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The features of this second regime appear as new phenomena.
The second regime occurs at high activation energies and sufficiently large heat release values.
Second regime involves slow growth of the graphitic layers and slow improvement of their stacking order.
The second regime is characterized by a rapid deterioration of contrast.
The second regime is mainly dominated by crack initiation and propagation.
It is in the second regime that fractal geometry can be used most effectively to control the array sidelobes.
In particular, the adsorption in second regime displays a power-law time dependence with an exponent unrelated to bulk concentrations and diffusion coefficients.
During the second regime, however, no more RAP is observed, indicating that the new lamellae that appear during this stage are nearly individual and not forming lamella stacks.
It is found that middle and top impellers reach their second regime at a much higher gas flow rate than single or bottom impellers under the same conditions.
For the first regime, the water transport in the air layer is diffusion driven, in the second regime it is of a convective nature.
Both carbon monoxide and carbon dioxide can be formed in the first regime, but carbon monoxide can only be formed in the second regime.
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