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Several rheological signatures of phase transition were found.
The optical band gaps, defined as the onset of the π π* transition, were found to be 1.15 eV for PFETQ, 1.2 eV for PFMTQ and 1.34 eV for PFTQ.
On this basis, the effects of capillarity and back-diffusion on dendrite fragmentation during mushy zone solidification, as well as the effects of back-diffusion and cooling rate on the prediction of the microstructure transition, were found.
The linear mechanical properties above the glass rubber transition were found to be drastically enhanced for all three of the nanocomposites as compared to the neat polypropylene matrix, and these effects were attributed to a mechanical coupling between the polypropylene crystallites and filler/filler interactions.
Nonnative hydrogen bonds in a simulation on the helix-coil transition were found to be most populated around the transition temperature [29].
Cells at the light-to-dark transition were found in various stages of the cell cycle including approximately 50% in early G1, 10% in late G1, 25% in S, and 15% in G2/M [17].
Similar(52)
A 4-state HMM topology with one skip transition was found to be appropriate.
The transition was found to be highly cooperative and two-state-like.
The bubbly-to-slug flow transition was found to be dependent on axial locations.
This transition was found to be reversible, when temperature fluctuated between 70 and 4 °C.
The transition is found to occur in the range 300 K–500 K.
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