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At 450 °C, diffusion zones thicknesses were 4 μm (MSS) and 6 μm (SMSS).
When this value is reached at any depth of the diffusion zone, two distinct diffusion zones will appear.
This classification has strong engineering implication and can give a more rational division of convection and diffusion zones of chloride ion transport.
However, after removal of the thin nitride layers, the toughened diffusion zones were revealed, being uniformly distributed through the entire sample area.
In essence, a model based on the concept of planar diffusion zones can only work just because it is not based on a flux balance.
Accordingly, non-steady-state and steady-state distribution functions are deduced, depending on the system parameter characterizing the finite diffusion zones.
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Besides the head surface interaction, in this work, the effects of surfactant diffusivity, bulk concentration, the length of diffusion zone and surfactant architecture on the adsorption kinetics are also considered.
Reaction zone and reaction-diffusion zone and diffusion zone in the course of the reaction progression.
Local internal stress states in the diffusion zone are estimated.
Both layers grow over a nitrogen diffusion zone in ferrite.
AZD2563 disk diffusion zone diameters were generally 2-3 mm smaller than the corresponding linezolid zone diameters.
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