshold-adjusting circuit is a finite-impulse-response filter of order 1.

5. The device of claim 1, further comprising a circuit ensuring the threshold signal has a minimum value.

6. The device of claim 5, comprising an operational amplifier mounted in follower mode between its output and its positive input, a voltage source connected to its negative input, and a diode between the output of the operational amplifier and the threshold-adjusting circuit.

7. The device of claim 6, further comprising a triggering circuit comprising an operational amplifier mounted in comparator mode one input of which receives the measurement signal, and the other input of which is connected to the voltage source.

8. A method for counting particles comprising: a) producing a measurement signal in response to the detection of the passage of one or more particles by a detector; b) producing a mobile threshold signal by applying a lowpass filter of chosen frequency to the signal generated in a); and c) comparing the measurement signal and the mobile threshold signal and emitting a signal indicating the detection of a particle when the measurement signal exceeds the mobile threshold signal by a chosen amount, wherein the measurement signal is produced according to the Coulter principle, and wherein the cut-off frequency of the lowpass filter is lower than 200 Hz.

Description

DETAILED DESCRIPTION OF VARIOUS EMBODIMENTS

(1) Other features and advantages of the invention will become more clearly apparent on reading the following description, which is drawn from nonlimiting examples given by way of illustration, which are drawn from the drawings

BRIEF DESCRIPTION OF FIGURES

(2) FIG. 1 shows a schematic diagram of a portion of a device according to the invention;

(3) FIG. 2 shows a circuit diagram of an element of FIG. 1; and

(4) FIG. 3 shows a circuit diagram of a variant of FIG. 2.

(5) The drawings and the description below contain, for the most part, elements of certain character. They will therefore possibly not only serve to better understand the present invention, but also contribute to its definition, where appropriate.

(6) FIG. 1 shows a counting device 2 according to the invention. The device 2 is considered in the following to be dedicated to the inspection (or analysis) of a fluid taking the form of a hematological sample, with a view to counting blood cells. However, the invention is limited neither to this type of fluid, nor to impedance-based counting. Specifically, it relates to any type of fluid, to any type of in-flow counter, and in particular to in-flow cytometers. It will possibly also be used to count beads or any other particles.

(7) As is illustrated in FIG. 1, the device 2 according to the invention firstly includes a measurement cuvette 4, of the hydrodynamically focused type, such as for example the measurement cuvette described in patent document FR 2 653 885. It will be understood that the device may not be of hydrodynamically focused type.

(8) To simplify, such a cuvette 4 includes an internal wall in which is placed a focusing nozzle 6, generally made of sapphire and defining a calibrated orifice, in the example described here of 60 m diameter. The wall defines an internal housing 8 in which a capillary tube (not shown) is placed, and the end of which is located facing the nozzle 6 at a small distance therefrom. This capillary tube it is intended to transport the fluid to be inspected upstream of the nozzle 6, in order to allow it to be channeled thereto, in the form of a primary flow 10, by a secondary sheathing fluid flowing through said internal housing 8 around the capillary.

(9) This embodiment allows the sample containing the blood cells injected into a so-called measurement region or zone to be hydrodynamically sheathed. FIG. 1, with the nozzle 6, is a close-up view of the device level with this measurement zone. In the example described here, the analyzed primary flow 10 is prepared blood, which flows through the channel 2 in the direction designated by an arrow in FIG. 1.

(10) A detector 12 is connected to the cuvette 4 level with the nozzle 6, and comprises a current source so that an electrical current passes through the nozzle 6. In the absence of cells, the primary flow 10 and the sheathing fluid define a load impedance that is measured by two electrodes 9 placed on either side of the nozzle 6. When the primary flow 10 contains a blood cell the latter leads to an impedance increase. This impedance variation on the one hand allows the volume of the cell to be determined (qualitative measurement), and on the other hand allows a cell count to be made (quantitative measurement). The detector 12 therefore forms a detector that produces an electrical signal in response to the passage of one or more particles. The detector 12 may comprise an amplifier and filters in order to produce a measurement signal that is exploitable by the electronic circuit 14.

(11) The detector 12 sends an electrical signal that reflects the impedance measured level with the nozzle 6 to an electronic circuit 14. The role of the electronic circuit 14 is to perform cell measurement on the basis of the signal sent by the detector 12.

(12) The electronic circuit 14 will now be described with reference to FIG. 2.

(13) The electronic circuit 14 comprises two sections: a threshold-adjusting circuit 50 comprising a resistor 52 and a capacitor 54; and a comparator 56.

(14) The threshold-adjusting circuit 50, which consists of the resistor 52 and the capacitor 54 placed in series, forms a lowpass filter. It is directly connected to the detector 12 on the side of the resistor 52 and to ground on the side of the capacitor 54. In the example described here, the resistor 52 has a resistance of 6 k, and the capacitor 54 has a capacitance of 1 nF, i.e. the cut-off frequency is 166.67 Hz. The value of the cut-off frequency is calculated to obtain a compromise between resolution of coincident passages and immunity to noise and other effects such as the deformation due to edge passages in the case of measurement in-flow without hydrodynamic focusing. Tests carried out by the Applicant have shown that a variation of 10% in the value of RC results in a variation of 0.6% in the number of cells counted and therefore in a high tolerance to commercial components.

(15) In the example described here, the comparator 56 is a TLE2071 operational amplifier as sold by Texas Instruments (registered trademark). The negative input of the comparator 56 is connected to the adjusting circuit 50 between the resistor 52 and the capacitor 54. Study of the threshold-adjusting circuit 50 has shown that the voltage S(t) on the negative input of the comparator 56 is related to the measurement signal M(t) generated by the detector 12 by the following relationship:

(16) $M\left(t\right)=\mathrm{RC}\frac{\mathrm{dS}\left(t\right)}{\mathrm{dt}}+S\left(t\right)$
or, discretely:

(17) $M\left(n\right)=\frac{S\left(n\right)-S\left(n-1\right)}{\mathrm{dt}}+S\left(n\right)$

(18) The operational amplifier is thus mounted in comparator mode, so that it emits on its output a positive voltage if the measurement signal M(t) generated by the detector 12 is higher than the threshold signal S(t) generated by the threshold-adjusting circuit 50, and 0 if not.

(19) By virtue of this electronic arrangement, the mobile threshold signal follows the value of the measurement signal. Thus, when a plurality of cells simultaneously pass the exit of the nozzle 6, even with the increase in the measurement signal, the device preserves an excellent resolution because the threshold signal remains close to the measurement signal, without preventing detection.

(20) Above, an in-flow cytometry device allowing quantitative measurements to be made was described. FIG. 3 shows a variant embodiment that is more sophisticated than the embodiment of FIG. 2, and which may for example be used in a particle-counting device furthermore allowing a qualitative measurement to be carried out.

(21) The electronic circuit 14 comprises, in this embodiment, four sections: a threshold-adjusting circuit 50 comprising a resistor 52 and a capacitor 54; a comparator 56 surrounded by two resistors 58 and 60, for the mobile-threshold counting; a comparator 62 surrounded by two resistors 64 and 66, for the qualitative measurements; and a comparator 68 coupled to a diode 70 and to a voltage source 72.

(22) The threshold-adjusting circuit 50 comprising the resistor 52 and the capacitor 54, which resistor and capacitor are placed in series, forms a lowpass filter. It is directly connected to the detector 12 on the side of the resistor 52, and to ground on the side of the capacitor 54. As for the embodiment of FIG. 2, the resistor 52 has a resistance of 6 k, and the capacitor 54 has a capacitance of 1 nF, i.e. the cut-off frequency is 166.67 Hz.

(23) The output of the comparator 56 is looped back on its positive input, and the resistor 64 is connected on the one hand to this positive input and on the other hand to the detector 12. The resistor 66 is connected in series in the loop. The negative input of the comparator 56 is connected to the threshold-adjusting circuit 50 between the resistor 52 and the capacitor 54.

(24) In the example described here, the resistor 64 has a resistance of 22 k, and the resistor 66 has a resistance of 1 M. Together the resistors 64 and 66 set a hysteresis of 110 mV for the comparator 56 in the example described here for an output voltage limited to 5 V. This hysteresis allows immunity to noise when the signal crosses the fixed threshold or mobile threshold.

(25) In the example described here, the comparator 62 is identical to the comparator 56, and the resistors 64 and 66 are identical to the resistors 58 and 60. The positive input of the comparator 62 receives the measurement signal of the detector 12, whereas the negative input is connected to the voltage source 72. As the comparator 62 is mounted in comparator mode, it emits a positive output voltage if the measurement signal is higher than the value of the voltage source 72, and 0 if not. Thus, the output of the comparator 62 may be used to perform qualitative measurements on the basis of the signal emitted by the detector 12, or even to control the triggering of a light source for a downstream measurement when the detector 12 detects the passage of a cell.

(26) In the example described here, the comparator 68 is identical to the comparator 56, and its output is connected to the diode 70, which is connected to the positive input of the comparator 56, whereas the voltage source 68 is connected to the negative input of the comparator 68. The diode 70 is mounted in order to let current pass only from the comparator 68, and is connected to the threshold-adjusting circuit 50 between the resistor 52 and the capacitor 54. Thus, this section ensures that the threshold signal S(t) cannot drop below a value set by the voltage source 72. In the example, this value is that of the fixed threshold voltage for triggering conventional counting or qualitative measurement.

(27) The two embodiments described in FIGS. 2 and 3 could be combined. Thus, the section intended to guarantee a threshold-signal value higher than that of the fixed threshold and the hysteresis resistors could nevertheless be included separately or together in the embodiment in FIG. 2; likewise they could be removed together or separately from the embodiment of FIG. 3.

(28) Above, the electronic circuit 14 was described as being an analogue device. As a variant, the device may comprise an analogue-digital converter that receives the measurement signal from the detector 12, the adjusting circuit 50 then being made up of a digital finite-impulse-response filter of order 1 and a digital comparator of the measured signal and the threshold signal output by the filter.

(29) This type of filter obeys the following equation:
S(n)=kM(n)+(1k)S(n1)

(30) In order to decrease the required resources, the coefficient k of the digital filter is chosen to be a power of 2, or its inverse. Thus, multiplication is achieved by a logic shift to the left or right. This method limits the possible values of the cut-off frequency of the filter, but it has the advantage of being easy to implement.