The present invention relates to a nitrogen dioxide sensor.
Nitrogen dioxide is a reddish brown gas at room temperatures that has a pungent acrid odor. Nitrogen dioxide is naturally occurring in the environment, such as from the stratosphere, bacterial respiration, where it absorbs sunlight and regulates the chemistry of the troposphere. While nitrogen dioxide is naturally occurring, it is also a byproduct of chemical processes, such as an internal combustion engine burning fossil fuels and other industrial processes. Prolonged exposure to nitrogen dioxide increases a risk of occupational lung diseases and high exposure to nitrogen dioxide can cause death. In general, it is desirable to have a sensor to detect nitrogen dioxide in different environments and provide an alarm condition when the level of nitrogen dioxide exceeds a threshold level.
To provide for environmental science and air quality control the nitrogen dioxide sensor should detect trace gases in the parts-per-million (ppm) and/or parts-per-billion (ppb or 109) and/or parts-per-trillion (ppt or 1012) levels. The nitrogen dioxide sensors may be based upon chemical conversion technology. The chemical conversion based sensor technology consumes the target gas species to generate a measurable signal, which inherently, distorts the desired measurement through the consumption of the gas. Further, the consumption of the NO2 gas results in an accumulation of waste products that degrade the performance of the chemical conversion based sensor over time. Further, solvents used in chemical conversion based sensors tend to evaporate. The evaporation of reaction solvents eventually degrades the accuracy performance of the reported gas concentration.
Other nitrogen dioxide sensors may include laser-based techniques because of their ability to provide real-time monitoring capabilities with a high degree of sensitivity and selectivity. A NO2 sensor capable of high sensitivity and selectivity can monitor atmospheric air quality as well as real-time study of the complex photochemical reactions that the NO2 gases undergo in the atmosphere. Different spectroscopic techniques have been developed for trace gas detection. Spectroscopic techniques that are commonly employed include, absorption spectroscopy using long pass absorption cells such as multipass and Herriott cells, optical cavity methods, photo-acoustic and quartz-enhanced photo-acoustic spectroscopy, and Faraday rotation spectroscopy. Different data processing and analysis procedures have been applied such as frequency modulated spectroscopy techniques to improve the signal to noise ratio and multiple line integrated absorption spectroscopy to improve the sensitivity of detection. Unfortunately, such sensors do not tend to be robust and are complex.
It is desirable to have an optical based sensor that is robust.
The foregoing and other objectives, features, and advantages of the invention will be more readily understood upon consideration of the following detailed description of the invention, taken in conjunction with the accompanying drawings.
NO2 has an absorption spectra in the ultraviolet and in the visible regions covering approximately 250-800 nm. The absorption spectra in this region are relatively high with a broad peak in the 350-450 nm range and a large number of intense sub-peaks extending over the 350-450 nm region. This region of the absorption spectra contains a strong, dense spectrum that is well suited for use in the trace detection of NO2 using an optical technique. High power diode lasers are currently available at 405±10 nm which covers a portion of this absorption spectra.
While trying to detect NO2 there can be other atmospheric elements and trace gasses that may impact the ability to differentiate the NO2. For example, some elements that have a potential for interference include H2O, O3, SO2, and NO3. While the absorption spectrum of each of these elements is relatively broad, the absorption near the range of 405 nm is minimal. Accordingly, using a wavelength in the 405 nm range, such as generally 405±10 nm reduces the interference posed by other types of likely elements. The NO2 concentrations are typically between 1 part per million to 10 parts per million.
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In a preferred embodiment, the photo inversion diode included with the laser diode assembly typically includes a relatively small volume of gas operatively located between the output of the laser diode and the photo inversion diode. Preferably, this relatively small volume of gas is the same gas that is included within the enclosure which the laser diode assembly provides an optical output into. Accordingly, the laser diode assembly is preferably supported by the enclosure in such a manner that the gas within the enclosure is capable of also flowing to provide the relatively small volume of gas operatively located between the output of the laser diode and the photo inversion diode. Furthermore, having the same gas that is sensed within the enclosure to be the same as the gas operatively located between the output of the laser diode and the photo inversion diode, the temperature variations within the enclosure, and thus the temperature variations of the gas, will be the same (or substantially the same). In this manner, the feedback of the photo inversion diode will be affected in a similar manner to that of the photo-detector sensor.
In a preferred embodiment, the volume of the gas within the enclosure that is operatively located between the laser diode assembly and the photo-detector sensor is preferably greater than 50 times the relatively small volume of gas operatively located between the output of the laser diode and the photo inversion diode, and more preferably greater than 100 times the relatively small volume of gas operatively located between the output of the laser diode and the photo inversion diode. In this manner, the distortion that is a result of the relatively small volume of gas operatively located between the output of the laser diode and the photo inversion diode will be substantially smaller than the distortion that is a result of the gas within the enclosure that is operatively located between the laser diode assembly and the photo-detector sensor.
In a preferred embodiment, the class of material used in the photo inversion diode is the same class (or substantially the same class) of material used in the photo-detector sensor. For example, the material of the photo-inversion diode may be silicon, germanium, indium gallium arsenide, lead sulfide, and mercury cadmium telluride. Further, the material may be doped with different compounds. Further the material may be doped with different doping concentrations. In this manner, the photo inversion diode and the photo-detector sensor will respond in a substantially similar manner to temperature variations. With the gas of the photo-inversion detector and the photo-detector sensor being the same, the thermal environment of each of the detectors are the same, and likewise the thermal characteristics of the sensors substantially track one another.
In a preferred embodiment, the electrical bias (typically voltage) applied to the photo inversion diode and the photo detector sensor are substantially the same (e.g., reverse bias on a PIN diode). In this manner, the bias condition of each of the photo inversion diode and the photo detector sensor are the same, and thus provide substantially similar responses.
In other embodiments, depending on the nature of the sensor and the nature of the gas being sensed, a different wavelength or range of wavelengths of light may be used.
In other embodiments, depending on the nature of the gas desired to be sensed, the laser diode assembly may be modified to a different wavelength or range of wavelengths of light.
In other embodiments, depending on the desirable size of the housing the path of light may be generally direct from one side of the housing to the other.
In other embodiments, depending on the desirable size of the housing the path of light may be reflected, or otherwise directed in different directions with one or more lenses, to increase the path length before the light is sensed.
In other embodiments, the desirable size of the sensor may be modified, such as 1 square inch or more, 2 square inches or more, 12 square inches or more, etc.
In other embodiments, the sensor may be manufactured using other processes to provide a different range of sensitivities to light.
All the references cited herein are incorporated by reference.
The terms and expressions which have been employed in the foregoing specification are used therein as terms of description and not of limitation, and there is no intention, in the use of such terms and expressions, of excluding equivalents of the features shown and described or portions thereof, it being recognized that the scope of the invention is defined and limited only by the claims which follow.
This application claims the benefit of U.S. Provisional Patent Application No. 62/440,577, filed Dec. 30, 2016.
Number | Date | Country | |
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62440577 | Dec 2016 | US |