The patent badge is an abbreviated version of the USPTO patent document. The patent badge does contain a link to the full patent document.

The patent badge is an abbreviated version of the USPTO patent document. The patent badge covers the following: Patent number, Date patent was issued, Date patent was filed, Title of the patent, Applicant, Inventor, Assignee, Attorney firm, Primary examiner, Assistant examiner, CPCs, and Abstract. The patent badge does contain a link to the full patent document (in Adobe Acrobat format, aka pdf). To download or print any patent click here.

Date of Patent:
Jun. 18, 2019

Filed:

Feb. 26, 2015
Applicant:

Sintef Tto As, Trondheim, NO;

Inventor:

Tormod Selbekk, Trondheim, NO;

Assignee:

Tomod Selbekk, Trondheim, NO;

Attorney:
Primary Examiner:
Int. Cl.
CPC ...
G01N 29/032 (2006.01); G01N 29/07 (2006.01); G01N 29/11 (2006.01); G01N 29/44 (2006.01); G01N 29/024 (2006.01);
U.S. Cl.
CPC ...
G01N 29/024 (2013.01); G01N 29/032 (2013.01); G01N 29/07 (2013.01); G01N 29/11 (2013.01); G01N 29/4472 (2013.01); G01N 2291/011 (2013.01); G01N 2291/02475 (2013.01); G01N 2291/044 (2013.01); G01N 2291/0421 (2013.01);
Abstract

A method of measuring a property of a medium using ultrasound, comprising: transmitting one or more ultrasound pulses into the medium from one or more transmitters and receiving at least a first echo signal and a second echo signal from within the medium at one or more receivers, wherein the first and second echo signals correspond to first and second pulse transmission paths within the medium from the one or more sources to the one or more receivers, the second path being different from the first path; and using the characteristics of the first and second echo signals together with an estimate of the property of the medium and a geometrical relationship between the first and second transmission paths to calculate a revised estimate of said property of the medium. By using two different beam paths within the medium, the first and second echoes will have had slightly different interactions with the medium. For example the different paths may well have different lengths thus giving different amounts of interaction such as different amplitude or phase effects on the different pulses. By comparing the similarities and differences between the pulses, certain properties of the medium can be discerned. Many different properties can be investigated using these principles. In particular, the speed of sound in a medium can be measured and the direction and magnitude of a flow or particle movement within the medium can be measured. An iterative process may be used.


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