The individual transfer function is a complex function of frequency that relates the (complex) current injected by the wind park into the public grid with the (complex) current injected by one individual turbine into the collection grid.
The new ADI finite-volume method is also extended for simulations on multi-block structured curvilinear grids with which complex geometries can be efficiently resolved.
Such an approach allows us to compare different patient-specific CAS scenarios, ranging from a healthy carotid to a post-stenting configuration after the treatment of a severe stenosis, and paves the way for rapid CFD-based investigations of the hemodynamic impact of novel endovascular devices with complex grid designs.
A Cartesian grid method for computing flows with complex immersed, moving boundaries is presented.
The coefficient of the grid with LSWI becomes more complex as indicated in Eqs. 10 and 11, so every submatrix can be regarded as an integral term when the overall numerical model is solved by block pretreatment of generalized minimal residual algorithm (Baohua et al. 2013).
Applications of the composite grid method to various model problems with complex geometry are used to illustrate the characteristics of the present procedure.
However, such an assumption is not valid in urban scenarios, where a complex road grid with multiple road directions must be considered when relaying data messages.
Overlap grid is usually used in numerical simulation of flow with complex geometry by high order finite difference scheme.
We present an immersed-boundary algorithm for incompressible flows with complex boundaries, suitable for Cartesian or curvilinear grid system.
We construct a fast method, O(NlogN), for the computation of discrete Gauss transforms with complex parameters, capable of dealing with unequally spaced grid points.
