Pyroclastic surge


A pyroclastic surge, also referred as a dilute pyroclastic density current, is a flowing mixture of gas and rock fragments ejected during some volcanic eruptions. Pyroclastic surge refers to a specific type of pyroclastic current which moves on the ground as a turbulent flow with low particle concentration with support mainly from the gas phase. Pyroclastic surges are thus more mobile and less confined compared to dense pyroclastic flows, which allows them to override ridges and hills rather than always travel downhill.
The velocity of the head of pyroclastic density currents has been measured directly via e.g. photography as for the case of Mount St. Helens, reaching. Estimates for other recent eruptions range from less than 10 m/s up to 100 m/s. Pyroclastic flows may generate surges. For example, the city of Saint-Pierre in Martinique was overcome by a pyroclastic surge in 1902. Pyroclastic surges can be subdivided into three types: base surge, ash-cloud surge, and ground surge.

Base surge

First recognized after the Taal Volcano eruption of 1965 in the Philippines, where a visiting volcanologist from USGS recognized the phenomenon as comparable to base surge in nuclear explosions. Very similar to the ground-hugging blasts associated with nuclear explosions, these surges are expanding rings of turbulent mixture of fragments and gas that surge outward at the base of explosion columns. Base surges are more likely generated by the interaction of magma and water or phreatomagmatic eruptions. They develop from the interaction of magma and water to form thin wedge-shaped deposits characteristic of maars.

Ash-cloud surge

Ash-cloud surges are considered the most devastating. They form thin deposits, but travel at great speed carrying abundant debris such as trees, rocks, bricks, tiles etc. They are so powerful that they often blast and erode material. They are possibly produced when conditions in an eruption column are close to the boundary conditions separating convection from collapse, that is, switching rapidly from one condition to the other.

Ground surge

These deposits are often found at the base of pyroclastic flows. They are thinly bedded, laminated and often cross-bedded. Typically they are about 1 m thick and consist mostly of lithic and crystal fragments. They appear to form from the flow itself, but the mechanism is not clear. One possibility is that the head of the flow expands through entrainment of air. This then results in the flow front surging forward, which is then over-run by the rest of the flow.