2.1 Dynamic Registration

Figure 3.2 shows the probes used to measure the detonation velocity for the detonating cord.. Figure 3.2 The picture of the pins with the cables for connection to the pin

CO 2 volume fraction (blue), pressure (lines every 1 bar) and water Darcy flux (vectors shown at every 16th grid point), for Case A with porosity 0.3 and permeability 3000 mDa (top)

Figure 5 displays the airflow velocity vectors and temperature distribution in the OR equipped with TcAF (Fig.5 (a)) and LAF (Fig.5 (b)) ventilation systems. The colour of

By using the along-beam wind velocity data from two synchronized lidars in a horizontal plane tangential to the vertically curved bridge (v r 1 and v r 2 ), it is possible to

We retrieve the velocity of the liquid from the velocity of the fluid simulation at a distance l away from the solid surface, and we recover the velocity of the solid surface

Figure 1: Groundwater model domain, final state of transient simulation (year 2005); groundwater levels, scaled velocity vectors with relative mass fraction; dashed lines

Seven methods were evaluated using the benchmark, namely: traditional non- rigid Iterative Closest Point (N-ICP) [BP13], anisotropic non-rigid registration [DLRT19], deep

To approximate the surface from unstructured points equipped with normal vectors, we rely on the Algebraic Point Set Surfaces (APSS) [GG07] for which we provide convergence