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Coefficient of shear

An explicit expression for the coefficient of shear viscosity can be obtained by assuming the system is in local themiodynamic equilibrium and using the previously derived expression for X and v. Thus we obtain... [Pg.675]

We notice, using (A3.1.20) and (A3.1.26), that this method leads to a simple relation between the coefficients of shear viscosity and themial conductivity, given by... [Pg.675]

In order to make this a direct relationship a proportionality factor is introduced, which is called the coefficient of shear viscosity or simply viscosity. [Pg.73]

The first equation of the set (9.62) confirms that rj is the coefficient of shear viscosity, which can be estimated according to the rule... [Pg.192]

Pokrovskii VN, Kruchinin NP, Danilin GA, Serkov AT (1973) A relation between coefficients of shear and extensional viscosity for concentrated polymer solutions. Mechanika Polymerov 1 124-131 (in Russian)... [Pg.249]

Polystyrene Solutions 23—300 MHz. Moore et al. (85,86) obtained complex moduli data in the range of 23-300 MHz by measuring the complex reflection coefficient of shear waves reflected from a solid-liquid interface. The measurements were performed for solutions of polystyrene in dibutyl phthalate over the concentration range of 3-20 Vol.-% (86). The result is shown in Fig. 4.4 where (rf — v1 rjs)/ (t] - vt rjs) is plotted against f(t] — v1 f]s) M/cR T, vx being the volume fraction of the solvent and / the frequency in Hz. It is seen that the... [Pg.54]

Argon matrix reactions of alkali-metal atoms with F2 have been studied, using laser Raman and i.r. spectroscopy. The F—F stretching motion in the F2 ion occurs at ca. 460 cm compared with 892 cm" for the neutral molecule the latter band is very close to that for the gaseous molecule, and this fact clearly shows that intermolecular fluorine bonding is very feeble. Absolute measurements of the coefficient of shear viscosity of compressed liquid F2 at 90—300 K and for pressures up to 20 MPa and of saturated liquid F2 at 70—144 K have been reported. ... [Pg.395]

Some plastic engineers nse the term Coefficient of shear sensitivity, relating it to a ratio of viscosity of a hot melt at 100 s to that at 1000 s However, this coefficient is based on two experimental points only and often is much less reliable compared to the power-law index. In fact, this coefficient is related to the power-law... [Pg.651]

The basic equations of motion contain coefficients of shear viscosity for the fluids. This gives rise to a dependency of porosity diffusion on the rate of fluid transmission through the pore space. In low viscosity cases such as crustal fluids in deep interconnected fracture networks, transmission is relatively rapid in reservoirs largely saturated with viscous oil, transmission of pressure effects can be quite slow. For a 10,(XX) cP oil filling 88% of the pore space of a 30% porosity 2-3 Darcy sand, it took about 5 weeks to see a substantial response at distances of 300 m from the excitation well which was being aggressively pulsed at the right frequency (Spanos et al., 2003). [Pg.518]

EVOLUTION OF THE VISCOSITY COEFFICIENT OF SHEARING OF THE GLYCEROL AND ITS ESTERS WITH ACETIC ACID AS A FUNCTION OF PRESSURE. [Pg.143]

While polymers are typically pseudoplastic, most oxide glasses are Newtonian, at least for the typical (low) strain rates employed in common forming operations. For a Newtonian liquid confined between two parallel plates, the lower one of which is stationary whilst the upper moves at a constant velocity Vo, the distance between them remaining constant, the liquid velocity is zero at the surface of the lower plate and varies linearly with distance between the plates. A shear stress r must be supplied to the upper plate to maintain this motion and the coefficient of shear viscosity ry, or simply viscosity, is the relation between the applied stress and the velocity gradient dv/dy ... [Pg.142]

The kinetic theory of gases attempts to explain the macroscopic nonequilibrium properties of gases in terms of the microscopic properties of the individual gas molecules and the forces between them. A central aim of this theory is to provide a microscopic explanation for the fact that a wide variety of gas flows can be described by the Navier-Stokes hydrodynamic equations and to provide expressions for the transport coefficients appearing in these equations, such as the coefficients of shear viscosity and thermal conductivity, in terms of the microscopic prop>erties of the molecules. We devote most of our attention in this article to this problem. [Pg.65]

Here A is called the coefficient of thermal conductivity, rj the coefficient of shear viscosity, and the coefficient of bulk viscosity p(r,t) is the local... [Pg.96]

Here we will not go through the detailed calculations that lead to the Enskog theory values for the transport coeflicients of shear viscosity, bulk viscosity, and thermal conductivity appearing in the Navier-Stokes hydro-dynamic equations. Instead we shall merely cite the results obtained and refer the reader to the literature for more details. One finds that the coefficient of shear viscosity 17 is given by ... [Pg.128]

Here rjo and Aq are the coefficients of shear viscosity and thermal conductivity as given by the Boltzmann equation, and x=x(n(r, t)), where the local density... [Pg.128]

The simplest way to determine the effective hard-sphere diameter d of the fluid molecules at temperature T and the corresponding value of x ts to fit exp( the experimental value for the coefficient of shear viscosity at low density, to the theoretical formula for hard-sphere molecules. That is, d is determined by using the first Sonine polynomial approximation to 17 for a gas of hard spheres [Eq. (115a)],... [Pg.129]

As a result of the secular growth of the /-body collision integrals with time, we are compelled to conclude that, although the cluster expansion method can be used successfully to derive the Boltzmann equation from the liouville equation and to obtain corrections to the Boltzmann equation, there are serious difficulties in trying to represent these corrections as a power series in the density. An example of the difficulties that appear if one attempts to apply the generalized Boltzmann equation as it stands now to a problem of some interest is provided by the calculation of the density expansion of the coefficient of shear viscosity. By constructing normal solutions to the generalized Boltzmann equation, one finds that the viscosity 17 has the expansion of the form mentioned in Eq. (224),... [Pg.157]

Similar results have been obtained for the time correlation functions that determine the coefficients of shear viscosity, thermal conductivity, and bulk viscosity for a pure system. That is, they all decay exponentially for short times and as for long times, i.e.. [Pg.168]

The states a < 5, may be called the hydrodynamic states since they are associated with the conserved variables of number density, longitudinal and transverse components of the current, and kinetic energy. The other two states, correspond to the stress tensor and heat current, respectively. Therefore, the diagonal matrix elements involving these states must be related to the transport coefficients of shear viscosity and thermal conductivity as is well known in conventional transport theory. We will see below that these elements are important in formulating kinetic models. Besides the matrix elements shown in Table 1, we will include one additional element, namely. [Pg.206]

In fact, two expressions of this type are very well known, the Stokes-Einstein law for the self-diffusion coefficient, and the Debye law for the rotational diffusion coefficient. Both of these laws for the appropriate diffusion coefficient D are derived by hydrodynamics and have Darj, where 17 is the coefficient of shear viscosity, a transport coefficient. The Stokes-Einstein and Debye laws were reconciled with formal theory with the use of mode-mode... [Pg.267]


See other pages where Coefficient of shear is mentioned: [Pg.450]    [Pg.675]    [Pg.267]    [Pg.61]    [Pg.162]    [Pg.233]    [Pg.359]    [Pg.168]    [Pg.272]    [Pg.372]    [Pg.4]    [Pg.254]    [Pg.255]    [Pg.158]    [Pg.4]    [Pg.677]    [Pg.570]    [Pg.664]    [Pg.675]    [Pg.158]    [Pg.156]    [Pg.374]    [Pg.66]    [Pg.95]    [Pg.104]    [Pg.160]    [Pg.277]   
See also in sourсe #XX -- [ Pg.156 ]




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Non-Newtonian shear viscosity and first normal stress coefficient of polymer melts

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