Similarly, when we test our method with a weak scenario, 2-fold, our method has low power (our unpublished data).
pBDM requires three parallel calculations: (1) a boundary-based method for a homogeneous full space (bottom), (2) a domain-based method for the target model (left top), and (3) a domain-based method for a weak heterogeneity model represented by a layered structure (right top).
As in the case of BDM, we carry out the following three calculations in parallel: (B) a boundary-based method for a homogeneous full space, (D1) a domain-based method for the target model that we want to simulate, and (D2) a domain-based method for a weak heterogeneity model represented by a layered structure, as shown in Fig. 1.
In the two cases, our method has a weak performance advantage.
The method involves a weak imposition of continuity conditions on the solution values and on fluxes across interelement boundaries.
The method possesses a weak form statement of geostrophic balance due to the compatible nature of the solution spaces and arbitrarily high order spatial error convergence.
This work is devoted to analyzing the feasibility study of a Moudafi viscosity projection method with a weak contraction for a finite family of quasinonexpansive mappings in a Hadamard space.
The purpose of this paper is to analyze the feasibility study of Moudafi viscosity type of projection method with a weak contraction for a finite family of quasinonexpansive mappings in a complete (operatorname{CAT}(0)) space, also known as a Hadamard space.
For launching a large balloon with a total lift above 1.5 ton, the new static launching method had a weak point in that if there was an air bubble in the folded part of the balloon, it may puncture the balloon as it is pushed by a spool.
When the availability of historical data is limited to six months, the method detects a "weak" signal at 90% of simulated cases using census tracts, while it detects a "strong" signal at about the same 90% using individual addresses.
