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Average bulk’ pressure

FIG. 20 (a) Density profiles p(z) vs z for e = —2 and four average bulk densities (f> as indicated, (b) Surface excess vs density in the bulk for four choices of e. (c) Profiles for the diagonal components of the pressure tensor and of the total pressure for (p = l.O and e = —2. Insert in (c) shows the difference between P, and Px to show that isotropic behavior in the bulk of the film is nicely obtained, (d) Interfacial tension between the polymer film and the repulsive wall vs bulk density for all four choices of e. Curve is only a guide for the eye [18]. [Pg.598]

In these experiments, the measured helium flux through the membrane was less than the flux predicted on the basis of the average bulk concentrations. Consequently, the helium permeability coefficients calculated from observed membrane flux and the bulk partial pressures are lower than the pure gas values obtained by the membrane supplier or independently by us. At the same time, observed nitrogen coefficients are higher than predicted. [Pg.22]

Fluid properties are evaluated at the average bulk temperature. Heat transfer and fluid friction inside the tubes are evaluated with the hydraulic diameter method discussed in Chap. 6. Pressure drop is calculated with the chart friction factor / and the following relation ... [Pg.561]

Ha = absolute viscosity of fluid at average bulk temperature or absolute viscosity of air at temperature and pressure of surroundings, lb/(sXft) or lb(hXft)... [Pg.575]

Figure 6.3 GCEMC results for the disjoining pressure /(s ) [see Eq. (5.57)] for a typical polar (Stockmayer) fluid as a function of the wall separation (data have been obtained at T = 1.60, m — 2.0, and p = -19.30 corresponding to an average bulk density p 0.6). Also shown are corresponding results for an atomic LJ (12,6) fluid at the same temperature and bulk density. Figure 6.3 GCEMC results for the disjoining pressure /(s ) [see Eq. (5.57)] for a typical polar (Stockmayer) fluid as a function of the wall separation (data have been obtained at T = 1.60, m — 2.0, and p = -19.30 corresponding to an average bulk density p 0.6). Also shown are corresponding results for an atomic LJ (12,6) fluid at the same temperature and bulk density.
Figure 6.8 Order parameter Pi as a function of the external parallel (bulk) pressure (a) and of the average density (b) for the confined system at Sx = 7.0 ( ) and the bulk system (O). Figure 6.8 Order parameter Pi as a function of the external parallel (bulk) pressure (a) and of the average density (b) for the confined system at Sx = 7.0 ( ) and the bulk system (O).
An air-water vapor mixture flows upward through a vertical copper tube of 25.4 mm OD, 1.65 mm wall thickness, which is surrounded by flowing cold water. As a result, water vapor condenses and flows as a liquid film down the inside of the tube. At one point in the condenser, the average velocity of the gas is 10 m/s, its bulk-average temperature is 339 K, the pressure is 1 atm, and the bulk-average partial pressure of water vapor is 0.24 atm. The film of condensed liquid is such that its heat-transfer coefficient is 6.0 kW/m2-K. The cooling water is at a bulk-average temperature of 297 K and has a heat-transfer coefficient of 0.57 kW/m2-K. Calculate the local rate of condensation of water from the airstream. For the gas mixture, Cp= 1.145 kJ/kg-K, Sc = 0.6,... [Pg.152]

From the studies conducted on dysprosium, the average bulk modulus is calculated to be 36 2 GPa and the pressure derivative of bulk modulus is given as 3.5 0.5. The third order Birch-Mumaghan fit is given by Eq. (1), where X=(Vo/V). [Pg.304]

Still accounts for the perceived spatial averaging effect, since the pad bulk pressure response is computed by the Boussinesq integral (Eqn (6.21)), which is a spatial... [Pg.157]

Figure lb. Average fluid density vs. pore size for different bulk pressures (T=195.5 K). [Pg.690]

We integrate the force balance equation in the volume of a prism of the same section S but smaller height i, < L, summing over all ionic and neutral species /, For central forces in the average over the surface S the pair interactions are cancelled out exactly. At the plane L these forces will contribute to the bulk pressure P. The statement of dynamic balance is that... [Pg.141]

Capacitive sensors are employed to measure the dew point temperature of gas in the flow chamber. Accurate empirical correlations exist between dew point temperatures and water vapor pressures. If the characteristic diffusion time for water in the gas is short compared to both the turnover time of gas in the flow chamber and the characteristic timescale for water transport through the bulk membrane, then the water vapor pressure of the outlet stream, equals the average vapor pressure in the flow chamber, P". [Pg.373]

When the total pressures at the two ends of the pore are different, there will be bulk flow. If conditions for Knudsen diffusion exist, then tbe molar average bulk flow velocity (v ) may be estimated from... [Pg.101]

Most importantly for computational viscoelastic fluid mechanics, most of the charmel DNS calculations are not performed for a constant flux (which would have naturally resulted in a constant bulk Reynolds number) but for a constant pressure drop per unit length that results in a constant zero shear rate friction Reynolds number. These runs lead to substantial variations in the (instantaneous and average) bulk Reynolds number from which the drag reduction needs to be estimated. Knowing roughly the relationship between the friction and the average bulk Reynolds number for a Newtonian fluid (from the experimentally determined and DNS confirmed empirical relationships for the skin friction factor - see, for example. Ref [34]), one can extract such a relationship that also takes into account the already mentioned (in Section 1.2) shear thinning effect in association with viscoelastic results [78]. [Pg.18]


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See also in sourсe #XX -- [ Pg.26 ]




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