The evolution of the plasma parameters in the termination phase of high confinement H-modes at JET with CFC plasma facing components (JET-C) has been analyzed with a view to predict the dynamics of the plasma energy decrease for sudden terminations of the ITER QDT =10 scenario caused by malfunction of additional heating systems. JET-C experiments show that the rate of decay of the plasma energy in the high performance H-mode termination phase is predominantly determined by the duration of the Type III ELMy H-mode phase after the end of the Type I ELMy H-mode regime. Longer Type III ELMy H-mode phase durations lead to slower plasma energy decay rates. The duration of the Type III ELMy H-mode phase is itself determined by the margin of the edge power flow (dominated by the rate of collapse of the plasma energy) over the H-mode threshold power in the termination phase, with larger margins leading to longer Type III ELMy H-mode phase durations. For most of the JET-C discharges analyzed the timescale for the plasma energy decrease in the termination of high energy confinement H-modes is comparable to the energy confinement time of the plasma in the high confinement phase rather than half of this value, which is to be expected for instantaneous H-L transitions. Modelling of the termination phase of ITER QDT =10 H-modes (with transport assumptions in this phase validated against JET-C experiments) shows that similar to JET-C results the timescale for the decrease of the plasma energy is comparable and can even be longer than the energy confinement time of the burning phase, provided that ELM control can be maintained. This is due to the long sustainment of the Type III ELMy H-mode mode by the substantial edge power flow compared to the H-mode threshold power during this phase. The large edge power flow in the termination phase of ITER high QDT plasmas is provided by the decrease of the plasma energy and the slow collapse of the alpha heating. Operational strategies in ITER to control the energy decay rate as well as the consequences of the lack of ELM control in the high QDT termination phase are presented.