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Spectroscopy in Atmospheric Science: Techniques, Relationships, and Trace Gas Processes, Study notes of Meteorology

The role of spectroscopy in atmospheric science, focusing on solar spectroscopy, uv-vis-ir absorption spectroscopy, and fluorescence spectroscopy. It discusses important relationships such as transition dipole moments, optical density, and absorption cross-sections. The document also covers trace gas exchange processes with soil, ocean, and vegetation and methods to measure trace gas fluxes using enclosures and micrometeorological techniques.

Typology: Study notes

Pre 2010

Uploaded on 02/13/2009

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Download Spectroscopy in Atmospheric Science: Techniques, Relationships, and Trace Gas Processes and more Study notes Meteorology in PDF only on Docsity! Spectroscopy in Atmospheric Science • Spectroscopy used for many atmospheric science analytical questions – Solar spectroscopy • Direct absorption or scattering in atmosphere (e.g. DOAS) • Remote sensing from space (e.g. UARS, GOME, etc.) – UV-vis-IR absorption spectroscopy • e.g. for ozone, H2O, CO2, CH4, CO, etc. – Fluorescence spectroscopy • High specificity, sensitivity, and resolution lab studies • Increasing amount of field-based instruments for important atmospheric species, such as HOx, etc. • Very specific and sensitive technique(s) ! Absorbing molecule co co co co co HsO 2 2 2 2 2 Op | HO | 03 _H20 [O03 Heo | |, TWHy +t odd t w + 4 + 100 T T T T T T TT T T T T T T & 804 oO 2 607 Ss — 407 wm Cc S 20+ _ 0 T T T T T T T T T T T T T T 0 61 2 3 4 5 6 7 & 9 10 11 12 #139 #14 «+15 Wavelength/(um) fq HE jel middle far 3 (a) infrared infrared infrared VB = 667 cm Vp = 667 om! Vag = 2349 emt Bending modes Stretching modes Figure 7.4 Representation of the two stretching modes and the two bending modes of CO). For the stretching modes we indicated three different positions. The bending modes correspond to two orthogonal planes, which are physically equivalent and therefore have the same frequency 1H 376 | 1H 35¢C] lll HL 2800 HM P-Branch R-Branch — v Acm!) Absorption Ws Figure 7.3 High-resolution vibrational-rotational spectrum of HCl. The lines appear in pairs because the spectrum reflects the presence of both H*°Cl and H*’Cl in their natural abundance ratio of 3:1. The AJ =0 branch is absent in these spectra. (Adapted and reproduced by permission of Oxford University Press from [1], Fig. 18.14) Figure 7.7 Schematic representation of the sequence of events leading to fluorescence, triplet formation and phosphorescence. Note that the maximum in the fluorescence spectrum again will correspond to the transition with the largest Franck—Condon factor Standard N QO, fluorescence NO-instrument SAMPLE &— (NO I MODE) TEFLON FLOVY PARTICULATE NO SENSOR FILTER Yr c MoDpEe os FILTER CAPILLARY yo P SOLENOID ! a ELECTRONICS L NO-NO CONVERTER _ PRESSURE REACTION I (NO, MODE) TRANSDUCER CHAMBER ! ey DRYAIR ¢ i PMT bocvnnnnsne & FLOW CAPILLARY ; SENSOR OZONATOR OPTICAL FILTER I CHAMBER PUMP Standard Gas Filter Correlation infrared absorption CO-instrument Modei 48CTL - FLOW DIAGRAM Electronics Preamplifier Pressure Transducer IR Detector sample (+ Sane Gas Filter Wheel Bandpass Filter Infrared Source Chopper Chopper Meteor Flow Sensor Exhaust Capillary Purp Trace Gas exchange processes • with soil only – NO, N2O, CH4, H2 • with soil – CO2, CO – NH3 – COS, H2S, DMS – (ozone) • with ocean – CO2, CO – VOCs – DMS, COS, etc. • with vegetation – CO2 – CO – ozone – VOCs (e.g. isoprene) – NO2, HNO3, etc. – COS, SO2 – alkyl-halides – NH3 – … -3 -2 -1 0 1 2 3 14:32:56 14:33:39 14:34:22 14:35:05 14:35:48 time w ( m s -1 ) Sonic anemometer time series 25 26 27 28 29 30 31 14:34:22 14:34:57 14:35:31 14:36:06 14:36:40 14:37:15 14:37:49 14:38:24 local time T ( d eg C ) -3 -2 -1 0 1 2 3 w ( m s -1 ) -2 -1 0 1 2 3 4 5 -3 -2 -1 0 1 2 3 w' (m s-1) T' ( K )
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