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These results illustrated that competitive adsorption behaviour was due to the greater maximum surface pressure (2.05 times) and diffusivity (19.6 times) of Triton X−100 than BSA.
The maximum surface pressure achieved using RcLPS (45 mN m 1; Figure 2) is similar to that from monolayers of P. aeruginosa smooth LPS (52 mN m 1).
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The results indicated increasing feed stress, and/or increasing roll friction lead to higher maximum roll surface pressure and attendant relative density at the exit.
This upper limit is still several times higher than the maximum possible surface pressure of the carbon dioxide, meaning that the measurements place essentially no constraints on parameters of the atmosphere.
It is also shown that the maximum rise in surface pressure under shut-in condition which is of the order of a fraction of one ppg, is approximately equivalent to the decrease in static bottomhole pressure under open condition.
The maximum increase in surface pressure induced by the adsorption of the peptide was defined as the difference between the initial pressure (πi) and the plateau value.
The performance of zigzag flow channels is evaluated in terms of maximum surface temperature, temperature uniformity and pressure drop.
From these assumptions, it is possible to obtain the surface pressure, horsepower requirements, maximum quantity of propping agent needed and also the productivity ratio.
surface tension (γ cmc), CMC, efficiency in surface tension reduction (C20), maximum surface excess (Γcmc), occupied area per molecule (A cmc) and surface pressure (Πcmc) at the CMC have been estimated for G16.
The maximum surface heat transfer coefficient strongly depended on inlet pressure.
The pulmonary surfactant formulation incubated with the control solvent (n-decane) reached a mean surface pressure of 71 mN/m at maximum compression (Fig. 2).
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