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                                                                      STEADY EXPLOSIVE ERUPTIONS  85













                 Fig. 6.6 The eruption plume from
                 the March 22, 1915, eruption of
                 Lassen Peak volcano, showing the
                 classic umbrella shape of the upper
                 part of the plume. (Photograph
                 credit: R.I. Meyers, courtesy of the
                 National Oceanic and Atmospheric
                 Administration, National Geophysical
                 Data Center.)



                 clasts, a point will be reached where the bulk den-  Table 6.2 Plume heights generated during selected
                 sity of the plume equals that of the surrounding air  20th century volcanic eruptions.
                 and the plume can rise no further through thermal
                                                              Eruption                    Plume height (km)
                 buoyancy alone. The height at which this occurs is
                 called the level of neutral buoyancy. However,
                                                              Santa Maria (Guatemala), 1902  27–48
                 the plume still has some inertia as it rises slowly  Soufriere (St Vincent), 1902  14.5–16
                 through the neutral buoyancy level and so it over-  Hekla (Iceland), 1947  24
                 shoots this level somewhat, spreading sideways  Bezymianny (Kamchatka), 1956  34–45
                 and downwind as it does so. This part of the plume  Hekla (Iceland), 1970  14
                                                              Fuego (Guatemala), 1971     10
                 is known as the umbrella region (Fig. 6.5) and an
                                                              Heimaey (Iceland), 1973     2–3
                  example can be seen in Fig. 6.6.
                                                              Ngauruhoe (New Zealand), 1974  1.5–3.7
                                                              Soufriere (St Vincent), 1979  18
                 6.5.2 Controls on plume height               Mount St Helens (USA), 1980  25
                                                              El Chichón (Mexico), 1982   20–24
                 The heights of plumes in historic eruptions vary
                 widely (Table 6.2). What controls the height to  Data taken from Wilson et al. (1978); Carey, S.N. and
                                                              Sigurdsson, H. (1982) Influence of particle aggregation on
                 which a given plume rises? The biggest factor is
                                                              deposition of distal tephra from the May 18, 1980, eruption
                 the thermal buoyancy of the plume, and this is
                                                              of Mount St Helens Volcano. J. Geophys. Res., 87,
                 controlled by the thermal energy available, so the
                                                              7061–7072; and Sparks, R.S.J., Moore, J.G. and Rice, C.J.
                 highest plumes are those with the most heat. The  (1986) The initial giant umbrella cloud of the May 18th,
                 plumes with the greatest heat are those with the  1980, explosive eruption of Mount St Helens. J. Volcanol.
                 largest  mass flux. Heat is provided to a rising  Geotherm. Res., 28, 257–274.
                  plume by the clasts (and the volcanic gas) con-
                  tained within it. The mass flux is a measure of the
                  mass of magma erupted per unit time, so the higher  dicted for pure gas plumes by Morton et al. (1956):
                  the mass flux the greater the amount of heat sup-  the height of the plume is proportional to the
                  plied to the plume in a given time. Wilson et al.  fourth root of the eruption rate. For a “standard
                  (1978) and Settle (1978) both showed that volcanic  atmosphere” on Earth the relationship is
                  plumes follow very nearly the same relationship
                  between mass flux and plume height that was pre-  H = 0.236 M 1/4                 (6.7)
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