The differences between dosimetric parameters for various breathing phases were small and their expected clinical impact is consequently quite small.
Thus, the application is limited to P T conditions at which we can assume that no additional phases are appearing, or that the molar amounts of newly appearing phases are small.
The results show that the differences in axial velocity between the two phases are small and the axial RMS velocities generally increases with increasing volume fraction and are larger for the dispersed phase compared to the continuous phase.
The estrogen effect appears to be highly specific to the damaged site because the differences in most EIMD markers (CK, soreness, and low-frequency fatigue) between the two menstrual cycle phases were small.
Although the relative phases were small at all velocities, the pattern of change between velocities was different for the case and control subjects, and different from the C7-sacrum and T8-sacrum relative phases seen in the present study and reported in the literature [ 13, 29].
This phase is small and runs parallel on the guest programme and calculates the data required by the monitoring process.
The crystal size change of β phase is small, and the defolding of the β lamellae triggers the β to α phase transformation.
When the η phase is small, it has no obvious influence on mechanical properties, but η phase becomes the crack initiation site with the further growth of η phase.
