The results show that the model reasonably describes the interactions between the gas and particle phases in dense flows.
A power law analytical model reasonably describes the variation of energy release rate with delamination and energy absorbed.
By comparison with the laboratory scale experimental measurements on the co-gasification process, it is shown that the developed model reasonably describes the thermodynamic features of the co-gasification process and, thus, provides a useful tool for the analysis of this process.
As an illustration, we find that a 4-component normal mixture model reasonably describes the birthweight distribution for a population of white singleton infants born to heavily smoking mothers.
The reduced-order model can reasonably describe different particle size variation modes for different initial particle sizes in different temperature ranges.
Results show that the current three dimensional gasification model can reasonably describe the reacting flow behavior in the supercritical water fluidized bed reactor, which may provide a convenient and low-cost way for the reactor design and optimization.
OUR predictions with the calibrated model could reasonably describe the OUR profile after pulse addition of acetate, i.e., the OUR transiently reached a very high level, and then increased gradually to a maximum level until the initial substrate was taken up for storage and biomass growth.
pcVPC plots demonstrated that the final model could reasonably describe the central tendency as well as the variability of all PK data.
If animal data are available, these can be utilised within the model to ensure the distribution is reasonably described or the physicochemical properties of the compound can be used to guide the selection of a predictive model ((31– 33), personal communication from Iain Gardner).
Results from experiments revealed that the oxidation behavior could be reasonably described using new model and the energy providing can be calculated by following equation: W= 1.56×1014 η(d2/V)C0EQ2(1+1+(V lnK /(3.63×1013 η2d2Q2C0E)).
