Furthermore the "effective" rigid molar volume Ve and the apparent B coefficient have been computed employing Breslau and Miller treatment from the relative viscosity data.
From the relative viscosity data, the "effective" rigid molar volume, Ve and apparent B coefficient have been computed employing the Breslau-Miller procedure at temperatures 25, 30, 35 and 40°C.
For fixed (tin 0,t_{0}]) the volume rigid inclusion is specified by the set (omega_{t}times[-1,1]), i.e. the boundary of the rigid inclusion is defined by the cylindrical surface ({partialomega_{t}}times[-1,1]).
The finite deformation simulations use a rigid-plastic, volume hardening plasticity model for the compacting powder and a hyperelastic model for the rubber.
Since the brain is confined in an inextensible, rigid structure, cell volume regulation is crucial as any excessive increase in cell volume resulting in brain swelling over a threshold of 10%% equates with severely elevated intracranial pressure, placing the patient at risk of serious brain injury and, ultimately, brain herniation [50, 51].
Since the brain is confined in an inextensible, rigid structure, cell volume regulation is crucial as any excessive increase in cell volume resulting in brain swelling over a threshold of 10%% equates with severely elevated intracranial pressure, placing the patient at risk of serious brain injury and, ultimately, brain herniation [ 50, 51].
Let us formulate an equilibrium problem for an elastic plate containing a volume rigid inclusion.
Let us formulate the family of contact problems for an elastic inhomogeneous plate containing a volume rigid inclusion.
Shape similarity scores are then evaluated in terms of the rigid body overlap volume with comparison timings in the milliseconds range.
In parallel with the contact problem for a plate with a volume rigid inclusion, we also consider the contact problem for an elastic plate with a thin inclusion.
