METHOD AND DEVICE FOR DETERMINING THE CONCENTRATION OF A SUBSTANCE BOUND TO PARTICLES CARRIED BY A FLOWING MEDIUM

Abstract: Method and device for determining the concentration of a substance, which is bound to particles in a flowing medium (1), which substance can prevail in varying concentration. The determination is carried out by light beams (2) so selected, that the substance is absorbent for the radiation within a certain wavelength range, while the remainder of the particle material is reflecting. By means of a detector (4) the radiation is determined which passes straight through the flowing medium, and by means of a detector (5) the radiation is determined which is scattered in a certain direction by the particles in the medium. The concentration is calculated from the equation (FORMULA) where I<uo>u is the intensity of incident radiation, I<ur>u is the intensity of radiation which has passed straight through the medium, Is is the intensity of detected scattered radiation, k is a constant between 1/2 and 1 depending on the detection angle for the scattered radiation, and A, c<u1>u, c<u2>u, c<u3>u are constants.

Description: Method and device for determining the concentration of a substance bound to particles carried by a flowing medium This invention relates to a method of the kind refer¬ red to in the preamble of the attached claims 1 and 2, and to devices for carrying out the respective method. The present invention is the result of efforts to find a simple and reliable method of obtaining a measured value, which has a well-defined relation to the so-called kappa number, which is a measure of the lignin content in wood fibres. When the method was well composed, however, it was found to have a much wider field of application. The method is well suited for determining the content of substances bound to particles, where the substance in question is radiation absorbing for a definite radiation wavelength interval and can be regarded as if it was placed as a thin layer in the surface of a particle, the surface of which bordering on the layer is reflecting for a radiation wavelength range, within which the radiation wavelength in question is located. The substance in question virtually may be a thin layer, but it is also possible to use the method when the substance is spread as local concentration variations in the particles. The method thereby also can be used, for example, for bright¬ ness determination of colour measurement on suspended particles, for surface structure examination of different substances on suspended particles, for studies of sur- face coats on suspended particles, a.s.o. At the preparation of cellulose pulp for paper manu¬ facture the pulp is analysed with respect to its content of residue lignin after the preparation. The lignin con¬ tent of the completed pulp heretofore has been determined by taking pulp samples for chemical analysis. It then was determined how much chlorine or potassium permanganate a definite amount of pulp consumes at oxidation. These chemical analyses are relatively complicated and ti e- -consuming. . Moreover, they cannot be carried out on-line at the process. A substantial improvement and simplification is ob¬ tained, in that the method according to the invention has . been given the characterizing features defined in the attached claims. The method can be carried out on-line automatically at short intervals. It can be initiated from a control room spaced from the place where the pulp manu¬ facture proper takes place. At experiments with the method good correlation was obtained with the values resulting from more or less direct methods being used at present, such as the kappa number method and the chlorine number method. The wood, from which the pulp is made, is built up of different cells joined together by.lignin. At the manu¬ facture of cellulose pulp, for example according to the sulphate method where the wood chopped to chips is digested under pressure at high temperature, the wood is subjected to a treatment for exposing the individual fibres and dissolving the lignin. The lignin remaining in the pulp after this treatment can be regarded as if existing only as a thin layer about each fibre. This does not fully agree with reality, but the lignin content in each fibre is substantially higher at the periphery than at the core of the fibre. Lignin was at examinations found to be strongly absorbing for ultraviolet light, while the mate- rial, of which the core in each fibre largely consists, is reflecting for these wavelengths of the light. The present invention makes use of this circumstance. The invention is described in greater detail in the following, with reference to the accompanying drawing, in - which Fig. 1 is a basic sketch of a measuring device arranged in agreement with the principles of the inven¬ tion, Fig. 2 shows the behaviour of the incident light for a cross-section of a fibre, and Fig. 3 shows a special diaphragm used. At the invention embodiment shown in Fig. 1 , fibre material 1 suspended in water is illuminated by ultra¬ violet light in a narrow beam 2. The suspended fibre material 1 flows at high-grade turbulence through a bulb 3. Two detectors 4, 5 are located on opposite sides of the bulb 3 toward the light source 6 with associated optical unit 7 producing the beam 2. One detector 4 is located so that it is influenced substantially only by light passing straight through the suspension. The second detector 5 is located so as to be affected only by light, which was reflected against one or more of the particles in the sus¬ pension. The light meeting the first detector 4 can with good approximation be said to have passed through the suspen¬ sion in such a manner, that the radiation has not inter¬ acted with any part of any fibre. The light meeting the second detector 5, however, always has been reflected against at least one fibre. The suspension should be so diluted that the probability is low that the light is reflected against several fibres and thereafter meets one of the detectors. As the light source 6 delivers a substantially con- stant known light flow incident to the suspension, light scattering against the particles implies that an increase in intensity of the scattered, i.e. reflected, light is corresponded by a proportionally equally great decrease in intensity of the light flow passing straight through the suspension. When no light is absorbed at the particles in the suspension, but the particles are entirely reflect¬ ing, the effect on the intensity of the scattered light is equal to the effect on -the intensity of the light passing straight through the suspension. - When the lignin itself, in .which the particles are suspended, is absorbent to some extent, the radiation to the two detectors 4, 5 is affected equally, if the paths of the light through the suspension to the two decectors are of equal length. When absorption does not occur at the particles themselves nor in the liquid, in which they are suspended, the total of the intensity I of the total scattered light and the intensity I of the light passing straight through is equal to the intensity I of the irradiated light, i.e. Is/Ir = (Io-Ir} / Ir = (Io/Ir)-1 (1) When now the particles carry a layer of light-absorb- ing lignin, the term I is affected, but not the term I . The equation (1) is not valid any longer. Due to the light absorption at the reflection against fibres in the suspen¬ sion, the light scattered to the second detector 5 is damped, while the light meeting the first detector 4 is not influenced by the effect of the surface layer on the i fibres. The lignin certainly is not in the form of a thin layer about every fibre, but rather has the form of local density variations in the fibres. However, for obtaining the equations on which the invention is based, the layer state of the lignin is assumed to apply with good approxi¬ mation. It also is assumed that every; fibre has substant¬ ially circular-cylindric or globe shape. The fibres flow with complete turbulence, in order to eliminate the influ- ence of the shape and orientation of the fibres on the measurement result. At illumination perpendicularly to the flow direct¬ ion, the light meeting a particle passes through a portion of a. circle segment with the height Δr of an annular cross-section of the particle consisting of the lignin layer, before the light meets the particle surface re¬ flecting the light used, whereafter the light again travels through an equally long path through the lignin - layer. Fig. 2 is a cross-sectional view of a fibre 1a and shows the circle segment ABC with the thickness _ r , through which the incident light 31 and the reflected light 32 at a certain angle of incidence pass through the distance 2a. The lowest value, which the distance a can assume, is Δr (see Fig. 2), where the light flows radially. The highest value, which the distance _a can c::τι assume is s = (r+Δr) sin < ^ , where the light flows tan- gentially toward the surface of the fibre core. Since the angle 3 = AT/2 s lτi Ot = 2 Δr s/(s 2 + Δr 2 ) = s/(r+Δr) = 2 r Δr -^Λr 1 2 Thereby the distance 2a, through which the light passes through the lignin layer, is obtained between the limits 2 /\r < 2a < 2 \/ 2 r r ' i.e. when r is assumed constant (equal fibre size) , then k 2a *~--Λ r where 1/2 < k < 1 The quotient between scattered light and light passing straight through the sample then is Is/Ir = (Io/Ir-1 C exp( -u k. Λ (2) where u is an optic constant dependent on the material (lignin), and k. is * "a constant dependent on the particle size. The exponential function is obtained by applying the Lambert-Beer law. Irrespective of whether the particles are spherical or oblong, the amount of absorbing material per particle is proportional to \ r, provided that the sample, on which the measurement is carried out has a sub¬ stantially constant composition of homogenous material particles. Thereby the concentration lignin, konc. is: This equation is not fully in agreement with prac¬ tise, but certain adjustments are to be made. At compara¬ tive measurements of cellulose pulp with varying kappa number the following equation has proved to yield a good correlation between measurement results obatined with the method according to the invention and measurement results obtained in conventional manner. konc. = A 1n (4) where. A is a proportionalization constant, c, ' is a con¬ stant selected so that konc. = 0 at measurement of non- -absorbing material, c ? is a constant obtained by the measurement of two or more calibration suspensions with the same kappa number, but with different concentration of suspended material, and selected so that konc. is in¬ dependent of concentration variations of the suspended material, and c. is a constant dependent on the dimensions of the measuring instrument and established at the mea¬ surement of clear water. The detector 5, however, is not arranged so that it is met by all light scattered by the particles in the suspension. The detector, instead, has a position to be met by light scattered substantially in a definite direct¬ ion. Thereby, the constant k in the equation (3) is de- fined and entirely depending on the location of the detec¬ tor 5, which indicates the scattered light, because the reflection .angle for the reflection against the particles is approximately defined thereby. For every angle, at which a particle is met by light, the light scattered to a detector 5 located in a certain angular position with some probability is a definite fraction of the entire scattered light flow. This implies, that the light intensity detected by the detector 5 can be expected to be b-I . ' where b is a constant smaller than 1. Consequently, the light arriving at the detector 5 can be expected to be a definite fraction of all scatt¬ ered light damped as if it had been scattered at an entirely definite angle by the particles in the suspension, The constant k, of course, can be calculated, but for a definite arrangement with bulb, light source and detectors it is most simply determined by comparative examination after chemical methods of several samples, which also are fed through the bulb. In the foregoing was assumed throughout, that all fibres in a sample have substantially the same appearance and the same size, whereby the radius r and the volume of the lignin layer are.equal for all fibres and can be regarded as constant factors. In reality, however, the situation is not quite so ideal. The fibres in a sample have varying sizes. The thickness r °f tne lignin layer depends on the size of the individual fibre, i.e. on the radius r. The concentration of lignin in a sample in relation to the pulp concentration is related to the fibre size. It was found possible, however, in spite of varying size distribution of the fibre material, to mea¬ sure on the basis of the above equation (4) when the op¬ tical unit is so designed that the ratio between increase of the signal from the detector 5 and . decrease of the signal from the detector 4 is constant for small as well as large particles. In Fig. 3 a diaphragm 21 is shown -located between the bulb and the detectors on the output side. Said dia¬ phragm 21 is fan-shaped, and its pointed portion 22 is located so that the. straight ray path to the detector 4 passes through this portion. The wider portion 23 of the diaphragm is located so that the scattered ray path to the detector 5 passes through this portion. The angle at the tip can be adjusted', in that the lateral pieces 24, 25 of the diaphragm 21 are hinged one to the other and rotatable about a centre 26. The lateral pieces 2 * 4, 25 at the wider portion 23 of the diaphragm are provided with end pieces 27, 28, which are angular relative to each other, and the diaphragm edges of whic are arcs with the centre in 26. One end piece 27 is located above the other one 28, so that they can be moved toward and away from each other upon a change of the angle o • At 29 and 30 the places inside the diaphragm are marked, through which the two straight lines from the centre of the bulb extend to the detectors 4 and, respect¬ ively, 5. The diaphragm shown provides by a simple struc¬ tural design a funcion, which is correct in practice. Other designs, for example elliptic shape or a design having two openings or the like, however, can yield a similar result. The essential feature is that the diaphragm effects an increase of the scattering signals which pro¬ portionally is of equal size as the decrease of the signals straight ahead for different particle sizes. The signals from the two detectors 4, 5 are fed each to a circuit 8, 9, which carry out analog-to-digital con¬ version and indicate the mean level of the signal during a definite period. This period preferably is longer than approx. 10 seconds. On a diaphragm 10 for the incident beam 2 a further detector 11 is provided to detect the incident light. In the ideal case, as mentioned, the sample is illuminated by a light source producing a constant light flow. This condition cannot be met when- the sample is to be illuminated by ultraviolet light, and the measuring in¬ strument is to be held within reasonable costs. The refe¬ rence detector 11, therefore, is provided in order to con¬ tinuously detect variations in the light intensity of the light from the light source 6 and to adjust measurement results in agreement wit these variations. The output signal from the detector 11 is fed to an analog-to-digital 12. The outputs from the units 8, 9 and 12 are coupled to -inputs on a calculating unit 13, which carries out the calculation according to the ■ above equation (4) and displays the calculation result on a display 14. The calculation unit may be a microprocessor. Calculation is carried out during the- entire measuring period at short intervals with instantaneous values avail- able from the detectors 4, 5 and 11. The mean value of the calculations is displayed after the end of the measur¬ ing period. It is also possible, however, to cause the calculation unit to calculate the mean value of each one of the sig¬ nals from the detectors 4, 5 and 11 during a perio * d longer than approx. 10 seconds, whereafter the unit carries out the calculation according to equation (4) with the mean values inserted. An alternative method with an alternative device is described in the following on the basis of equation (4) . The measured sig to nal Ir included in the numerator in the equation (4), of course, can be measured from the same sample, but in a different, adjacent measuring in¬ strument and in another radiation wavelength range than the measured signals included in the denominators. When for this other measuring instrument a radiation wavelength range is used where no radiation absorption occurs of such substances, which are dissolved in the carrier liquid, but have radiation absorption in the first mea¬ suring instrument, the equation (4) is not affected by such substances dissolved in the sample, because the mea¬ sured signals included in the denominator in the equation (4) are affected to the same degree by the radiation absorption. This implies that this effect disappears at quote formation of these signals. This in its turn implies that lignin dissolved in the liquid does not affect the kappa number measuring and, therefore, need not be washed off, either, when the wave¬ length in the adjacent measuring instrument is located in the near IR-range. The sample pretreatment, therefore, is considerably simpler. The sig°nal ■ Io in the numerator of the eq^uation can * in this case either be the measured signal from a refer¬ ence detector located in the ray path of the adjacent mea¬ suring instrument, or the measured signal I in the adjacent measuring instrument at clear water calibration. In the first entioned case the additional adjacent measur- ing instrument is built up in analogy with Fig. 1 : light source - optics - diaphragm - bulb - detector - analog-to- -digital converter. This instrument can be connected to the same calculation unit 13 as the first measuring in¬ strument. Finally a further alternative is described, which also is based on the equation (4) . In the equation (4) the factor 1/1 included both in the numerator and denominator is a direct function of the concentration and the fraction composition of the material suspended in the sample. This implies, in the case when the fraction composition is substantially constant, that when the material concentration of the suspension flowing past the measuring instrument can be held constant, the concentration lignin will be a unique function of I , i.e. of the signal from the detector 5 in Fig. 1 which indicates light scattered in a definite direction. This implies that the method according to the invention can be carried out with only one detector when the material concentration and the fraction composition in the suspension are held 'constant. This can be brought about, for example, by posi¬ tioning a concentration measuring instrument upstream of the measuring instrument according to the invention, in which case the signal from the concentration measuring in¬ strument must control the dilution of the suspension so that the signal of the concentration measuring instrument is held constant. The concentration lignin being a unique function of I , a great number of values of I corresponding to the lignin content can be stored in a memory in the calculation unit. The memory cell is for a received value of the input signal addressed with the value closest to the input signal, and the value in the memory cell is discharged on the display unit. The memory cells possibly may also be addressed with the two values closest to the input signal, and an inter¬ polation between the values of the lignin content stored in these cells is carried out prior to the display on the display unit. The lignin content also can be calculated by the help of a funktion of I. , which has been adapted to the lignin content * of the sample by empiric correlation. A great number of modifications can be imagined within the scope of the invention.

Claims: CLAIMS • 1. A method for determining the concentration of a substance bound to particles carried by a flowing medium, which substance within different zones with varying con¬ centration is located in the particles together with the remaining particle material, and where for a definite radiation wavelength range the substance is radiation absorbent and the remainder of the particle material is radiation reflecting, c h a r a c t e r i z e d in that the medium is radiated by a radiation source which emits radiation within the said radiation wavelength range, and that radiation passing straight through the medium is detected, and radiation which by particles in the medium has been scattered in a definite direction is detected, and that the concentration konc. of the said substance is calculated according to the formula where Io is the intensity J of the incident radiation, ' Ir is the intensity of the radiation passing straight through the medium, I is the intensity of the detected scattered radiation, k is a constant between 1/2 and 1 depending on the detection angle for the scattered radiation, and A, c. , c ? , c, are constants. 2. A method of determining the.concentration of a substance bound to particles carried by a flowing medium, where the substance in different zones with varying con¬ centration is located in the particles together with the remaining particle material, and where for a definite radiation wavelength range the substance is radiation ab¬ sorbent and the remainder of the particle material is radiation reflecting, and where also varying concentration of the substance can be dissolved in the flowing medium, but must not affect the concentration determination, c h a r a c t e r i z e d in that the medium is radiated by two radiation sources, one of v/hich emits radiation with¬ in said radiation wavelength range, and the second source emits radiation within a second wavelength range different from the first range, and where both radiation which with¬ in the first wavelength range has passed straight through the medium is detected, and radiation within said range which has been. scattered in a definite direction by par-_ tides in the medium is detected, and radiation within said second wavelength range which has passed straight through the medium is detected, and that the concentration kόnc. of the first substance is calculated according to where ' said second wavelength range or the intensity of the radiation within said range which has passed straight through the medium without any particles therein, I - is the intensity of the radiation within said second wave¬ length range which has passed straight through the medium, Ir_l. is the intensity J of the radiation within the first wavelength range which has passed straight through the medium, I is the intensity of the detected scattered radi- s • J ation within the first wavelength range, k is a constant between 1/2 and 1 depending on the detection angle for the scattered radiation, and A, c. , c ? , c, are constants. 3. A method of determining the concentration of a substance bound to particles carried by a flowing medium, where the substance withi-n different zones with varying concentration is located in the particles together with the remaining particle material, and for a definite radi¬ ation wavelength range the substance is radiation absorbent and the remainder of the particle material is radiation reflecting, c h a r a c t e r i z e d in that the particle concentration in the medium is held substantially constant at approximately constant fraction composition, and the medium is radiated by a radiation source, which emits radi¬ ation within the said radiation wavelength range, and that radiation which by particles in the medium has been scatt¬ ered in a definite direction is detected, and the mean value of the detected signal is in a unique relation to the concentration of the substance carried to the particles. 4. A device for carrying out the method according to claim 1 for determining the concentration of a substance bound to particles carried by a flowing medium, where the substance within different zones with varying concentrat¬ ion is located in the particles together with the remain¬ ing particle material, and for a definite radiation wave¬ length range the substance is radiation absorbent and the remainder of the particle material is radiation reflecting, c h a r a c t e r i z e d in that a radiation source (6) with radiation substantially within the said wavelength range illuminates the medium with the particles, and two detectors (4, 5) are located so that one detects radiation received straight through the medium, and the second one detects radiation scattered by the particles in the medium in a definite direction, and a calculation unit (13) carries out a calculation of the concentration of the first substance by guidance of the signals from the detectors (4, 5) according to the formula where Io is the intensity of the incident radiation, Ir is the intensity of the radiation which has passed straight through the medium, I is the intensity of the detected scattered radiation, k is a constant between 1/2 and 1 depending on the detection angle for the scattered radi¬ ation, and A, c _. 3 c , c, are constants. 5. A device for carrying out the method according to claim 2 for determining the concentration of a substance bound to particles carried by a flowing medium, where the substance within different zones with varying concentration is located in the particles together with the remaining particle material, and for a definite radiation wavelength range the substance is radiation absorbent and the re¬ mainder of the particle material is radiation reflecting, c h a r a c t e r i z e d in that two radiation sources are provided, one of which emits radiation within said radiation wavelength range, and the second one emits radi¬ ation within a second wavelength range different from the first range, and three detectors are so located that one detector detects radiation received straight through the medium within the first wavelength range, the second de¬ tector detects the radiation within the first wavelength range which has been scattered by the particles in a defi¬ nite direction, and the third detector detects the radi¬ ation received straight through the medium within the second wavelength range, and that a calculation unit carries out a calculation of the concentration with guid¬ ance by the signals from the three detectors according to the formula where Io is the intensity J of the incident radiation vrithin said second wavelength range or the intensity of the radi¬ ation within said wavelength range which has passed straight through the medium without any particles therein, I - is the intensity of the radiation within said second wavelength range which has passed straight through the medium, I _, is the intensity of the radiation within said first wave¬ length range which has passed straight through the medium, Is is the intensity J of the detected scattered radiation with- in said first wavelength range, k is a constant between ,6 1/2 and 1 depending on the detection angle for the scatt¬ ered radiation, and A, c. , c 2 , c_ are constants. 6. A device for carrying out the method according to claim 3 for determining the concentration of a substance bound to particles carried by a flowing medium, where the substance within different zones with varying concentrat¬ ion is located in the particles together with the remain¬ ing particle material, and for a definite radiation wave¬ length range the substance is radiation absorbent and the remainder of the particle material is radiation reflect¬ ing, c h a r a c t e r i z e d in that the particle con¬ centration in the medium is held on a constant level at approximately constant fraction composition, and a radi¬ ation source (6) with radiation substantially within the said wavelength range illuminates the medium with the par¬ ticles, and a detector (5) detects the radiation scattered in a definite direction by the particles in the medium, and that a signal processing unit calculates the mean value of the signal and displays a value of the content of the substance bound to the particles in a definite relation to the calculated mean value. 7. A device as defined in any one of the claims 4-6 for measuring the lignin content in cellulose fibres, c h a r a c t e r i z e d in that the radiation from the radiation source lies within the ultraviolet radiation range, and the radiation source (6) preferably is a mer¬ cury lamp. 8. A device as defined in claim 5 for measuring the lignin content in cellulose fibres, c h a r a c t e r - • i z e d in that the radiation source emits radiation within the near infrared range and preferably is a light emitting diode. 9. A device as defined in any one of the claims 4-8, c h a r a c t e r i z e d in that a reference detector (11) is provided to detect the intensity I for the light incident to the medium. 10. A device as defined in any one of the claims 4-9, c h a r a c t e r- i z e d in that the calculation unit (13) carries out the calculation by guidance of mean in¬ tensities ascertained during a period exceeding approx¬ imately 10 seconds. 11. A device as defined in any one of the claims 4-10, c h a r a c t e r i z e d in that the calculation unit (13) during a period exceeding approximately 10 seconds carries out many calculations by guidance of the instant¬ aneous value from each detector and calculates the means value of the same. 12. A device as defined in any one of the claims 4, 5, 7-11, c h a r a c t e r i z e d in that a diaphragm (21) is located on the same side of the flowing medium as .the detectors (4, 5) for light radiated through the medium and before said detectors, which diaphragm (21) is designed so, that for both small and large particles the ratio between the increase of the signal from the detector (5), which detects light scattered by the par¬ ticles, and the decrease of the signal from the detector (4), which detect-s radiation straight ahead, is constant. 13. A device as .defined in claim 12, c h r a c t¬ e r i z e d in that the diaphragm (21) is approximately fan-shaped and located with its pointed portion so, that the radiation straight through the medium passes near the pointed portion, and the radiation scattered by the particles passes near the wider circular portion of the diaphragm. 14. A device as defined in claim 13, c h a r a c t¬ e r i z e d in that the top angle of the diaphragm (21) is adjustable and can be adjusted to correct position by calibration. 15. A device as defined in any one of the claims S-14, c h a r a c t e r i z e d in that a turbulence former is located so as to cause the medium to flow with high-degree turbulence past the measuring position.

Inventors: FLADDA GERDT, KUBULNIEKS EGILS, PETTERSSON TORULF, FLADDA G, KUBULNIEKS E, PETTERSSON T
Applicants: FLADDA G, KUBULNIEKS E, PETTERSSON T, SVENSKA TRAEFORSKNINGSINST
Application year: 1980
Main classification: G01N21
IPC codes: G01N15, G01N21