Suppression and Separation of Interactive Acoustic Modes in a Fluid-Filled Resonator
A method and an apparatus for systematic suppression and separation of interactive acoustic modes within a liquid-filled spherical resonator are described. The method and apparatus allow for augmenting the response and acoustic energy of liquid-filled spherical shell resonators. In some aspects, manipulation of acoustic resonant modes is used to achieve desirable conditions. The response of a system can be influenced by one or more of the interactive modes, which are more sensitive to a change in the speed of sound. This is attained in some cases by changing parameters, which are a function of the speed of sound in a liquid medium, such as, temperature and pressure.
1 . A method for controlling an acoustic field in a cavitation resonance chamber, comprising:
coupling at least one acoustic driver to at least one corresponding location on a body of a cavitation resonance chamber;
driving said at least one acoustic driver with an electrical driving signal;
simultaneously exciting a plurality of acoustic modes in said body of said resonance chamber; and
altering a first characteristic frequency of a first acoustic mode of said body of said resonance chamber relative to a second characteristic frequency of a second acoustic mode of said body of said resonance chamber.
2 . The method of claim 1 , altering said first characteristic frequency relative to said second characteristic frequency comprising altering a property of a fluid within said body of said resonance chamber.
3 . The method of claim 2 , altering said property of said fluid comprising altering a speed of sound of said fluid.
4 . The method of claim 3 , altering said speed of sound comprising altering a temperature of said fluid.
5 . The method of claim 3 , altering said speed of sound comprising altering a static pressure of said fluid.
6 . The method of claim 1 , further comprising determining eigenfrequencies applicable to said plurality of acoustic modes.
7 . The method of claim 6 , further comprising altering a sound speed of a fluid within said body of said resonance chamber so as to match a first and second eigenfrequency corresponding to respective first and second modes at a given sound speed of said fluid.
8 . The method of claim 1 , further comprising providing a static fluid pressure greater than atmospheric pressure within said body of said resonance chamber.
9 . The method of claim 1 , further comprising causing acoustic cavitation within a fluid within said body of said resonance chamber.
10 . The method of claim 1 , further comprising monitoring for cavitation activity within a fluid within said body of said resonance chamber.
11 . The method of claim 10 , said monitoring comprising observing using a photon detector.
12 . The method of claim 10 , comprising application of pulse-echo steps to indicate the presence of a cavitation bubble within said fluid.