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Thus, the role of anharmonic effects or phonon decay is important as enhanced pressures as well temperatures allows a change in volume or dimensions.
In addition to soot volume fraction, time-resolved scattering measurements yielded particle diameters and number densities; all these give insight into both surface growth and coagulation at enhanced pressures.
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The simulation by Tanaka et al. (2010) reproduces sudden magnetic field depression (explosive growth phase after Ohtani et al. (1992)) and sudden enhancement of the Region 2 (R2) FAC due to enhanced pressure in the inner boundary of the plasma sheet invoked by the highspeed plasma flow from the plasma sheet at the substorm onset.
This compensating effect is an enhanced pressure, designated by π and called osmotic pressure.
A growth in Δ 2 3 and Δ 3 3 and decay in with enhanced pressure is witnessed with enhanced pressure till phase-transition pressure.
Starting from zero pressure, normalized heat capacity decreases gradually with enhanced pressure in B1 phase.
Both compression and shear waves increases with enhanced pressure in B2 structure.
It is noticed that with enhanced pressure, θ D decreases in B3 phase for SiC.
The fluid impacts on the substrate, resulting in enhanced pressure [40].
This figure also suggests that with enhanced pressure, the increase of α th.exp.exp
Thus, G V decreases as C 44 decreases with enhanced pressure in ZnS phase.
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