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Handbook of Solvents - George Wypych - ChemTech - Ventech!

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7.2 Bubbles dynamics and boiling 371<br />

Figure 7.2.7. Relative decrement <strong>of</strong> free oscillations <strong>of</strong><br />

air bubble versus concentration <strong>of</strong> POE in water. [By<br />

permission <strong>of</strong> IOP Publishing Limited from W.D.<br />

McComb, and S. Ayyash, J. Phys. D: Appl. Phys., 13,<br />

773, 1980, the reference 39]<br />

Figure 7.2.9. Collapse <strong>of</strong> a bubble near a solid wall in<br />

water (curves 1 and 4) and in dilute POE aqueous solution<br />

(curves 2, 3). [By permission <strong>of</strong> the American Institute<br />

<strong>of</strong> Physics from G.L. Chahine, and D.H. Fruman,<br />

Phys. Fluids., 22, 1406, 1979, the reference 37]<br />

Figure 7.2.8. Geometrical parameters <strong>of</strong> the collapsing<br />

bubble. [By permission <strong>of</strong> the American Institute <strong>of</strong><br />

Physics from G.L. Chahine, and D.H. Fruman, Phys.<br />

Fluids., 22, 1406, 1979, the reference 37]<br />

nomenon observed 40<br />

in ultrasonic<br />

insonification <strong>of</strong> liquid polybutadiene with<br />

molecular massM~10 5 and η p ~10 6 Pas. At<br />

ultrasound frequency f~18 kHz the acoustic<br />

cavitation and well-developed pulsations <strong>of</strong><br />

bubbles were detected, in spite <strong>of</strong> for<br />

low-molecular liquids with so high viscosity<br />

it is completely impossible. 41<br />

For non-spherical bubbles the effect <strong>of</strong><br />

polymeric additives becomes essential at<br />

lower concentrations, as compared to the<br />

spherical bubbles. For example, retardation<br />

<strong>of</strong> the bubble collapse near a solid wall was<br />

observed 37,42 in such concentration interval<br />

where dynamics <strong>of</strong> spherical bubbles has remained<br />

unchanged. In Figures 7.2.8 and<br />

7.2.9 the data 37 are reproduced, where the Rayleigh time, t 0, was chosen for a scaling time,<br />

t R, and for curves 1- 4 R c,max/L = 0.5, 0.56, 1.39, 1.25, respectively. The bubble collapse is<br />

accompanied by generation <strong>of</strong> a microjet towards the wall and addition <strong>of</strong> polymer led to<br />

stabilization <strong>of</strong> the bubble shape and retardation <strong>of</strong> the jet formation. This effect is connected<br />

with the increase in the elongational viscosity <strong>of</strong> a polymeric solution in flow around<br />

collapsing bubble.<br />

The effect <strong>of</strong> polymeric additives on collective phenomena, associated with the dynamics<br />

<strong>of</strong> bubbles, can be illustrated by the example <strong>of</strong> hydrodynamic cavitation, caused by<br />

abrupt decrease in local pressure (in flows around bodies, after stream contraction, in jets).<br />

It has been found that the use <strong>of</strong> polymers permits to decrease the cavitation noise, lower the<br />

cavitation erosion, and delay the cavitation inception. For example, adding a small amount<br />

<strong>of</strong> POE to a water jet issuing from the orifice caused the decrease <strong>of</strong> the critical cavitation<br />

number, κ cr, by 35-40%. 43,44 In experiments with rotating disk 45 the value <strong>of</strong> κ cr was decreased<br />

by 65% with addition <strong>of</strong> 500 ppm POE. Note, however, that these features are<br />

linked not only to the changes in individual bubble dynamics, but to the influence <strong>of</strong><br />

macromolecules on the total flow regime as well. In particular, phenomena listed above are

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