This invention relates to the field of detection of nitrogen-containing trace-gases, and in particular to a detector unit that uses a converter that converts nitrogen-containing compounds into nitrogen dioxide, and a low cost and compact nitrogen dioxide (NO2) detector comprising a blue semiconductor laser and quartz-enhanced photo-acoustic sensor.
U.S. Pat. No. 6,612,306 “RESPIRATORY NITRIC OXIDE METER”, issued 2 Sep. 2003 to James R. Mault, and incorporated by reference herein, teaches a respiratory gas meter for detecting gas components of respiratory gas flowing along a flow path. As detailed in this reference, endogenous production of nitric oxide (NO) is increased in patients with asthma and other inflammatory lung diseases, as well as in patients with reactive airways disease. Mault cites U.S. Pat. No. 5,922,610 “SYSTEM TO BE USED FOR THE DETERMINATION OF NO LEVELS IN EXHALED AIR AND DIAGNOSTIC METHODS FOR DISORDERS RELATED TO ABNORMAL NO LEVELS”, issued 13 Jul. 1999 to Alving et al., incorporated by reference herein, for teaching the use of nitric oxide measurements in the diagnosis of inflammatory conditions of the airways, such as allergic asthma and rhinitis, in respiratory tract infections in humans and Kartagener's syndrome, as well as gastric disturbances. Other uses of nitric oxide detection for medical diagnoses are also cited by Mault.
In addition to detecting nitric oxide for medical diagnoses, detectors for measuring the concentrations of various nitrogen oxides, generally referred to as NOx are used to detect environmental concentrations, including vehicle emissions, and for industrial process control. Nitric oxide detectors may also be used to detect explosive material, which is an area of increased security concerns.
U.S. Pat. No. 6,612,306 (Mault) discloses a variety of techniques for detecting nitric oxide, including the detection of fluorescence from the gas induced by radiation, the detection of resonance changes on a micromechanical structure, and the detection of chemiluminescence when ozone is introduced in the airflow.
U.S. Pat. No. 6,160,255 “LASER-BASED PHOTOACOUSTIC SENSOR AND METHOD FOR TRACE DETECTION AND DIFFERENTIATION OF ATMOSPHERIC NO AND NO2”, issued 12 Dec. 2002 to Rosario C. Sausa and incorporated by reference herein, teaches a dual-laser photoacoustic sensor that excites the air with pulsed, tunable lasers around 227 nm and 454 nm, and then detects the acoustic effects produced by the heat released from the excited nitric oxide and nitrogen dioxide. The excitation is caused by the nitric oxide absorbing the UV radiation around 227 nm, and the nitrogen dioxide absorbing the visible radiation around 454 nm.
Besides absorptions in UV, nitric oxide has absorption features in the mid-infrared spectrum. However, the cost of components in the UV and mid-infrared range are orders of magnitude more expensive than their visible-range counterparts, and thus the cost of components for photoacoustic sensing of nitric oxide does not currently provide for a low-cost nitric oxide detector. In U.S. Pat. No. 6,160,255 (Sausa), a doubling crystal and wavelength compensator are selectively enabled via an arrangement of mirrors to derive the 227 nm laser from the 454 nm laser. In converting the 454 nm radiation into 227 nm radiation less than 1% of the power remains, which results in a significant reduction in detection sensitivity in the UV. On the other hand, because components in the visible range continue to be developed for high-volume applications, such as optical storage devices (CDs, DVDs) and lighting devices, the cost of these visible-range components continues to decrease.
If a low-cost nitric oxide detector were available, each physician's office could be equipped with a diagnostic tool that will facilitate the detection and diagnosis of pulmonary and other physiological conditions, and asthmatic patients could be provided with a monitoring device for home use. A low cost NOx sensor could also be used for permanent/continuous exhaust-gas monitoring in cars and environmental-air quality monitoring. Similarly, low-cost nitric oxide detectors could be provided to security personnel at office buildings, train terminals, airports, and other potential terrorist targets.
It is an object of this invention to provide a low-cost, compact and highly sensitive detector for detection of nitrogen-containing gases. It is a further object of this invention to provide a detector that uses photoacoustic techniques.
These objects, and others, are achieved by a system that uses a semiconductor laser or light emitting diode emitting in the blue-violet-green wavelength range and a narrow bandwidth photo-acoustic sensor with a resonant pickup unit. Nitrogen dioxide is directly detected by its absorption in the blue-violet wavelength range while other nitrogen-containing compounds are chemically converted into nitrogen dioxide before photosensitive sensing of the amount of nitrogen dioxide produced. A surface chemical oxidation unit is preferably used to convert nitric oxide to nitrogen dioxide, using, for example potassium permanganate (KMnO4) filter, or a platinum (Pt) catalyst unit.
The invention is explained in further detail, and by way of example, with reference to the accompanying drawings wherein:
Throughout the drawings, the same reference numeral refers to the same element, or an element that performs substantially the same function. The drawings are included for illustrative purposes and are not intended to limit the scope of the invention.
European Patent application 05300164, Applicant's reference number FR050029, “PHOTOACOUSTIC SPECTROSCOPY DETECTOR AND SYSTEM”, filed 4 Mar. 2005 for Hans van Kesteren, discloses a technique for detecting acoustic signals generated in a photoacoustic spectroscopy system through absorption of light that includes a sensing unit that exhibits structural resonance at or near a frequency of the acoustic signals. The sensing unit forms at least part of a cavity resonator that is arranged to enable a formation of standing pressure waves inside the cavity resonator at a cavity resonance frequency substantially coinciding with a structural resonance frequency of the sensing unit. PCT patent application PCT/US03/18299, published as WO 03/104767, “QUARTZ-ENHANCED PHOTOACOUSTIC SPECTROSCOPY”, filed 10 Jun. 2003 for Anatoliy A. Kosterev, discloses the fundamental techniques for resonance-enhanced detection of photoacoustic signals.
Preferably, the sensor 10 incorporates the principles of application FR050029 by choosing the radius of the cylindrical cavity 161 between the prongs of the tuning-fork 160 to be the same as the radii of the tube-shaped signal enhancing means 182a, 182b. The acoustic resonator has a resonance frequency close to or coinciding with the resonance frequency of the tuning fork so both the structural resonance of the tuning fork and the cavity resonance help in obtaining a high photo-acoustic detection sensitivity.
The tuning-fork 160 is provided with electrodes on the various tuning-fork surfaces, using techniques commonly known to those skilled in the field of quartz tuning fork resonators, so as to provide an electric signal that corresponds to the symmetric vibration of the prongs moving in opposite directions. Wires 112 are attached to the tuning fork electrodes to provide the signal from the tuning-fork sensing element to detection electronics (not illustrated).
The tuning-fork pickup element and acoustic resonator are incorporated in a gas cell 120 with gas inlet 121 and gas outlet 122. The gas mixture flows through the gas cell 120 and sensing unit 111. Windows 130 are incorporated in the gas cell 120 to enable a laser beam 131 to pass through the acoustic resonator and between the tuning fork prongs. The laser light with a wavelength in the 370-480 nm wavelength range is provided by a small semiconductor laser in a laser module 132. The divergent light form the laser module 132 is collimated by a lens or lens system 133. To obtain a compact sensor, a GRIN (Gradient Index) lens can be used for this purpose.
During operation, the current fed to the laser by wires 113 is modulated to obtain a modulated laser beam at a frequency corresponding to the resonance frequency of the sensing unit, such as an integer multiple (1×, 2×, etc.) or sub-multiple (½×, ⅓×, etc.) of the resonance frequency. In the referenced patent application, WO 03/104767, an embodiment is described wherein the wavelength of an infrared laser is modulated at half the resonant frequency of the sensing unit, so as to avoid a direct excitation of the tuning fork by the laser beam. In a preferred embodiment of this invention, however, because low-cost blue semiconductor lasers are more easily power modulated than wavelength modulated and the absorption wavelength range of nitrogen dioxide is broader than the wavelength range available from a blue semiconductor laser, a power modulation of the laser beam, at a frequency equal to the resonant frequency is preferred. In such an embodiment, the beamwidth of the laser inside the tuning fork and acoustic resonator is sufficiently controlled, or other methods employed, to avoid direct excitation of the tuning fork. The shorter wavelength of blue radiation compared to infrared radiation as well as the availability of high-quality optical components in the visible wavelength range make it easier to obtain these small beamwidths in the blue wavelength range than in the infrared wavelength range. Laser modulation at other multiples or sub-multiples of the resonant frequency may also be used, albeit with a possible loss of efficiency.
During absorption by the nitrogen dioxide, heat is dissipated in the gas mixture and pressure waves are generated that are amplified by the acoustic resonator and picked up by the tuning fork. Amplification and phase-sensitive detection of the tuning fork response communicated by the wires 112, using techniques common in the art of photoacoustic detection, provides a result that corresponds to the nitrogen dioxide concentration.
Nitrogen dioxide has a broad absorption band in the visible-light spectrum. As such, because of the greater production quantities of semiconductor lasers and optical components that operate in the visible spectrum, the cost of providing the visible-light sensor 10 can be expected to be substantially less than the cost of an ultraviolet-light or infrared sensors as taught in for instance U.S. Pat. No. 6,160,255 (Sausa, above). Quartz tuning fork sensor elements can also be produced at low cost because this technology is similar to the technology for making tuning-fork frequency reference crystals. Semiconductor lasers and quartz tuning forks have millimeter size dimensions and low power consumption, which enables the integration of all components into a very compact and low power device, suitable for portable applications.
The converter 210 can use any of a variety of techniques that are well known in the art to convert nitrogen-containing compounds to nitrogen dioxide. Examples of nitrogen-containing compounds are nitric oxide (NO), ammonia (NH3), and amines. Nitric oxide can be converted into nitrogen dioxide by an oxidation step while ammonia can be converted by, for example, the Oswald process. In the Oswald process, NH3 is converted into NO2 by a Pt catalytic reaction and subsequent reaction with oxygen.
A number of example configurations for the detector 200 are provided in
Alternatively, as illustrated in
The scrubber 312 preferably removes the NO and NO2 from the inhaled air, while the converter 310 is preferably based on a surface chemical conversion of nitric oxide into nitrogen dioxide. The scrubber 312 and converter 310 are part of a replaceable unit 315. Because the inhaled air is free of nitric oxide, all the nitric oxide present in the exhaled gas stream is generated in the body that provides the exhaled air. Therefore, the amount of nitrogen dioxide measured in the sensor 10 directly corresponds to the amount of nitric oxide generated in the body.
A pressure sensor 311 is also provided to monitor exhalation and inhalation. During exhalation, the flow is preferably restricted by 360 to a fixed flow rate that conforms to the generally accepted measuring conditions for nitric oxide measurements in exhaled air. Electronics for signal detection, pressure monitoring, laser power control, etc, are illustrated in block 317. The results of the breath test can be presented to the physician or patient via a user interface 316.
The exhaled breath tester in
The exhaled air in
In interpreting these claims, it should be understood that:
a) the word “comprising” does not exclude the presence of other elements or acts than those listed in a given claim;
b) the word “a” or “an” preceding an element does not exclude the presence of a plurality of such elements;
c) any reference signs in the claims do not limit their scope;
d) several “means” may be represented by the same item or hardware or software implemented structure or function;
e) each of the disclosed elements may be comprised of hardware portions (e.g., including discrete and integrated electronic circuitry), software portions (e.g., computer programming), and any combination thereof;
f) hardware portions may be comprised of one or both of analog and digital portions;
g) any of the disclosed devices or portions thereof may be combined together or separated into further portions unless specifically stated otherwise;
h) no specific sequence of acts is intended to be required unless specifically indicated; and
i) the term “plurality of” an element includes two or more of the claimed element, and does not imply any particular range of number of elements; that is, a plurality of elements can be as few as two elements.
This invention relates to the field of detection of nitrogen-containing trace-gases, and in particular to a detector unit that uses a converter that converts nitrogen-containing compounds into nitrogen dioxide, and a low cost and compact nitrogen dioxide (NO2) detector comprising a blue semiconductor laser and quartz-enhanced photo-acoustic sensor.
U.S. Pat. No. 6,612,306 “RESPIRATORY NITRIC OXIDE METER”, issued 2 Sep. 2003 to James R. Mault, and incorporated by reference herein, teaches a respiratory gas meter for detecting gas components of respiratory gas flowing along a flow path. As detailed in this reference, endogenous production of nitric oxide (NO) is increased in patients with asthma and other inflammatory lung diseases, as well as in patients with reactive airways disease. Mault cites U.S. Pat. No. 5,922,610 “SYSTEM TO BE USED FOR THE DETERMINATION OF NO LEVELS IN EXHALED AIR AND DIAGNOSTIC METHODS FOR DISORDERS RELATED TO ABNORMAL NO LEVELS”, issued 13 Jul. 1999 to Alving et al., incorporated by reference herein, for teaching the use of nitric oxide measurements in the diagnosis of inflammatory conditions of the airways, such as allergic asthma and rhinitis, in respiratory tract infections in humans and Kartagener's syndrome, as well as gastric disturbances. Other uses of nitric oxide detection for medical diagnoses are also cited by Mault.
In addition to detecting nitric oxide for medical diagnoses, detectors for measuring the concentrations of various nitrogen oxides, generally referred to as NOx are used to detect environmental concentrations, including vehicle emissions, and for industrial process control. Nitric oxide detectors may also be used to detect explosive material, which is an area of increased security concerns.
U.S. Pat. No. 6,612,306 (Mault) discloses a variety of techniques for detecting nitric oxide, including the detection of fluorescence from the gas induced by radiation, the detection of resonance changes on a micromechanical structure, and the detection of chemiluminescence when ozone is introduced in the airflow.
U.S. Pat. No. 6,160,255 “LASER-BASED PHOTOACOUSTIC SENSOR AND METHOD FOR TRACE DETECTION AND DIFFERENTIATION OF ATMOSPHERIC NO AND NO2”, issued 12 Dec. 2002 to Rosario C. Sausa and incorporated by reference herein, teaches a dual-laser photoacoustic sensor that excites the air with pulsed, tunable lasers around 227 nm and 454 nm, and then detects the acoustic effects produced by the heat released from the excited nitric oxide and nitrogen dioxide. The excitation is caused by the nitric oxide absorbing the UV radiation around 227 nm, and the nitrogen dioxide absorbing the visible radiation around 454 nm.
Besides absorptions in UV, nitric oxide has absorption features in the mid-infrared spectrum. However, the cost of components in the UV and mid-infrared range are orders of magnitude more expensive than their visible-range counterparts, and thus the cost of components for photoacoustic sensing of nitric oxide does not currently provide for a low-cost nitric oxide detector. In U.S. Pat. No. 6,160,255 (Sausa), a doubling crystal and wavelength compensator are selectively enabled via an arrangement of mirrors to derive the 227 nm laser from the 454 nm laser. In converting the 454 nm radiation into 227 nm radiation less than 1% of the power remains, which results in a significant reduction in detection sensitivity in the UV. On the other hand, because components in the visible range continue to be developed for high-volume applications, such as optical storage devices (CDs, DVDs) and lighting devices, the cost of these visible-range components continues to decrease.
If a low-cost nitric oxide detector were available, each physician's office could be equipped with a diagnostic tool that will facilitate the detection and diagnosis of pulmonary and other physiological conditions, and asthmatic patients could be provided with a monitoring device for home use. A low cost NOx sensor could also be used for permanent/continuous exhaust-gas monitoring in cars and environmental-air quality monitoring. Similarly, low-cost nitric oxide detectors could be provided to security personnel at office buildings, train terminals, airports, and other potential terrorist targets.
It is an object of this invention to provide a low-cost, compact and highly sensitive detector for detection of nitrogen-containing gases. It is a further object of this invention to provide a detector that uses photoacoustic techniques.
These objects, and others, are achieved by a system that uses a semiconductor laser or light emitting diode emitting in the blue-violet-green wavelength range and a narrow bandwidth photo-acoustic sensor with a resonant pickup unit. Nitrogen dioxide is directly detected by its absorption in the blue-violet wavelength range while other nitrogen-containing compounds are chemically converted into nitrogen dioxide before photosensitive sensing of the amount of nitrogen dioxide produced. A surface chemical oxidation unit is preferably used to convert nitric oxide to nitrogen dioxide, using, for example potassium permanganate (KMnO4) filter, or a platinum (Pt) catalyst unit.
The invention is explained in further detail, and by way of example, with reference to the accompanying drawings wherein:
Throughout the drawings, the same reference numeral refers to the same element, or an element that performs substantially the same function. The drawings are included for illustrative purposes and are not intended to limit the scope of the invention.
European Patent application 05300164, Applicant's reference number FR050029, “PHOTOACOUSTIC SPECTROSCOPY DETECTOR AND SYSTEM”, filed 4 Mar. 2005 for Hans van Kesteren, discloses a technique for detecting acoustic signals generated in a photoacoustic spectroscopy system through absorption of light that includes a sensing unit that exhibits structural resonance at or near a frequency of the acoustic signals. The sensing unit forms at least part of a cavity resonator that is arranged to enable a formation of standing pressure waves inside the cavity resonator at a cavity resonance frequency substantially coinciding with a structural resonance frequency of the sensing unit. PCT patent application PCT/US03/18299, published as WO 03/104767, “QUARTZ-ENHANCED PHOTOACOUSTIC SPECTROSCOPY”, filed 10 Jun. 2003 for Anatoliy A. Kosterev, discloses the fundamental techniques for resonance-enhanced detection of photoacoustic signals.
Preferably, the sensor 10 incorporates the principles of application FR050029 by choosing the radius of the cylindrical cavity 161 between the prongs of the tuning-fork 160 to be the same as the radii of the tube-shaped signal enhancing means 182a, 182b. The acoustic resonator has a resonance frequency close to or coinciding with the resonance frequency of the tuning fork so both the structural resonance of the tuning fork and the cavity resonance help in obtaining a high photo-acoustic detection sensitivity.
The tuning-fork 160 is provided with electrodes on the various tuning-fork surfaces, using techniques commonly known to those skilled in the field of quartz tuning fork resonators, so as to provide an electric signal that corresponds to the symmetric vibration of the prongs moving in opposite directions. Wires 112 are attached to the tuning fork electrodes to provide the signal from the tuning-fork sensing element to detection electronics (not illustrated).
The tuning-fork pickup element and acoustic resonator are incorporated in a gas cell 120 with gas inlet 121 and gas outlet 122. The gas mixture flows through the gas cell 120 and sensing unit 111. Windows 130 are incorporated in the gas cell 120 to enable a laser beam 131 to pass through the acoustic resonator and between the tuning fork prongs. The laser light with a wavelength in the 370-480 nm wavelength range is provided by a small semiconductor laser in a laser module 132. The divergent light form the laser module 132 is collimated by a lens or lens system 133. To obtain a compact sensor, a GRIN (Gradient Index) lens can be used for this purpose.
During operation, the current fed to the laser by wires 113 is modulated to obtain a modulated laser beam at a frequency corresponding to the resonance frequency of the sensing unit, such as an integer multiple (1×, 2×, etc.) or sub-multiple (½×, ⅓×, etc.) of the resonance frequency. In the referenced patent application, WO 03/104767, an embodiment is described wherein the wavelength of an infrared laser is modulated at half the resonant frequency of the sensing unit, so as to avoid a direct excitation of the tuning fork by the laser beam. In a preferred embodiment of this invention, however, because low-cost blue semiconductor lasers are more easily power modulated than wavelength modulated and the absorption wavelength range of nitrogen dioxide is broader than the wavelength range available from a blue semiconductor laser, a power modulation of the laser beam, at a frequency equal to the resonant frequency is preferred. In such an embodiment, the beamwidth of the laser inside the tuning fork and acoustic resonator is sufficiently controlled, or other methods employed, to avoid direct excitation of the tuning fork. The shorter wavelength of blue radiation compared to infrared radiation as well as the availability of high-quality optical components in the visible wavelength range make it easier to obtain these small beamwidths in the blue wavelength range than in the infrared wavelength range. Laser modulation at other multiples or sub-multiples of the resonant frequency may also be used, albeit with a possible loss of efficiency.
During absorption by the nitrogen dioxide, heat is dissipated in the gas mixture and pressure waves are generated that are amplified by the acoustic resonator and picked up by the tuning fork. Amplification and phase-sensitive detection of the tuning fork response communicated by the wires 112, using techniques common in the art of photoacoustic detection, provides a result that corresponds to the nitrogen dioxide concentration.
Nitrogen dioxide has a broad absorption band in the visible-light spectrum. As such, because of the greater production quantities of semiconductor lasers and optical components that operate in the visible spectrum, the cost of providing the visible-light sensor 10 can be expected to be substantially less than the cost of an ultraviolet-light or infrared sensors as taught in for instance U.S. Pat. No. 6,160,255 (Sausa, above). Quartz tuning fork sensor elements can also be produced at low cost because this technology is similar to the technology for making tuning-fork frequency reference crystals. Semiconductor lasers and quartz tuning forks have millimeter size dimensions and low power consumption, which enables the integration of all components into a very compact and low power device, suitable for portable applications.
The converter 210 can use any of a variety of techniques that are well known in the art to convert nitrogen-containing compounds to nitrogen dioxide. Examples of nitrogen-containing compounds are nitric oxide (NO), ammonia (NH3), and amines. Nitric oxide can be converted into nitrogen dioxide by an oxidation step while ammonia can be converted by, for example, the Oswald process. In the Oswald process, NH3 is converted into NO2 by a Pt catalytic reaction and subsequent reaction with oxygen.
A number of example configurations for the detector 200 are provided in
Alternatively, as illustrated in
The scrubber 312 preferably removes the NO and NO2 from the inhaled air, while the converter 310 is preferably based on a surface chemical conversion of nitric oxide into nitrogen dioxide. The scrubber 312 and converter 310 are part of a replaceable unit 315. Because the inhaled air is free of nitric oxide, all the nitric oxide present in the exhaled gas stream is generated in the body that provides the exhaled air. Therefore, the amount of nitrogen dioxide measured in the sensor 10 directly corresponds to the amount of nitric oxide generated in the body.
A pressure sensor 311 is also provided to monitor exhalation and inhalation. During exhalation, the flow is preferably restricted by 360 to a fixed flow rate that conforms to the generally accepted measuring conditions for nitric oxide measurements in exhaled air. Electronics for signal detection, pressure monitoring, laser power control, etc, are illustrated in block 317. The results of the breath test can be presented to the physician or patient via a user interface 316.
The exhaled breath tester in
The exhaled air in
In interpreting these claims, it should be understood that:
a) the word “comprising” does not exclude the presence of other elements or acts than those listed in a given claim;
b) the word “a” or “an” preceding an element does not exclude the presence of a plurality of such elements;
c) any reference signs in the claims do not limit their scope;
d) several “means” may be represented by the same item or hardware or software implemented structure or function;
e) each of the disclosed elements may be comprised of hardware portions (e.g., including discrete and integrated electronic circuitry), software portions (e.g., computer programming), and any combination thereof;
f) hardware portions may be comprised of one or both of analog and digital portions;
g) any of the disclosed devices or portions thereof may be combined together or separated into further portions unless specifically stated otherwise;
h) no specific sequence of acts is intended to be required unless specifically indicated; and
i) the term “plurality of” an element includes two or more of the claimed element, and does not imply any particular range of number of elements; that is, a plurality of elements can be as few as two elements.
Number | Date | Country | Kind |
---|---|---|---|
05300323.2 | Apr 2005 | EP | regional |
Filing Document | Filing Date | Country | Kind | 371c Date |
---|---|---|---|---|
PCT/IB06/51288 | 4/25/2006 | WO | 00 | 10/26/2007 |