Bjerknes force and bubble levitation under single-bubble sonoluminescence conditions

Journal of the Acoustical Society of America

Volumn 102, Issue 3, 1997, Pages 1522-1527

  Matula, Thomas J ^a   Cordry, Sean M ^a,b   Roy, Ronald A ^a,c   Crum, Lawrence A ^a  

^a UNIVERSITY OF WASHINGTON   (United States)

^b YORK COLLEGE OF PENNSYLVANIA   (United States)

^c BOSTON UNIVERSITY   (United States)

Author keywords

[No Author keywords available]

Indexed keywords

ACOUSTICS; ARTICLE; CALCULATION; FORCE; MATHEMATICAL ANALYSIS; MEASUREMENT; PRESSURE; PRIORITY JOURNAL;

EID: 0030768711     PISSN: 00014966     EISSN: None     Source Type: Journal    
DOI: 10.1121/1.420065     Document Type: Article

References (23)

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18. The bubble actually translates vertically during an acoustic cycle. This is due to a change in the buoyancy and Bjerknes force with a change in the bubble's volume. In our work we simply average over an acoustic cycle, and do not consider the instantaneous position of the bubble.
19. B. P. Barber, C. C. Wu, R. Löfstedt, P. H. Roberts, and S. J. Putterman, "Sensitivity of sonoluminescence to experimental parameters," Phys. Rev. Lett. 72, 1380 (1994).
20. The hydrophone calibration is discussed in S. M. Cordry, "Bjerknes forces and temperature effects in single-bubble sonoluminescence," Ph.D. thesis, University of Mississippi, 1995.
21. S. M. Cordry, "Bjerknes forces and temperature effects in single-bubble sonoluminescence," Ph.D. thesis, University of Mississippi, 1995.
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23. M. Longuet-Higins (private communication).