Infrared Absorption Coefficients for Certain Pollutant Gases

1972 ◽  
Vol 26 (3) ◽  
pp. 372-378 ◽  
Author(s):  
P. Campani ◽  
C. S. Fang ◽  
H. W. Prengle

Quantitative analysis of gas mixtures by infrared spectroscopy requires a knowledge of the absorption coefficients,: kν−, as a function of optical path length and temperature. For the majority of pollutant gases, information is scarce or incomplete. The objective of this work was to determine absorption coefficients for CH4, C2H4, CO2, CO, SO2, NO2, NO, and H2S. Measurements were made at room temperature and elevated temperatures for certain wave lengths, and kν− was determined over a very wide range of optical path length, x. The validity of the Bouguer-Beer law was confirmed for a limiting range of x, and for larger values of x, kν− decreased and was correlated as a function of x and T.

2014 ◽  
Vol 69 (8) ◽  
Author(s):  
Tay Ching En Marcus ◽  
Michael David ◽  
Maslina Yaacob ◽  
Mohd Rashidi Salim ◽  
Mohd Haniff Ibrahim ◽  
...  

Ultraviolet absorption spectroscopy is reliable for ozone concentration measurement. Concentration range and optical path length are inversely related based on theoretical calculation and observation of previous work. However, gas cells for ozone application are typically not expandable. In addition, they incur cost for custom fabrication. Here we design a reconfigurable brass gas cell that may interchange optical path length between 5.6 cm and 10.8 cm. Components are available at low cost, easy to joint and ready to use. Theoretical background and gas cell structure are discussed. Practical transmittance values between e-0.65 and e-0.05 are proposed for theoretical calculation of concentration via Beer-Lambert law. The concentration values are used in SpectralCalc.com gas cell simulation to obtain transmittance. Both approaches yield comparable result. Simulation result shows concentration range of 5.6 cm optical path length gas cell (31.82 ppm to 413.67 ppm) is wider than concentration range of 10.8 cm optical path length gas cell (16.50 ppm to 214.49 ppm). Simulation condition is at transmittance from 0.5291 to 0.9522, sampling wavelength 253.65 nm, temperature 300 K and pressure 1 atm. Thus, we strongly recommend short optical path length gas cell (5.6 cm) for wide range of concentration measurement (31.82 ppm to 413.67 ppm).


1990 ◽  
Vol 12 (2) ◽  
pp. 140-144 ◽  
Author(s):  
J.S. Wyatt ◽  
M. Cope ◽  
D.T. Delpy ◽  
P. van der Zee ◽  
S. Arridge ◽  
...  

1984 ◽  
Vol 38 (1) ◽  
pp. 35-38 ◽  
Author(s):  
R. A. Briesmeister ◽  
G. W. Read ◽  
K. C. Kim ◽  
J. R. Fitzpatrick

A unique long-path absorption cell has been developed for spectroscopic studies of alpha radioactive compounds. The cell is temperature programmable from room temperature down to 100 K and has an optical path length up to 0.5 km. Special design features and performance characteristics are described.


2016 ◽  
Vol 23 (2) ◽  
pp. 316-322 ◽  
Author(s):  
Kotaro Nakamura ◽  
Kazuki Kurihara ◽  
Hiroshi Kawaguchi ◽  
Takayuki Obata ◽  
Hiroshi Ito ◽  
...  

1997 ◽  
Vol 352 (1354) ◽  
pp. 649-659 ◽  
Author(s):  
D. T. Delpy ◽  
M. Cope

In near–infrared spectroscopy (NIRS) of tissue, light attenuation is due to: (i) absorption from chromophores of fixed concentration, (ii) absorption from chromophores of variable concentration, and (iii) light scatter. NIRS is usually concerned with trying to quantify the concentrations of chromophores in category (ii), in particular oxy– and deoxyhaemoglobin (HbO 2 and Hb) and cytochrome oxidase. In the absence of scatter the total light absorption in the medium is a linear sum of that due to each chromophore. In a scattering medium like tissue, this linear summation is distorted because the optical path length at each wavelength may differ. This distorted spectrum is then superimposed upon a further wavelength–dependent attenuation arising from light loss due to scatter, which is a complex function of the tissue absorption and scattering coefficients ( μ a and μ s ), scattering phase function, and tissue and measurement geometry. Consequently, quantification of NIRS data is difficult. Over the past 20 years many differing approaches to quantification have been tried. The development of methods for measuring optical path length in tissue initially enabled changes in concentration to be quantified, and subsequently methods for absolute quantification of HbO 2 and Hb were developed by correlating NIRS changes with an independent measurement of arterial haemoglobin saturation. Absolute determination of tissue optical properties, however, requires additional information over and above the detected intensity at the tissue surface, which must then be combined with a model of light transport to derive μ a and μ s . The additional data can take many forms, e.g. the change in intensity with distance, the temporal dispersion of light from an ultrashort input light pulse, or phase, and modulation depth changes of intensity–modulated light. All these approaches are now being actively pursued with considerable success. However, all the approaches are limited by the accuracy of the light transport models, especially in inhomogeneous media.


1996 ◽  
Vol 39 (5) ◽  
pp. 889-894 ◽  
Author(s):  
Arlene Duncan ◽  
Judith H Meek ◽  
Matthew Clemence ◽  
Clare E Elwell ◽  
Penny Fallon ◽  
...  

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