Classifications

• • G—PHYSICS
  • G01—MEASURING; TESTING
  • G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
  • G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
  • G01N21/01—Arrangements or apparatus for facilitating the optical investigation
  • G01N21/03—Cuvette constructions
  • G01N21/05—Flow-through cuvettes
• • G—PHYSICS
  • G01—MEASURING; TESTING
  • G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
  • G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
  • G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
  • G01N21/25—Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands
  • G01N21/31—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry
  • G01N21/35—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry using infrared light
  • G01N21/3504—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry using infrared light for analysing gases, e.g. multi-gas analysis
• • G—PHYSICS
  • G01—MEASURING; TESTING
  • G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
  • G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
  • G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
  • G01N21/25—Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands
  • G01N21/31—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry
  • G01N21/314—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry with comparison of measurements at specific and non-specific wavelengths
  • G01N2021/317—Special constructive features
• • G—PHYSICS
  • G01—MEASURING; TESTING
  • G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
  • G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
  • G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
  • G01N21/25—Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands
  • G01N21/31—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry
  • G01N21/35—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry using infrared light
  • G01N21/3504—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry using infrared light for analysing gases, e.g. multi-gas analysis
  • G01N2021/3513—Open path with an instrumental source
• • G—PHYSICS
  • G01—MEASURING; TESTING
  • G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
  • G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
  • G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
  • G01N21/25—Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands
  • G01N21/31—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry
  • G01N21/39—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry using tunable lasers
  • G01N2021/396—Type of laser source
  • G01N2021/399—Diode laser
• • G—PHYSICS
  • G01—MEASURING; TESTING
  • G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
  • G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
  • G01N21/01—Arrangements or apparatus for facilitating the optical investigation
  • G01N21/15—Preventing contamination of the components of the optical system or obstruction of the light path
• • G—PHYSICS
  • G01—MEASURING; TESTING
  • G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
  • G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
  • G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
  • G01N21/25—Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands
  • G01N21/27—Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands using photo-electric detection ; circuits for computing concentration
  • G01N21/274—Calibration, base line adjustment, drift correction
  • G01N21/276—Calibration, base line adjustment, drift correction with alternation of sample and standard in optical path
• • G—PHYSICS
  • G01—MEASURING; TESTING
  • G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
  • G01N2201/00—Features of devices classified in G01N21/00
  • G01N2201/02—Mechanical
  • G01N2201/024—Modular construction
  • G01N2201/0245—Modular construction with insertable-removable part
• • G—PHYSICS
  • G01—MEASURING; TESTING
  • G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
  • G01N2201/00—Features of devices classified in G01N21/00
  • G01N2201/12—Circuits of general importance; Signal processing
  • G01N2201/121—Correction signals
  • G01N2201/1211—Correction signals for temperature

Definitions

• the present invention relates generally to gas analysis, and more particularly to systems and methods for measuring concentrations of gases.
• a gas analyzer can be used to analyze the transmittance of light in appropriate wavelength bands through a gas sample.
• a sample gas containing unknown gas concentrations of carbon dioxide and water vapor is placed in a sample cell, and a reference gas with zero or known concentrations of carbon dioxide and water vapor is placed in a reference cell.
• the analyzer measures the unknown gas concentrations in the sample cell from calibrated signals that are proportional to the difference between light transmitted through the sample cell and light transmitted through the reference cell.
• Systems and methods are provided for measuring concentrations of gases and in particular dry mole fraction of components of a gas.
• the systems and method according to various embodiments allow for rapid measurement of the gas density and/or dry mole fraction of gases for a number of environmental monitoring applications, including high speed flux measurements.
• systems and methods are provided that enable rapid measurements of gas concentrations simultaneously with rapid measurements of pressure and temperature of sampled gas.
• devices according to various embodiments can advantageously use substantially shorter intake tubes as compared to previously existing devices, and substantially lower power consumption.
• Various embodiments also provide unique mechanical-optical design solutions for a gas analyzer that include several novel elements in a tool-free removable gas cell.
• Various embodiments also allow for measuring the dry mole fraction of a gas in a removable gas cell using temperature and pressure measurement in the gas stream.
• a gas analyzer typically includes a detector section including a detector, a source section including a light source, and a removable gas cell removably disposed between the source and detector sections.
• the removable gas cell typically includes a housing structure defining a gas flow channel, e.g., an enclosed gas flow channel, wherein, when attached, emitted light from the light source passes through the gas flow channel to the detector section along a light path.
• the gas cell also typically includes a gas inlet port, a gas outlet port, wherein the inlet and outlet ports are located on the housing structure, and a first temperature sensor adapted to measure a temperature of gas flowing in the flow channel, and a pressure sensor located at an interior point of the housing structure in the gas flow channel, the pressure sensor adapted to measure a pressure of the gas at an interior point in the flow cell.
• the removable gas cell further includes a second temperature sensor located proximal to the outlet port, wherein the first temperature sensor is located proximal to the input port.
• a gas analyzer typically includes a detector section including a detector, a source section including a light source, and a removable gas cell removably disposed between the source and detector sections.
• the removable gas cell typically includes a housing structure defining a gas flow channel, e.g., an enclosed gas flow channel, wherein, when attached, emitted light from the light source passes through the gas flow channel to the detector section along a light path.
• the gas cell also typically includes a gas inlet port, a gas outlet port, wherein the inlet and outlet ports are located on the housing structure, and a first temperature sensor located proximal to the inlet port, and a second temperature sensor located proximal to the outlet port.
• the gas analyzer includes a pressure sensor located at an interior point of the housing structure in the gas flow channel, the pressure sensor adapted to measure a pressure of the gas at an interior point in the flow cell.
• the gas analyzers include an intelligence module coupled with the temperature sensor(s), with the pressure sensor and with the detector.
• the intelligence module is typically adapted to determine a dry mole fraction of components of a gas within the flow channel based on a detector signal and substantially simultaneous measurements of the pressure of the gas by the pressure sensor and the temperature of the gas by the temperature sensor(s).
• the intelligence module corrects for a delay due to spatial separation in the temperature signals received from the first and second temperature sensors, wherein the delay is typically a function of a flow rate of the gas in the flow channel.
• the gas analyzers include a first optical window proximal to the detector section and a second optical window proximal to the source section, wherein the first and second optical windows provide an airtight seal for components within the source and detector sections.
• a method for measuring dry mole fraction of components of a gas in a flow cell of a gas analyzer.
• the method typically includes flowing a gas through the flow cell, measuring an absorbance of light of the components of the gas in the flow cell, substantially simultaneously measuring a temperature, Tl, of the gas at an input port of the flow cell, substantially simultaneously measuring a temperature, T2, of the gas at an output of the flow cell, and substantially simultaneously measuring a pressure, P, of the gas at an interior point of the flow cell.
• the method also typically includes determining a dry mole fraction of the components of the gas based on the measured absorbance, P, Tl and T2.
• the components of the gas include CO 2 and H 2 O, and wherein the gas is air.
• a gas analysis system that measures dry mole fraction of components of a gas.
• the system typically includes a flow cell within which a gas is flowed from an inlet port to an outlet port, a light source configured to transmit light through the flow cell, and a detector subsystem configured to output an absorbance signal representing an absorbance of light by the components of the gas in the flow cell.
• the system also typically includes a first temperature sensor positioned proximal to the input port of the flow cell, a second temperature sensor positioned proximal to the output port of the flow cell, and a pressure sensor adapted to measure pressure at an interior point of the flow cell, the system further typically includes an intelligence module coupled with the first and second temperature sensors, the pressure sensor, and with the detector subsystem.
• the intelligence module is typically adapted to determine a dry mole fraction of the components based on the absorbance signal and the substantially simultaneous measurements of the pressure of the gas and of the temperature of the gas by the first and second temperature sensors.
• the measurements of the pressure and of the temperature of the gas by the first and second temperature sensors occur within about 0.2 seconds or less of each other.
• the measurements of the pressure and of the temperature of the gas by the pressure sensor, and the first and second temperature sensors are taken at a rate of about 1.0 Hz or faster.
• a removable gas cell adapted to be disposed between light source and detector sections of a gas analyzer system.
• the removable gas cell typically includes a housing structure defining a gas flow channel, a first opening at one end of the gas flow channel, a second opening at the other end of the gas flow channel, wherein the first and second openings define a light path along which light from a light source passes through the cell to the detector section.
• the gas cell also typically includes a gas inlet port, a gas outlet port, wherein the inlet and outlet ports are located on the housing structure off of the optical axis, a first temperature sensor located proximal to the inlet port, and a second temperature sensor located proximal to the outlet port.
• the gas cell includes a pressure sensor located at an interior point of the housing structure in the gas flow channel, the pressure sensor adapted to measure a pressure of a gas at an interior point in the flow cell.
• at least one of the first and second temperature sensors includes a thermocouple positioned at a central point of a flow path defined by the respective port.
• the removable gas cell typically includes a housing structure defining a gas flow channel, a first opening at one end of the gas flow channel, a second opening at the other end of the gas flow channel, wherein the first and second openings define a light path along which light from a light source passes through the cell to the detector section.
• the gas cell also typically includes a gas inlet port, a gas outlet port, wherein the inlet and outlet ports are located on the housing structure off of the optical axis, a first temperature sensor adapted to measure a temperature of a gas flowing in the flow channel, and a pressure sensor adapted to measure a pressure of the gas at an interior point in the flow cell.
• the removable gas cells include, or can be coupled with, a gas intake tube that couples the atmosphere with the input port.
• the intake tube can advantageously have a length of less than 2.0 meters and more advantageously less than about 1.0 meters.
• FIG. 1 illustrates a gas analyzer including a removable sample flow cell according to one embodiment.
• FIG. 2 illustrates a thermocouple design used in the sample cell inlet and outlet according to one embodiment.
• FIG. 3 is a diagram of a pressure measurement scheme according to one embodiment.
• FIG. 4 illustrates thermal conductivity within a flow cell for an un-insulated (top) flow cell and an insulated (bottom) flow cell.
• FIG. 5 illustrates one embodiment including a sample cell with a cell insert removed.
• FIG. 6 illustrates a temperature and pressure measurement scheme for a gas flow cell according to one embodiment.
• the present invention provides systems and methods for measuring densities of gasses such as carbon dioxide and water vapor.
• the systems and methods are particularly useful in turbulent air structures.
• the systems and methods advantageously sample and measure gas concentration, temperature and pressure at high speed and at high bandwidth, and allow for calculation of dry mole fraction of gas components.
• the gas analyzers generally include a light source, a sample cell, and a detector.
• the sample cell is removable in certain aspects to facilitate in-field cleaning and repair.
• the gas analyzers disclosed herein can be used to measure a concentration of one or more gases that have a high absorbance at different wavelength bands.
• a gas analyzer can be used to measure a concentration of CO 2 and water vapor (H 2 O) in a sample gas, typically air.
• the gas analyzer uses non-dispersive infrared (NDIR) absorption to measure concentration of a gas in a sample cell based on the difference between absorption of infrared radiation passing through the sample cell and a reference cell, or against a calibrated reference signal.
• NDIR non-dispersive infrared
• the gas analyzers do not require long intake tubes and are capable of taking high speed measurements which enable, inter alia, calculation of dry mole fraction of gas components.
• a light source transmits light having a spectrum of wavelengths through sample and reference cells. Gases present in the sample cell absorb light at different wavelength bands. For example, CO 2 has a high absorbance at 4.255 ⁇ m, and water vapor has a high absorbance at 2.595 ⁇ m.
• Light exiting the sample cell is detected by the detector, which is sensitive to wavelength bands absorbed by the gases (e.g., CO 2 and H 2 O), or two detectors can be used, each sensitive to the wavelength band absorbed by one of the gases.
• the gases e.g., CO 2 and H 2 O
• the concentration of the gases in the sample cell can be determined by calculating the difference between absorption in the sample cell and the reference cell or a reference signal. For example, when a reference cell contains a non-absorber gas, the signal detected in the sample cell is compared to the signal detected in the reference cell to provide an absolute measurement of gas concentration in the sample cell.
• US Patents 6,317,212 and 6,369,387 which are each hereby incorporated by reference in its entirety, disclose various features of open and closed path gas analyzers, including optical filter configurations and techniques.
• a gas analyzer includes a packaging scheme that enables simple, tool-free removal of the sample flow cell to facilitate in-field cleaning of optical components such as source and detector optical windows.
• a packaging scheme also advantageously allows for maintaining a desiccant and scrub path (see e.g., US Patent 6,317,212, previously incorporated by reference) and advantageously allows for repeatable set distance between the source and detector.
• FIG. 1 illustrates a gas analyzer 10 including a removable sample flow cell 20 according to one embodiment.
• Sample cell 20 includes a housing structure having a gas inlet port 25 and a gas outlet port 30.
• a cylindrical portion 40 defines a gas flow path which has two openings at either end. The cylindrical portion may be part of the housing structure of cell 20 or it may itself be separable from the housing structure.
• gas enters input port 25 flows through the flow path defined by cylindrical portion 40 and exits outlet port 30.
• a pressure sensor 35 (external portion shown) is positioned to measure the pressure at an internal point within the flow path.
• Removable sample cell 20 is configured to couple with structure 22 of gas analyzer 10.
• Structure 22 includes a source portion 60 that houses a light or radiation source and associated electrical and optical components.
• Structure 22 also includes a detector portion 50 that houses one or more detectors and associated optical and electrical components.
• a first optical window 70 is provided in one embodiment proximal to source portion 60 as shown in FIG. 1.
• a second optical window (not shown) is provided in one embodiment proximal to detector portion 50.
• light typically IR light
• an O-ring is provided proximal the first and second optical windows to provide a more robust seal between the sample cell 20 and the housing 22 when in a coupled state.
• the gas flow path defined by cylindrical portion 40 substantially aligns with the optical path defined by the first and second optical windows. It should be appreciated that the optical path and the flow path do not need to align, and that only a portion of the gas flow path need be contiguous with the optical path. It should also be appreciated that although cylindrical portion 40 includes an open-ended flow path when decoupled from housing 22, optical windows could be coupled to or located on sample cell 20 at either end of the flow path in place of or in addition to the first and second optical windows of structure 22.
• one or more thumbscrews are provided to increase or decrease the distance of detector section 50 relative to column 23.
• a user need only activate the thumbscrews, separate detector section 50 a sufficient distance from column 23 and remove sample cell 20.
• the user would extend the detector section 50 a sufficient distance, insert cell 20 adjacent to column 23 and activate the thumbscrews to re-engage the detector section 50 with column 23 and simultaneously engage sample cell 20 between detector section 50 and source section 60.
• the optical windows and O-rings help ensure an airtight seal for the gas flow path in sample cell 20.
• FIG. 1 enables easy removal of the sample cell 20 and associated components.
• the mechanical packaging scheme enables easy, tool- free removal of the sample cell to clean the source and detector optical windows.
• This enables use of the gas analyzer (e.g., an IR gas analyzer or IRGA) without need to filter the air sample for dust (which lowers the power requirements for air flow).
• the detector enclosure 50 is extended away from the rest of the assembly as shown in FIG. 1.
• Air-tight paths are provided from the detector enclosure 50, through circulation column portion 23, to the source enclosure 60 to run CO 2 and H 2 O free air as well as necessary electrical components. It should be appreciated that the gas analyzer could be configured such that attachment mechanisms enable the source section 60 to extend away from column 23 in addition to or in lieu of detector section 50 extending away from column 23.
• the temperature of the sample gas is important for various measurements, such as for calculating the mole fraction from the number density.
• the temperature is measured at the inlet port 25 and at the outlet port 30 of the sample cell 20 in a manner that does not block any of the optical signal (e.g., IRGA signal) in the flow path.
• the volume average temperature in the cell can be calculated from a relationship between the inlet and outlet temperatures along with the flow rate of the sample gas.
• a generic function is T 1 RGA T OM «, Tbiock, U), where U is the mean velocity through the cell,
• additional temperature sensors may be used, e.g., to measure the block temperature of cylinder 40, and/or to measure the gas temperature at different points in the flow path.
• the inlet and outlet temperatures are measured using a disposable thermocouple (e.g., type-E thermocouple).
• a thermocouple is strung taught across a printed circuit board with a hole through for the sample gas to flow.
• FIG. 2 illustrates a thermocouple design used in the sample cell inlet and outlet ports according to one embodiment.
• a printed circuit board 80 includes an aperture across which is strung a thermocouple bead 85.
• the printed circuit board is included in structure 20 or mounted on structure 20 such that the aperture is contiguous with the gas flow path of the entry/exit port 25/30.
• An O-ring 90 provides an air tight gas path.
• thermocouples to be easily replaced as well as making sure the temperature measurement is in the center axis of the gas flow.
• a .002" thermocouple advantageously provides a frequency response to a 15 liter/minute (LPM) flow that is substantially the same as the signal attenuation due to the volume averaging within the IRGA.
• the measurements are synchronized with each other to account for slight timing variations and frequency variations.
• the measurements of gas concentration e.g., CO 2 and H 2 O
• temperature and pressure are advantageously taken within about 0.2 seconds, and more advantageously within about 0.1 seconds of each other in certain embodiments, this enable a calculation of dry mole fraction as will be described more below.
• gases concentration e.g., CO 2 and H 2 O
• temperature and pressure are advantageously taken within about 0.2 seconds, and more advantageously within about 0.1 seconds of each other in certain embodiments, this enable a calculation of dry mole fraction as will be described more below.
• These signals may be aligned in real time to account for time variations/delays as will be discussed more below.
• a single temperature sensor is used.
• a single temperature sensor may be located proximal to the inlet port, proximal to the outlet port, or proximal to an internal portion of the flow cell. Temperature measurements can be taken and a volume temperature can be calculated using the single temperature sensor signal and known parameters, such as flow rate, flow cell volume, etc.
• two (or more) temperature sensors as described above will provide a more robust and accurate temperature for the gas in the flow cell.
• FIG. 3 is a diagram of a pressure measurement scheme according to one embodiment.
• the pressure sensor e.g., sensor 35 includes a differential pressure sensor
• a coupled set of absolute/differential pressure transducers are used to obtain high frequency pressure data from the sample cell (since pressure sensor that measures absolute sensor may be quite bulky).
• the pressure of the gas at the interior of the flow cell can be determined by adding the differential pressure and the mean pressure.
• the pressure sensor is a high speed pressure sensor.
• Useful pressure sensors include a piezoresistive silicon differential pressure transducer (e.g., MPX2010DP, Freescale Semiconductor Inc. (Motorola)) and a piezoresistive silicon absolute pressure transducer (MPX4115 A, Freescale Semiconductor Inc. (Motorola)). Other pressure sensors as would be apparent to one skilled in the art may be used.
• the sample flow cell includes an insulating sleeve made out of a low thermal conductivity material and/or pockets of air or vacuum.
• Useful materials include low-CO 2 absorption plastics (e.g., Teflon PTFE (polytetrafluoroethylene) which can be very useful because all plastics absorb some CO 2 and water vapor, but Teflon is exceptionally low in absorption) and other suitable materials.
• a double-wall vacuum metal sleeve or other designs may be used. Such sleeves advantageously minimizes the temperature change between the inlet and outlet thermocouples (to maximize accuracy) by decoupling the air flow from the heat dissipation of the gas analyzer, e.g., heat dissipation due to electronics of gas analyzer. In general, the bigger the temperature change, the more the characterization between the volume average temperature as a function of the two measured temperatures is relied on.
• FIG. 4 illustrates an example of the thermal conductivity within a flow cell for an un-insulated (top) flow cell and an insulated (bottom) flow cell.
• the top image is a typical metal sample cell, while the lower image shows an insulated cell where the only heat flux comes from the windows on either end.
• the heat flux is greatly reduced and the error in temperature measurement is also greatly reduced, hi both cases, the error is calculated by the actual temperature minus an un-weighted average of the inlet and outlet temperatures.
• FIG. 5 illustrates one embodiment including a sample cell with a cell insert 95 (defining the gas flow path) removed. As can be seen, a position and sealing scheme for the thermocouple boards 80 proximal to both the inlet and outlet ports is also shown.
• the inlet temperature is measured at point 'A'
• the pressure is measured at point 'B'
• the outlet temperature is measured at point 1 C
• the gas concentrations are a volume- averaged measurement contained within the dotted outline.
• signal alignment occurs in real time as signals are received (e.g., by an intelligence module adapted to process such signals). It should be appreciated, however, that signal processing may be performed later.
• the signals, or data representing the signals may be stored and provided to an intelligence module for processing at a later time, after measurements have been taken.
• the dry mole fraction is determined using a gas analyzer according to the various embodiments disclosed herein.
• gas analyzers as disclosed herein are capable of making dry mole fraction measurements at high bandwidth. For example, it is desirable to determine a dry mole fraction of CO 2 or other gas component at a certain frequency response, e.g., 10 Hz.
• a flow rate is introduced through the IRGA that purges the volume, for example, at about a 10 Hz or greater purge rate. For example, a flow of ambient air into the inlet port, through the flow cell and out the outlet port is initiated at the desired flow rate.
• the temperature is then measured at points A and C with a frequency response similar to the volume-average (e.g., type 1 E 1 thermocouples of .002" diameter provides a similar response to a flow rate of 15 liters-per-minute (LPM) through the IRGA).
• the pressure e.g., differential pressure
• the temperature measurements are taken substantially simultaneously with each other and with the pressure measurement.
• the temperatures at A and C are corrected for spatial separation (e.g., T A (t+delay) and Tc(t-delay) where the delay is a function of the flow rate and flow path/IRGA geometry).
• the detector system is determining concentration of gas components (e.g., carbon dioxide and water vapor).
• concentration of gas components e.g., carbon dioxide and water vapor.
• the bandwidth of all the signals e.g., temperature, pressure, absorbance
• Appendix A illustrates exemplary calculations for determining the dry mole fraction. Once determined, the dry mole fraction may be returned, e.g., displayed or stored for later use.
• the term "mole fraction” when referring to a mole fraction (e.g., CO 2 mole fraction) that includes water vapor, the term “mole fraction” is typically used; when referring to a mole fraction after water vapor is removed, the term “dry mole fraction” is typically used, and in certain instances the term “instantaneous mole fraction” or “instantaneous dry mole fraction,” may be used to refer to high speed measurements.
• the gas analysis processes including the mole fraction determination processes, may be implemented in computer code running on a processor of a computer system. The code includes instructions for controlling a processor to implement various aspects and steps of the gas analysis processes.
• the code is typically stored on a hard disk, RAM or portable medium such as a CD, DVD, etc.
• the processes may be implemented in a gas analyzer including an intelligence module, typically having one or more processors executing instructions stored in a memory unit coupled to the processor(s).
• the intelligence module may be part of the gas analyzer, or part of a separate system directly or indirectly coupled with the gas analyzer. Code including such instructions may be downloaded to the gas analyzer memory unit over a network connection or direct connection to a code source or using a portable medium as is well known.

Landscapes

• Physics & Mathematics (AREA)
• General Health & Medical Sciences (AREA)
• Life Sciences & Earth Sciences (AREA)
• Chemical & Material Sciences (AREA)
• Analytical Chemistry (AREA)
• Biochemistry (AREA)
• Health & Medical Sciences (AREA)
• General Physics & Mathematics (AREA)
• Immunology (AREA)
• Pathology (AREA)
• Spectroscopy & Molecular Physics (AREA)
• Investigating Or Analysing Materials By Optical Means (AREA)
• Optical Measuring Cells (AREA)

Priority Applications (6)

Applications Claiming Priority (1)

Publications (1)

Family

ID=42153123

Family Applications (1)

Country Status (6)

Cited By (2)

Families Citing this family (6)

Citations (5)

Family Cites Families (8)

• 2008
  • 2008-11-06 CN CN2008801326519A patent/CN102272577A/zh active Pending
  • 2008-11-06 AU AU2008363810A patent/AU2008363810A1/en not_active Abandoned
  • 2008-11-06 WO PCT/US2008/082671 patent/WO2010053486A1/en active Application Filing
  • 2008-11-06 CA CA2742728A patent/CA2742728C/en active Active
  • 2008-11-06 JP JP2011535547A patent/JP2012507734A/ja active Pending
  • 2008-11-06 EP EP08878042A patent/EP2352987A4/en not_active Withdrawn

Patent Citations (5)

Non-Patent Citations (1)

Also Published As

Similar Documents

Legal Events