C15.
MEASUREMENTS OF TRACE WATER VAPOR IN A CARBON DIOXIDE REMOVAL ASSEMBLY PRODUCT STREAM USING A TUNABLE DIODE LASER SPECTROMETER
J. Wormhoudt, J. H. Shorter, J. B. McManus, D. D. Nelson and M. S. Zahniser
Aerodyne Research, Inc. 45 Manning Road
Billerica, MA 01821-3976
A tunable diode laser spectrometer configured for the measurement of trace concentrations of water vapor was used in diagnostic tests of a Space Station Carbon Dioxide Removal Assembly (CDRA) in a simulation facility at the NASA Marshall Space Flight Center. A primary issue in further CDRA development, involving addition of a compression stage to its exhaust, is the possibility that condensation of liquid water may damage the compressor. In five days of round-the-clock data acquisition, the water content of the exhaust was characterized, and enough evidence was accumulated that the source of high water concentrations was found.
A key feature of the apparatus was a sampling system that allowed response times short compared to the time scales of changing water vapor concentrations. One important component of this system was a small-volume (0.3 liters), long-path (36 m) multipass absorption cell, of the astigmatic Herriott cell design developed at Aerodyne. Other important components included a valving system that allowed automated switching between sample and reference flows and allowed sample gas to flow through the sampling line at all times, and a cell pressure regulator that minimized the effect of this switching on the absorption spectrum. The spectrometer used a lead-salt laser to measure absorption at one of the strongest of all water lines, at 1616.712 cm-1. Aerodyne’s TDLWintel laser control, data acquisition and analysis software wrote a continuous record of concentrations, saved files of spectra and instrument parameters such as multipass cell pressures, and kept the laser locked to a low pressure water absorption line in a reference cell.
The tunable diode laser spectrometer met or exceeded all the specifications for the test, including sensitivity, time response, and time of operation. Detection levels of well under the specified 50 ppbv were achieved, while the high water levels of greatest interest turned out to be about 400 ppmv. Its good sensitivity, good time resolution, high dynamic range (measured concentrations varied over four orders of magnitude), its first-principles calibration, its excellent stability, and its ability to display and analyze data in real time, were all critical to the success of the test.
C16.
UF6 Enrichment Measurements Using TDLS Techniques
A. Nadezhdinskii and Ya. Ponurovskii
NSC of A.M.Prokhorov General Physics Institute
Vavilov str. 38, 119991 Moscow, Russia
Yu. Selivanov
P.N. Lebedev Physical Institute
Leninski 53, 119991 Moscow, Russia
G. Grigorev, Sh. Nabiev, and N. Gorshunov
Institute of Molecular Physics of RRC "Kurchatov Institute"
Kurchatov sqv.1, 123182 Moscow, Russia
G. Bosler, R. Olsen, and V. Ryjikov
International Atomic Energy Agency
Wagramer Str. 5, P.O. Box 100, A-1400 Vienna, Austria
The first use of Tunable Diode Laser Spectroscopy (TDLS) in a number of countries was related to examining one molecule. This was the uranium hexafluoride molecule (UF6) as used with laser uranium isotopic enrichment experiments. The dramatic progress in TDLS techniques achieved during last decades and the success of detection of trace complex molecules having unresolved spectra brought our attention to examining the UF6 molecule in addressing IAEA safeguards requirements. The goal of present work has been to develop an instrument and associated algorithms for relatively quick field measurements of UF6 isotope enrichment with high accuracy (better than 0.6%).
Spectra of UF6 gas mixtures have been investigated using Fourier Transform Spectrometers Vector 22 and Bruker 66v. The observed spectral features were identified, and model spectra of different gas mixture components have been developed. An optimal spectral range for measurements is determined near the maximum UF6 combination band v1+v3. UF6 is an example of a molecule with a broadband absorption structure with many unresolved spectral lines. The absorption spectrum of the gas sample under investigation is the sum of two main molecular isotopic spectra (238UF6 and 235UF6). At the present stage of TDLS development, the technique is able to distinguish these spectra and to determine the enrichment of a gas sample under investigation.
A laboratory multi-channel prototype instrument using a tunable diode laser has been built, and algorithms of its operation have been developed to measure the isotopic ratios of gaseous UF6. The diode laser operates at a wavelength of 7.68 m and is cooled by liquid nitrogen. Three instrument channels are used for laser frequency calibration and spectra recording.
The instrument has been successfully tested using a UF6 gas mixture. The observed accuracy has been analyzed, and error sources have been identified. A random measurement error of isotope 235U is characterized by a root-mean-square spread of about 0.27% for short measurement times and 1% for long measurment times of more than an hour. Overcoming present known experimental problems should improve the error by at least an order of magnitude. Finally the prototype instrument has been tested at the IAEA UF6 test loop located in Seibersdorf, Austria.
C17.
MEASURING AIR CONTENT INSIDE INSULATING GLASS WINDOWS
A.I. Nadezhdinskii, Ya. Ya. Ponurovskii, M.V. Spiridonov
Natural Sciences Center of A.M.Prokhorov General Physics Institute
of the Russian Academy of Sciences. 38 Vavilov street, Moscow 11991, Russia
Filling the space between insulating glass (IG) windows by noble gas (Ar, Kr, Xe) allows to reduce heat conductance of windows. The technique in commercial window manufacturing is to inject argon between layers of IG. The standard argon content after refilling is about 90%. Insufficient argon concentrations result in lower energy efficiency, and increased heating and cooling costs; and wasted money replacing windows that don’t need it. However, there is no method to quickly and accurately measure the amount of argon between the window panes when they are manufactured or determine if argon has depleted in windows that are already installed in buildings. Existing methods of measuring argon content in windows are not sufficiently precise, reliable, or timely. Costly and time consuming laboratory techniques are required to make an accurate measurement.
Argon content cannot be measured directly by diode laser spectroscopy technique, but, when windows are injected with argon, the space between contains a mixture of argon and air, and air contains about 20% oxygen. This means that if one can measure level of oxygen inside IG, then the argon level can be easily calculated.
A portable device to measure oxygen concentration between IG was constructed. This device is based on commercial 760 nm Fabri-Perot diode laser. A detection limit of oxygen is about 0.1% at the optical pathlength 3 cm, and this makes it possible to measure argon content between IG with accuracy better than 0.5%.
The device is compact, battery powered and can be used for field measurements.
Poster Session D.
D1. High-Sensitivity Measurements of Hydrocarbon
Species Using Interband Cascade Lasers
Operating Near 3.3 Microns
Mark G. Allen, David M. Sonnenfroh, and Seonkyung Lee
D2. HIGH SENSITIVE 1.31 um DIODE LASER HYDROGEN
FLUORIDE SENSOR WITH DETECTION LIMIT 1 ppb
A.G.Berezin, O.V.Ershov, A.I.Nadezhdinskii, Ya.Ya.Ponurovskii
D3. RAPID PASSAGE AND POWER SATURATION EFFECTS
IN PULSED QUANTUM CASCADE LASER SPECTROMETERS
M.T. McCulloch, G. Duxbury and N.Langford
D4. Process Gas Analysis by Infrared Spectroscopy
in the Semiconductor Industry
L. Emmenegger, J. Mohn
D5. MEASUREMENTS OF RELATIVE INTENSITY NOISE OF
QUANTUM CASCADE LASERS
T. Gensty, W. Elsäßer
D6. Diode laser two-line atomic fluorescence
thermometry in flames
J. Hult, I. Burns and C.F. Kaminski
D7. A dual-wavelength diode laser spectrometer
for water isotope ratio analysis
L. Gianfrani, G. Gagliardi, M. van Burgel, and E. R. Th. Kerstel
D8. RAPID ABSORPTION SPECTROSCOPY FOR IN-SITU OXYGEN
MEASUREMENTS IN HOSTILE ENVIRONMENTS (MULTI-PHASE
AND FLAMES) USING A 761 NM VERTICAL-CAVITY
SURFACE-EMITTING LASER (VCSEL)
Maximilian Lackner, Gerhard Totschnig, Franz Winter
D9. DIODE LASER SPECTROSCOPY OF AMMONIA AND
ETHYLENE OVERTONES
A. Lucchesini, S. Gozzini
D10. An Axial Molecular Beam Mid-Infrared
Tunable Diode Laser Spectrometer
H. D. Osthoff, J. Walls, W. A. van Wijngaarden, and W. Jäger
D11. NEAR-INFRARED DIODE LASER SPECTROSCOPY OF CO2
AND ATMOSPHERIC APPLICATIONS
B. Parvitte, V. Zeninari, L. Joly, I. Pouchet, and G. Durry
D12. CO2 DECOMPOSITION IN A NON-SELF-SUSTAINED
DISCHARGE WITH A CONTROLLED ELECTRONIC
COMPONENT OF PLASMA.
S.N. Andreev, V.V. Zakharov, V.N. Ochkin, S.Yu.Savinov
D13. High resolution tunable diode laser spectrum
of OH group second overtone in ethanol
S.Shaji, Shibu M Eapen, T.M.A.Rasheed and K.P.R.Nair
D14. OPTIMAL PARAMETER FIT FOR BORN-OPPENHEIMER
BREAKDOWN OF CaH IN X2+ STATE
Hiromichi Uehara
D15. A mid-infrared laser spectrometer for the in-situ
measurement of stratospheric nitrous oxide
F. D'Amato, M. De Rosa, P. Mazzinghi, M. Pantani, P. Poggi,
P. W. Werle, F. Castagnoli
D16. NEW IMPROVEMENTS IN PHOTOACOUSTIC
DETECTION OF METHANE
V. Zeninari, B. Parvitte, D. Courtois, V. A. Kapitanov,
and Yu. N. Ponomarev
D17. STAND-OFF ETHANOL SENSOR
A.G.Berezin, O.V.Ershov, A.I.Nadezhdinskii,
Y.P.Shapovalov, D.B.Stavrovskii.
D18. Analysis of Tunable Diode Laser Spectra of RQ(J,0)
lines in CH3F near 1475 cm-1 Using a Multi-spectrum
Fitting Technique
Muriel Lepere, R. Gobeille, N. Kolodziejski, V. malathy Devi,
D. Chris Benner, M. A. H. Smith, W. McMichael, B. Aoaeh,
K. Wilkinson and A. W. Mantz
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