Acoustic device for localized contactless measurement of elastic and dissipative non-linearities and viscoelasticity

1. A localized and contactless acoustic measuring device to measure elastic and dissipative non-linearities and viscoelasticity of a sample, the device comprising:

a tank operably taking up the sample;

an emitter of a low-frequency acoustic wave capable of creating a periodic low-frequency variation of a hydrostatic pressure in the sample;

a measurer operably measuring the variation of the hydrostatic pressure due to the low-frequency acoustic wave generated by the emitter;

a generator of high-frequency ultrasound pulses;

a receiver arranged vis-à-vis the generator such that the high-frequency ultrasound pulses having passed through the sample are received and measured by the receiver;

a synchronization equipment to generate a synchronization signal to synchronize the measurements of the high-frequency ultrasound pulses and the variation of the hydrostatic pressure; and

an analysis unit comprising a calculation module to calculate modulations of time of flight and of amplitude of the ultrasound pulses caused by passage of the low-frequency acoustic wave in the sample to quantify the elastic and dissipative non-linearities and the viscoelasticity of the sample.

2. The acoustic measuring device of claim 1 , further comprising a multi-parametric imaging module to generate a representation of viscoelastic effects and of non-linear acoustic elastic effects and dissipative effects.

3. The acoustic measuring device of claim 1 , wherein the emitter of the low-frequency acoustic wave comprises a vibrating pot for resonating a dedicated piston capable of creating the periodic low-frequency variation.

4. The acoustic measuring device of claim 1 , wherein the emitter of the low-frequency acoustic wave comprises an acoustic projector operably creating the low-frequency variation.

5. The acoustic measuring device of claim 1 , wherein the generator of the high-frequency ultrasound pulses and the emitter of the low-frequency acoustic wave are oriented such that propagation directions of the ultrasound pulses and of the low-frequency acoustic wave are perpendicular.

6. The acoustic measuring device of claim 1 , wherein the analysis unit operably instantaneously represents the viscoelasticity and dissipative non-linearities as a function of phases of compression and relief of the periodic low-frequency variation of the hydrostatic pressure.

7. The acoustic measuring device of claim 1 , wherein the analysis unit operably conducts representation of frequential components, zero frequency (order 0), a fundamental resonance frequency (order 1) and a double frequency of a piston (order 2), of the elastic and dissipative non-linearities as a function of an average amplitude of the periodic low-frequency variation of the hydrostatic pressure.

8. A localized and contactless acoustic measuring method to measure elastic and dissipative non-linearities and viscoelasticity of a sample arranged in a tank, the method comprising:

emitting a low-frequency acoustic wave to create a periodic low-frequency variation of a hydrostatic pressure in the sample;

measuring the variation of the hydrostatic pressure due to the low-frequency acoustic wave;

generating high-frequency ultrasound pulses passing through the sample;

receiving and measuring the high-frequency ultrasound pulses having passed through the sample;

synchronizing the measurements of the high-frequency ultrasound pulses and the variation of the hydrostatic pressure; and

calculating modulations of time of flight and of amplitude of the ultrasound pulses caused by passage of the low-frequency acoustic wave in the sample to quantify the elastic and dissipative non-linearities and the viscoelasticity of the sample.

9. The acoustic measuring method of claim 8 , further comprising representing instantaneous values of the viscoelasticity and dissipative non-linearities as a function of phases of compression and relief of the periodic low-frequency variation of the hydrostatic pressure.

10. The acoustic measuring method of claim 8 , further comprising representing frequential components, zero frequency (order 0), a fundamental resonance frequency (order 1) and a double frequency of a piston (order 2), of the elastic and dissipative non-linearities as a function of an average amplitude of the periodic low-frequency variation of the hydrostatic pressure.

11. The acoustic measuring method of claim 8 , further comprising quantifying a level of damage of the sample.

12. The acoustic measuring method of claim 8 , wherein a frequency of the low-frequency acoustic wave is between 2 Hz and 100 kHz, the ultrasound pulses exhibiting a frequency range from 20 kHz to 100 MHz and a firing rate around 10 times greater than the frequency of the low-frequency acoustic wave.

13. The acoustic measuring method of claim 8 , further comprising using an analysis unit to process a sequence resulting from an averaging of 2 to 100 successive firings of trains of the low-frequency acoustic wave.

14. The acoustic measuring device of claim 1 , wherein a wavelength of the low-frequency acoustic wave is greater than a distance between the generator and the receiver.

15. The acoustic measuring device of claim 1 , wherein a wavelength of the low-frequency acoustic wave is greater than a size of the sample in a medium holding the sample.

16. The acoustic measuring device of claim 1 , wherein the sample is placed in (i) fluid media and non-prehensible gels in a mechanical test machine, (ii) media to be protected from external contamination, or (iii) solid media with complex geometries.