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                                                                                 MAGMA STORAGE    61


                 volume (s > 0) then the chamber pressure in-  added). Just as in the replenishment model, failure
                 creases less for a given volume of magma added and  occurs because the pressure in the chamber gra-
                 so more magma must be added for the chamber   dually increases to the point where the tensile
                 failure criterion to be met. This simple model has  strength of the chamber walls is exceeded and
                 two important implications for the patterns of  fracturing occurs. However, in this case the pres-
                 activity at a given volcanic center.         sure increases because of the exsolution of volatiles
                   First, as long as the chamber walls behave elasti-  from the magma. Volatile species such as carbon
                 cally, the volume added prior to failure is equal   dioxide (CO ) and water (H O) are contained dis-
                                                                        2            2
                 to the maximum volume that can be erupted from  solved in magmas as they form at great depths in
                 the chamber during a single eruption without the  the mantle. Chapter 5 describes in detail how the
                 danger of caldera collapse, and this volume is ∼0.1  solubility of these gases decreases with decreasing
                 to 1% of the chamber volume (see Fig. 4.20). Thus  pressure so that as magma rises it will eventually
                 this model predicts that the larger the size of the  reach a pressure level at which the magma be-
                 magma chamber feeding an eruption, the larger the  comes saturated in one or more volatile species
                 volume of the eruptions it can produce. Second,  and gas will exsolve from the magma forming gas
                 the frequency of eruptions can be thought of in  bubbles. The low solubility of CO in magmas
                                                                                            2
                 terms of the repose time, R , between eruptions  means that it is often present as a separate gas phase
                                         T
                  and expressed as:                           within shallow magma chambers. In addition, as
                                                              magma cools and crystallizes within a magma cham-
                  R =∆V/M                             (4.4)   ber, the volatile species become increasingly
                   T      m
                                                              concentrated in the residual melt and, by this
                  where, as above, ∆V is the volume of magma added  mechanism, the melt may also eventually become
                 to the magma chamber prior to failure and M is   saturated in more soluble volatiles, particularly
                                                       m
                 the volume rate at which magma is supplied to the  water. The formation of gas bubbles within the
                 chamber. If M does not vary too greatly between  magma requires space to be created. This space can
                             m
                  different magma chambers, it follows that for big-  be created by the compression of the magma, the
                  ger chambers the repose time between eruptions  deformation of the chamber walls and by the crys-
                  will be longer. Or, put another way, the bigger the  tallization process itself. Just as with the addition
                  magma chamber, the less frequent its eruptions.  of magma to the chamber, the exsolution of gas
                   Taken together, these two implications of the  and formation of gas bubbles increases the pressure

                  model match the observed behavior of real vol-  in the chamber. Modeling suggests that only a
                  canic systems, i.e., that larger magma chambers  few percent crystallization is necessary to cause
                  feed larger but less frequent volcanic eruptions. So  sufficient exsolution to raise the pressure to failure
                  magma chamber size plays a crucial role in regula-  levels.
                  ting the scale and frequency of volcanic activity at  This mechanism of chamber failure can occur
                  any given volcanic center.                  only if the gas stays trapped within the chamber.
                                                              Observations in the summit regions of many volca-
                                                              noes show that gas is constantly escaping upwards
                  4.4.3 Volatiles and chamber failure
                                                              from the magma chamber. (Visitors to volcanoes
                  The model just discussed represents one extreme  such as Kilauea in Hawai’I will be immediately
                  scenario for magma chamber failure: failure occurs  aware of this gas leakage in the summit region
                  because of the replenishment of the magma cham-  because of the sulfurous fumes, and caution is
                  ber with fresh magma from deeper levels. At the  advised in spending too much time in certain local-
                  opposite extreme, models have been developed in  ities because the gas release is so great that it is
                  which the failure of the magma chamber occurs  potentially lethal to someone with breathing prob-
                  solely as the result of exsolution of volatiles as  lems!) The ability of gas to escape will depend
                  magma cools and crystallizes within a closed cham-  primarily on whether the gas bubbles can move
                  ber (i.e., one in which no fresh magma is being  upwards through the magma in the chamber. In
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