Pyroclastic density currents (PDCs) are flowing mixtures of hot gas and volcanic particles. They are the dominant single cause of fatalities around volcanoes (S. K. Brown et al., 2017) and can be generated by the fountaining of eruption columns, lateral blasts, and growing lava domes (Branney et al., 2021;Druitt, 1998). They transport large volumes of hot, ash-rich pyroclastic debris rapidly across the landscape, and span a wide range of scales, particle concentrations and grain-sizes (Branney & Kokelaar, 2002). A key factor in the hazard they present is the distance they travel (the "runout distance") over a given topography, and this is significantly affected by the current's mass flux at the source (e.g., Bursik & Woods, 1996; Shimuzu et al., 2019;Williams et al., 2014). In many cases, it can be assumed that the mass flux of the pyroclastic current derives directly from the vent discharge rate (mass flux) of the eruption (e.g., Roche et al., 2021;Sparks et al., 1997). However, PDCs are known to entrain loose substrate