IP Library › Granted Patent US 12,510,513
Granted Patent B2
US 12,510,513 · App. 18/272,031 · Granted Dec 30, 2025

Acoustic microscope system and method for measuring an object disposed in a medium

Inventors: Paul Louis Maria Joseph Van Neer (Bergschenhoek, NL); Maurits Sebastiaan Van Der Heiden ('s-Gravenhage, NL); Michiel Peter Oderwald (Delft, NL)
Assignee: Nederlandse Organisatie voor toegepast-natuurwetenschappelijk onderzoek TNO
G01N29/0681G01N29/043G01N29/075G01N29/221G01N29/24G01N29/348G01N2291/011G01N2291/012G01N2291/02475G01N2291/0421G01N2291/0422G01N2291/104
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Quick Facts
Patent No.
US 12,510,513
App. No.
18/272,031
Granted
Dec 30, 2025
Kind
B2
Abstract

An acoustic microscope system is described that includes a container for holding a medium with an object to be measured. Compressional waves are generated by a probe into the medium. The compressional waves travel along an acoustic axis to interact with the object. Shear waves are generated by a shear wave source into the medium. The shear waves travel along a secondary axis which intersects with the acoustic axis at the object with a non-zero angle. The shear waves are configured to cause shear wave oscillations directed transverse to the secondary axis and at least partially directed along the acoustic axis. A measurement of the object is determined based on the compressional waves having interacted with the object as a function of the generation of the shear waves.

Claims (30)

1 . An acoustic microscope system comprising:

a container configured to hold a medium with an object to be measured disposed in the medium, wherein the container has a first side and a second side, wherein the first side and the second side form opposite sides of the container configured to hold the medium there between;

an acoustic probe comprising a compressional wave transducer disposed on the first side of the container and configured to carry out operations of:

generating compressional waves, at a compressional wave frequency into the medium, traveling along an acoustic axis to interact with the object disposed along the acoustic axis, wherein the acoustic axis is directed from the first side of the container towards the second side of the container, and

obtaining a measurement of the compressional waves having interacted with the object along the acoustic axis;

a shear wave source comprising at least one shear wave element disposed on the second side of the container, opposite the acoustic probe and laterally offset with respect to the acoustic axis from the acoustic probe through the object, wherein the at least one shear wave element is configured to generate shear waves at a shear wave frequency into the medium traveling along a secondary axis that intersects with the acoustic axis at the object with a non-zero angle, wherein the shear waves are configured to cause shear wave oscillations that are directed transverse to the secondary axis and that are at least partially directed along the acoustic axis for further interacting with the object to cause a change in the measurement of the compressional waves having interacted with the object; and

a processor configured to determine a measurement of the object based on the change in the measurement of the compressional waves having interacted with the object as a function of the generation of the shear waves interacting with the object.

2 . The system according to claim 1 , wherein the compressional wave frequency is more than one megahertz and the shear wave frequency is between 1 kHz-500 kHz.

3 . The system according to claim 1 , wherein the measurement of the object is based on respective frequency components in the measurement of the compressional waves having interacted with the object.

4 . The system according to claim 1 , wherein the compressional wave transducer is configured to measure the compressional waves reflected back from the object, wherein the compressional wave transducer is configured to both inject and measure the compressional waves.

5 . The system according to claim 1 , wherein the processor is configured to calculate a cross-correlation or Doppler shift of consecutive pulse echo traces of the compressional waves affected by the shear waves for determining a shear wave modulus of the object, and wherein the processor is configured to create an image of one or more objects in the medium based on a shear wave modulus of the one or more objects measured at different locations in the container.

6 . The system according to claim 1 , wherein the acoustic probe comprises a probe end formed by a rounded tip configured to push into a wall of the container for transmitting the compressional waves through the wall into the medium, and wherein the acoustic probe is configured to generate the compressional waves with a focus at a boundary of the medium.

7 . The system according to claim 1 , wherein the compressional wave transducer comprises a layer of piezoelectric material disposed on top of a rounded surface to focus the compressional waves towards a probe end, which is opposite the layer of piezoelectric material, from which the compressional waves are injected into the medium and/or container.

8 . The system according to claim 1 , wherein the processor is configured for converting measurement data, obtained from a focused beam of compressional waves, to data corresponding to a pencil beam, wherein the converting measurement data is based on a wavefield migration algorithm.

9 . The system according to claim 1 , wherein the shear wave source comprises at least two shear wave elements disposed on the second side of the container, wherein the at least two shear wave elements are disposed with a respective lateral offset on opposite sides of the acoustic axis of the acoustic probe and configured to generate and inject shear waves at the same shear wave frequency into the medium traveling along a respective secondary axis which both intersect with the acoustic axis at the object with a respective non-zero angle between the axes, and wherein the shear waves of the at least two shear wave elements are generated with a relative phase configured to cause respective shear wave oscillations that arrive in phase at the object at least in a direction along the acoustic axis.

10 . The system according to claim 1 , wherein the shear wave source comprises an array of shear wave element, disposed on the second side of the container opposite to the medium from the acoustic probe.

11 . The system according to claim 1 , wherein the acoustic microscope system comprises a set of actuators configured to scan the acoustic probe across a wall of the container, and wherein the processor is configured to determine an image of the object based on the measurement of the compressional waves at different positions of the acoustic probe along a surface of the wall.

12 . The system according to claim 1 , wherein the compression wave transducer comprises an array of compressional wave transducers arranged along at least a first dimension, wherein the acoustic microscope system comprises an actuator configured to scan the acoustic probe across a wall of the container in a second dimension transverse to the first dimension, and wherein the processor is configured to determine an image of the object based on the measurement of the compressional waves at different compressional wave transducers along the first dimension and different positions of the acoustic probe along the second dimension.

13 . The system according to claim 1 , wherein the acoustic microscope system comprises a two-dimensional array of compressional wave transducers, wherein the processor is configured to determine an image of the object based on the measurement of the compressional waves at different compressional wave transducers along the two dimensions.

14 . A method for measuring an object disposed in a medium, the method comprising:

generating, by an acoustic probe comprising a compressional wave transducer disposed on a first side of the medium, compressional waves, at a compressional wave frequency into the medium, traveling along an acoustic axis to interact with the object;

generating, by a shear wave source comprising at least one shear wave element disposed on a second side of the medium, shear waves at a shear wave frequency into the medium, wherein the medium is disposed between the compressional wave transducer and the at least one shear wave element, wherein the shear wave element is disposed on the second side laterally offset with respect to the acoustic axis, which extends from the acoustic probe through the object, to generate the shear waves traveling along a secondary axis which intersects with the acoustic axis at the object with a non-zero angle, wherein the shear waves cause shear wave oscillations directed transverse to the secondary axis and at least partially directed along the acoustic axis for further interacting with the object to cause a change in measured compressional waves having interacted with the object;

obtaining a measurement of the change in the compressional waves having interacted with the object while the shear waves further interact with the object; and

determining a measurement of the object based on the measurement of the change in the compressional waves having interacted with the object as a function of the generation of the shear waves interacting with the object.

15 . The method according to claim 14 , wherein the measured object is one of a plurality of biological cells disposed in a medium comprising one or more of a viscous liquid, gel, or tissue.

16 . The method according to claim 14 , comprising calculating a cross-correlation or Doppler shift of consecutive pulse echo traces of the compressional waves affected by the shear waves for determining a shear wave modulus of the object, and creating an image of one or more objects in the medium based on a shear wave modulus of the one or more objects measured at different locations in the container.

17 . The method according to claim 14 , comprising converting measurement data, obtained from a focused beam of compressional waves, to data corresponding to a pencil beam, wherein the converting measurement data is based on a wavefield migration algorithm.

18 . The method according to claim 14 , wherein the acoustic probe is scanned across a wall of the container, and an image of the object is determined based on the measurement of the compressional waves at different positions of the acoustic probe along a surface of the wall.

19 . The method according to claim 14 , wherein the acoustic probe comprises an array of compressional wave transducers arranged along at least a first dimension, wherein the acoustic probe is scanned across a wall of the container in a second dimension transverse to the first dimension, wherein determine an image of the object is determined based on the measurement of the compressional waves at different compressional wave transducers along the first dimension and different positions of the acoustic probe along the second dimension.

20 . The method according to claim 14 , wherein the acoustic probe comprises a two-dimensional array of compressional wave transducers, wherein an image of the object is determined based on the measurement of the compressional waves at different compressional wave transducers along the two dimensions.

Assignments (2)
CORRECTIVE ASSIGNMENT TO CORRECT THE THE SECOND INVENTORS MIDDLE NAME PREVIOUSLY RECORDED AT REEL: 064773 FRAME: 0145. ASSIGNOR(S) HEREBY CONFIRMS THE ASSIGNMENT. Recorded Sep 22, 2023
From: VAN NEER, PAUL LOUIS MARIA JOSEPH; VAN DER HEIDEN, MAURITS SEBASTIAAN; ODERWALD, MICHIEL PETER
To: NEDERLANDSE ORGANISATIE VOOR TOEGEPAST-NATUURWETENSCHAPPELIJK ONDERZOEK TNO
Reel/Frame 065017/0435 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Sep 1, 2023
From: VAN NEER, PAUL LOUIS MARIA JOSEPH; VAN DER HEIDEN, MAURITS SEBASTIAN; ODERWALD, MICHIEL PETER
To: NEDERLANDSE ORGANISATIE VOOR TOEGEPAST-NATUURWETENSCHAPPELIJK ONDERZOEK TNO
Reel/Frame 064773/0145 →
Priority Claims (1)
EP 21152574 · Jan 20, 2021 · regional
Continuity (1)
Related Publication 20230408452A1 · Dec 21, 2023
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