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No method is currently available to combine stochastic, particle-based PBE modeling by means of Monte-Carlo simulation of individual particles and CFD.
This task can be formulated as a large-scale nonlinear, nonconvex optimization problem, where function values and derivatives are obtained by simulation of individual gates.
However, while soakaways are usually small-scale structures, most urban drainage network models operate on a larger spatial scale and the simulation of individual soakaways in these models is therefore often not readily feasible.
These results illustrate that the micro-level simulation of individual pedestrians gives ISAPT the ability to reproduce identified macro-level pedestrian behavior, as well as the capability to reproduce the operational statistics of an observed pedestrian corridor.
For simulation of individual parameter, the number of the neurons in hidden layer was varied from 1 to 12. Too many neurons can lengthen the time required for training the network, whereas too few may not be adequate to train it at all.
Stage-wise simulation of individual heat transfer coefficients and fouling factors showed that both clean overall heat transfer coefficients (Uc) and fouling factors (FF) are stage dependent and conversely the operating overall heat transfer coefficient (UD) is to a great extent less dependent.
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This approach allows concurrent simulation of individuals with a variety of different physiological capabilities (phenotypes) and hence by implication differing genotypic composition.
We generated hybrids by random simulation of individuals of which the genotype is half F_ves/half F_spi.
This paper presents an analysis in which control measures are tested for a hypothetical influenza outbreak in Eemnes, a small city in the Netherlands, generated from the simulation of individuals' movements around the city and consequent interactions using a published ABM: Individual Space-Time Activity-based Model (ISTAM) [ 39, 40].
Comparison of simulations of individual drop motion with experimental measurements proved to be very accurate.
In 2D, the generic index of s ∼ 3 4 is retained as in previous simulations of individual current sheets.
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