Surface and Interfacial Tension
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technique as a function of the alcohol activity for butanol solutions. The arrow indicates the limit of solubility. (From Ref. 80.)

Surface and Interfacial Tension ◽

10.1201/9780203021262-33 ◽

2004 ◽

pp. 116-116

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FIG. 8 Effects of the number of EO units on the dynamic surface tension, γ , vs. bubble surface lifetime, t, curve

Surface and Interfacial Tension ◽

10.1201/9780203021262-34 ◽

2004 ◽

pp. 117-119

Keyword(s):

Surface Tension ◽

Dynamic Surface Tension ◽

Bubble Surface ◽

Dynamic Surface

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(left, t=0.57×10 sec) and without (right, t= 0.37×10 sec) capillary

Surface and Interfacial Tension ◽

10.1201/9780203021262-87 ◽

2004 ◽

pp. 293-293

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FIG. 19 Advancing θ (curve 1),

Surface and Interfacial Tension ◽

10.1201/9780203021262-102 ◽

2004 ◽

pp. 350-353

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FIG. 24 Dependencies of flow rate v on pressure difference ∆P in a hydrophobed quartz capillary, r=3.6 µm, when D-8 solution displaced silicon oil (v>0) and when silicon oil displaced surfactant solution (v<0).

Surface and Interfacial Tension ◽

10.1201/9780203021262-105 ◽

2004 ◽

pp. 358-359

Keyword(s):

Flow Rate ◽

Pressure Difference ◽

Surfactant Solution ◽

Silicon Oil ◽

Quartz Capillary

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FIG. 23 Aqueous core thickness (d)

Surface and Interfacial Tension ◽

10.1201/9780203021262-43 ◽

2004 ◽

pp. 136-138

Keyword(s):

Core Thickness ◽

Aqueous Core

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FIG. 3 Definition of the contact angle θ.

Surface and Interfacial Tension ◽

10.1201/9780203021262-56 ◽

2004 ◽

pp. 168-169

Keyword(s):

Contact Angle ◽

Definition Of

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FIG. 25 Rate of advancing (v>0) and receding (v<0) motion of menisci of CTAB solution in thin quartz capillaries in dependence on pressure difference ∆P. (a) C = 10 M, l=9.28

Surface and Interfacial Tension ◽

10.1201/9780203021262-106 ◽

2004 ◽

pp. 360-360

Keyword(s):

Pressure Difference ◽

Ctab Solution

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FIG. 20 A plot of experimental data from Skripov [6] for the homogeneous boiling of pentane. The part ACB is the normal superheat limit. As the temperature is increased, so the time required for explosive boiling of liquid drops rapidly decreases. In going from 145.6 to 146.0°C, the waiting time drops from 550 to about 0.5 sec. If the superheated liquid droplets are exposed to radiation, very much lower superheats are needed to cause bubble nucleation. Temperatures as low as 129.5°C can cause bubble formation.

Surface and Interfacial Tension ◽

10.1201/9780203021262-161 ◽

2004 ◽

pp. 542-545

Keyword(s):

Experimental Data ◽

Waiting Time ◽

Bubble Formation ◽

Bubble Nucleation ◽

Superheated Liquid ◽

Liquid Droplets ◽

Liquid Drops ◽

Explosive Boiling ◽

Time Required ◽

Superheat Limit

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of the v(∆P) data (curve 1) and using air bubble method (curve 2).

Surface and Interfacial Tension ◽

10.1201/9780203021262-108 ◽

2004 ◽

pp. 362-363

Keyword(s):

Air Bubble

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