The heterogeneous nucleation of gas bubbles from cavities in a surface in contact with a liquid is a widely recognized phenomenon. This process has previously been theoretically analyzed extensively for a conical crevice, although in practice a wide range of cavity geometries might be expected. The method of analysis originally presented by Atchley and Prosperetti [J. Acoust. Soc. Am.86, 10651084 (1989)] for the unstable growth of a gas-liquid interface in a conical crevice is here extended to any axisymmetric cavity geometry and four such different geometries are analyzed. Although the method presented neglects gas transfer, and therefore is most directly suitable for acoustic cavitations, this method is still valuable in comparing the nucleation behavior of different cavity types. It is found that once the interface has emerged outside the cavity, its behavior is determined by the size of the cavity’s opening. Given that the behavior of the interface once it is outside the cavity will also be determined by the local flow conditions, the threshold for unstable growth of the interface inside the cavity leading to its emergence is the important value and will determine differences between cavity geometries in practice, as shown in the examples presented.

1.
Apfel
,
R. E.
(
1970
). “
The role of impurities in cavitation-threshold determination
,”
J. Acoust. Soc. Am.
48
,
1179
1186
.
2.
Atchley
,
A. A.
, and
Prosperetti
,
A.
(
1989
). “
The crevice model of bubble nucleation
,”
J. Acoust. Soc. Am.
86
,
1065
1084
.
3.
Bai
,
H.
, and
Thomas
,
B. G.
(
2001
). “
Bubble formation during horizontal gas injection into a downward flowing liquid
,”
Metall. Mater. Trans. B
32
,
1143
1159
.
4.
Brubakk
,
A. O.
(
2004
). “
Endothelium and bubble injury: The role of endothelium in decompression illness
,”
30th Annual Scientific Meeting of the European Underwater Baromedical Society
, Ajaccio, Corsica, France, EUBS.
5.
Chappell
,
M. A.
, and
Payne
,
S. J.
(
2006
). “
A physiological model of the release of gas bubbles from crevices under decompression
,” Respiration Physiology & Neurobiology,
153
,
166
180
6.
Harvey
,
E. N.
,
Barnes
,
D. K.
,
McElroy
,
W. D.
,
Whiteley
,
A. H.
,
Pease
,
D. C.
, and
Cooper
,
K. W.
(
1944
). “
Bubble formation in animals. I. physical factors
,”
J. Cell. Comp. Physiol.
24
,
1
22
.
7.
Jones
,
S. F.
,
Evans
,
G. M.
, and
Galvin
,
K. P.
(
1999
). “
Bubble nucleation from gas cavities-A review
,”
Adv. Colloid Interface Sci.
80
,
27
50
.
8.
Liger-Belair
,
G.
,
Vignes-Alder
,
M.
,
Voisin
,
C.
,
Robillard
,
B.
, and
Jeandet
,
P.
(
2002
). “
Kinetics of gas discharging in a glass of champagne: The role of nucleation sites
,”
Langmuir
18
,
1294
1301
.
9.
Liger-Belair
,
G.
,
Voisin
,
C.
, and
Jeandet
,
P.
(
2005
). “
Modeling nonclassical heterogeneous bubble nucleation from cellulose fibers: Application to bubbling in carbonated beverages
,”
J. Phys. Chem. B
109
,
14573
14580
.
10.
Sluyter
,
W. M.
,
Slooten
,
P. C.
,
Copraij
,
C. A.
, and
Chesters
,
A. K.
(
1991
). “
The departure size of pool-boiling bubbles from artificial cavities at moderate and high pressures
,”
Int. J. Multiphase Flow
17
,
153
158
.
11.
Tikuisis
,
P.
(
1986
). “
Modeling the observations of in vivo bubble formation with hydrophobic crevices
,”
Undersea Biomed. Res.
13
,
165
180
.
12.
Uzel
,
S.
,
Chappell
,
M. A.
, and
Payne
,
S. J.
(
2006a
). “
A model of the growth, detachment and transport of bubbles in blood vessels
,” IEEE Trans. Biomed Eng. (in reveiw).
13.
Uzel
,
S.
,
Chappell
,
M. A.
, and
Payne
,
S. J.
(
2006b
). “
Modelling the cycles of growth and detachment of bubbles in carbonated beverages
,”
J. Phys. Chem. B
110
,
7579
7586
.
You do not currently have access to this content.