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Marginal DNL simulation, introduced in this paper, exploits the fact that the successive simulations often exhibit a large overlap.
The first was successive simulations of incident spectra with central energy in the range of 50 70 keV.
Successive simulations showed the orientation of the dominant ripples to vary between (vec q_{2}) and (vec q_{3}), as the randomized initial surface allowed for the competition between wave vectors to vary.
The simulations displayed this degeneracy in the direction of the emergent ripples (i.e. the x- and y- components changed between positive and negative with successive simulations), but both components were shown to be equal in magnitude, as expected analytically.
Most of the computational efforts are spent on these successive simulations over a cycle.
Our approach was to parameterize in a step-wise manner: CG forcefield parameters were determined through successive simulations at the atomistic molecular-dynamics level, the simulations chosen such that no more than three CG interaction parameters were derived in any one fitting procedure.
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DPD (as well as similar MD) code consists basically of a main loop over (non-parallelizable) successive simulation steps in which (parallelizable) particle pair force evaluations are the most time-consuming part [13, 14].
The number of mesh elements on the stent was doubled with successive simulation until convergence of the mass transport residual.
Consequently, over the course of successive simulation generations, the remainder of the landscape was filled at a rate associated with values of δ specified during simulation runs.
Successive simulation studies have focused on studying the designs that yielded the best results in previous simulations.
As can be seen from Fig. 3, the HPA predicted a pending hypoglycemic event when glucose concentration was ∼104 mg/dl and suspended the pump for 90 min. This resulted in prevention of the event where, in successive simulation without the use of the algorithm, the glucose dropped to extremely low values.
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