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公开(公告)号:US20240102972A1
公开(公告)日:2024-03-28
申请号:US18371664
申请日:2023-09-22
Applicant: SUPPLYZ Holding B.V.
Inventor: Fabian OBERNDORFER , Eshagh KARGAR , Felix WASSMANN
CPC classification number: G01N29/4472 , G01N29/04 , G01N2291/023 , G01N2291/0289
Abstract: The present invention relates to a device for detecting and/or analyzing an object or a material, wherein the device comprises a receiver configured to detect a first signal, the first signal being generated, at least in part, by vibrations of at least a part of the material or the object, and the device configured to communicate with a remote component, and to send a signal based, at least in part, on the first signal to the remote component. The present invention also relates to a remote component configured to communicate with a device, wherein the remote component is configured to at least receive data from the device and, based thereon, to determine data related to a material or an object, a system comprising the device and the remote component, a corresponding method, and a use of the system and method to detect and/or analyze the object or the material of a container.
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公开(公告)号:US20240053303A1
公开(公告)日:2024-02-15
申请号:US17819515
申请日:2022-08-12
Applicant: Palo Alto Research Center Incorporated
Inventor: Morad BEHANDISH
CPC classification number: G01N29/4472 , G01N29/041 , G01N29/4481 , G01N2291/02818
Abstract: A nondestructive method for detecting damage in parts and/or characterizing effective material properties may include: exposing a material to one or more nondestructive stimuli; measuring a response of the material to the stimuli; selecting at least one of a specific length scale or a specific time scale; and analyzing the measurement of the response with a scale-aware single- or multi-physics model to identify anomalies in the measurements as compared to an expected response of the material to the stimuli, wherein the scale-aware single- or multi-physics model is based on the at least one of the specific length scale or the specific time scale.
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63.
公开(公告)号:US20230333062A1
公开(公告)日:2023-10-19
申请号:US18028441
申请日:2021-09-23
Inventor: Tom DRUET , Tinh HOANG HUU
CPC classification number: G01N29/0672 , G01N29/30 , G01N29/4472 , G01N2291/106 , G01N2291/023
Abstract: A method for performing tomography on a structure supporting modes of guided propagation of elastic waves, the method includes the steps of: acquiring a plurality of signals propagating through the structure by means of a plurality of pairs of non-collocated elastic-wave sensors; for each pair of sensors, i. selecting one mode of guided propagation, ii. converting the measured signal into wave field for the selected mode, iii. determining an anisotropic calibration coefficient on the basis of a wave-field propagation model evaluated depending on the anisotropic wavenumber and on the distance between the sensors of the pair, and on the basis of the wave field or of a reference wave field corresponding to a healthy state of the structure, calibrating the wave fields using the determined calibration coefficients, performing tomography on the structure on the basis of the calibrated wave fields.
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64.
公开(公告)号:US20190234911A1
公开(公告)日:2019-08-01
申请号:US16337339
申请日:2017-09-28
Inventor: Todd W. Murray , Peter Burgholzer , Markus Haltmeier
CPC classification number: G01N29/4472 , G01N21/1702 , G01N21/4795 , G01N29/00 , G01N29/0672 , G01N29/2418 , G01N2021/1706 , G01N2021/479 , G01N2021/8444 , G01N2201/106
Abstract: A method for high resolution photoacoustic imaging in scattering media using structured illumination may include illuminating a sample of an absorption object with structured illumination, including illuminating the sample with multiple different speckle patterns at different times. The method may also include detecting multiple photoacoustic signals generated by the absorption object in response to illumination with the different speckle patterns to generate multiple photoacoustic responses. The method may also include reconstructing an absorber distribution of the absorption object by exploiting joint sparsity of sound sources in the plurality of photoacoustic responses.
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65.
公开(公告)号:US20180275108A1
公开(公告)日:2018-09-27
申请号:US15468005
申请日:2017-03-23
Applicant: Palo Alto Research Center Incorporated
Inventor: Eric D. Cocker , Scott A. Elrod , Uriel A. Rosa , Jessica L. B. Rivest , George W. Daniel , David E. Schwartz
CPC classification number: G01N33/0098 , G01N29/11 , G01N29/343 , G01N29/348 , G01N29/4472 , G01N2291/011 , G01N2291/015 , G01N2291/02466 , G01N2291/044 , G01N2291/101
Abstract: Embodiments of the present invention provide a system and method for accurate, field-ready, non-destructive, and three-dimensional plant root characterization using acoustic signals. The system is portable, fast, precise, and can be used in field conditions, including moist soil, to visualize root structure or mass distribution, without damaging growing crops. The system may also be applied to characterize other underground objects, such as pipes, building foundations, archaeological artifacts, or mineral ores. During operation, the system generates a source acoustic signal. The system sends the source acoustic signal to an actuator acoustically coupled directly to a plant. The system obtains a response acoustic signal from an underground transducer monitoring a root of the plant. The system analyzes the response acoustic signal according to a model and based on the source acoustic signal. The system then determines, based on the analyzed response acoustic signal, a physical configuration of the plant root.
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公开(公告)号:US10007885B1
公开(公告)日:2018-06-26
申请号:US15650216
申请日:2017-07-14
Inventor: Alexey V. Gorshkov , Michael S. Foss-Feig , Zachary Eldredge , Steven L. Rolston
CPC classification number: G06N10/00 , G01N24/00 , G01N24/008 , G01N29/4472 , G01N35/0098 , G01R33/24 , G06F17/10 , H04B10/70
Abstract: Determining a modal amplitude of an inhomogeneous field includes: preparing an initial entangled state of a quantum sensor; subjecting the quantum sensor to the inhomogeneous field of the analyte; subjecting a first qudit sensor of the quantum sensor to a first perturbation pulse; receiving the first perturbation pulse by the first qudit sensor to prepare a first intermediate entangled state of the quantum sensor, the first intermediate entangled state comprising a first intermediate linear superposition; changing the initial linear superposition to the first intermediate linear superposition in response to receiving the first perturbation pulse by the quantum sensor; and determining a final entangled state of the quantum sensor after applying the first perturbation pulse to determine the modal amplitude of the inhomogeneous field of the analyte.
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公开(公告)号:US09970905B2
公开(公告)日:2018-05-15
申请号:US14914679
申请日:2014-09-01
CPC classification number: G01N29/07 , G01N29/043 , G01N29/44 , G01N29/4472 , G01N2291/0289 , G01N2291/103 , G01N2291/106
Abstract: A defect monitoring system has ultrasound transmitters and receivers on a wall of a structure under test such as a pipeline. The receivers are arranged in an array of locations that substantially encloses an area under test on a wall of a structure under test. The array may comprise two circumferential rings along a pipeline at different axial positions. The array of ultrasound receivers is used to measure signals that result ultrasound that leave the area through the wall for other parts of the wall. From the measured signals backward propagated signals are computed for a location within the enclosed area, compensated for a modelled effect of propagation from the location within the area to the locations of the receivers at the perimeter. The backward propagated signals for the location in the enclosed area are summed over the locations of the receivers to obtain an approximate integral over the perimeter of the area. The integral is used as a normalization factor for the backward propagated signals for the location within the area. In this way reflection and/or transmission coefficients are obtained that are indicative of the size of defects in the wall, independent of calibration of ultrasound coupling coefficients.
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68.
公开(公告)号:US20180128781A1
公开(公告)日:2018-05-10
申请号:US15564368
申请日:2016-06-13
Applicant: MARQUETTE UNIVERSITY , CHEVRON U.S.A. INC.
Inventor: Fabien J. JOSSE , Florian BENDER , Antonio J. RICCO , Rachel Ellen MOHLER , Ravindra Vasant KOLHATKAR
IPC: G01N29/02 , G01N29/036 , G01N33/18 , G01N29/22 , G01N29/44
CPC classification number: G01N29/022 , G01N29/036 , G01N29/222 , G01N29/4418 , G01N29/4472 , G01N33/1833 , G01N2291/014 , G01N2291/02491 , G01N2291/0423
Abstract: An exemplary embodiment of a method of detecting hydrocarbons in Systems and methods for sensing analytes in an aqueous solution, include pretreating a water sample to provide a test sample. A flow cell includes at least one sensor with a polymer coating having at least partial selectivity for at least one analyte. The flow cell receives a test sample and a reference sample. At least one output signal from the at least one sensor is processed with a microcontroller using a model of the sensor response and a bank of Kalman filters to estimate a concentration of at least one analyte in the aqueous solution.
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公开(公告)号:US09945716B2
公开(公告)日:2018-04-17
申请号:US14856160
申请日:2015-09-16
Applicant: ROLLS-ROYCE PLC
Inventor: Stephen Samuel Wiseall , Anthony Bernard Phipps , David Cameron Wright , Sree Vamsi Tammineni , James William Cheang Meas
CPC classification number: G01H1/006 , G01N29/043 , G01N29/4472
Abstract: The ultrasonic inspectability of a supplied part out of which a final component is to be machined is determined by following a set of inspection rules for ultrasonic inspection of the supplied part. The rules determine which parts of the polygon cannot be inspected by a scan at a given ultrasound beam angle (typical beam angles are 0°, +20° and −20° relative to the perpendicular direction to the edge) along a given edge of the polygon.
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公开(公告)号:US09927402B2
公开(公告)日:2018-03-27
申请号:US14444561
申请日:2014-07-28
Applicant: ABB Schweiz AG
Inventor: Axel Kramer , Hubert Brandle , Thomas Alfred Paul
CPC classification number: G01N29/036 , G01N9/002 , G01N9/34 , G01N11/16 , G01N29/022 , G01N29/4472 , G01N2009/006 , G01N2291/02818 , G01N2291/0427
Abstract: A method and device for estimating a density value ρm indicative of a true density ρ or for estimating a viscosity value ηm indicative of a true viscosity η of a fluid is disclosed. For this, a first resonance frequency fR of a first mechanical oscillator in a reference volume and a second resonance frequency fF of a second mechanical oscillator in contact with the fluid are measured. The estimated value ρm or ηm is then derived using these resonance frequencies fR and fF. During this derivation, at least one fluid-temperature- or fluid-pressure-dependent parameter of the fluid is used. Additionally or alternatively, the first (i.e. reference) mechanical oscillator is arranged in contact with a reference fluid. Thus, fundamental errors in the derivation of the estimated value ρm or ηm are reduced and the estimated value becomes more reliable.
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