In-situ sensing of tropospheric water vapor using an airborne near-IR diode laser hygrometer

1998 ◽  
Vol 67 (3) ◽  
pp. 275-282 ◽  
Author(s):  
D.M. Sonnenfroh ◽  
W.J. Kessler ◽  
J.C. Magill ◽  
B.L. Upschulte ◽  
M.G. Allen ◽  
...  
2020 ◽  
pp. 103114
Author(s):  
Shruti Ghanekar ◽  
Rajavasanth Rajasegar ◽  
Nicholas Traina ◽  
Constandinos Mitsingas ◽  
Richard M. Kesler ◽  
...  

2007 ◽  
Vol 31 (1) ◽  
pp. 799-806 ◽  
Author(s):  
Andrew R. Awtry ◽  
Brian T. Fisher ◽  
Robert A. Moffatt ◽  
Volker Ebert ◽  
James W. Fleming

1999 ◽  
Author(s):  
William J. Kessler ◽  
Mark G. Allen ◽  
Steven J. Davis ◽  
Phillip A. Mulhall ◽  
Jan A. Polex

2005 ◽  
Vol 44 (1) ◽  
pp. 91 ◽  
Author(s):  
Wolfgang Gurlit ◽  
Rainer Zimmermann ◽  
Carsten Giesemann ◽  
Thomas Fernholz ◽  
Volker Ebert ◽  
...  

2008 ◽  
Vol 25 (10) ◽  
pp. 1733-1743 ◽  
Author(s):  
J. M. Livingston ◽  
B. Schmid ◽  
P. B. Russell ◽  
J. R. Podolske ◽  
J. Redemann ◽  
...  

Abstract In January–February 2003, the 14-channel NASA Ames airborne tracking sun photometer (AATS) and the NASA Langley/Ames diode laser hygrometer (DLH) were flown on the NASA DC-8 aircraft. The AATS measured column water vapor on the aircraft-to-sun path, while the DLH measured local water vapor in the free stream between the aircraft fuselage and an outboard engine cowling. The AATS and DLH measurements have been compared for two DC-8 vertical profiles by differentiating the AATS column measurement and/or integrating the DLH local measurement over the altitude range of each profile (7.7–10 km and 1.1–12.5 km). These comparisons extend, for the first time, tests of AATS water vapor retrievals to altitudes >∼6 km and column contents <0.1 g cm−2. To the authors’ knowledge, this is the first time suborbital spectroscopic water vapor measurements using the 940-nm band have been tested in conditions so high and dry. Values of layer water vapor (LWV) calculated from the AATS and DLH measurements are highly correlated for each profile. The composite dataset yields r 2 0.998, rms difference 7.7%, and bias (AATS minus DLH) 1.0%. For water vapor densities AATS and DLH had r 2 0.968, rms difference 27.6%, and bias (AATS minus DLH) −4.2%. These results for water vapor density compare favorably with previous comparisons of AATS water vapor to in situ results for altitudes <∼6 km, columns ∼0.1 to 5 g cm−2, and densities ∼0.1 to 17 g m−3.


Author(s):  
Ritobrata Sur ◽  
Thomas J. Boucher ◽  
Michael W. Renfro ◽  
Baki M. Cetegen

A robust, accurate and fast in-situ sensor was developed for detection of water vapor partial pressure and temperature simultaneously at the anode and cathode channels of a PEM fuel cell. Tunable diode laser absorption spectroscopy (TDLAS) utilizing wavelength modulation (WMS) was employed for these measurements. This method determines the ratio of the second and first harmonics (2f/1f) of the spectroscopic absorption profile of water vapor by the aid of a software lock-in amplifier. Measurements were taken using a diode laser emitting around a wavelength of 1471 nm where the water vapor absorption exhibits significant sensitivity to partial pressure and temperature. Measurements of water vapor concentration and temperature in were taken at steady and dynamic operating conditions in the anode and cathode gas channels near the inlet and outlet ports of a serpentine channel PEM fuel cell with Nafion membrane of active area 50 cm2. Different load and inlet humidity conditions were tested to characterize the operation at different conditions. The partial pressure of water vapor increases towards the exit of both the gas channels, but the increase is found to be more significant on the cathode side. The dynamic operation of the fuel cell was also examined in this study as well as the simultaneous measurements at the anode and cathode gas channels.


Sign in / Sign up

Export Citation Format

Share Document