no. 33 a determination of the martian coa abundance
TRANSCRIPT
No. 33 A DETERMINATION OF THE MARTIAN COa ABUNDANCE
by T. C. Owen *
June 8,1964Revised August 26,1964
Lunar and Planetary Laboratoryand
Kitt Peak National Observatory**
Contribution No. 66 of the Kitt Peak National Observatory
ABSTRACTTwo independent determinations are presented of the C02 content of the Martian atmosphere derived from the Mt.
Wilson plate obtained by Kaplan, Munch, and Spinrad.
I. Introduction
T^he two preceding papers (Comm. LPL 31 and32) present new spectra of the planet Mars inthe 1.0-2.5 p, region and their laboratory calibrationwith a long absorption tube. This calibration leadsto a relationship between total atmospheric pressureand C02 abundance. Before the atmospheric pressure (and, by inference, an approximate composition) can be found, independent data on the MartianC02 abundance are required. The best source of thisinformation at present is the Martian A 8689A C02band observed by Kaplan, MUnch, and Spinrad(1964) (referred to hereafter as KMS). These authorsthemselves calibrated this C02 band from laboratoryobservations supplied by Rank, but because of thepeculiar role played in this band by the effects ofblending by solar Fraunhofer lines it appeared important to recalibrate the spectrum in such a manner that the effects of solar blending would beaccurately allowed for. The interest in the A 8689Aband stems from the fact that the lines in this band
are very weak so there is almost no saturation. Thusthey are on the linear part of the curve of growthand their intensities are directly proportional to theabundance.
After calculating the effective air mass corresponding to the Martian observation and makingslight corrections for collisional broadening andsaturation effects due to the narrowness of the lines,KMS derived a value of 55 ± 20 m atm for the C02abundance. This value corresponds to an assumedtemperature of 230°K in the Martian atmosphere.For 200°K, the corresponding value was 50 ± 20m atm. The reason cited for the large probable errorassociated with these values was the difficulty indetermining the equivalent widths of the weak C02lines.
The new calibration of the Mt. Wilson spectrogram was done in two steps. A preliminary calibration was made prior to the completion of ourhigh-dispersion laboratory spectrograph by meansof observations of the 8689A band of C02 in the
♦Graduate Research Student, 1963, Kitt Peak National Observatory.** Operated by the Association of Universities for Research in Astronomy, Inc., under contract with the National Science
Foundation.133