We present a nonlinearly implicit, conservative numerical method for integration of the single-fluid resistive MHD equations.
Furthermore, in this approach, both linear and nonlinear drag forces (resistive fluid forces), the added mass effect (reactive fluid forces), the fluid moments, and current effects are considered.
The hydrodynamic modeling approach from [2] that is considered in this paper, takes into account both the linear and the nonlinear drag forces (resistive fluid forces), the added mass effect (reactive fluid forces), the fluid moments and current effects.
The driving force for solute migration is the moving fluid, and the resistive force is the solute affinity for the stationary phase; the combination of these forces, as manipulated by the analyst, produces the separation.
We present results from analog bench-scale experiments aimed at evaluating the ability of ERT to quantify the volume and spatial distribution of a resistive fluid injected into a brine-saturated porous medium.
It is also evident from this figure that the skin friction coefficient is negative for all values of β, Gr, and K which indicates that fluid experiences a resistive force at the boundary.
We study a semi-implicit time-difference scheme for magnetohydrodynamics of a viscous and resistive incompressible fluid in a bounded smooth domain with a perfectly conducting boundary.
Steady-states of a resistive two-fluid model, self-consistently including flows, anisotropic viscosity (including gyroviscosity) and heat flux, are calculated for diverted plasmas in geometries typical of the National Spherical Torus Experiment NSTXX) [M. Ono et al., Exploration of spherical torus physics in the NSTX device, Nucl. Fusion 40 (3Y) (2000) 557–561].
This is due to the fact that the application of the transverse magnetic field to an electrically conducting fluid gives rise to a resistive type of force known as the Lorentz force.
Increasing transverse magnetic field on the electrically conducting fluid gives rise to a resistive type force called Lorentz force which is similar to drag force and upon increasing the value of M, increases the drag force which has the tendency to slow down the fluid velocity.
Splenic Doppler Resistive Index changes after fluid challenge were +16%% (±9 %) in fluid challenge responders and +4 % (±3 %) in fluid challenge non-responders.Cardiac index variations (DCI) showed a strong correlation with splenic Doppler resistive index changes (DSDRI) after fluid challenge in the overall population (r = 0.85, p < 0.001).
