METHOD AND DEVICE FOR DETERMINING A SUBSTANCE CONCENTRATION OR A SUBSTANCE IN A LIQUID MEDIUM
20180266939 · 2018-09-20
Assignee
Inventors
Cpc classification
G01N21/0303
PHYSICS
G01N21/1717
PHYSICS
International classification
G01N21/17
PHYSICS
Abstract
Method and device for determining at least one substance concentration (c) or at least one substance in a liquid medium, wherein the method consists of the following steps, liquid medium is introduced at a predefined flow speed into a vessel having a known shape, electromagnetic waves having predefined wavelength or having predefined wavelength range are coupled into the liquid medium contained in the vessel, wherein the electromagnetic waves cover a path length in the liquid medium which is dependent on a fill level (x.sub.i) of the liquid medium in the vessel, intensities (.sub.i) of the electromagnetic waves are measured after covering the path length in the liquid medium at at least two predefined points in time (t.sub.i) and/or at at least two predefined fill levels (x.sub.i) of the vessel, and
after a last intensity measurement, the at least one substance concentration (c) or the at least one substance is determined using the measured intensities (.sub.i) and the at least two predefined points in time (t.sub.i) or the at least two predefined fill levels (x.sub.i), respectively.
Claims
1. A method for determining at least one substance concentration (c) or at least one substance in a liquid medium (3), wherein the method consists of the following steps, liquid medium (3) is introduced at a predefined flow speed into a vessel (1) having a known shape, electromagnetic waves having predefined wavelength or having predefined wavelength range are coupled into the liquid medium (3) contained in the vessel (1), wherein the electromagnetic waves (8) cover a path length in the liquid medium which is dependent on a fill level (x.sub.i) of the liquid medium (3) in the vessel (1), intensities (.sub.i) of the electromagnetic waves are measured after covering the path length in the liquid medium (3) at at least two predefined points in time (t.sub.i) and/or at at least two predefined fill levels (x.sub.i) of the vessel (1), and after a last intensity measurement, the at least one substance concentration (c) or the at least one substance is determined using the measured intensities (.sub.i) and the at least two predefined points in time (t.sub.i) or the at least two predefined fill levels (x.sub.i), respectively.
2. The method according to claim 1, furthermore comprising the following steps, n intensities (.sub.i) are measured at n fill levels (x.sub.i), wherein the n fill levels (x.sub.i) are preferably selected as equidistant, and substance concentrations are determined according to the following formula:
3. The method according to claim 1, furthermore comprising the following steps, a first fill level (x.sub.0) is detected, at which a first intensity (.sub.0) is measured, a last fill level (x.sub.n) is detected, at which a last intensity (.sub.n) is measured, wherein the detection of the first level (x.sub.0) and/or the last fill level (x.sub.n) is preferably performed using a light barrier.
4. The method according to claim 2, furthermore comprising the step that the substance concentration c is computed either by averaging from n substance concentrations c.sub.i where i=1 . . . n or by means of linear regression, in particular by means of simple linear regression.
5. The method according to claim 1, wherein the flow speed of the liquid medium (3) is constant.
6. The method according to claim 1, wherein the vessel (1) is a cuvette, the longitudinal axis of which extends essentially vertically, and which has a constant cross-sectional area, wherein the electromagnetic waves are preferably coupled from below into the cuvette and the intensity (.sub.i) is preferably measured above the cuvette.
7. The method according to claim 1, furthermore comprising the steps that the vessel (1) is automatically emptied after the last intensity measurement and after completed emptying, the vessel (1) is automatically filled with new liquid medium (3) for a new measuring cycle.
8. The method according to claim 1, furthermore comprising the step that the fill levels (x.sub.i) are ascertained via a time measurement.
9. The method according to claim 1, wherein the electromagnetic waves have a wavelength of 254 nm or 550 nm.
10. A device for determining at least one substance concentration (c) or at least one substance in a liquid medium (3), wherein the device comprises: a vessel (1) having a known shape, a source (4) for generating electromagnetic waves (8), a measuring unit (7) for measuring electromagnetic waves, and a conveyor unit (13) that is connected to the vessel (1) via a connecting channel (2), characterized in that the source (4) can emit electromagnetic waves into the vessel (1), so that the electromagnetic waves cover a path length in the liquid medium (3) which is dependent on a fill level (x.sub.i) of the liquid medium (3) in the vessel (1), the measuring unit (7) is adapted for measuring intensities of the electromagnetic waves after covering the path length in the liquid medium (3) at at least two predefined points in time (t.sub.0, t.sub.n) and/or at at least two predefined fill levels (x.sub.0, x.sub.n) of the vessel (1), and a computer unit (16) is operationally connected to the source (4), the measuring unit (7) and the conveyor device (13), the computer unit (16) being adapted for determining of the at least one substance concentration (c) or the at least one substance on the basis of the measured intensities and the at least two predefined points in time (t.sub.i) or the at least two predefined fill levels (x.sub.i), respectively.
11. The device according to claim 10, characterized in that n intensities (.sub.i) are measurable at n fill levels (x.sub.i), wherein the n fill levels (x.sub.i) are preferably selected as equidistant, and substance concentrations are determinable in the computer unit (16) according to the following formula:
12. The device according to claim 10, characterized in that, a first fill level (x.sub.0) is detectable, at which a first intensity (.sub.0) is measurable, a last fill level (x.sub.n) is detectable, at which a last intensity (.sub.n) is measurable, wherein preferably a first light barrier (LS1) or a second light barrier (LS2) is respectively provided for detecting the first fill level (x.sub.0) and/or the last fill level (x.sub.n).
13. The device according to claim 10, characterized in that the substance concentration c is computable in the computer unit (16) either by averaging from the n substance concentrations c.sub.i where i=1 . . . n or by means of linear regression, in particular by means of simple linear regression.
14. The device according to claim 10, characterized in that a conveyor device (13) is provided, which is operationally connected to the connecting channel (2), wherein the conveyor device (13) conveys liquid medium (3), preferably at constant flow speed, into the vessel (1).
15. The device according to claim 10, characterized in that the conveyor device (13) for filling and emptying the vessel (1) comprises an automatically actuable switching valve.
16. The device according to claim 10, characterized in that the vessel (1) is a cuvette, the longitudinal axis of which extends essentially vertically, and which has a constant cross-sectional area, wherein the electromagnetic waves are preferably coupled from below into the cuvette (1) and the intensity (.sub.i) is preferably measured above the cuvette (1).
17. The device according to claim 10, characterized in that the vessel (1) is arranged inverted in the sense of an immersion probe, wherein a fill level (x.sub.i) in the vessel (1) is settable by means of air displacement.
18. The device according to claim 10, characterized in that electromagnetic waves having wavelengths of 254 nm and 550 nm can be generated using the source (4).
19. The device according to claim 10, characterized in that a viewing tube (12) has a communicative connection to the vessel (1), via which at least the first fill level (x.sub.0) and the last fill level (x.sub.n) are determinable.
Description
[0058] Exemplary embodiments of the present invention will be explained in greater detail hereafter on the basis of figures. In the figures:
[0059]
[0060]
[0061]
[0062]
[0063]
[0064] A first embodiment variant of the device according to the invention is schematically illustrated in
[0067] The mentioned functions do not necessarily have to be implemented in one unitthe conveyor device 13 according to
[0068] The predetermined flow speed is generated, for example, using a metering pump (for example, in the form of a displacement pump, in particular a gearwheel pump) or using a vessel having constant sample level (constant head) and using a capillary as a sample drain into the cuvette.
[0069] A source 4 for generating electromagnetic waves 8 (light) is arranged below the vessel 1, for example, so that the electromagnetic waves 8 are coupled into the vessel 1 such that a path length covered by these electromagnetic waves is dependent on a fill level of liquid medium 3 in the vessel 1. Accordingly, the electromagnetic waves 8 run from below (as shown in
[0070] Lenses or lens systems 5 and 6 can be provided to bundle the electromagnetic waves 8 emitted by the source 4 and to concentrate the electromagnetic waves after the penetration of the liquid medium 3 contained in the vessel 1. The efficiency is thus increased by better light yield.
[0071] The source 4, the measuring unit 7, and the conveyor device 13 are operationally connected to a computer unit 16, whereby a control of the device according to the invention can be performed according to a sequence to be explained hereafter.
[0072] The vessel 1as is apparent in
[0073] The electromagnetic waves 8 emitted by the source 4 have, for example, a wavelength of 254 nm or of 550 nm according to the above-mentioned norm DIN 38404-3 (July 2005). Depending on an absorption maximum, which is dependent on the ingredients to be detected, the wavelength can be selected arbitrarily. Accordingly, wavelengths other than the above-mentioned wavelengths are entirely conceivable.
[0074] In particular, it is also conceivable thatas indicated abovethe electromagnetic waves 8 emitted by the source 4 cover a predefined spectrum, therefore a predefined wavelength range, and not only one or possibly two wavelengths, as is provided according to DIN 38404-3. At the same time, the measuring unit 7 has to be designed so that intensities can be ascertained and/or measured at multiple frequencies, therefore also in a predefined spectrum and/or wavelength range. The possibility is thus also provided of being able to determine the substances present and the proportions thereof in the liquid medium 3 in the meaning of the known method and/or device according to EP-0 600 334 B1. Corresponding to EP-0 600 334 B1, an array of measuring channels is provided, the results of which are processed accordingly in the computer unit 16.
[0075]
[0076] In the embodiment variant shown in
[0077] Furthermore, a partially transmissive transmission unit 9 (for example, in the form of a partially transmissive mirror) is provided in the region of the source 4, which transmits the electromagnetic waves of the source 4 in the direction of the measuring unit 7, but also deflects the electromagnetic waves generated by a further source 11 in the direction of the measuring unit 7. Therefore, the sources 4 and 11 can generate electromagnetic waves having different wavelengths and can couple them simultaneously or offset in time into the liquid medium 3 in the vessel 1. Based on the requirement of norm DIN 38404-3 (version July 2015), for example, the source 4 can generate electromagnetic waves having a wavelength of 254 nm and the source 11 can generate electromagnetic waves having a wavelength of 550 nm. A compact instrument is therefore obtained, which enables a targeted measurement of the residual intensities at two different wavelengths .
[0078] As already in the case of the source 4, a lens or a lens system 10 is also connected downstream in the case of the further source 11, so that a maximum light yield can be achieved during a measuring procedure. Furthermore, the further source 11 is also operationally connected to the computer unit 16 for activation. This also applies to the light barriers LS1 and LS2, the detection signal of which is also supplied to the computer unit 16 for further processing.
[0079] Of course, it is also conceivable in this embodiment that the sources 4 and 11 can emit a predefined wavelength range as defined in EP-0 600 334 B1, to be able to ascertain the substances and/or substance concentrations provided in the liquid medium 3again according to the teaching of EP-0 600334 B1.
[0080]
[0081] The embodiment variant of the present invention shown in
[0082] Furthermore, the distance x between the two windows 21 and 22 can be ascertained using a read unit 23 via a scale applied to the lateral walls of the vessel 1 and the container 20, which are displaced in relation to one another depending on the distance x.
[0083] A further embodiment variant of the present invention is shown in
[0084] If the absorption measurements for a sample are completed, the vessel 1 is in turn emptied by pressing airfor example, from an existing compressed air system, which consists of a pressurized containerthrough the connecting channel 2 into the vessel 1, whereby the liquid medium 3 is displaced out of the vessel 1 via the opening 24. As soon as the vessel 1 has been completely or nearly completely emptied, a new measuring cycle can be started.
[0085] If the connecting channel 2 is arranged spaced apart from the measuring unit 7as shown in
[0086] The method according to the invention will be explained hereafter on the basis of the flow chart illustrated in
[0087] In a step I, the conveyor device 13 (
[0088] In a step II, electromagnetic waves 8 having predefined wavelength are coupled into the liquid medium 3 contained in the vessel 1, wherein the electromagnetic waves 8 cover a path length in the liquid medium 3 which is dependent on a fill level x.sub.i of the liquid medium 3 in the vessel 1. The intensities of the received electromagnetic waves are measured using the measuring unit 7 (
[0089] The intensity measurement is repeated at at least one further point in time, i.e., with increased fill level in the vessel. In the flow chart according to
[0090] As soon as the measurements are completed (i.e., i=n), the substance concentration c is or substance concentrations c.sub.i are determined using the measured intensities .sub.i and the at least two predefined fill levels x.sub.i in step III.
[0091] Therefore, in step IV, the vessel 1 can in turn be emptied and therefore made ready for a next concentration determination c. It is to be expressly noted that it is not necessary to wait after the last intensity measurement for step IV. In particular, it is not necessary to wait until the concentration determination according to step III is completed. Rather, the emptying of the vessel 1and therefore step IVcan be begun immediately after the last intensity measurement under step II.
[0092] The measurement according to the invention of at least two intensities .sub.i at at least two fill levels x.sub.i of the vessel 1 has the great advantage that a possible drift of the zero point as a result of soilingfor example, of the cuvette region, through which the electromagnetic waves are coupled into the liquid mediumhas no influence on the measurement results and/or on the concentration c to be determined.
[0093] The substance concentrationwith application of and by derivation of the known law of Lambert, Beer, and Bouguercan be determined according to the following formula:
wherein c.sub.i is the i-th substance concentration, x.sub.i is the i-th fill level, .sub.i(x.sub.i) is a measured i-th intensity at a fill level x.sub.i, i is the index, which extends in integers from 1 to n, and is the coefficient of extinction, and wherein n has a value in the range of 1 to several hundred, preferably a value in the range of 10 to 100.
[0094] Accordingly, n intensities .sub.i are measured at n fill levels x.sub.i, wherein the n fill levels x.sub.i are preferably selected as equidistant.
[0095] The essential advantage in relation to known solutions manifests itself directly in the above formula: The intensity, which is responsible for the zero point, of the magnetic waves originating from the source 4 and coupled into the liquid medium 3 is eliminated by the differentiation according to the invention and/or by the derivation. For this reason, at least two measurements are necessary at different fill levels x.sub.i in the vessel.
[0096] The point in time t.sub.i and/or the fill level x.sub.i, at which an intensity .sub.i(x.sub.i) is measured can be produced in different ways: firstly, the option exists of initiating a first measurement by means of time measurement after completion of step IV and performing a further measurement or further measurements in each case after a further time span or after further time spans. Since if the flow speed is known during the filling of the vessel and the shape of the vessel is known, the fill level x.sub.i may also be readily determined. Fill level x.sub.i and point in time t.sub.i are directly related to one another under these conditions and if one variable is known, the other may be readily determined.
[0097] If n is selected as greater than 1, multiple values are obtained for the concentration c, namely n values for the concentration, so that an improved result is obtained for the concentration c, for example, by averaging or by means of linear regression, in particular by means of simple linear regression.
[0098] The above-explained method may also be determined in a similar manner for determining substances and/or substance proportions in the liquid medium 3. The embodiments in EP-0 600 334 B1 are applied accordingly.