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                                             PYROCLASTIC FALLS AND PYROCLASTIC DENSITY CURRENTS  123







































                  Fig. 8.13 The deposit from a pyroclastic density current erupted from Mount St Helens volcano in August, 1980. The current
                  bifurcated just before coming to rest, forming two lobes, each about 10 m wide. The coarse, rubbly levées are about 2 m high
                  and the mainly fine-grained central channel deposit is ∼1 m deep. (Photograph by Lionel Wilson.)


                   be related to the height from which it is released.  and magma volatile contents (Table 8.1). If we

                   The wind blows all clasts downwind, but if their  add up the deposit volume from the isopachs,
                   positions on the ground are measured at right-  convert this to a corresponding total mass, and
                   angles to the wind direction we obtain a record  then divide the mass by the mass flux, the dura-
                   of their release distances and hence the release  tion of the eruption can be calculated. Finally,
                   heights.                                     the asymmetry of the deposit, together with the
                  • The release height of a clast of a given size and  cloud height, can give us an estimate of the wind
                   density is an indicator of the rise speed of the col-  speed during the eruption.
                   umn at that height. Low down in the column,   • When a mixture of gas and pyroclasts forming
                   the rise speed depends mainly on the speed of  an eruption column in a steady explosive erup-
                   the gas coming out of the vent and hence on the  tion cannot obtain enough buoyancy from
                   magma volatile content. Higher in the column,  mixing with the surrounding air as it emerges
                   the rise speed depends mainly on the heat flux  from a vent, the lower part of the column
                   driving the column and hence on the mass flux of  collapses to form a fountain over the vent. The
                   magma being erupted from the vent (Fig. 8.6).  upper part of the column continues to convect
                  • Observations of pyroclast dispersal patterns   and drifts away in the direction of the wind. The
                   (Fig. 8.5) can be compared with theoretical   fountain now being fed by the eruption leads to
                   predictions (Fig. 8.7) to deduce erupted mass  the formation of one or more pyroclastic density
                   fluxes, which also define the column heights,  currents.
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