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On the inner L shell boundary (L = 1.2), E2 and b1 were set to zero.
All edges around the shell boundary are simply supported by adhesive flexible films.
Similarly, Christensen (2015) find Ganymede-like drivens driven by iron snow with a stably stratified layer below the outer shell boundary; R m≈500 in his optimal simulation.
This survey is complemented by the S14 dataset focusing on low Ekman, low magnetic Prandtl number simulations: 3×10−7≲E≲10−6, 0.05≤P m≤1, and 108≲R a≲1010 with χ=0.35, an isothermal inner shell boundary, and fixed heat flux on the outer shell boundary.
Gradient-based optimization is then used to locate the wing structure that maximizes the thrust, or minimizes the power under a thrust constraint, for a variety of shell boundary conditions.
For the liquid contained in the shell, boundary conditions are prescribed and the behaviour of the liquid is expressed by a potential function.
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As for a possible improvement, we should take shell boundaries and anisotropic pressures for exotic stars into account.
By using the infinite fluid-loaded shell Green's tensor, the system of partial differential equations governing the shell displacement and the radiated sound pressure is reduced to a system of integral equations along the shell boundaries.
Core and shell boundaries were determined based on visual inspection of relative density of NeuN immunoreactivity staining and position relative to anatomical landmarks (anterior commisure, islands of Calleja and lateral ventricles).
A forward BEM transformation matrix was calculated based on the spatial configuration of EEG electrodes, information from a three-shell boundary element model (BEM) and the location of dipole seeds on the reconstructed surface.
The shell's boundary was fixed at its end.
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