Encapsulated contrast microbubble radial oscillation associated with postexcitation pressure peaks
This work combines modeling and experiment to assess encapsulated microbubble oscillations associated with broadband pressure peaks detected after microbubble excitation (postexcitation signals). Data were acquired from albumin-shelled and phospholipid-shelled microbubbles using a passive cavitation...
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| Published in: | The Journal of the Acoustical Society of America Vol. 127; no. 2; pp. 1156 - 1164 |
|---|---|
| Main Authors: | , , , , , |
| Format: | Journal Article |
| Language: | English |
| Published: |
Melville, NY
Acoustical Society of America
01-02-2010
American Institute of Physics |
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| Abstract | This work combines modeling and experiment to assess encapsulated microbubble oscillations associated with broadband pressure peaks detected after microbubble excitation (postexcitation signals). Data were acquired from albumin-shelled and phospholipid-shelled microbubbles using a passive cavitation detector consisting of a confocally aligned 2.8-MHz transmitter and 13-MHz receiver. Microbubbles in weak solutions were insonified with a 5-cycle pulse at a peak rarefactional pressure of
2.0
±
0.2
MPa
. For each microbubble type, at least 100 received signals were identified as individual-microbubble responses. The average broadband noise from signals with postexcitation response was 4.2-7.2 dB higher than from signals without postexcitation. Pressure-time responses for each microbubble type were simulated using the model by
Marmottant
[
J. Acoust. Soc. Am.
118
,
3499-3505
(
2005
)]
, with insonification conditions matching the experiment. Increased broadband noise predicted for microbubbles with postexcitation response was consistent with that observed experimentally (4.0-8.9 dB). The model predicted that postexcitation signals occur only when the radial oscillation exceeds both the shell break-up threshold and twice the initial radius (free bubble inertial cavitation threshold). |
|---|---|
| AbstractList | This work combines modeling and experiment to assess encapsulated microbubble oscillations associated with broadband pressure peaks detected after microbubble excitation (postexcitation signals). Data were acquired from albumin-shelled and phospholipid-shelled microbubbles using a passive cavitation detector consisting of a confocally aligned 2.8-MHz transmitter and 13-MHz receiver. Microbubbles in weak solutions were insonified with a 5-cycle pulse at a peak rarefactional pressure of 2.0±0.2 MPa. For each microbubble type, at least 100 received signals were identified as individual-microbubble responses. The average broadband noise from signals with postexcitation response was 4.2–7.2 dB higher than from signals without postexcitation. Pressure-time responses for each microbubble type were simulated using the model by
Marmottant et al. [J. Acoust. Soc. Am. 118, 3499–3505 (2005)]
, with insonification conditions matching the experiment. Increased broadband noise predicted for microbubbles with postexcitation response was consistent with that observed experimentally (4.0–8.9 dB). The model predicted that postexcitation signals occur only when the radial oscillation exceeds both the shell break-up threshold and twice the initial radius (free bubble inertial cavitation threshold). This work combines modeling and experiment to assess encapsulated microbubble oscillations associated with broadband pressure peaks detected after microbubble excitation (postexcitation signals). Data were acquired from albumin-shelled and phospholipid-shelled microbubbles using a passive cavitation detector consisting of a confocally aligned 2.8-MHz transmitter and 13-MHz receiver. Microbubbles in weak solutions were insonified with a 5-cycle pulse at a peak rarefactional pressure of 2.0 ± 0.2 MPa . For each microbubble type, at least 100 received signals were identified as individual-microbubble responses. The average broadband noise from signals with postexcitation response was 4.2-7.2 dB higher than from signals without postexcitation. Pressure-time responses for each microbubble type were simulated using the model by Marmottant [ J. Acoust. Soc. Am. 118 , 3499-3505 ( 2005 )] , with insonification conditions matching the experiment. Increased broadband noise predicted for microbubbles with postexcitation response was consistent with that observed experimentally (4.0-8.9 dB). The model predicted that postexcitation signals occur only when the radial oscillation exceeds both the shell break-up threshold and twice the initial radius (free bubble inertial cavitation threshold). This work combines modeling and experiment to assess encapsulated microbubble oscillations associated with broadband pressure peaks detected after microbubble excitation (postexcitation signals). Data were acquired from albumin-shelled and phospholipid-shelled microbubbles using a passive cavitation detector consisting of a confocally aligned 2.8-MHz transmitter and 13-MHz receiver. Microbubbles in weak solutions were insonified with a 5-cycle pulse at a peak rarefactional pressure of 2.0+/-0.2 MPa. For each microbubble type, at least 100 received signals were identified as individual-microbubble responses. The average broadband noise from signals with postexcitation response was 4.2-7.2 dB higher than from signals without postexcitation. Pressure-time responses for each microbubble type were simulated using the model by Marmottant et al. [J. Acoust. Soc. Am. 118, 3499-3505 (2005)], with insonification conditions matching the experiment. Increased broadband noise predicted for microbubbles with postexcitation response was consistent with that observed experimentally (4.0-8.9 dB). The model predicted that postexcitation signals occur only when the radial oscillation exceeds both the shell break-up threshold and twice the initial radius (free bubble inertial cavitation threshold). This work combines modeling and experiment to assess encapsulated microbubble oscillations associated with broadband pressure peaks detected after microbubble excitation (postexcitation signals). Data were acquired from albumin-shelled and phospholipid-shelled microbubbles using a passive cavitation detector consisting of a confocally aligned 2.8-MHz transmitter and 13-MHz receiver. Microbubbles in weak solutions were insonified with a 5-cycle pulse at a peak rarefactional pressure of 2.0±0.2 MPa. For each microbubble type, at least 100 received signals were identified as individual-microbubble responses. The average broadband noise from signals with postexcitation response was 4.2–7.2 dB higher than from signals without postexcitation. Pressure-time responses for each microbubble type were simulated using the model by Marmottant et al. [J. Acoust. Soc. Am. 118, 3499–3505 (2005)], with insonification conditions matching the experiment. Increased broadband noise predicted for microbubbles with postexcitation response was consistent with that observed experimentally (4.0–8.9 dB). The model predicted that postexcitation signals occur only when the radial oscillation exceeds both the shell break-up threshold and twice the initial radius (free bubble inertial cavitation threshold). |
| Author | King, D. A. Foiret, J. Haak, A. Santin, M. D. O'Brien, W. D. Bridal, S. L. |
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| Cites_doi | 10.1016/j.ultrasmedbio.2006.07.015 10.1109/58.883539 10.1109/TUFFC.2007.272 10.1121/1.388622 10.1088/0031-9155/51/4/003 10.1016/j.ultrasmedbio.2007.04.018 10.1016/j.ultrasmedbio.2006.07.008 10.1121/1.2109427 10.1121/1.398328 10.1080/02656730701194131 10.1016/S0301-5629(03)01051-2 10.1016/S0894-7317(99)70096-9 10.1121/1.2346132 10.1097/00004424-200011000-00003 10.1109/58.741536 10.1016/j.ultrasmedbio.2007.03.009 10.1016/j.jconrel.2006.12.015 10.1016/j.ultrasmedbio.2006.06.020 10.1109/TUFFC.2006.1588398 10.1016/j.ultrasmedbio.2003.12.002 10.1121/1.380799 10.1097/01.rli.0000199292.88189.0f 10.1109/TUFFC.2006.1610573 10.1109/58.896136 10.1016/j.ultrasmedbio.2007.05.011 |
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| Copyright | 2010 Acoustical Society of America 2015 INIST-CNRS Copyright © 2010 Acoustical Society of America 2010 Acoustical Society of America |
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| Keywords | Radial vibration Bubble Contrast media |
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| SubjectTerms | Albumins Algorithms Bioacoustics Biological and medical sciences Cardiovascular system Computer Simulation Contrast Media Fluorocarbons Humans Investigative techniques, diagnostic techniques (general aspects) Medical sciences Microbubbles Models, Theoretical Periodicity Phospholipids Pressure Sulfur Hexafluoride Time Factors Ultrasonic investigative techniques Ultrasonics |
| Title | Encapsulated contrast microbubble radial oscillation associated with postexcitation pressure peaks |
| URI | http://dx.doi.org/10.1121/1.3277216 https://www.ncbi.nlm.nih.gov/pubmed/20136236 https://search.proquest.com/docview/733401467 https://pubmed.ncbi.nlm.nih.gov/PMC2852442 |
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