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Result shows that explicit finite element method is computational efficient and can effectively avoid convergence problem.
All criteria are programmed with the explicit user subroutines employing element deletion to avoid convergence problems caused by element distortion.
A linear approximation of the system is used to avoid convergence issues in the iterative adjustment of reactive power.
In addition, to avoid convergence trouble, a strategy based on a feasibility test relative to the objective value of the outer program is used.
This specific finite element model has been developed in order to avoid convergence problems that sometimes occur with the introduction of contact-friction elements in 3D models.
According to the characteristics of the model, a new approach was proposed to avoid convergence difficulties and to improve the stability of the calculations.
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The GA method increases the probability of finding the global optimum solution and avoids convergence to a local minimum which is a drawback of gradient-based methods.
Bayesian results were comparable to maximum likehood method but they avoided convergence problems, the marginal likelihood allowed to compare all models, and credible interval gave directly the uncertainty of sorption parameters θ.
The method is designed to make possible the use of large P spaces while avoiding convergence problems traceable to intruder states, which often beset multi-reference coupled cluster approaches.
The fictitious viscosity technique for avoiding convergence problems in finite element simulations of crack nucleation and growth on cohesive interfaces allows us to explore a wider parametric space that a conventional cohesive model cannot handle.
Formally, for ψ ∈ S (R n ), H ˆ ψ (x ) = (1 2 π ħ ) n ∫ ∫ e i p ⋅ (x − y ) / ħ H (1 2 (x + y ), p, t ) ψ (y ) d p d y ; more rigorously (that is avoiding convergence problems in the integral above) H ˆ ψ (x ) = (1 2 π ħ ) n ∫ H σ (z 0 ) T ˆ ħ (z 0 ) ψ (x ) d z 0 where H σ is the symplectic Fourier transform of H and T ˆ ħ (z 0 ) is the Heisenberg Weyl operator defined by formula (18).
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com