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                    150  CHAPTER 10



                  variation in magma gas content or in magma rise  vidual Strombolian explosions produce very small
                  speeds, that viscosity is probably the dominant fac-  volumes of material, eject this material from the
                  tor controlling whether significant bubble coales-  vent at relatively low speeds, and usually occur
                  cence can occur in different magmas. This can be  more closely spaced in time than Vulcanian erup-
                  demonstrated by some simple calculations such as  tions. Strombolian eruptions usually involve basaltic
                  those performed for basaltic magmas in section 5.5.3.  magmas whereas Vulcanian eruptions are typically
                    Let us consider the case of bubble rise in an inter-  associated with the eruption of intermediate mag-
                  mediate or very evolved high-silica magma. Say that  mas. Thus, there seems to be a strong connection
                  in both cases magma exsolution begins at a depth of  between the composition of the erupting magma
                  5 km beneath the surface. Typical rise speeds for  and the character of the transient explosion which
                  intermediate and evolved magmas are thought to  results. In what way is the chemical composition
                                               −1
                  be in the range 0.001 to 0.015 m s . This means  controlling the eruption dynamics?
                                   5
                                            6
                  that it takes 3.3 × 10 to 5 × 10 seconds for the  Field observations and mathematical modeling
                  magma to rise from 5 km depth to the surface.  of Strombolian and Vulcanian eruptions suggest
                  Whether bubble coalescence can occur during   that the differing “violence” of the eruptions is
                  this ascent depends on the rise speed of bubbles  related to the strength of the “cap” on the magma
                  through the rising magma (section 5.5.3). If we con-  column prior to eruption (see section 7.2.1 and Fig.
                  sider the intermediate magma first and assume   7.1). In Strombolian eruptions, the gap between
                                             3
                  that it has a magma viscosity of 10 Pa s then a bub-  explosions is too short to allow much cooling of
                  ble 1 mm in radius will rise at a speed of ∼6.5 ×  the magma at the top of the magma column, and
                        −1
                  10 −6  ms and thus can rise a distance of between 2.1  the cooled “skin” that does develop tears easily as
                  and 32.5 m through the overlying magma during  gas bubbles accumulate beneath it causing weak
                  the time it takes the magma to rise to the surface. If  explosions (Figs 1.14 & 7.1). In Vulcanian explo-
                  the bubbles are larger, say 1 cm in radius, their   sions the magma at the top of the magma column
                                        −1
                  rise speed is ∼6.5 × 10 −4  ms (eqn 5.12) and the dis-  cools much more between explosions forming a
                  tance traveled by the bubbles relative to the magma  solid “cap” (Figs 7.1 & 7.2) and so the pressure
                  is correspondingly greater at 214 to 3250 m. By  beneath it must build to considerably greater
                  contrast, in a more evolved magma with a viscosity  levels prior to explosion. This is probably because
                      6
                  of 10 Pa s the rise speed of a bubble 1 mm in radius  of the different viscosities of the magmas involved.
                  decreases to 6.5 × 10 −9  ms −1  and the distance trav-  In basaltic magmas the low viscosity allows rela-

                  eled through the magma during ascent to the sur-  tively rapid rise of gas bubbles through the magma
                  face is only 2.1 × 10 −3  to 0.03 m. Even at a bubble  and this means that the surface of the magma col-
                  radius of 1 cm the bubble rise speed is only 6.5 ×  umn is disrupted and removed frequently so that
                  10 −7  ms −1  and the distance risen by the bubbles  there is not time for a thick crust to develop, i.e.,
                  only 0.2 to 3.3 m. Thus in this simple example   the rise speed of the bubbles controls the time avail-
                  bubble coalescence is likely to occur in the inter-  able for the skin on the magma column to develop
                  mediate magma case but is very unlikely in the case  and hence the violence of the resulting explosion.
                  of the high-silica magma even at very low magma  Thus basaltic magmas commonly give rise to
                  rise speeds. The low rise speeds of gas bubbles in  Strombolian eruptions. The rise speeds of bubbles
                  these magmas explains why transient explosions  in intermediate magmas will be lower due to the
                  are commonly associated only with basaltic and  higher viscosity of the magma (sections 5.5.3 and
                  intermediate magmas but not with evolved magmas.  10.4.1). The slower rise and accumulation rate of
                                                              gas at the top of the magma column then means
                  10.4.2 Chemical composition and transient   that the top of the magma column has more time
                  explosive activity                          to cool than in the Strombolian case. This greater
                  We have seen that transient explosions occur when  cooling means that the pressure necessary to
                  magma rise speeds are slow. The two main types of  cause failure of the cap is greater. The brittle failure
                  transient eruption – Strombolian and Vulcanian –  of this cap gives rise to Vulcanian explosions
                  differ from each other in a number of ways. Indi-  (Fig. 1.16).
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