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Volume functions

The surfaces in Fig. 4(d,e,f,) obtained from the functional (1) are the surfaces already discovered by Schoen [28] and named by him O, C-TO, I-WP, F-RD. O, C-TO is the only structure which cannot be minimized with respect to the cell length. For all the structures except this one we are able to find the minimal cell length i.e., by varying the cell length we are able to find the length for which the free energy per unit volume (functional (1)) has a minimum. The O, C-TO structure collapses to I-WP when the cell... [Pg.705]

The kinetics of alkaline hydrolysis of an ester can be followed by the pH-stat method, in which the pH is held constant by adding a solution of strong alkali to the reacting ester solution. The volume of alkali added in order to keep the pH constant is recorded as a function-time. Find the volume function needed to determine the rate constant that is, given the volume-time data for this type of experiment, what plot or calculation will yield the rate constant ... [Pg.57]

Fig. 9. Upper (parallel model) and lower (series model) bounds for the microhardness of a two-component composite as function of crystalline volume function. Hardness expressed as H/Hc for Hc/H = 120... Fig. 9. Upper (parallel model) and lower (series model) bounds for the microhardness of a two-component composite as function of crystalline volume function. Hardness expressed as H/Hc for Hc/H = 120...
Conversion Formulas. Often no convenient experimental method exists for evaluating a derivative needed for the numerical solution of a problem. In this case we must convert the partial derivative to relate it to other quantities that ate readily available. The key to obtaining an expression for a particular partial derivative is to start with the total derivative for the dependent variable and to realize that a derivative can be obtained as the ratio of two differentials [8]. For example, let us convert the derivatives of the volume function discussed in the preceding section. [Pg.13]

These illustrations, which are based on the example of the volume function, are typical of the type of conversion that is required so frequently in thermodynamic manipulations. [Pg.15]

The volume function then is homogeneous of the first degree, because the parameter X, which factors out, occurs to the first power. Although an ideal solution has been used in this illustration. Equation (2.31) is true of all solutions. However, for nonideal solutions, the partial molar volume must be used instead of molar volumes of the pure components (see Chapter 9). [Pg.19]

As we have seen previously, the volume function is known from experience to be homogeneous of the hrst degree that is, if we double the number of moles of each component, we also double the total volume. In other words, a homogeneous... [Pg.20]

Equation (5.51) states that the particular temperature-volume function shown is constant during a reversible adiabatic expansion. Hence we can write... [Pg.93]

A particularly simple case is shown in Figure 18.1, in which the volume is a linear function of the mole number of glycolamide in a kilogram of water. In this case, the partial molar volume of solute is constant and is equal to the slope of the line. The partial molar volume represents the effective volume of the solute in solution, that is, the increase in volume per mole of solute added. From Equation (9.27), written for the volume function. [Pg.408]

After 2 h of ozone exposure, there was a significant change (p < 0.05) in Fvc, KMF, and airway resistance (Raw) Several other measures (feVi, Vjq, and V35) were lower after 2 h of exposure, but the statistical significance was borderline. However, after 4 h of exposure, all flow measures were significantly decreased, compared with controls. After 4 h, increased, FVC decreased further, and feV decreased significantly. Residual volume, functional residual capacity, and total lung volume did not change as a result of the ozone exposure. [Pg.407]

Fig. 5 Generation of linear features bv particles of filler (XlZOOl. Volume function of filler - 0.05. Crack propagated from top to bottom. Fig. 5 Generation of linear features bv particles of filler (XlZOOl. Volume function of filler - 0.05. Crack propagated from top to bottom.
In both equations, Dw is the solute diffusion coefficient in pure water, rs is the molecular radius of the solute, ls is its characteristic size, Vw is the water free volume, Mc is the molecular weight between crosslinks in the amorphous phase, Mn is the number average molecular weight of the polymer before crosslinking, M is the minimum value of Mc below which the solute cannot diffuse, 4>(V) is the free volume function mentioned earlier, and k3 is a constant. [Pg.172]

As Eqs. (66) and (67) involve integration of the function Qt(7) over an experimentally nonrealizable region 0 < T < Te, the authors have given a method for the required extrapolation using reduced temperature-volume functions. [Pg.79]

P T] = meshgrid(linspace(Pstart,Pend,N),1inspace(Tstart,Tend,N)) z = realgas(P,T,om,Pc,Tc) °/, evaluate volume function... [Pg.126]

By definition only one phase can be present at any point r e R3. It is further required that the set P, c IR3, P, = f ff) — 1 be a compact set, i.e., that the inter-phase boundaries are smooth in the mathematical sense. In a discrete form, the phase function f becomes the phase volume function which assigns... [Pg.140]

In a practical implementation, the domain on which the phase volume functions are specified is typically a cubic grid of Nx x Ny x Nz voxels, which corresponds to real dimensions of Lx — hNx, Ly - hNy, and Lz — hNz, where h is the voxel size. We will further call this region of real space the computational unit cell. The relationship between the unit cell and the multiphase medium of interest depends on the absolute dimensions of the medium and on the spatial resolution at which the medium is represented (feature dimensions). The unit cell can either contain the entire medium and some void space surrounding it, as in the case of virtual granules described in Section IV.D below, or be a sample of a much larger (theoretically infinite) medium, as in the case of transport properties calculation, described in Section II.E below. [Pg.141]

Let us introduce the VOF method in more detail. The phase volume function fi(r) is defined by/) = 1 in phase 1 and f x — 0 in phase 2 cf. Eq. (1). A discrete analog of the phase volume function fx is the scalar field tpi known as the volume fraction (or area fraction in spatially 2D cases). It represents the fraction of the volume of the voxel with size h and the coordinate of its center r filled with the phase 1,... [Pg.163]

Fitting of ki2 using different EOS (PR with volume correction (PRc r), SRK, PR with modified volume function (PR )) and pure prediction using UNIFAC model with scaling factor... [Pg.268]

Recently, new classes of proteins that are responsible for the homeostasis of copper and for its delivery to specihc intracellular targets have been identified. Copper cannot be present as the free ion in solution as its high reactivity leads to the production of radicals. It appears always to be bound to some proteins and is present as copper(I) due to the reducing conditions of the cell environment. Small soluble proteins, called copper chaperones (see chapter by Elam et al., this volume), function to shuttle copper to specihc target proteins. Other large, membrane-bound proteins are present to pump copper from one cell compartment to another. [Pg.437]

All the static lung volumes and capaeities except FRC and RV can be measured directly through use of a simple spirometer (an apparatus traditionally consisting of a cylindrical bell immersed in water and equipped with outlets that a person can breathe into, or inhale from, to measure expiratory or inspiratory volumes). Functional residual capacity and RV are measured indirectly by using several alveolar gas dilution techniques. [Pg.315]

Several possible forms exist for the disruption terms, Bd and Dd- The most tractable form is the two-body equation volume function. It is assumed that one particle breaks into two smaller equal volume particles... [Pg.110]

Deposition in the thoracic region is the sum of aerodynamic and thermodynamic deposition of particulate material. Aerodynamic deposition depends on aerodynamic particle size, total volumetric flow rate, anatomical dead space, tidal volume, functional residual capacity (FRC) (combined residual and expiratory reserve volume or the amount of air remaining in the lungs after a tidal expiration) and diameter of the airways. Thermodynamic deposition depends on anatomical and physical characteristics, such as tidal volume, anatomical dead space, functional residual capacity and the transit time of air within each region. Thermodynamic particle size, which is derived from the diffusion coefficient, particle shape factor and the particles mass density, influence thermodynamic deposition. [Pg.262]

Stocks J, Quanjer PH. Reference values for residual volume, functional residual capacity and total lung capacity. ATS Workshop on Lung Volume Measurements. Official statement of the European Respiratory Society. Eur Respir J 1995 492-506. [Pg.94]

Curro et al. [1981] followed a similar procedure in studies of the aging kinetics of poly(methyl methacrylate) (PMMA). For predicting the shift factors of aging experiments at 23°C, the authors computed from PVT the free-volume function, h = h P, V), and then substituted these into Doolittle s equation (6.63). The resulting prediction agreed with the experimental values, contrasting with the inadequacy of the WLF relation. Next, the polymer aging process was modeled as a diffusion of free volume [Curro et al., 1982]. [Pg.265]


See other pages where Volume functions is mentioned: [Pg.605]    [Pg.57]    [Pg.128]    [Pg.195]    [Pg.141]    [Pg.141]    [Pg.266]    [Pg.287]    [Pg.180]    [Pg.81]    [Pg.407]    [Pg.209]    [Pg.36]    [Pg.36]    [Pg.96]    [Pg.120]    [Pg.540]    [Pg.261]    [Pg.10]    [Pg.167]    [Pg.174]    [Pg.595]    [Pg.729]   
See also in sourсe #XX -- [ Pg.196 , Pg.215 ]




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Composition, copolymer, function retention volume

Departure Functions with Temperature, Molar Volume and Composition as the Independent Variables

Entropy as a function of temperature and volume

Excess functions heat, volume)

Filler volume fraction modulus, function

Free-volume autocorrelation function

Functional Foods: Biochemical and Processing Aspects, Volume

Indicator function volume

Lung volume measurement, functional

Lung volumes functional residual capacity

Mayer -function and excluded volume

Modulus as Function of Filler Volume Fraction

Molecular weight retention volume, function

Muscle Function volume

Partition function per unit volume

Physiological functions volume regulation

Polymer volume fraction function

Pores volume distribution function

Retention corrected volume, function

Volume In radius distribution function

Volume as a function of conversion

Volume as a function of time

Volume distribution functions

Volume relaxation function

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