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                    208  CHAPTER 13



                  oxygen, sodium, and other volatile elements accom-
                  panies Io in its orbit around Jupiter. The ease with
                  which gases are lost from an atmosphere depends
                  on their molecular weight, and the values for water,
                  carbon dioxide, diatomic sulfur (the commonest
                  form), and sulfur dioxide are close to 18, 44, 64,
                  and 64, respectively. The inference is that over the
                  course of geological time Io has erupted and lost
                  essentially all of the water and carbon dioxide from
                  its mantle. It may well have erupted most of the
                  sulfur-related compounds onto the surface, but
                  they have not yet been completely lost but instead
                  are recycled through volcanic activity. The recy-  Fig. 13.19 Near the left edge of this 250 km wide image a
                                                              mildly explosive eruption is taking place in one of the chain
                  cling is not in the form of subduction back into the
                                                              of calderas forming the Tvashtar Catena on Io. The image is
                  mantle, for there are no signs of plate tectonics on
                                                              a composite of data obtained through near-infrared, clear,
                  Io, but instead consists of sulfur and sulfur dioxide
                                                              and violet filters on the Galileo spacecraft. (Image courtesy
                  collecting on the surface as solids, being buried  of NASA/JPL/University of Arizona.)
                  under layers of pyroclasts and lavas, being heated
                  by the  geothermal gradient, and melting to form
                  “aquifers” in the crust. The dikes feeding new erup-  whether these magma reservoirs have formed at
                  tions sometimes cut through these aquifers and the  neutral buoyancy levels in the crust, but this is hin-
                  volatile-poor magmas in the dikes absorb the aquifer  dered by uncertainties about the volatile content, if
                  liquids. The liquids then boil to vapor and drive the  any, of the ascending magmas and also the density
                  violently explosive eruptions just as if they were  structure of the crust. The low value of the acceler-
                  expanding magmatic volatiles. The heights of the  ation due to gravity on Io would lead us to expect
                  largest plumes, commonly up to at least 300 km,  that levels of neutral buoyancy might be at depths
                  and their widths, up to 1200 km, imply eruption  of order 15 km and that magma reservoirs might
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                  speeds of more than 1000 m s , and the analysis in  have large vertical extents.
                  Chapter 6 shows that this could be achieved only if  Many calderas are clearly the sites of eruptions
                  the magma contained about 30 wt% of volatiles.  from fissures, both explosive and effusive (Fig. 13.19).

                  This is vastly more than could be dissolved in any  Attempts have been made to estimate eruption rates
                  possible juvenile magma from the mantle.    by analyzing the sizes and dynamics of plumes, by
                    Some plumes seem to be caused not by dikes  measuring the heat release rate from eruption sites,
                  absorbing liquid volatiles but by lava flows advanc-  and by measuring the increases in areas of lava
                  ing over a surface rich in solid volatiles. A finite time  flows with time. The latter is not easy because the
                  is taken for enough heat to be conducted down-  Galileo spacecraft only made close approaches to
                  ward to melt and evaporate the solids, and so jets of  Io every few months. Also, the resolution of the
                  gas punch holes through many places in the lava  images was not good enough to allow flow thick-
                  flow after its front has gone by and combine to form  nesses to be estimated accurately. Nevertheless,
                  a plume. This is somewhat akin to the formation of  there is some convergence on eruption rates up
                                                                     3 −1
                                                                  5
                                                                                                    3 −1
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                  pseudocraters around rootless vents in terrestrial  to 10 m s with occasional bursts up to 10 m s
                                                                                          3
                  lava flows crossing marshy ground, and also can   and erupted volumes up to 100 km . The high erup-
                  be thought of as a kind of hydromagmatic activity,  tion rates are consistent with the high temperatures
                  although the volatile involved is not water.  and low viscosities of the magmas and, if the lava
                    There are many calderas on Io (Fig. 13.19), typ-  flows are being fed from magma reservoirs beha-
                  ically with diameters of several tens of kilometers,  ving elastically, the arguments in Chapter 4 imply
                  implying that beneath them are magma reservoirs  that the reservoirs should have volumes of up to
                                                                       3
                  of similar size. Attempts have been made to infer  30,000 km . This is possible with ∼50 km diameter
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