After the discovery of the landslide on the northern slopes of Monte Toc, it was decided to deepen the studies on these effects: • Dynamic actions on the dam • Wave effects in the reservoir and possible dangers for nearby locations, with particular attention to the town of Erto • Hypothesis of a partial breakage of the dam and consequent examination of the rout wave and its propagation along the last stretch of the Vajont and along the Piave, up to Soverzene and beyond The study of point 1 was performed at the Experimental Institute for Models and Structures (ISMES) of
Bergamo, while for the others, the SADE decided to build a physical-hydraulic model of the basin, in which to perform some experiments on the effects of a landslide fall in a reservoir. The 1: 200 scale model of the basin, which can still be visited today, was set up at the SADE hydroelectric plant in Nove (Borgo Botteon di
Vittorio Veneto), and became the Hydraulic Models Centre. The experiments were entrusted to professors Ghetti and Marzolo, university professors of the Institute of Hydraulics and Hydraulic Constructions of the
University of Padua, and were carried out with funding of SADE, under the control of the study office of the company itself. The study aimed to verify the hydraulic effects on the dam and on the banks of the landslide reservoir, so was directed in this sense rather than reproducing the natural phenomenon of the landslide. The experiments were carried out in two different series (August–September 1961 and January–April 1962), of which the first served substantially to refine the model.
First set of experiments The first series of five experiments began on 30 August 1961, with a sliding surface of the flat landslide inclined by 30°, consisting of a wooden plank covered with a sheet. The sliding mass was simulated with gravel, held in place by flexible metal nets, which were initially held in position by ropes that were then suddenly released. At the beginning of September, another four tests were carried out intended for orientation purposes. The first always with a 30° inclined plane, the following three with a 42° inclined plane. Having found it impossible to reproduce the natural geological phenomenon of the landslide in the model, the model was elaborated by modifying the movement surface of the landslide, which was replaced with a masonry one (the relative profiles were elaborated by
Semenza, who also used the surveys that had already been carried out and that had provided sufficient elements of judgment in this sense), to make it possible to vary the speed of the landslide fall into the reservoir (made difficult by the new "back" shape of the movement surface). To simulate the compactness of the moving material (which in the model remained the gravel), rigid sectors were inserted that were towed by ropes pulled by a tractor.
Second set of experiments In the second set of 17 experiments, conducted from 3 January 1962, to 24 April 1962, the "collapsing" material was still gravel, this time held in place by hemp nets and cords. Starting from the Muller hypothesis relating to the different characteristics of the mass moving between the downstream part of the Massalezza stream (west) and the upstream part of the same (east), all the experiments were performed by making those two hypothetical parts of the landslide descend separately. In the model, however, the two landslides were initially made to descend at different times, so that their effects were totally separate, and subsequently, when the wave produced by the first came back, so as to obtain a total increase in the water of the even greater lake.
Final Ghetti report The total increase of the water in the tank (measured by means of special instruments) was broken down into "static increase", which was the nontransient effect of increasing the level of the water left in the tank after the landslide due to the immersion of the landslide in the tank (once the state of rest is reached again), and in "dynamic boost", due to the temporary wave motion produced by the landslide. The static increase depended on the volume of the landslide that remained immersed in the tank, while the dynamic boost depended almost exclusively on the speed of the landslide fall (while it was negligibly linked to the volume of the same). Based on this simulation (following the disaster object of criticism, as considered approximate by some), placing a reservoir limit at an altitude of predicted that no damage would occur above above mean sea level along the banks of the reservoir, while a minimum quantity of water would have exceeded the edge of the dam (), causing negligible damage downstream of the same. :With the reported experiences, carried out on a 1:200 scale model of the Vajont lake-reservoir, we tried to provide an evaluation of the effects that will be caused by a landslide, which is possible to occur on the left bank upstream of the dam. . Given that the extreme limit downstream of the landslide is more than 75 m from the embankment of the dam, and that the formation of this embankment is of compact and consistent rock and well distinct, even geologically, from the aforementioned mass, it is absolutely not to be fear of any static perturbation to the dam with the occurrence of the landslide, and therefore only the effects of the wave rise in the lake and in the overflow on the dam crest as a consequence of the fall are to be considered. ==Landslide and wave==