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1 method was found to accurately determine the critical pressure (-0.98 +/- 2.47 cm H(2)O vs. -1.07 +/-
2                                         High critical pressures are also seen in binary mixtures of p
3 th a latent period, T (the slope), between a critical pressure being reached and the abrupt increase
4                              The miscibility critical pressures depend on subphase pH and ionic stren
5 ng flow are recorded simultaneously with the critical pressure drop for the rupture of the membrane.
6                                   Changes in critical pressures due to changes in subphase compositio
7 the model gives explicit predictions for the critical pressure for membrane detachment and for the va
8 ing and simplifying the ascertainment of the critical pressure for studies examining the effect of th
9                               The calculated critical pressure for the phase transition and evolution
10 electron-scale turbulence is observed once a critical pressure gradient is exceeded.
11             Nevertheless, the utility of the critical pressure has not yet been realized in the clini
12 can lead to an enhanced cage effect near the critical pressure in supercritical fluid solvents.
13  cells to generate an initial calculation of critical pressures in a hypothetical spherical cell with
14                         The presence of this critical pressure is a manifestation of the crossover fr
15  regions are clearly differentiated, and the critical pressure is measured at 1.2% error with respect
16                                 Upper airway critical pressure measurements correlate with the degree
17 ed to much lower temperatures near a quantum critical pressure of approximately 4.8 GPa where the ant
18                            In this case, the critical pressure of the ternary mixture can be remarkab
19 ixture can be remarkably high, exceeding the critical pressures of the corresponding binary mixtures.
20 r solution theory, we interpret the elevated critical pressures of these mixtures as an attractive in
21                                      Above a critical pressure P ~ 2 GPa, the Shubnikov-de Haas frequ
22 ntravascular pressure (dP/dt) influenced the critical pressure (P(B)) which increases wall permeabili
23 ed frogs, we assessed wall strength from the critical pressure, PB, which has to be applied within th
24 erature TC of MnP sharply increases near the critical pressure PC approximately 8 GPa, which is in go
25 the ground electronic state of Fe(2+) at the critical pressure Pc of the spin transition close to T =
26 e magnetotransport in fine detail around the critical pressure, Pc approximately 10 GPa, in a diamond
27  collapsibility of the hypotonic airway, the critical pressure (Pcrit) and nasal resistance upstream
28  inspiratory airflow (Vimax), the pharyngeal critical pressure (Pcrit) and the nasal resistance (Rn)
29                               The pharyngeal critical pressure (Pcrit) of older obese rats was signif
30  pressure, pi, is lower than the miscibility critical pressure, pi(c).
31 ihydrocholesterol have been reported to have critical pressures that are linearly proportional to the
32                                      Above a critical pressure, the well-defined mobility separation
33 s per level were sufficient to determine the critical pressure with a minimum of variability.

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