T. Mulder et al., NUMERICAL MODELING OF A MID-SIZED GRAVITY FLOW - THE 1979 NICE TURBIDITY-CURRENT (DYNAMICS, PROCESSES, SEDIMENT BUDGET AND SEA-FLOOR IMPACT), Sedimentology, 44(2), 1997, pp. 305-326
The 1979 Nice turbidity current is modelled using a visco-plastic anal
ysis of flow velocity because the initial flow concentrations are expe
cted to have been very high. The complete history of the failed sedime
nt from debris flow to turbidity current plume is therefore addressed.
The turbidity current portion is considered as a steady state flow di
vided into a dense bottom flow and an upper plume. Model results show
that a dense flow can be generated from the debris flow by the disaggr
egation of the initial slide. The dense flow would be strongly erosive
and able to create and maintain a low-density plume at its surface. T
he depth of erosion of the channel floor by the dense flow is predicte
d to reach 6-11 m in overconsolidated sediments, with the main erosion
taking place in Var Canyon and the Upper Fan Valley. The eroded volum
e (10(8) m(3)) provides additional material to the sediment mass of th
e initial failure. The dense flow appears able to inject fine sand and
silt into the overlying plume during 90 km, and would disintegrate be
fore being able to deposit sediment. The extensive sand layer along th
e travel path of the turbidity current may have been deposited from th
e tail of the trailing plume: a result of the velocity difference betw
een the plume and the dense flow. Observations on sedimentary structur
es, erosion features and distribution of the sand deposit are quite in
agreement without modelling approach. For example, gravel waves can b
e generated when loose deposits are reworked by the supercritical dens
e flow. The methodology and equations presented here provide a good es
timate of the geological consequences of a high-velocity gravity flow
undergoing rheological transition.