WO1993016368A1

WO1993016368A1 - Particle measurement system

Info

Publication number: WO1993016368A1
Application number: PCT/GB1993/000289
Authority: WO
Inventors: Robert Jones; Michael Stuart Hazell
Original assignee: Cambridge Consultants Limited
Priority date: 1992-02-12
Filing date: 1993-02-11
Publication date: 1993-08-19
Also published as: GB9202887D0; DE69318632D1; JPH06507025A; DE69318632T2; JP3144687B2; DK0579829T3; EP0579829B1; EP0579829A1; ATE166458T1

Abstract

The invention concerns a method of and apparatus for measuring particles in a fluid medium in which the particles are moved relative to a structured light field preferably produced by a multi-facet laser light source. Light scattered by the particles is detected to generate an output signal which is analysed to give an indication either of particle size or particle velocity.

Description

PARTICLE MEASUREMENT SYSTEM

The present invention relates to the optical measurement of particles and particularly, though not exclusively, to the measurement of particle sizes.

Particle sizing by means of optical techniques using Doppler methods which measure the amount of light scattered by the particle as it passes through a light field is widely practised. For biological particles of diameter 1-1Oum and sub-micron particles the scattered light levels are low. Usually therefore particles are made to flow in a focused light field through a flow cell.

Particular sizing techniques based on Doppler methods require the interferometric combination of crossed laser beams to create a structured pattern. This requires the coherent laser light sources and precision lasers, or more recently, the use of diffraction gratings. The extent of the structured light field necessarily occupies a large part of the inspection volume and consequently requires quality optical components. These requirements are not consistent with the manufacture of a low cost particle sizing equipment.

A problem of known techniques that rely purely on scattered light is that the region of focus is frequently subject to significant variations in radiant intensity when it occupies practical sample volumes. A given particle passing a region of high focal intensity can therefore scatter the same signal as a larger particle in a region of defocus . It has been proposed to overcome this problem by providing a composite light beam incorporating a concentric trigger of one wavelength through the centre of a surrounding analysis beam having a second wavelength. Only particles whose presence is indicated by the trigger beam are analysed. This occurs when the particle traverses the uniform region of the analysis beam. Measurements of the intensity of scattered light are thus made under repeatable conditions of particle illumination. This technique still requires high precision optics however and does not overcome the difficulty that the intensity of light scattered by particles is not a single valued function of the particle size, so that light intensity does not necessarily provide a reliable indication of particle size.

For example in medical bacteria tests in urine, tests for bacteria (typically l-4um) may not clearly be distinguished from residual red cells (5-8um) or even white cells (10-15um). Additionally still greater expense and complexity is involved.

The present invention is concerned with reducing the above mentioned disadvantages.

According to one aspect of the present invention a method for particle detection comprises passing particles in a fluid medium relative to a light source which generates a light field having a plurality of variations in intensity spaced along the relative direction of movement, and detecting variations in light intensity caused by the particles passing through the variations in the light field.

According to a second aspect the present invention comprises apparatus for particle measurement comprising apparatus for measuring particles comprising a light source for generating a light field having a plurality of spaced variations in intensity, means for moving particles in a fluid medium relative to the light field so that the particles pass successively through the intensity variations, and means for detecting variations in light intensity caused by the passage of the particle relative to the light field.

Various embodiments of the invention will now be described by way of example and with reference to the following drawings in which:

Figures 1 and 1A illustrate the layout of optical components in one form of particle sizer according to the invention;

Figure 2 is a block diagram of a typical signal processing system for the analysis of a particle size distribution based on signals from the light detector of Figure 1; Figure 3 shows a general form of an output signal generated by the embodiment of Figure 1;

Figure 4(a)-(d) shows experimental results of^{* "}the voltage output signal from the detector of the embodiment of Figure 1;

Figure 5 shows a scatter plot derived from structured outputs showing distribution of particles in the range 9u to 3um; and

Figures 6A and B show alternative embodiments of light detection optics systems.

Referring now to Figure 1 of the accompanying drawings this shows the optical layout of one embodiment of apparatus according to the present invention for sizing particles in a fluid stream and is generally indicated at 10 for sizing particles in a fluid stream. A potential application of the apparatus is to detect the presence of bacteria in urine. However it will be appreciated that the apparatus could also be used in a similar manner to measure particles carried in a gaseous medium, and that the term "fluid medium" as used in the present specification is intended to cover both gaseous and liquid media.

The apparatus 10 comprises a light source 12, a flow cell 14 and a light detector 16.

The light source 12 is a structured light source comprising an array of discrete light emitting elements uniformly separated. In a preferred form the structured light source 12 is realised by laser diodes having multiple facets. The source illustrated comprises three facets, but may in practice incorporate any suitable number of uniformly separated emitting elements.

The light source 12 is imaged by the aperture 15 and cylindrical lenses 17 and 18 into the inspection volume of the flow cell 14. In the preferred embodiment of the invention the structured light source comprises a laser diode, e.g. Sharp type LTO90MFO(TM) in which the three light emitting facets are strips approximately 3 microns by 1 micron and separated by 50 microns. For the detection of E coelli in urine the magnification of the lens systems 17 and 18 is chosen so that the separation of the intensity peaks in the focused image is approximately 5 microns. Thus in the embodiment being described the actual volume of fluid in the effective area of light is approximately 20 x 20 x 20 microns. It is possible for the fluid under test to be passed through a standard flow cell but it is preferred to inject a stream of fluid into a cell 14 by means of a narrow bore pipe 15 such as a hypodermic needle so that the stream passes through the focused light. In such a case the diameter of the bore of the needle is preferably between 100 to 300 microns. The fluid can be supplied under gravity or by a suitable pump.

Figure la s-hows a stream of fluid passing through the three focused facets of the light source 12. As shown in Figure la the image of the line source facets section the flow cell normal to the flow direction and extend beyond the width (w) of the flow cell. The depth of focus is ideally made greater than the cell depth although this is not a fundamental requirement. The magnification of the cylindrical lenses is also chosen so that the separation (q) of the image bars or lines approximate to the range of particle size to be measured.

Light from the image volume in the flow cell is collected by lens 22 into the detector 16. A stop 20 is sized so that normally in the absence of particles or other scattering sites in the image column the detector 16 is not illuminated, whilst forward scattered light is collected and detected. The detector 16 can be a PIN diode or an avalanche photo-diode.

Particles that traverse the focused light field are thus exposed to light from each facet or focused variation in—light intensity in turn. The intensity of light detected is thus modulated with a frequency q/u, where u is the particle traverse velocity and with intensity given by the convolution of the particle scattering cross section with the structured light image. A particle p of diameter d where d>>q effectively smears out the structure and an event of uniform intensity is displayed. Particles for which d>q partially resolve the structure and thus partially modulate the signal intensity and particles for which d>>q fully resolve the structure and display full modulation with intensity limited only by the detection noise limit.

It will be appreciated that the embodiment being described is capable of measuring bacterial particles which are poor absorbers of light. If the apparatus is intended to measure particles which are good light absorbers then a simple obscuration method could be employed. In such a case the stop 20 could be omitted so that the output of detector 16 would normally be high and the passage of particles through the inspection volume would cause appropriate reductions in the measured light input. However with poorly absorbent particles the signals caused by particle obstruction are small compared to the noise level of the light sensor gemerated by the directly incident radiation and it is for this reason that a system which detects scattered light is preferred. The processing of the output signal will now be described by reference to the block diagram illustrated in figure 2.

When a particle traverses the inspection volume of the flow cell light scattered in the structured light field by the particle is collected in the detector 16 to generate an output signal which is amplified by an amplifier 22, thresholded by a threshold circuit 24, sampled by an Analogue-to-Digital convertor 24 and analysed by a suitable microprocessor unit 26. A display unit is shown at 28 for displaying the results of the analysis and can take a wide number of different formats such as a CRT-based video system or hard copy device such as a plotter, whilst the microprocessor unit can be a PC.

A general form of the output signal 16 generated by the passage of a single particle is shown in Figure 3.

Considering this general form of signal the A-D detector typically generates samples from which mean values of the background voltage V, , a set of three peak voltages V . , V _ and V -. corresponding to each

facet of the light source structure and two trough voltages V . and V ₂ are generated.

System noise in general varies even during the period of a single pulse, as will be apparent from the experimental results illustrated in figure 4(a)-(f), generally due to thermal and flow effects.

Accordingly values of the mean peak voltages V and

trough voltages V are corrected for the background

voltage value by subtracting the latter as is shown in the following equations.

tn' tn b

Further calculations for each particle sampled are then performed

n—j m n=l and the visibility V is then calculated

_ V - V_τ V=(_^p ) V_p + V_τ

Figure^" 5 shows particularly clearly the effect of this calculation of the normalised peak-to-trough variation. Thus the layer, i.e. 9um particles shown in the left hand side of the figure are particles which have displayed the highest mean peak scatter level and smallest depth of modulation as defined by the mean visibility of the signal. Similarly the smallest, i.e. 3um particles which occupy the bulk of the right hand side of the figure display the lowest mean peak scatter level and highest depth of modulation.

Evidently for a source having a greater number of facets than 3, corresponding summations for the greater number of peak and trough events can be performed. These calculations are carried out in microprocessor unit 26 and the results displayed at 28. The particle size can be collected and displayed in histogram form or in other suitable form of display to illustrate the sizes of particles present. In general the visibility is found to be a single valued function of the particle size, and calibration of the particle sizing instrument is therefore simplified. Figure 5 shows a scatter plot from experimental results for particles of 9um, 5um and 3um diameters.

The detection optics illustrated in Figure 1 places the detector 16 under dark field illumination when there is no particle present in the inspection volume, due to the stop 20. This has the advantage that the scattered light signal can be focused into a small area detector and all the light collected is employed to generate the output signal, thereby minimizing noise. However as already mentioned the stop may be removed, thereby normally exposing the detector 15 to continuous light illumination. When a particle passes through the inspection volume it partly shadows the detector, lowering the illumination. In that case the signal of figure 3 is in effect inverted, so that V

and V.T. are lower than V.£>. However the same

calculation is performed to extract the visibility and thus the size of the particle. It is normally to be expected however that the noise component of this arrangement is greater than that described above, so that the accuracy of particle size denomination is lower and the least particle size that can be detected greater. The system without stop 20 in as accordingly less practicable where the particles to be measured have poor light absorbtion characteristics, such as bacteria and blood cells.

Alternative systems for collecting and detecting the scattered light are illustrated by reference to figure 6, in each case using forward scatter. Alternatively it is perfectly feasible to use either side or back scattered light and in fact the actual geometry chosen may be dictated by the practical constraints of the application.

One alternative light collection system in figure 6(a) comprises a detector 16' partially screened by stop 20' placed adjacent to the flow cell 14. In this case the detector collects the light without the benefit of a collection lens 22, and consequently the detector is somewhat larger in area. Such an arrangement may be built at less cost, but owing to the larger detection area is subject to increased noise in the detection circuit.

A more compact arrangement is also obtained by incorporating the mirror 19 as well as lens 22'. Alternatively the mirror 19 can be appropriately curved so that it also acts as a lens so as to provide a simple component which collects and focuses scattered light from the flow cell 14. ___

In the prior art the structured light field has been generated interferometrically in the form of fringes by focusing light from a coherent laser source via two paths into the inspection volume. In the present invention a structured light field is developed using incoherent methods and may take a number of forms. One convenient form described above takes the form of a muli-faceted light emitting or laser diode which is focused into the inspection volume by means of suitable cylindrical lenses or an equivalent optical system. However it will be evident that in general the source may be comprised of a number of structurally separate light sources optically combined by suitable beam splitters and cylindrical lenses to provide an equivalent structured image in the inspection volume; or alternatively may be obtained by an array of slits exposing a common light source suitably focused into the image plane; or alternatively may be obtained from a line source divided by a prism (or prisms) or diffraction grating into two or more line sources: and any other structured light field developed using incoherent imaging methods. The objective of the invention is to develop a structured light field having two or more basis of focused light having a predetermined separation (q) having a low manufacturing cost but providing high light intensity.

Although the invention has been described above with regard to particle size measurement it will be evident that the particle speed may also be extracted by monitoring the frequency of the voltage signals obtained. Additionally particle speed in more than one direction can be measured by having a second structured light field and associated optical system. In such a case the facets of the second field could be orthogonal with respect to those of the first field. It will also be appreciated that apparatus of the types just described could be cascaded along the path of particle flow with the facets being separated by varying distances.

Claims

1. A particle measurement method comprising passing particles in a fluid medium relative to a light source which generates a light field having a plurality of variations in intensity spaced along the relative direction of movement, and detecting variations in light intensity caused by the particles passing through the variations in the light field.

2. A method as claimed in claim 1, wherein the light detected is light scattered by the particles.

3. A method according to claim 1 or claim 2 , wherein the light ^"source generates three variations in intensity through which particles successively pair to generate pulses.

4. A method according to any one of the preceding claims wherein the size of a detected particle is measured by plotting the mean peak signal as a function of the normalised peak-to-trough variation in the output pulses generated by the passage of the particle through the light field.

5. A method according to any one of claims 1 to 3 wherein the velocity of a particle relative to the light source is measured by calculating the frequency content in output pulses generated by the passages of the particle through the light field.

6. Apparatus for measuring particles comprising a light source for generating a light field having a plurality of spaced variations in intensity, means for moving particles in a fluid medium relative to the light field so that the particles pass successively through the intensity variations, and means for detecting variations in light intensity caused by the passage of the particle relative to the light field.

7. Apparatus as claimed in claim 1, wherein the light source generates a light field having three spaced variations in intensity.

8. Apparatus according to either claim 6 or claim 7, wherein the means for detecting are arranged to detect light scattered by particles as they move relative to the light field.

9. Apparatus as claimed in any one of claims 6 to 8 wherein the light source comprises three spaced sources of light.

10. Apparatus according to claim 9, and including at least one lens arranged to focus light from the light source into the light field so that the spacing between the variations in intensity is approximately equal to the size of a particle to be measured.

11. Apparatus as claimed in any one of claims 6 to 10 in which the fluid medium carrying the particles is supplied to the light field in a stream in a narrow bore pipe.

12. Apparatus as claimed in claim 12, wherein the pipe has a diameter between approximately 100 and 300 microns .

13. Apparatus as claimed in any one of claims 6 to 12, and including a stop to prevent direct illumination of the detecting means.

14. Apparatus as claimed in claim 13, wherein the stop is located, in the optical path, before a lens which focuses light scattered by particles onto the light detector.

15. Apparatus as claimed in claim 13, wherein the stop is provided adjacent the light detector so that active area of the light detector only receives light scattered by particles.

16. Apparatus as claimed in claim 13, and including a mirror having a central aperture through which unscattered light emitted by the light source can pass, the mirror reflecting light scattered by particles onto a lens for focusing the scattered light onto the light detector.

17. Apparatus as claimed in claim 13, and including a mirror having a central aperture through which unscattered light emitted by the light source can pass, the mirror being curved to act as a lens to focus light scattered by particles onto the light detector.

18. Apparatus as claimed in any one of claims 6 to 17, and including means for deriving particle size by plotting the mean peak signal as a function of the normalised peak-to-trough variation in the output pulses generated by the passage of the particle through the light field.