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Cell boundaries were modelled as a reflective 2.5 µm × 0.4 µm rectangular.
Sedimentation boundaries were modelled as numerical finite element solutions of the Lamm equation using c(s) analysis.
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High-angle grain boundaries are modeled as those containing grain boundary dislocations with small Burgers vectors.
The amount of sorbed time on the boundaries is modeled as a random variable that can vary over a wide range of values.
The grain boundaries are modeled as disclination dipole walls with energies given as a weighted sum of individual disclination energies determined from special low-sigma structures, elastic terms and disclination core energies.
Responses with values that are outside the boundary are modeled as a continuous function.
The grain boundaries and surface layers are modeled as initially impenetrable to dislocations while allowing for relaxation at a critical stress level.
We consider a slug moving in a slit microchannel (w⪢h) and flow field in a plane far from the boundary walls is modelled as a two-dimensional low-Reynolds-number flow (Stokes flow).
The remaining boundaries, air-agarose, and air-plastic, were modeled as Robin boundary conditions to accommodate the possibility of adsorption-desorption reactions at the boundary.
We modeled the floor as concrete (i.e., relative permitivity of 7.5, and conductivity of 0.12 Siemens per meter), whereas the walls and ceiling were modeled as perfectly absorbing boundaries.
The TT and SR membranes were modeled as reflective, no-flux, boundaries, ∂ΩN2 in Fig. 6.
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