Enhanced optical data capture using NDIR for liquids

1. An apparatus for determining a concentration of a targeted molecule M within a given time period in a liquid sampling matrix in which at least one interfering molecule M J coexists with the targeted molecule, comprising:

a signal source;

an interference source;

a reference source;

a multiplexer and a collimator configured to pulse infrared radiation from the signal source, the interference source and the reference source into a pulsed beam which is directed at a first inclined angle (θ i1 ) to a normal of a first spot of the liquid sampling matrix;

a detector configured to detect infrared radiation after it emerges from the first spot as a first pulsed signal and reference channel output and a first pulsed interference signal and reference channel output from the pulsed beam after it penetrates into the first spot;

means for changing the imposed location of the pulsed beam so that it is directed at a second inclined angle (θ i2 ) to a normal of a second spot of the liquid sampling matrix and the detector is configured to detect infrared radiation after it emerges from the second spot as a second pulsed signal and reference channel output and a second pulsed interference signal and reference channel output from the pulsed beam after it penetrates into the second spot;

signal processing for:

obtaining a first average ratio value of R ave (t 1 ) for a first preselected period of time (“t 1 ”) from the first pulsed signal and reference channel output, where R ave (t 1 )=signal channel/reference channel output for the first preselected period of time;

obtaining a first average ratio value of R Jave (t 2 ) for a second preselected period of time (“t 2 ”) from the first pulsed interference and reference channel output, where R Jave (t 2 )=interference channel/reference channel output for the second preselected period of time;

obtaining a second average ratio value of R ave (t 3 ) for a third preselected period of time (“t 3 ”) from the second pulsed signal and reference channel output, where R ave (t 3 )=signal channel/reference channel output for the third preselected period of time, and

obtaining a second average ratio value of R Jave (t 4 ) for a fourth preselected period of time (“t 4 ”) from the second pulsed interference and reference channel output, where R Jave (t 4 )=interference channel/reference channel output for the fourth preselected period of time; and

electronics configured to use R Jave (t 2 ) and R Jave (t 4 ) to determine that a calibration curve is valid for the given time period and, if the calibration curve is valid, to calculate the concentration of the targeted molecule M in the liquid sampling matrix by use of R ave (t 1 ), R ave (t 3 ) and the calibration curve and provide the concentration of the targeted molecule M in the liquid sampling matrix as an output;

wherein the signal source emits radiation at a signal wavelength which is within a first absorption band of the targeted molecule M, the interference source emits radiation at an interference wavelength which is within a second absorption band of said at least one interfering molecule M J , and the reference beam emits radiation at a reference wavelength which is neutral and is not within either the first absorption band or the second absorption band;

wherein said at least one interfering molecule M J absorbs radiation at the signal wavelength; and

wherein the signal source, the interference source and the reference source are each pulsed at a preselected frequency of at least N Hz which is sufficiently fast so that a given molecule of the targeted molecule M or said at least one interfering molecule M J will not pass in and out of the liquid sampling matrix within the preselected frequency.

2. The apparatus of claim 1 , wherein the means for changing the imposed location of the pulsed beam does not change the physical location of either the pulsed beam or the detector.

3. The apparatus of claim 2 , wherein the means for changing the imposed location of the pulsed beam uses an optical device to change the direction of the pulsed beam.

4. The apparatus of claim 3 , wherein the means for changing the imposed location of the pulsed beam uses a piezo/electronic device to move the optical device.

5. The apparatus of claim 3 , wherein the means for changing the imposed location of the pulsed beam uses an electronic device to move the optical device.

6. The apparatus of claim 3 , wherein the means for changing the imposed location of the pulsed beam uses a magnetic device to move the optical device.

7. The apparatus of claim 3 , wherein the means for changing the imposed location of the pulsed beam uses a mechanical device to move the optical device.

8. The apparatus of claim 1 , wherein the means for changing the imposed location of the pulsed beam changes the physical location of the pulsed beam.

9. The apparatus of claim 1 , wherein the means for changing the imposed location of the pulsed beam changes the physical location of the detector in tandem with the pulsed beam.

10. The apparatus of claim 1 , wherein the targeted molecule M is glucose, said at least one interfering molecule M J is comprised of a plurality of interfering molecules contained in a body interstitial fluid and radiation emerging from the spot is collected by a lens onto the detector.

11. A process for determining a concentration of a targeted molecule M within a given time period in a non-homogenous liquid sampling matrix in which at least one interfering molecule M J coexists with the targeted molecule by use of a non-invasive apparatus, comprising the steps of:

pulsing infrared radiation from a signal source, an interference source and a reference source into a multiplexer and collimating radiation leaving the multiplexer into a pulsed beam which is directed at a scanning sample of three or more spots of the liquid sampling matrix;

detecting infrared radiation by a detector after it emerges from the scanning sample of three or more spots as a pulsed signal and reference channel output and a pulsed interference signal and reference channel output from the pulsed beam after it penetrates into the scanning sample of three or more spots;

using signal processing to obtain an average ratio value of R ave (t) for a first preselected period of time (“t”) from the pulsed signal and reference channel output, where R ave (t)=signal channel/reference channel output for the first preselected period of time;

using signal processing to obtain an average ratio value of R Jave (t 2 ) for a second preselected period of time (“t 2 ”) from the pulsed interference and reference channel output, where R Jave (t 2 )=interference channel/reference channel output for the second preselected period of time;

determining a chosen calibration curve for the non-invasive apparatus;

using electronics to calculate the concentration of the targeted molecule M in the liquid sampling matrix by use of R ave (t) and the chosen calibration curve; and

providing the concentration of the targeted molecule M in the liquid sampling matrix as an output from said electronics

wherein the signal source emits radiation at a signal wavelength which is within a first absorption band of the targeted molecule M, the interference source emits radiation at an interference wavelength which is within a second absorption band of said at least one interfering molecule M J , and the reference beam emits radiation at a reference wavelength which is neutral and is not within either the first absorption band or the second absorption band;

wherein said at least one interfering molecule M J absorbs radiation at the signal wavelength;

wherein the signal source, the interference source and the reference source are each pulsed at a preselected frequency of at least N Hz which is sufficiently fast so that a given molecule of the targeted molecule M or said at least one interfering molecule M J will not pass in and out of the liquid sampling matrix within the preselected frequency; and

wherein the chosen calibration curve is obtained by the steps of:

using the non-invasive apparatus to obtain a set of calibration curves for a set of different known concentration samples wherein each of the set of calibration curves contains a plurality of assumed β values, wherein β is a parameter indicating the ratio of the absorption strength of interfering molecules measured respectively at the signal wavelength and the interference wavelength;

using the non-invasive apparatus to calculate the concentration of the targeted molecule M in a known concentration calibration sample by use of R ave (t) and determining a best calibration curve of the set of calibration curves which achieves a calculated concentration closest to a known concentration of the known calibration sample; and

using the best calibration curve as the chosen calibration curve.