Abstract

Abstract. OH-equivalent temperatures were derived from all of the temperature profiles retrieved in 2004 and 2005 by the ACE-FTS instrument in a 5 degree band of latitude centred on a ground-based observing station at Maynooth. A globally averaged OH volume emission rate (VER) profile obtained from WINDII data was employed as a weighting function to compute the equivalent temperatures. The annual cycle of temperature thus produced was compared with the annual cycle of temperatures recorded at the ground-based station more than a decade earlier from the OH*(3-1) Meinel band. Both data sets showed excellent agreement in the absolute value of the temperature minimum (~162 K) and in its time of occurrence in the annual cycle at summer solstice. Away from mid-summer, however, the temperatures diverged and reach a maximum disagreement of more than 20 K in mid-winter. Comparison of the Maynooth ground-based data with the corresponding results from two nearby stations in the same time-period indicated that the Maynooth data are consistent with other ground stations. The temperature difference between the satellite and ground-based datasets in winter was reduced to 14–15 K by lowering the peak altitude of the weighting function to 84 km. An unrealistically low peak altitude would be required, however, to bring temperatures derived from the satellite into agreement with the ground-based data. OH equivalent temperatures derived from the SABER instrument using the same weighting function produced results that agreed well with ACE-FTS. When the OH 1.6 μm VER profile measured by SABER was used as the weighting function, the OH equivalent temperatures increased in winter as expected but the summer temperatures were reduced resulting in an approximately constant offset of 8.6±0.8 K between ground and satellite values with the ground values higher. Variability in both the altitude and width of the OH layer within a discernable seasonal variation were responsible for the changes introduced. The higher temperatures in winter were due to primarily to the lower altitude of the OH layer, while the colder summer temperatures were due to a thinner summer OH layer. We are not aware of previous reports of the effect of the layer width on ground-based temperatures. Comparison of OH-equivalent temperatures derived from ACE-FTS and SABER temperature profiles with OH*(3-1) temperatures from Wuppertal at 51.3° N which were measured during the same period showed a similar pattern to the Maynooth data from a decade earlier, but the warm offset of the ground values was lower at 4.5±0.5 K. This discrepancy between temperatures derived from ground-based instruments recording hydroxyl spectra and satellite borne instruments has been observed by other observers. Further work will be required by both the satellite and ground-based communities to identify the exact cause of this difference.

Highlights

  • Inter-comparison of geophysical datasets measured by different techniques is valuable for the validation of the techniques themselves in addition to offering the possibility of uncovering new physical phenomena

  • This study reports on a comparison of temperatures retrieved by two satellite instruments, Atmospheric Chemistry Experiment (ACE)-Fourier transform spectrometer (FTS) and SABER for the period January 2004 to December 2005 with temperatures obtained from the OH*(3-1) Meinel band which were recorded more than a decade earlier

  • Layer, we found that correcting 30-day averaged temperature profiles for SABER using the 30-day averaged altitudes and widths shown in Fig. 11 did not reproduce exactly the 30day averaged temperatures obtained when each temperature profile was weighted by its corresponding the OH 1.6 μm volume emission rate (VER) profile

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Summary

Introduction

Inter-comparison of geophysical datasets measured by different techniques is valuable for the validation of the techniques themselves in addition to offering the possibility of uncovering new physical phenomena. The ideal case for such comparisons arises when the measurements are taken at the same time and place. P. Lowe: OH-equivalent temperatures derived from ACE-FTS and SABER temperature profiles occur due to differences in signal levels and instrument characteristics (e.g. Oberheide et al, 2006). On the other hand, She and Lowe (1998) have pointed out that valuable intercomparison between two instruments at different sites may be achieved on a statistical basis, when the comparison is restricted to parameters which are of large spatial scale and long period

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