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After mathematic modeling, the obtained equations must be solved to simulate the column.
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Three-dimensional turbulent Navier-Stokes equations are solved to simulate freestream-jet interactive flowfields.
Poisson Boltzmann model is solved to simulate the flow by the finite element method.
Reynolds averaged Navier Stokes equations (RANS) are solved to simulate the flow past a circular cylinder.
The full Navier Stokes equations for airflow are solved to simulate the forced convection cooling in the electronic module.
Non linear, non-stationary heat conduction partial differential equations were solved to simulate the freezing of pouches, using a computational program in finite elements coded by the authors.
The Reynolds-averaged Navier-Stokes equations with the k-ε turbulence model were solved to simulate both steady and unsteady states of the inflows.
The distribution functions for flow, temperature, and concentration fields are solved to simulate the regeneration process of diesel particulate filter (DPF).
The hydrologic model considers major processes of the water cycle through physically based governing equations, which are solved to simulate the propagation of water in each of these processes.
In addition to such a measurement strategy, the population balance equations were solved to simulate the time variations of the CSD, and used to identify nucleation and growth kinetic parameters.
Finally, the system of differential equations has to be solved to obtain the simulated data.
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