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The sliding cell method is slow, but the kernel is normalized such that no assumption is needed about data beyond the field edges.
The application scope of present unit cell method is clarified from the thermal and mechanical point of views.
The representative cell method is employed for the construction of Green's functions for the displacements jumps along the crack line.
The representative cell method is employed in the first analysis for the construction of Green's functions elastic fields for the fiber matrix interfacial jumps problem.
The effect of electromechanInal coupling on the dynamic response is discussed.
A new implicit fully electromagnetic particle in cell method is presented in which the full ion dynamic and all the electron guiding centre drifts of a magnetized collisionless plasma are retained.
Similar(52)
We report on three different methods to prepare nanostructured materials using highly ordered porous alumina membranes as templates: (1) firstly, a new and simple method, termed as the paired cell method, was developed for the preparation of inorganic nanowires.
The optimal pH of the resting cell method was determined by incubation at 30°C for 8 h in the pH range of 4.5 to 9.0 as described in Materials and Methods.
A three-dimensional, incompressible, multiphase particle-in-cell method is presented for dense particle flows.
The Monte-Carlo based particle-in-cell method is used in the vicinity of the cathode.
The particle-in-cell method is coupled with boundary-fitted grids in order to model the stationary Maxwell-Lorentz problem in technical devices.
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