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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 +/-
3 th a latent period, T (the slope), between a critical pressure being reached and the abrupt increase
5 ng flow are recorded simultaneously with the critical pressure drop for the rupture of the membrane.
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
13 cells to generate an initial calculation of critical pressures in a hypothetical spherical cell with
15 regions are clearly differentiated, and the critical pressure is measured at 1.2% error with respect
17 ed to much lower temperatures near a quantum critical pressure of approximately 4.8 GPa where the ant
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
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)
31 ihydrocholesterol have been reported to have critical pressures that are linearly proportional to the
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