ライフサイエンスコーパス: critical pressure

1 fluctuations increase near the liquid-liquid critical pressure.

2 y fluctuations at pressures proximate to the critical pressure.

3 method was found to accurately determine the critical pressure (-0.98 +/- 2.47 cm H(2)O vs. -1.07 +/-

4 At a critical pressure, A( ) and superconducting transition t

5 s followed by highly cooperative uptake at a critical pressure, above which adsorption rapidly approa

6 is anticipated as a function of temperature, critical pressure and temperature, and acentric factor.

7 Near the critical pressure and temperature, Gamma(s) becomes sign

8 tracted throat, the relationship between the critical pressure and the elastic modulus/particle-throa

9 Molecular weight, critical pressure, and critical temperature of solvents

10 High critical pressures are also seen in binary mixtures of p

11 th a latent period, T (the slope), between a critical pressure being reached and the abrupt increase

12 mpression due to octahedral tilting, and the critical pressure can be tuned by the A-site cation.

13 The miscibility critical pressures depend on subphase pH and ionic stren

14 diameter ratio shows a greater impact on the critical pressure difference than the elastic modulus of

15 ng flow are recorded simultaneously with the critical pressure drop for the rupture of the membrane.

16 Changes in critical pressures due to changes in subphase compositio

17 the model gives explicit predictions for the critical pressure for membrane detachment and for the va

18 termed isoreticular curves that relates the critical pressure for pore condensation (alpha), gravime

19 ing and simplifying the ascertainment of the critical pressure for studies examining the effect of th

20 The calculated critical pressure for the phase transition and evolution

21 electron-scale turbulence is observed once a critical pressure gradient is exceeded.

22 Nevertheless, the utility of the critical pressure has not yet been realized in the clini

23 can lead to an enhanced cage effect near the critical pressure in supercritical fluid solvents.

24 cells to generate an initial calculation of critical pressures in a hypothetical spherical cell with

25 The presence of this critical pressure is a manifestation of the crossover fr

26 We have unambiguously shown that (1) this critical pressure is associated with the onset of cavita

27 regions are clearly differentiated, and the critical pressure is measured at 1.2% error with respect

28 Upper airway critical pressure measurements correlate with the degree

29 ed to much lower temperatures near a quantum critical pressure of approximately 4.8 GPa where the ant

30 the Neel-ordered phase breaks down beyond a critical pressure of P(c) ~ 1.0 GPa through a continuous

31 The pore-scale modelling obtains the critical pressure of the DMP for different particle-thro

32 In this case, the critical pressure of the ternary mixture can be remarkab

33 ixture can be remarkably high, exceeding the critical pressures of the corresponding binary mixtures.

34 r solution theory, we interpret the elevated critical pressures of these mixtures as an attractive in

35 Above a critical pressure P ~ 2 GPa, the Shubnikov-de Haas frequ

36 ntravascular pressure (dP/dt) influenced the critical pressure (P(B)) which increases wall permeabili

37 ed frogs, we assessed wall strength from the critical pressure, PB, which has to be applied within th

38 erature TC of MnP sharply increases near the critical pressure PC approximately 8 GPa, which is in go

39 the ground electronic state of Fe(2+) at the critical pressure Pc of the spin transition close to T =

40 e magnetotransport in fine detail around the critical pressure, Pc approximately 10 GPa, in a diamond

41 collapsibility of the hypotonic airway, the critical pressure (Pcrit) and nasal resistance upstream

42 inspiratory airflow (Vimax), the pharyngeal critical pressure (Pcrit) and the nasal resistance (Rn)

43 The pharyngeal critical pressure (Pcrit) of older obese rats was signif

44 pressure, pi, is lower than the miscibility critical pressure, pi(c).

45 ihydrocholesterol have been reported to have critical pressures that are linearly proportional to the

46 Above a critical pressure, the well-defined mobility separation

47 trary, we have observed a material-dependent critical pressure value above which a sudden decrease in

48 s per level were sufficient to determine the critical pressure with a minimum of variability.