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The destruction experiments & Introduction to cavitation Sheng-Chieh Lu (盧聖介) and Chih-Kuang Yeh (葉秩光) Ultrasound Imaging Laboratory Department of Biomedical Engineering and Environmental Sciences, National Tsing Hua University

The destruction experiments & Introduction to cavitationmx.nthu.edu.tw/~ckyeh/classnotes/seminar/9512506.pdf · The destruction experiments & Introduction to cavitation Sheng-Chieh

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  • The destruction experiments & Introduction to cavitation

    Sheng-Chieh Lu () and Chih-Kuang Yeh ()

    Ultrasound Imaging LaboratoryDepartment of Biomedical Engineering and Environmental

    Sciences, National Tsing Hua University

  • OUTLINE

    Review for molecular imageDestruction experiments of liposomesIntroduction to cavitationApplications of cavitationDiscussions & ConclusionsFuture worksReference

  • Molecular imaging by ultrasound

    Molecular imaging is to SEE the specific tissue at molecular level

    Red blood cell

    Specific molecule

    Ultrasound transducer

    Targeted agent

    Too tiny to see

    Small vessel or capillary

  • Liposomes as UCAscz = Mismatch impedance

    11c22c echo signal

    incident ultrasound

    hydrophile side

    anti-hydrophile side

    Lipid-dissolved

    Lipid-dissolvedBi-layer structure

    Diameter of Liposomes< 1 um

  • B-scan setup

    A 25-MHz transducer (13-mm focal length, 0.5-inch aperture) was aligned at a motion stage and focused on a vessel in phantom

    B-mode scan, sample rate 120-MHz, width 4-mm, depth 4-mm

    Motion Controller

    5900PR

    PCI-6602

    Trigger

    Position

    A/D

    Clock

    RF

    Diameter = 2.4 mm

    TransducerB-modescan

    Diplexer

  • Properties of air liposomes

    Low buffer temperature Proper vortex time (~120 seconds)Effective working time is about 10 min

  • Destruction experiments of liposomes

  • Setup for destruction

    Motion Controller

    5900PR

    PCI-6602

    Trigger

    Position

    A/D

    Clock

    RFCase 1Pressure: No

    Case 2Sine wave 5 cyclesPressure: 0.4 MPa

    Case 3Sine wave 5 cyclesPressure: 1.8 MPa

    25 MHz transducer

    B-modescan

    WaveGenerator

    33120

    Diameter = 2.4 mm

    PowerAmplifier

    Trigger

    Sine wave

    Pulse

    2.25 MHz transducer

    Diplexer

  • Results of destruction

  • Images of dstructionNon-pressure 0.4 MPa 1.8 MPa

    1st min

    110th sec

    3rd min

    10th min

  • SpectrumNon-pressure 0.4 MPa 1.8 MPa

  • Spectrum

  • Short conclusions & discussions

    The acoustic pressure threshold of destruction of liposomes is below 0.4 MPa at 2.25 MHz central-frequency.It is observed that some broadband signals in high frequency.

  • Introduction to cavitation

  • Cavitation phenomenon

    Inertial cavitation was first studied by Lord Rayleigh in the late 19th century.

    When a volume of liquid is subjected to a sufficiently low pressure it may rupture and form a cavity. This phenomenon is termed cavitation inception.

    May occur behind the blade of a rapidly rotating propeller or on any surface vibrating underwater with sufficient amplitude and acceleration.

  • Cavitation phenomenon

    Shrimp light phenomenon Francis turbine, cavitation damage

  • Animation of cavitation

    High Pressure

    Low Pressure

    Acoustic shock wave

    Acoustic shock wave

    High Temperature, several thousand kelvins

  • Two types of cavitation

    Cavitation is generally classified into two typesstable cavitation and inertial cavitation

    stable cavitation inertial cavitation

  • Setup for detecting IC & SC

  • Signals of SC & IC

    (a) typical background noise level

    (b) stable cavitation. (c) inertial

    cavitation. (d) both inertial and

    stable cavitation.

  • Broadband signal of liposomes

    Non-pressure 0.4 MPa 1.8 MPa

  • Applications of cavitation

  • Gene transfection with ultrasound

    Micro bubblePlasmid DNA

    Exterior

    Interior

    Plasmid DNA

    Exterior

    Interior

    Cell membrane

    Cell membrane

  • Other applicationsAlthough cavitation is undesirable in many circumstances, but not always the case.

    Supercavitating torpedoes the torpedo in a large bubble of cavitation. By greatly reducing contact with water, these torpedoes can go faster.

    Ultrasonic cleaning.

    Water purification

    In industry, cavitation is often used to homogenize.

  • Discussions & Conclusions

    Threshold of the experiment to induce cavitation?It is almost sure that liposomes will be destructed under burst pulses at 1.8 MPa in pressure.From spectrum, broadband was found and as well a peak at 12.5 MHz. Is that peak a sub-harmonic of 25 MHz pulse?From destruction, we observe the broadband noise caused by inertial cavitation.

  • Future works

    Substitute microbubble UCAs with liposomes to produce cavitationexperiment includes:Determine the threshold Gene transfection experiment

  • Reference

    O. Couture et al. (2006) Ultrasound in Med. & Biol., 32:73-82

    S. H. Huang et al. (2001) Journal of Pharmaceutical Sciences, 90:1917-1926.

    C. K. Yeh et al. (2006),9th Western Pacific Acoustics Conference, Seoul, Korea.

    Paul A. Dayton et al. (2002) Journal of magnetic resonance imaging 16:362377.

  • THANK YOU!

    The destruction experiments & Introduction to cavitationOUTLINEMolecular imaging by ultrasoundLiposomes as UCAsB-scan setupProperties of air liposomesDestruction experiments of liposomesSetup for destructionResults of destructionImages of dstructionSpectrumSpectrumShort conclusions & discussionsIntroduction to cavitationCavitation phenomenonCavitation phenomenonAnimation of cavitationTwo types of cavitationSetup for detecting IC & SCSignals of SC & ICBroadband signal of liposomesApplications of cavitationGene transfection with ultrasoundOther applicationsDiscussions & ConclusionsFuture worksReferenceTHANK YOU!