Back to Search Start Over

Comparison of temperature dependent calibration methods of an instrument to measure OH and HO2 radicals using laser-induced fluorescence spectroscopy.

Authors :
Winiberg, Frank A. F.
Warman, William J.
Brumby, Charlotte A.
Boustead, Graham
Bejan, Iustinian G.
Speak, Thomas H.
Heard, Dwayne E.
Stone, Daniel
Seakins, Paul W.
Source :
Atmospheric Measurement Techniques Discussions; 6/15/2023, p1-33, 33p
Publication Year :
2023

Abstract

Laser Induced Fluorescence (LIF) spectroscopy has been widely applied to fieldwork measurements of OH radicals, and of HO<subscript>2</subscript>, following conversion to OH, over a wide variety of conditions, on different platforms, and in simulation chambers. Conventional calibration of HO<subscript>x</subscript> (OH + HO<subscript>2</subscript>) instruments has mainly relied on a single method, generating known concentrations of HO<subscript>x</subscript> from H<subscript>2</subscript>O vapour photolysis in a flow of zero air impinging just outside the sample inlet (SHO<subscript>x</subscript> = CHO<subscript>x</subscript>.[HO<subscript>x</subscript>], where SHO<subscript>x</subscript> is the observed signal and CHO<subscript>x</subscript> is the calibration factor). The FAGE (Fluorescence Assay by Gaseous Expansion) apparatus designed for HO<subscript>x</subscript> measurements in the Highly Instrumented Reactor for Atmospheric Chemistry (HIRAC) at the University of Leeds has been used to examine the sensitivity of FAGE to external gas temperatures (266 -- 348 K). The conventional calibration methods give the temperature dependence of C<subscript>OH</subscript> (relative to the value at 293 K) of (0.0059 ± 0.0015) K<superscript>-1</superscript> and CHO<subscript>2</subscript> of (0.014 ± 0.013) K<superscript>-1</superscript>. Errors are 2σ. C<subscript>OH</subscript> was also determined by observing the decay of hydrocarbons (typically cyclohexane) caused by OH reactions giving C<subscript>OH</subscript> (again, relative to the value at 293 K) of (0.0038 ± 0.0007) K<superscript>-1</superscript>. Additionally, CHO<subscript>2</subscript> was determined based on the second order kinetics of HO<subscript>2</subscript> recombination with the temperature dependence of CHO<subscript>2</subscript>, relative to 293 K being (0.0064 ± 0.0034) K<superscript>-1</superscript>. The temperature dependence of CHO<subscript>x</subscript> depends on HO<subscript>x</subscript> number density, quenching, relative population of the probed OH rotational level and HO<subscript>x</subscript> transmission from inlet to detection axis. The first three terms can be calculated and, in combination with the measured values of CHO<subscript>x</subscript>, show that HO<subscript>x</subscript> transmission increases with temperature. Comparisons with other instruments and the implications of this work are discussed. [ABSTRACT FROM AUTHOR]

Details

Language :
English
ISSN :
18678610
Database :
Complementary Index
Journal :
Atmospheric Measurement Techniques Discussions
Publication Type :
Academic Journal
Accession number :
164358972