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Viscosity droplet

Generally, the occurrence of a specific mode is determined by droplet impact properties (size, velocity, temperature), surface properties (temperature, roughness, wetting), and their thermophysical properties (thermal conductivity, thermal capacity, density, surface tension, droplet viscosity). It appeared that the surface temperature and the impact Weber number are the most critical factors governing both the droplet breakup behavior and ensuing heat transfer. I335 412 415]... [Pg.225]

Fig. 8. Ink droplet viscosity gain mechanism on a heated substrate. Fig. 8. Ink droplet viscosity gain mechanism on a heated substrate.
While the ink droplet spreads up to 105 jtrm when no heat is supplied to the substrate, spreading is very hmited once the substrate is heated — the droplet viscosity increases and the spreading is limited accordingly. Most wide format printers, aimed to print on a variety of commercially available substrates, are using the "heated substrate" technology on flat-bed printers as well as on drum or roll printers. [Pg.87]

We chose the acidic polymer as the interior member of the capsule forming pair due to the expected compatibility with cells of acidic polysaccharides such as alginate and carboxymethyl cellulose. For this reason, droplet viscosity and, therefore, stability was improved by synthesizing the acidic polymers as higher molecular weight analogues of the corresponding polybases. [Pg.179]

Above this value, oscillations induced on the free surface are stable, while below this value, it is possible to induce instability on the surface and form droplets. Viscosity caimot prevent the instability, but it does increase the acceleration necessary to cause the instability to appear. In the equation of motion (6), acceleration due to gravity, g, also acts to stabilize the interface. There are different ways to destabilize the surface, the simplest of which is to i/>(f) to a constant value above g + dipiAjK), forming a gravity wave. Other ways include harmonic excitation with where i = W is the ampli-... [Pg.2761]

Theories that take into account the droplet viscosity 0 or use different boundary conditions will result in somewhat different results. Drop phase viscous effects should be negligible compared to film phase viscous effects if O/y L/6 where L is some characteristic length measure of the drop dimensions (say the undeformed radius). Since L/6 1, the above theory has a wide range of practical application. [Pg.576]

Fig. 7.65 Effect of binder mass fraction in the sprayed droplets (droplet viscosity) on the agglomeration rate of glass particles. Fig. 7.65 Effect of binder mass fraction in the sprayed droplets (droplet viscosity) on the agglomeration rate of glass particles.
Only minor differences can be found in the shapes of the collision complex as shown in Fig. 1.12. In the Newtonian case, the minimum thickness of the lamella is 4.8 pm, while in shear-thinning case the thickness of the lamella is 5.6 pm. A comparison of the velocity fields shows almost no difference. The evolution of the droplet viscosity for the Newtonian collision as well as the maximum, minimum, and mean droplet viscosity for the shear-thinning collision is shown in... [Pg.19]

Fig. 1.13 Evolution of the mean and minimum droplet viscosity for the case We = 766 [11]... Fig. 1.13 Evolution of the mean and minimum droplet viscosity for the case We = 766 [11]...
Fig. 1.13. The shear-thinning viscosity is significantly reduced at the beginning when the droplet collides with its mirror image. Subsequently, it rises during the expansion of the rim and drops again when the rim contracts. The effective viscosity which leads to the same droplet collision complex diameter is the same as the mean droplet viscosity of the shear-thinning case at the moment shortly after the collision. This implies the fact that relatively small region of high shear rates and reduced viscosity at the beginning of the collision is more important than the mean viscosity during the collision. The reason for this phenomenon can be seen in Fig. 1.14 and is explained as follows ... Fig. 1.13. The shear-thinning viscosity is significantly reduced at the beginning when the droplet collides with its mirror image. Subsequently, it rises during the expansion of the rim and drops again when the rim contracts. The effective viscosity which leads to the same droplet collision complex diameter is the same as the mean droplet viscosity of the shear-thinning case at the moment shortly after the collision. This implies the fact that relatively small region of high shear rates and reduced viscosity at the beginning of the collision is more important than the mean viscosity during the collision. The reason for this phenomenon can be seen in Fig. 1.14 and is explained as follows ...

See other pages where Viscosity droplet is mentioned: [Pg.156]    [Pg.208]    [Pg.368]    [Pg.410]    [Pg.76]    [Pg.246]    [Pg.32]    [Pg.143]    [Pg.536]    [Pg.400]    [Pg.659]    [Pg.237]    [Pg.273]    [Pg.360]    [Pg.692]    [Pg.435]    [Pg.69]    [Pg.81]    [Pg.87]   
See also in sourсe #XX -- [ Pg.328 ]




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