Exact(9)
Using the simulation we could see that with an increase in heat transfer, thermal plume by the effect of buoyancy filled the entire region of the channel.
From this simulation, we could estimate a deposition rate of about 0.059 Å shot−1.
By means of simulation, we could model and evaluate different delivery strategies, which allowed us to extract reasonable cost values.
By overall analysis of docking results, predicted activity, and molecular dynamics (MD) simulation, we could conclude that Tetrahydropalmatine, Reserpiline, and -Corydaline had better binding affinity than the control.
Because we knew the exact chromosomal location each read was sampled from in the simulation, we could unambiguously compute the true abundance of each repetitive element.
With our first simulation, we could rule out the possibility that the convergence was the result of simple linear decay of neural responses.
Similar(51)
In the simulations, we could basically confirm the sheath waves propagating along the metal plasma interface at the frequencies lower than those of normal wave modes for uniform plasma with no external magnetic field.
From the simulations, we could evaluate a value of 2.8×10−13 cm2/s for the solid-state diffusion coefficient of lithium in Li1−δMn2O4 particles, a value of 5.5×10−8 cm/s for the standard heterogeneous rate constant, and a value of 0.30 for the transfer coefficient α.
By the aid of MD simulations we could detect the existence of conserved water molecules into the GABA (occluded) and tiagabine (open-to-out) binding sites, respectively.
Also, using stepwise docking simulations, we could identify DDX3X-CRM-1 interface and its critical functional residues.
Through extensive simulations, we could determine the probability of detecting transcripts with a certain expression level at a given sampling stage, which provides important implications for future experimental design.
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Justyna Jupowicz-Kozak
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