A depletion of ammonia and water by storms in the deep atmosphere of Jupiter

2020 ◽  
Author(s):  
Tristan Guillot ◽  
David J Stevenson ◽  
Scott J Bolton ◽  
Cheng Li ◽  
Sushil K Atreya ◽  
...  

<p>Microwave observations by the Juno spacecraft have shown that, contrary to expectations, the concentration of ammonia is still variable down to pressures of tens of bars in Jupiter. While mid-latitudes show a strong depletion, the equatorial zone of Jupiter has an abundance of ammonia that is high and nearly uniform with depth. In parallel, Juno determined that the Equatorial Zone is peculiar for its absence of lightning, which is otherwise prevalent most everywhere else on the planet. We show that a model accounting for the presence of small-scale convection and water storms originating in Jupiter’s deep atmosphere accounts for the observations. At mid-latitudes, where thunderstorms powered by water condensation are present, ice particles may be lofted high in the atmosphere, in particular into a region located at pressures between 1.1 and 1.5 bar and temperatures between 173K and 188K, where ammonia vapor can dissolve into water ice to form a low-temperature liquid phase containing about 1/3 ammonia and 2/3 water. We estimate that, following the process creating hailstorms on Earth, this liquid phase enhances the growth of hail-like particles that we call ‘mushballs’. Their growth and fall over many scale heights can effectively deplete ammonia, and consequently, water to great depths in Jupiter’s atmosphere. In the Equatorial Zone, the absence of thunderstorms shows that this process is not occurring, implying that small-scale convection can maintain a near homogeneity of this region. We predict that water, which sinks along with ammonia, should also be depleted down to pressures of tens of bars. Except during storms, Jupiter's deep atmosphere should be stabilized by the mean molecular weight gradient created by the increase in abundance of ammonia and water with depth.  This new vision of the mechanisms at play, which are both deep and latitude-dependent, has consequences for our understanding of Jupiter’s deep interior and of giant-planet atmospheres in general.</p>

2016 ◽  
Vol 55 (4S) ◽  
pp. 04EJ13 ◽  
Author(s):  
Shuhei Funaki ◽  
Yasuji Yamada ◽  
Ryota Okunishi ◽  
Yugo Miyachi

1991 ◽  
Vol 15 ◽  
pp. 247-253
Author(s):  
Devinder S. Sodhi

The data from a small-scale experimental study on ice-structure interaction are used to compute the energy exchanges that take place during creep deformation and intermittent and continuous crushing of ice. The energy supplied by the carriage is partly stored in the structural spring, partly converted to kinetic energy, partly dissipated in deforming and extruding the ice and partly dissipated as heat in the damping mechanisms of the structure. Except for the heat dissipation, all other forms of energy were computed from the experimental data, and the heat dissipation was computed from the energy balance using the first law of thermodynamics. Plots of all forms of energy are shown in graphical form, in which their relative magnitudes, times of occurrence and interplay can be seen. The main result of this study is the thesis that intermittent crushing or ice-induced vibration takes place whenever there is an imbalance between the rates of work done by the carriage and the indentor and that there are no vibrations when these rates of work are equal.


1969 ◽  
Vol 47 (14) ◽  
pp. 2655-2660 ◽  
Author(s):  
N. H. Sagert ◽  
J. A. Reid ◽  
R. W. Robinson

The room temperature, liquid phase radiolysis of cyclohexane has been investigated using perfluorocyclohexane (C6F12) and perfluorobenzene (C6F6) as electron scavengers. Yields of the respective monohydrofluorocarbons were investigated over several orders of magnitude scavenger concentration. The C6F11H yield from the C6F12–cyclohexane system has previously been shown to result from electron capture by C6F12. The data over the extended concentration range were used to calculate a total ion yield of 4.3 ± 0.2 G units and a free ion yield of 0.14 ± 0.02 G units. With C6F6 as an electron scavenger, hydrogen, cyclohexene, and dicyclohexyl yields were all reduced. However, C6F5H yields were much lower than the C6F11H yields from C6F12. On changing the neutralization step by adding the proton scavenger ethanol, C6F5H yields were obtained equal to the C6F11H yields from C6F12. Thus C6F6 is as efficient an electron scavenger as C6F12. Since a change in the neutralization process produces a large change in yield, it is likely that C6F5H (or C6F5) is produced in the neutralization process.


2019 ◽  
Vol 41 (3) ◽  
pp. 439-444 ◽  
Author(s):  
Chih C. Hu ◽  
Mon-Sen Lin ◽  
Tsu-Yi Wu ◽  
Feri Adriyanto ◽  
Po-Wen Sze ◽  
...  

Author(s):  
M. G. Voronkov ◽  
B. A. Trofimov ◽  
V. M. Nikitin ◽  
A. Sh. Mintsis ◽  
F. A. Letnikov ◽  
...  

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