Abstract:Abstract.While the protein folding problem on lattices is known to be NP-hard, we prove in this paper that lattice protein structures of size n matching specific lists of O(n) distance constraints can be determined in linear time on 2D honeycomb, 2D square, 3D diamond and 3D CUM]C lattices.
“…Present generation models are limited to liquid fuels in the form of pools (i.e., a defined amount of fuel constrained in a pool with fixed, known geometry) and spills onto non-absorbing substrates. (See Martinez and Hopkins [67] for a model of fuel spill in a porous medium.) Although the form of the submodel will allow first order estimates of fire growth rates, data acquired to date (Saito et al [68]) tend to show that relevant flame spread mechanisms include features which occur at lengths scales several orders of magnitude below the resolution of present grids.…”
PrPrandtl number, the ratio of viscous and thermal diffusivities
ReReynolds number, the ratio of inertial and viscous forces
ScSchmidt number, the ratio of viscous and mass diffusivities
“…Present generation models are limited to liquid fuels in the form of pools (i.e., a defined amount of fuel constrained in a pool with fixed, known geometry) and spills onto non-absorbing substrates. (See Martinez and Hopkins [67] for a model of fuel spill in a porous medium.) Although the form of the submodel will allow first order estimates of fire growth rates, data acquired to date (Saito et al [68]) tend to show that relevant flame spread mechanisms include features which occur at lengths scales several orders of magnitude below the resolution of present grids.…”
PrPrandtl number, the ratio of viscous and thermal diffusivities
ReReynolds number, the ratio of inertial and viscous forces
ScSchmidt number, the ratio of viscous and mass diffusivities
“…Present generation models are limited to liquid fuels in the form of pools (i.e., a defined amount of fuel constrained in a pool with fixed, known geometry) and spills onto non-absorbing substrates. (See Martinez and Hopkins [65] for a model of fuel spill in a porous medium.) Although the form of the submodel will allow first order estimates of fire growth rates, data acquired to date (Saito et al [66]) tend to show that relevant flame spread mechanisms include features which occur at lengths scales several orders of magnitude below the resolution of present grids.…”
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PrPrandtl number, the ratio of viscous and thermal diffusivities
ReReynolds number, the ratio of inertial and viscous forces
ScSchmidt number, the ratio of viscous and mass diffusivities
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