Vulnérabilité cardiaque au stress au cours du remodelage ventriculaire pathologique induit par surcharge volumique : rôle du pore de perméabilité transitionnelle (PTP)

operations, the perceived clarity and success of AMLA; (2) the current AML process inside the Swiss banks with a focus on the monitoring and reporting procedures and (3)

Figure 5-27 plots the effect of the hysteresis in contact angle on the water amplitude in the two types of tubes. Primarily, one can see that the absolute difference between

Figure 7.4: Proposed model predictions of wave amplitude, wave width and wave spacing with film Reynolds number and comparison with experiments in the Sawant test case for p =

Simulation results presented as (a) electrokinetic coupling coefficient and (b) effective excess charge density as a function of the ionic concentrations for the different pore

In this work, we have derived the incompressible Euler equations from the Boltz- mann equation in the case of the initial boundary value problem, for a class of boundary conditions

However, in a recent work [12] Liew and Savona numerically showed that a strong antibunching can be obtained with a surprisingly weak nonlinearity (U ≪ γ) in a system consisting of

However, while profiles outside the vor- tex match observations well, the model underestimates HF and overestimates CH 4 concentrations inside the vortex, par- ticularly in the

On the positive side, we show that when considering signature schemes with appropriate restrictions on the message length O-SNARKs for the corresponding signing oracles exist, based