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Shear scale

There is a wide variety of impellers usiu fluidfoil principles, which are used when flow from the impeller is predominant in the process requirement aud macro- or micro-scale shear rates are a subordinate issue. [Pg.1623]

Fig. 22. Radius of drops produced by capillary breakup (solid lines) and binary breakup (dotted lines) in a hyperbolic extensional flow for different viscosity ratios (p) and scaled shear rate (p,cylo) (Janssen and Meijer, 1993). The initial amplitude of the surface disturbances is ao = 10 9 m. Note that significantly smaller drops are produced by capillary breakup for high viscosity ratios. Fig. 22. Radius of drops produced by capillary breakup (solid lines) and binary breakup (dotted lines) in a hyperbolic extensional flow for different viscosity ratios (p) and scaled shear rate (p,cylo) (Janssen and Meijer, 1993). The initial amplitude of the surface disturbances is ao = 10 9 m. Note that significantly smaller drops are produced by capillary breakup for high viscosity ratios.
The convective turbulence tend to dissipate large scale shears (wave length a > pressure scale height H ). The rate of dissipation... [Pg.191]

We further propose that studies of coupled systems such as major orogen-scale shear zones and coeval basins permit previously unavailable interpretations of the history of surface elevation. In addition, approaches that integrate surface processes (sedimentation and erosion... [Pg.110]

Rabin Y, Ottinger HCh (1990) Dilute polymer solutions internal viscosity, dynamic scaling, shear thinning, and frequency-dependent viscosity. Europhys Lett 13(5) 423—428 Rallison JM, Hinch EJ (1988) Do we understand the physics in the constitutive equation J Non-Newton Fluid Mech 29(l) 37-55... [Pg.249]

With 0.05 jLim latex particles in a glycerol-salt solution, large-scale shear aggregates have been shown to have the same fractal dimension as that of Brownian aggregates (i.e.. Dp = 1.8 0.1) when the shear rate is less than 1500/sec [88]. Due to shear allegation, the aggregation rate for these experiments was much faster than that of comparative Brownian aggregation rates. [Pg.487]

Figure 6. Transient scaled shear stress after flow reversal for the PBLG sample ... Figure 6. Transient scaled shear stress after flow reversal for the PBLG sample ...
At the macroscopic scale, shear localization flow in the alloy develops during initial increments of deformation. Softening and globularization of structure in the macro shear band lead to realization of deformation at mesoscopic scale. In this case the mesoscopic scale deformation is determined by cooperative grain boundary sliding leading to superplastic flow. Superplastic flow results in deformation accumulation in the central area of the sample and impedes in structure transformation in periphery regions. [Pg.407]

Figure 11.27 Deformation maps of (a) a nonnucleated PP/EPR with 15% EPR and (b) its p-nucleated counterpart for different temperatures and crack-tip loading rates as deduced from the fracture surfaces of compact tension specimens. A rough indication of the test speed is provided by the upper scale. ( ) shearing, ( ) shearing and crazing, (A) multiple crazing, and (X) single craze. (From Reference 32 with permission from Springer Science and Business Media.)... Figure 11.27 Deformation maps of (a) a nonnucleated PP/EPR with 15% EPR and (b) its p-nucleated counterpart for different temperatures and crack-tip loading rates as deduced from the fracture surfaces of compact tension specimens. A rough indication of the test speed is provided by the upper scale. ( ) shearing, ( ) shearing and crazing, (A) multiple crazing, and (X) single craze. (From Reference 32 with permission from Springer Science and Business Media.)...
For drops smaller than the Kolmogoroff length scale, shear forces rather than periodic inertial forces dominate the break-up mechanism and theoretically ... [Pg.308]

The RlOO (Figure 12.4) draws the most power and has the highest micro-scale shear rate. [Pg.330]

Recently, one of the most practical results of these studies has been the ability to design pilot plant experiments (and, in many cases, plant-scale experiments) that can establish the sensitivity of process to macro-scale mixing variables (as a function of power, pumping capacity, impeller diameter, impeller tip speeds, and macro-scale shear rates) in contrast to micro-scale mixing variables (which are relative to power per unit volume, RMS velocity fluctuations, and some estimation of the size of the micro-scale eddies). [Pg.332]

The shear rates are expressed in units of. The scaled shear rate, being a product of the true shear rate and the relevant relaocation time, is also referred to as Deborah-number . Instead of the ratio Tap/ro, the parameter... [Pg.303]

Figure 8.4 Fluctuations measured in the sheared region of the velocity profile. Scaled mean squared displacements in (a) flow direction and (b) gradient direction plotted against the scaled shear rate, (c) Velocity autocorrelation function in the flow and gradient direction. Different colours represent measurements made at different positions (shear rate) along the mean velocity profile shown in Figure 8.3c. Open symbols represent data in gradient direction while filled symbols represent data in the flow directions. Dashed lines in (a) and (b) are of slopes of 1 (i.e., diffusive motion) and dashed line in (c) is of slope 7/2 (i.e., a faster decay). (Adapted from Rycroft, C.H. et al., Phys. Rev. E, 80,031305, 2009 Orpe, A.V. et al., Europhys. Lett., 84, 64003, 2008.)... Figure 8.4 Fluctuations measured in the sheared region of the velocity profile. Scaled mean squared displacements in (a) flow direction and (b) gradient direction plotted against the scaled shear rate, (c) Velocity autocorrelation function in the flow and gradient direction. Different colours represent measurements made at different positions (shear rate) along the mean velocity profile shown in Figure 8.3c. Open symbols represent data in gradient direction while filled symbols represent data in the flow directions. Dashed lines in (a) and (b) are of slopes of 1 (i.e., diffusive motion) and dashed line in (c) is of slope 7/2 (i.e., a faster decay). (Adapted from Rycroft, C.H. et al., Phys. Rev. E, 80,031305, 2009 Orpe, A.V. et al., Europhys. Lett., 84, 64003, 2008.)...

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See also in sourсe #XX -- [ Pg.1086 ]




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