Zonal mean properties of Jupiter's upper troposphere from voyager infrared observations

Abstract

The highest spatial resolution Voyager IRIS spectra are used to produce zonal averages of the temperature at the 150- and 270-mb pressure levels, of the para-hydrogen fraction at 270 mb, of the ammonia abundance near the 680-mb level, and of two infrared cloud optical depths, one near 5 μm and one near 45 μm wavelength. There are two cloud components, one uniformly distributed and only apparent at 5 μm, and another that correlates strongly with the ammonia abundance and that is apparent at both 5 and 45 μm. From the ratio of optical depths at the two wavelengths, the particles in the variable cloud are between 3 and 10 μm in radius. This cloud is located near the ammonia condensation level. The other particles are either smaller or deeper. The cloud and ammonia distribution is consistent with concentration by upward vertical motion at the equatorward edges of prograde atmospheric jets. The temperature field is also consistent with such vertical motion, with radiative heating balancing adiabatic expansional cooling. The para-hydrogen distribution also appears consistent, but noise levels are high. The thermal wind shear indicates decay of the jets with height within the upper troposphere, with a vertical scale of two or three scale heights. The entire set of upper troposphere data is consistent with a simple axisymmetric dynamical model with Coriolis acceleration of the zonal wind balanced by a linear drag. The meridional residual mean circulation in the model, if interpreted also as a Lagrangian mean circulation, would explain nicely the distribution of ammonia and para-hydrogen. The circulation is a response to a deeper tropospheric flow of unknown origin. However, the horizontal scale of jets is on the order of the deformation radius based on a scale height at the base of the upper troposphere. It is conjectured that the physics of the flow may require this to be true, and may also require that the relative vorticity gradient be of the same order as the planetary vorticity gradient, thereby fixing both the dimensions and amplitudes of the jets.