ACOUSTIC METHOD FOR MEASURING PROPERTIES OF A MOBILE MEDIUM

Abstract: The invention relates to a method for measuring parameters and/or13roperties in a mobile medium, e.g. a liquid or a gas. If acoustic energy is transmitted into a mobile medium, flow is initiated in the medium. This flow is measured by any known method, and this provides information on the properties of the medium. If the medium contains bodies which reflect acoustic and/or optical signals, ultrasound or laser-Doppler can be used for measuring the velocity of the bodies. The Doppler-shifted signal can provide information on the viscosity of the medium and on the bodies in the medium.

Description: A c o u s t i c m e t o d f o r a e a s u r i n g p r o p e r t i e s o f a m o b l e m e d i u m The present invention relates to the technical field of measuring . 5 technique and more particularly to a method making it possible through the intentional application of acoustic energy to perform a non- destructive remote measurement and/or monitoring of properties of viscous media, • . • 10 In many areas the need . for an accurate measurement and/or charac¬ terisation of a series of physical parameters of liquids and gases, ..referred to hereinafter as mobile media, has become more and more . evident. The rapid development in recent years of electronic semi¬ conductor components has led up to to-day's plentiful offer of 15 very powerful, fast, inexpensive and thus generally accessible personal computers. They can now replace in many applications the minicomputer system of yesterday, and it is an established fact to¬ day that future uses and developments of measuring, control and regulating systems are limited more through the lack of suitable • 20 measurement transmitters than of access to computer power. It does • not make sense to attempt controlling an industrial process on a per mil level if the available measurement transmitter only has an accuracy of 10% ! . 25 Whilst it is possible to measure ' simple parameters such as electric voltage, current, length; weight etc. with high accuracy, it is not as easy to obtain access to accurate transmitters for the measurement of more complex material properties such as lubricity, flαwability, thixσtropy, assessment of the quality of paper pulp 30 etc., that is to say areas where human senses often perform better than the foremost measuring system of the day. An experiences process engineer frequently is able by the visual appearance and feel of a paper pulp to assess its suitability; ccorrespαndingly,a physician, simply by talking to a patient, can sense whether the 35 patient is healthy or sick, without being able directly to point to a primary reason for his feeling. Insofar as transmitters for this type of measuring problem are concerned, it is often not even possible to specify exactly which properties of the measuring object it would be desirable to measure- Hare important than the absolute measuring accuracy will be that the measurement transmitter should be consistent and ' in a given measuring situation each time provide the same measured value . Other desirable characteristics of the .measurement transmitter are that it must not have a negative effect on the measuring process, and that it should be possible to carry out the measurement by means of a telemetering technique. Finally the price of the transmitter is always important, though in these cases not wholly decisive. Let us look at an- example from the foodstuff or processing -industry where the need exists for continuous monitoring of e.g. flσwability or viscosity of the product during the course of the process. Keasurement of the viscosity is associated with a relatively cumbersome method of analysis which involves having to withdraw a sample from the process and placing it e.g. in a rotating cylinder visσosimeter. Other analyses may require the determination of the quantity of solid particles in a liquid, where the sample has to be evaporated to dryness so that the quantity of solid substance can be weighed. In many cases it is impossible for practical reasons to withdraw a sample for closer analysis. In many biotechnical processes, e.g. fermentation, the process vessel often is a closed container. To allow keeping the production at a high and even level, a continuous checking of how the process develops inside the closed vessel is desirable. Industries which mass produce e.g. provisions at times may be hit by breakdowns which result in parts of the production being of reduced quality. It should be possible then to be able rapidly and reliably to separate out the faulty products from the production so as to discard them. It will then not be a matter of just one single point of measurement, but may involve e.g. millions of packages of non-returnable packages of milk. Eaturally it is not possible in this situation to open all packages, but instead the measuring method for the assessment of the. contents ought to ' function through the unbroken package.. Against the background of the risk of many infectious diseases, such ' ase.g. AIDS, it may be expected that an increasing part of . ' blood transfusions to patients with planned need of blood will take place by means of so-called autαlogαus blood transfusion. This means . that patients themselves in good time before an operation provide their own blood which is then stored e.g. in plastic bags in cold storage, until the time when it is needed. It will be necessary in such cases to be able to check the quality of the stored, blood without opening the bags. The equipment for this • purpose naturally has to be subjected to very stringent environmental requirements, e.g. sterilization. In the following is described an invention which can be used to ' measure certain properties of a mobile medium rapidly and without disturbing effects on the process . A basic block diagram ofthe invention is shown in Figure 1. The signal generator <1> drives an ultrasound transmitter (2) which consequently generates acoustic energy which 'is transmitted into a mobile medium <3). The acoustic energy generates a movement in the medium, see also below. By studying this movement by means of some known measuring method (4) reproducible information is obtained which after a certain signal processing (5) may be used for an assessment of the physical properties of the medium. The acoustic signal may be generated with the help of an ultrasonics transmitter, e.g. of the piezoelectric type. It has been known for a ' long time that the propagation of ultrasonic waves through a viscous medium is associated with a unidirectional movement in ' the medium, the so-called "acoustic flow". Historically seen the effect was studie already at the end of the nineteenth century G.884) by the father of acoustics, Lord Rayleigh. In principle the acoustic flow can be divided into two main types. The first type relates to the passage of a plain acoustic wave through an attenuating medium. The acoustic flow then arising is ■ usually known, for historical reasons, as "quartz wind". The second type of acoustic flow is either associated with inhomogeneities in a sound field or the joint action between a sound field and . changes, in -impedance at boundary faces. For a more detailed description of the phenomenon reference is' made to "Methods of experimental physics", Vol.19, Ultrasonics, Editor: Peter D. Edmonds, Academic Press, 1981. Other parameters which affect the magnitude of the movement are the viscosity of the medium, the frequency and intensity and shape of the acoustic signal transmitted and the distance to surrounding stationary waves. If bodies are present in the medium which reflect the acoustic signal, these will be affected by a radiation pressure proportional to the intensity of the acoustic signal.The term "body" hereinafter refers to a region with an acoustic impedance different from that of the environment, for example particles in a liquid or liquid " drops in. a gas. The bodies in the medium will be acted upon by a force, whose magnitude depends on the intensity of the acoustic signal, the size etc.of the bodies , by which they will be put in motion relatively to the surrounding medium. The magnitude of this movement depends on the magnitude of the force, the physical properties of the surrounding medium etc. The movement of the bodies in relation to the ultrasonics transmitter thus will depend on the movement of the surrounding medium as well as on the the bodies' own movement in relation to the surrounding medium. A series of different ways exist for measuring the movement in the medium. In the following are given a few examples of practical measurement situations with a description of how properties of the actual medium can be measured according to the above principle. A medium is enclosed in a sealed container and the task of the measurement consists in determining the movement of the medium without having to open the container. Such a task may be considered to occur in connection with the aforementioned problem which may be that of checking whether milk packaged sterile is fresh, or whether blood in the blood bags has commenced to deteriorate. In both these cases bodies are present in the medium, fat emulsion and blood corpuscles respectively, which means that Doppler technique can be applied for the detection of movement of- the bodies in relation ' to a receiver. A measuring situation in accordance with Figure 2 , where a so-called continuous ultrasound . Doppler technique is used, can be applied in this case. A signal generator (6) with a suitably chosen output and frequency drives an ultrasound transmitter (7) to generate acoustic energy which is transmitted into the medium (8) straight through the package wall, his is a acceptable solution in practice, since most normal packing material does not constitute any major obstacle for an acoustic wave. A part of the acoustic energy transmitted will be reflected by the bodies in the medium and its frequency shifted in accordance with the so-called Doppler effect. ' The magnitude of the frequency shift, Δf , is given by Δf = k v f /c where Δf ■ = ' Doppler shift k = constant, depending on the actual measuring situation v • = velocity of the bodies f = frequency of the acoustic signal transmitted c . = velocity of sound in the medium It follows from the above that the magnitude of the frequency shift is directly proportional to the velocity of the bodies. The reflected signal is detected with the help of a further ultrasound transmitter (9) , whereafter the frequency-shifted part of the signal received, the so-called Doppler shift, is separated, e.g. by multiplying the signal received by the signal from the signal generator (6) in a mixer <10) . The magnitude of the Doppler shift can be measured thereafter in any type of frequency analyzer (11 ) . -6- In this case it is possible therefore to use the same acoustic energy both for generating movement in the medium and for measuring the resulting flow. Since the bodies have been put in motion by the acoustic signal transmitted and their velocity is a 5 function of factors * named above, inter ali the intensity of the signal and the- iscosity of the medium, velocities of o the bodies and therefore the frequency content of the Doppler shift will constitute an indicator of the viscous properties of the medium, • provided ' other parameters, such as the intensity, are known. It is 10 interesting to note that the effect we propose here for measuring properties, of the medium has been observed previously but had been considered, to be a difficult artifact, which greatly limited the 'signal to noise ratio 'of the ultrasound- Doppler method. 15 The intensity .of the Doppler—shifted signal is a direct measure of ho . great a part of the signal introduc ed has been reflected by the mobile bodies in the medium. The reflected intensity depends among other things on the number of the bodies and their acoustic cross^sectional plane. If the acoustic.cross-sectional plane of the 20. bodies, is known, e.g. from a reference solution, the intensity of the Doppler signal constitutes a measure of the quantity of mobile bodies in • the medium. In order to increase the reproducibility of the measurements the Doppler-shifted signal may be standardized through division by the non-freσuency-shifted, reflected acoustic 25 signal. The reflecting bodies can be accelerated to different velocities in the medium e.g. as a function of the appearance of the flow profile in the so-called "sensitive- volume" or on the grounds of the 30 different bodies having varying size or acoustic impedance. As a ■ result the Doppler e fect will contain a number of different frequency components with diverse amplitudes, where the respective amplitude, inter alia, depends on the product of quantity times acoustic cross-sectional plane. It will be of great interest 35 therefore to know more closely which frequencies enter into the Doppler signal as well as their relative intensities. This can be done quite easily by the frequency analyzer <11). Correspondingly there can be special advantages in the use in certain measuring situations of other known types of Doppler measuring equipment e.g. so-called direction-sensing Doppler or so- 5 called pulsed Doppler. which both bring about an improved spatial resolution of the measurements and detection of other flow directions, turbulence etc. The pulsed Doppler, moreover, can . perform- measurements at varying distance from the . ultrasound transmitter. By the combination of several such measurements, 10 independent parameters of the mobile medium can be determined. The frequency .content of the Doppler signal provides information on the velocities of ■ the bodies in the , medium in relation to / transmitter and receiver, which, is a well-known ' property of the •15"-- .• ' ϋXtrasαuhd Doppler . equipment " used at -present, inter alia, in infirmaries for so-called non-invasive blood flow measurements. The analogy is not quite perfect.however, since in the normal medical ' usage of ultrasound .Doppler blood flow velocities in the order of. magnitude of 5 - 100 cm/s are measured, which are appreciably 20 'higher than the velocities which the bodies in the aforementioned ' , measuring situation can be expected to attain. As a matter of fact,, commercially available ultrasound Doppler apparatuses cannot be used for the type ' ,of measurements which are claimed for the .above-said invention, since these apparatuses contain high-pass 25 filters which for various reasons filter out all low-frequency Doppler signals corresponding to velocities below approx. 5 cm/s. In a dissertation from the Lunds Tekniska och Saturvetenskapliga Hδgskola (Technical and Scientific University of Lund ) , 30. "Measurement of .blood perfusion in tissue using Doppler ultrasound", LUTEDX/(TEE ' K-1027)/l-4/(1985), Stephan Dymling recently has shown that it is possible to design highly stable Doppler measuring equipment with performances which also manage to measure the extremely small Doppler shifts which a measuring equipment 35 according to the above-said invention is expected to produce. For further clarification of the method of measurement, a practical embodiment for the measurement of changes in milk is given in the following. As a signal generator (6) a highly stable oscillator is required which is obtained simplest by using a crystal oscillator or a crystal-controlled synthesis generator with a frequency stability of better than 1Q ~7 . The signal used is selected as a function of the actual measuring medium: For milk a frequency of 10 KHz. and an amplitude of 1-10 V . are suitable starting values. This signal drives an ultrasound transmitter whose transmitter element may consist of piezoeletric material such as e.g. Ferroperm type P2. the acoustic energy so generated in fresh milk will have an acoustic intensity of the order of magnitude of 100 mW/cm^, which results in an acoustic flow of aprox. 1 cm/s. The reflected ultrasound signal, hich is detected with the help of the ultrasound transmitter (9),is therefore Dαppler-shifted. With the help of a mixer CIO) the Doppler shift which in this case ought to be of the order of magnitude 100 Hz is detected. The Doppler signal detected is analyzed with the help of a Hewlett Packard Spectrumanalyzer model 3582A (11) and the measuring result is substantiated through digital data storage or through printout on a plotter. With this equipment practical measurements can be carried out and some measuring results are represented in Figure 3. Figure 3A shows a frequency spectrum from a measurement of fresh milk whereas Figure 3B shows how the spectra have been changed after the milk had been stored for 2 days at room temperature. It can be seen clearly that in the deteriorated milk the particles move at lower velocity. Figure 3C shows a frequency spectrum of the Doppler signal on measuring warm (35 * C) glycerαl with addition of reflecting bodies, and Figure 3D shows corresponding spectra after the temperature has been lowered to 20"C. The reduced Doppler shift agrees well with previously known facts suggesting that the viscosity αf glycerol is a function of the temperature. Instead of the acoustic Doppler technique,it is also feasible,ifthe bodies have an optical impedance which differs from that of the surrounding medium, to use optical Doppler technique for measuring the resulting acoustic flow. The measuring set-up in this case will be modified in accordance with Figure 4. A signal generator ( 12 ) with suitably chosen output and frequency drives an ultrasound ' transmitter (13) to generate acoustic energy in the •medium (14) (corresponding to 6,7 and 8 in Figure 2). The measuring method is now an optical so-called laser Doppler (15), whereafter the measuring signal obtained is signal-processed in (16) according to the above-said. The advantage of the laser Doppler as against the ultrasound Doppler rests above all in the possibility of obtaining very good spatial resolution, that is to say permitting measurement, of the movement in a single point. The disadvantage is that the method functions only in more or less transparent media. In certain media it is not possible tα use Doppler technique as a measuring method for the detection of the acoustic flow.e.g. when the medium does not contain any reflecting bodies. However in such cases too an acoustic flow may be developed e.g. through the aforementioned "quartz wind". The movement now has to be detected in a different manner. Figure 5 shows a possible measuring set-up. The acoustic energy in the medium (19) is produced in the customary manner with the help of a signal generator (17) and an ultrasound transmitter (18). Instead of measuring the reflected energy it is now the trans¬ mitted sound signal which is detected with the help of a further ultrasound transmitter (20 ) . The actual measurement of the acoustic flow can be done in a number of different ways, e.g a ) through phase comparison in (21) pf the transmitted and the detected acoustic signals, b)through the generated signal containing a repetitive transient disturbance whose transmission time up to ( 20 ) is measured in (21), or c) through generation by the signal generator of a randomized signal whose transmission time up to (20) is detected with the help of correlation technique in ( 21 ) A further method for carrying out the measurement is shown in Figure 6. The acoustic flow in the medium (24) is generated from the signal generator (22) via the ultrasound transmitter (23). The measurement now is done by determinations of the transmission time with the help of two other ultrasound transmitter, (26) and (27). The measuring signal may be e.g. ultrasonic energy of a different ultrasonic frequency or it may consist of any form of pulse sequence- where phase or cycle time are measured in (28)." Finally the measurement naturally also can be carried out by means of "sing-around"-technique. Regardless of the measuring method it is possible before the start of the actual measurement, that is to say before the acoustic energy is supplied ' to the medium, to use the measuring method in order to investigate the presence of any disturbing movements in the medium. This may be applied as an autotest to assess hoW far it is possible to use the measuring method in the particular measuring set-up and regarding the expected signal-to-noise level for the coming measurement. With a suitable signal processing technique, measurements of physical properties may take place- also on media in motion, e.g. in conveyor pipe lines. By variation of the intensity of the acoustic signal transmitted other properties, of the medium can be investigated, especially non¬ linear properties such as thixotropy etc. By watching the acceleration of the acoustic flow when the acoustic energy is introduced, further information concerning the medium concerned can be obtained. Beside the aforementioned examples from infirmary, foodstuffs and processing industry the invention can be applied in many other fields, e.g. for ' monitoring the condition of cooking oils in ham¬ burger restaurants, cutting oils in machine tools and lubricating oils in cars. Many modifications are possible within the.scope of the invention.

Claims: C AiKS. 1. A method for determining the nature and the properties of a medium comprising a liquid and any substances of an acoustic impedance differing from the carrier liquid suspended in, or . blended into, the liquid, c h a r a c t er i z e d i n : a)- that acoustic energy in the form of acoustic waves is introduced into, and is made to propagate in, the medium, • ' b) that to the said medium a flow movement is imparted by means of the said acoustic energy, c) that the said acoustic waves, after they , have passed the medium, are detected and determined with regard to their ■ frequency' or their phase position, the difference in frequency. or phase position between acoustic waves introduced and detected constituting a (relative) measure of the velocity of the liquid and of the substances suspended or mixed in the liquid. • 2. A method in accordance.with claim 1, c h a r a c t e r i z e d i n t h a t the acoustic energy is con . stituted of ultrasound αf a frequency between 20 kHz and 100 MHz. 3. A method in accordance with claim 1, c h a r a c t e r i z e d i n t h a t the acoustic waves introduced are made to reflect in the medium and that the frequency spectrum of the reflected acoustic waves, is compared with the frequency of the acoustic waves introduced into the medium in order to determine the velocity of the medium, that is to say the carrier liquid and substances of differing acoustic impedance present in the carrier liquid. 4. A method in accordance with claim 1, c h a r a c t e r i z e d i n t h a t the acoustic waves introduced into the medium are caused to propagate in the medium and be detected with regard to phase position, the phase shift between waves introduced and detected constituting a relative measure αf the velocity which is imparted to the medium. 5. A method in accordance with claim 1, c h a r a c t e r i z e d i- n t h a t the movement of the medium is detected by means of Doppler technique. 6. A method in accordance with claim 1, c h a r a c t e r i z e d i n t h a t the movement of the ' medium is detected through measurement of the transmission time of the wave movement. 7. -A method in accordance with claims 1 and 4, .c h a r a c t e r i z e d i n t h at the Doppler-shifted components are standardized through division by the whole of the reflected signal. 8. A method in accordance with claim 1, c h a r a c t e r i z e d i n t h a t changes in a medium are compared with -corresponding changes in a reference medium which is -. subjected to the same effect. 9. A method in accordance with claim 1, c h a r a c t e r i z e d i n t h a t the quantity of mobile reflecting bodies in the medium is measured as a function of the intensity αf the frequency-shifted reflected signal. 10. A method in accordance with claim 1, c h a r a c t e r i z e d i n t h a t the intensity of the acoustic signal emitted is varied during the course of detection. 11. A method for determining changes in viscosity and occurrence αf gas bubbles and solid particles in contents enclosed in a package by introducing acoustic energy from the outside of the package via a portion of the package wall comprising a homogeneous ■ - 'material, and-that the sound waves reflected are sensed through a portion of the package wall which likewise comprises a homogeneous wall section. 12. A method in accordance with claim 11, c h a r a c t e r i z e d i n t h a t the acoustic energy in the case of non-returnable packages manufactured from paper or cardboard is introduced through a wall portion wherein the paper material has been removed and replaced by a cover foil of homogeneous material, and the reflected acoustic waves likewise are picked up through a wall portion where the paper material has been punched out and replaced by a cover foil of homogeneous material.

Inventors: DYMLING STEPHAN, HERTZ TOMAS, LINDSTROEM KJELL, PERSSON HANS W, DYMLING, STEPHAN, HERTZ, TOMAS, LINDSTROEM, KJELL, PERSSON, HANS, W.
Applicants: DYMLING STEPHAN, HERTZ TOMAS, LINDSTROEM KJELL, PERSSON HANS W, DYMLING, STEPHAN, HERTZ, TOMAS, LINDSTROEM, KJELL, PERSSON, HANS, W.
Application year: 1988
Main classification: G01N29
IPC codes: G01F1, G01N29