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In this research, the drop test of pear sample was simulated using FEM.
Then, the overall system including source, collimator and sample was simulated for achieving radiographic images of standard samples.
The EPR spectrum of 17O-enriched rutile sample was simulated as a superposition of Ti III)–17O sites and photogenerated ozonide in the rutile matrix.
Each sample was simulated with separate parameter settings estimated from one of the four real human ENCODE samples (e.g. the simulation parameters for A Rep 1 were estimated from HUVEC Rep 1).
The probability of state change is calculated as shown in (2) P → (t + n Δ t ) = Q t n P → t, where P → denotes a vector signifying the state of the calcium channel, Δ t denotes the sampling time of the simulation, and n denotes how many samples ahead we simulate (for this study every time sample was simulated; therefore n = 1).
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The salt rock sample is simulated by bonded particle model implemented in Particle Flow Code (PFC).
The unsteady-flow of water inside the sample is simulated to evaluate the expected permeability for different specimens and compaction.
Crack initiation and propagation in dog-bone sample were simulated for epoxy and clay/epoxy nanocomposites using the eXtended Finite Element Method (XFEM).
A sample of 20,000 cells is taken from the resulting population of cells, the inducer is introduced, and the sample is simulated for another 5 h.
Sampling was simulated through a tessellation stratified design.
The dependence of the ratios of these two components of the G′ mode on the nominal amount of SWCNT and DWCNT in the samples was simulated so that the residual amount of SWCNT in the original DWCNT could be determined.
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