The present embodiments pertain to systems, apparatuses, and methods for analyzing rotation or reciprocation in machinery, machine components, and inanimate physical structures; processing of visual data related to such movements; and calculating the frequency of rotation or reciprocation of a component with high accuracy without physically contacting the structure through the use of digital photography. Instantaneous changes in the speed of rotation measured at fractional positions within each revolution can be made using an internal or added gear wheel or by applying a graduated or patterned tape around the rotating element to determine the torsional vibration of the shaft through the use of digital photography.
All machines and physical structures produce vibrations and resonances of various kinds, some of which may be characteristic of normal operation and others of which may indicate off-normal conditions, unusual wear, incipient failure, or other problems. In the field of predictive maintenance, the detection of vibrational signatures is a key element of the diagnostic process in which the goal is to identify and remedy incipient problems before a more serious event such as breakdown, failure, or service interruption occurs. When analyzing the vibration frequency spectrum of a mechanical component, it is critical to have an accurate knowledge of the frequency at which the machine rotates or reciprocates. The identity of all the peaks present in the frequency spectrum is tied to the ratio of the frequency of a peak to the operating frequency. This ratio is referred to as the order of the frequency peak and often frequency is displayed with the x-axis (frequency) in orders. The measurement of the frequency of rotation or reciprocation can be accomplished using both contact and noncontact methods. When there is adequate access to the shaft of the machine, instruments with rubber rotating wheels can be placed against the shaft. Noncontact methods usually employ optical sensors, such as laser-based tachometers, or displacement probes to measure the speed. In these cases, it is most helpful for there to be reflective tape applied to the shaft or for the shaft to have a mechanical discontinuity such as a keyway that will serve to generate a once per revolution pulse that can be converted by an electronic instrument to provide a readout of the machine operating frequency. Some laser-based instruments have been developed which capture reflected light from the shaft and determine the operational frequency using autocorrelation or the Fast Fourier Transform (FFT) algorithm to automatically locate the desired frequency and calculate, record, and display the rotational speed of a machine or machine component. Moreover, there are numerous vendors that sell speed sensors which utilize contact wheels or once-per-rev discontinuities on the shaft. Stroboscopes can also be used to measure speed by freezing the motion of a component using a flashing light source.
Notwithstanding such capability, there are several disadvantages to using an external tachometer or stroboscope to measure the speed of operation of a machine that is being analyzed using video recording. In addition to the need to own or have access to these additional instruments at the troubleshooting site, the use of these instruments may result in the following disadvantages: access to or contact with moving components, stopping the machine to apply reflective tape or to mount a sensor in close proximity to the shaft, or holding an optical or laser tachometer or stroboscope with minimal motion, and synchronizing the speed with the video recording of the vibratory motion.
An alternative to the use of these known methods for measuring the machine speed is to use the same camera sensor that will record the motion of the machine and apply specialized processing algorithms to identify the speed. This process is much simpler and does not require the expense of a tachometer instrument and the additional time to setup and make the speed measurement. The normal measurement of the motion in a recorded video is based on the change in the pixel intensity in the scene and determines motion along the two axes which are orthogonal to the line of sight between the camera and the objects in the scene. In most cases, the measurement is based on comparing the pixel in one frame to the corresponding pixel in the following frames. When a shaft or other component of a machine is rotating or reciprocating, the position of pixels corresponding to such object generally will be associated with a different portion of the machine in each frame. For example, when looking at a rotating shaft, the light intensity present at the same pixel in each frame is reflected from different angular positions on the shaft as it rotates. This same phenomenon is true for a reciprocating shaft. By determining a frequency of rotation or reciprocation, recordings which are captured with negligible time delay can be synchronized with the measured frequency with high confidence that the machine speed has not changed. It also is true that if speed measurements are taken at different points in time and are substantially the same, it is unlikely that there have been large speed deviations during the data recording. The objective, therefore, has been to develop a more efficient system or processing method that does not rely upon contact with the machine or component, which determines a frequency of rotation or reciprocation—a determination which would be associated with the component's speed as well.
In addition to measuring the average speed of a rotating or reciprocating machine element, it may be important to determine how the rotational speed is changing during each cycle of repetition. These changes provide a means of measuring torsional vibration which characterizes the twisting motion of a shaft or angular vibration. Torsional measurements are made in the angular domain and often expressed in units of degrees. Various combinations of equipment components such as internal combustion engines, reciprocating compressors, flywheels, universal joints, couplings, gearing, blading, etc. can affect the torsional characteristics of the entire system. Torsional vibrations may also be affected by drive, operating or load conditions and may vary with the frequency of operation.
Torsional measurements can be made using strain gauges, optical sensors, or proximity probes which are focused on a component that has equally spaced divisions embedded or attached to the component. Commonly a geared element or reflective tape which has been marked with equally spaced lines is attached to the shaft in one or more locations and a tachometer is used to measure the time between each pulse in the waveform that is generated. The measurement of torsional twist, or the twist angle, between two points along a shaft or through a gear train may be derived from a pair of tachometer signals, one at each end of the shaft. Typically, the tachometer signals would be derived from gear teeth giving a known number of pulses per revolution. For example, in the case of a crankshaft, a 20-tooth gear wheel might be attached to the front end giving 20 pulses per revolution and a 60-tooth gear wheel might be attached to the rear end of a shaft giving 60 pulses/revolutions when measured with an inductive or eddy current probe. With the proper mathematical transformation applied, the minimum, maximum, and mean torsional vibration amplitude or its full frequency spectrum can be determined. The application of a tape with evenly spaced lines circumferentially can be used to provide equivalent results; however, there is some additional mathematical processing needed to handle the position of overlap which will cause one interval that is unequal from the others. These approaches, however, do not use or take advantage of the capabilities of digital photography and recording of such machines and components in motion.
The use of digital photography to make non-contacting measurements of torsional vibrations provides a much simpler system that is easier to implement while providing equivalent or improved accuracy over existing methods. The inventive embodiments herein may require one or more cameras depending on the ability to get all measurement locations in a single field of view. The measurements can be made using the standard gear wheels, or by wrapping a graduated tape or a tape with a uniform pattern, such as honeycomb, triangular, or diamond grid around the shaft.
Present embodiments pertain to systems, apparatuses, and methods for analyzing and reporting the movements in mechanical structures, machinery, and machine components, including measuring the speed of rotation or reciprocation of a component on the structure which is useful in identifying other frequencies measured on the structure. In some aspects, the use of a gear wheel or a graduated or patterned tape wrapped around the shaft allows for instantaneous speed measurements within each cycle of repetition and torsional vibration measurements to be made. Given that a position on a rotating or reciprocating component changes pixel locations in the field of view and may even be temporarily hidden from the field of view, special processing of the visual data is provided for herein which facilitates measurement of motion associated with the rotating or reciprocating component in the field of view. In other aspects of present embodiments herein, image processing algorithms utilize repeating patterns which occur in the video data to measure the speed of the asset. The above capabilities provide further benefits because the sensor (video camera, in some embodiments) does not contact the machine, component or mechanical structure being studied, and efficiency of the process may be further enhanced by using the same camera that will be employed to analyze motion in the scene.
In an exemplary embodiment, the user (user and analyst are used interchangeably herein) follows the typical steps necessary to obtain good recordings:
1. Position the camera to acquire the perspective of the equipment of interest, containing at least a portion of the rotating or reciprocating component,
2. Focus the camera, and
3. Adjust the aperture; this may require the addition of external light or shielding the field of view in the presence of bright light conditions to achieve acceptable lighting conditions for recording.
At this point, the user only needs to request a speed calculation, provide an estimated speed value, and select a location on the component whose speed is to be measured. The software will adjust the size of the image using the user selected region of interest to obtain an improved view of the location being measured, optionally adjust the bit depth to 12-bit resolution, determine an appropriate acquisition frame rate, collect a short recording, and calculate the speed of the identified component. The user can then proceed to acquire the desired recording and the system will reset the acquisition parameters to the recording parameters that had been selected and begin collecting data. As described more fully herein, in some embodiments, this speed of the asset is stored with the recording. This stored speed value can be used to produce order-based data graphs. In regards to settings of the recording device to obtain useful recordings, U.S. Pub. No. 2016/0300341 (Ser. No. 14/999,660, filed Jun. 9, 2016) titled “Apparatus and Method for Visualizing Periodic Motions in Mechanical Components” (Hay, Jeffrey R., et al.; published Oct. 13, 2016 and subsequently issued as U.S. Pat. No. 10,062,411), the contents of which are fully incorporated by reference herein, describes among other features a user interface as part of a system that, among other capabilities, allows the selection of at least one component whose frequency of movement is measured as being relevant to the operation of a machine, e.g., a frequency of movement for a component used to drive tension in a cable.
In addition, U.S. Pub. No. 2016/0171309 (Ser. No. 14/757,255, filed Dec. 9, 2015) titled “Non-contacting monitor for bridges and civil structures” (Hay, Jeffrey R.; published Jun. 16, 2016 and subsequently issued as U.S. Pat. No. 9,704,266) describes the contents of which are fully incorporated by reference herein, describes among other features a user-controlled movable area selector on a graphical user interface, which enables the selection of a region of interest within a scene. In certain described aspects, such a system provides a display of a physical parameter, including displacement versus time for one or more components within the region of interest including calculated data such as values of time and displacement, such that from amplitude (displacement) and frequency motion is evaluated and used to determine the damping of a civil structure.
In an exemplary embodiment to measure torsional vibration, the user follows the typical steps necessary to obtain good recordings:
1. Attach one or more gear wheels or tape with an appropriate pattern to the shaft in selected locations or use existing elements if appropriate for such a measurement.
2. Position the camera to acquire the perspective of the equipment of interest, containing at least a portion of the rotating or reciprocating component where the target(s) of interest are in the field of view (use an additional camera whose sampling is synchronized with the first camera if necessary to view all target positions adequately).
3. Focus the camera, and
4. Adjust the aperture; it may be necessary to add external light or shield the field of view in the presence of brightly lit conditions to achieve acceptable lighting conditions for recording.
5. Establish a sampling rate high enough to view the highest order of torsional vibration of interest and a duration of M cycles of repetition necessary to view the lowest fractional order (1/M) of interest and make a recording.
At this point, the user only needs to position a region of interest upon the locations where the targets are mounted and request a torsional vibration calculation. The system will determine the average frequency of repetition as well as minimum, maximum, and mean torsional vibration amplitude and its full frequency spectrum. This average speed value can be used to produce order-based torsional vibration graphs. If more than one target is mounted on the shaft, then differential measurements can be calculated or graphs from the respective locations can be overlaid or stacked to compare behavior at the different locations.
It is known that an intensity of light present at the same pixel in each frame is reflected from different angular positions on the shaft or other component as it rotates or reciprocates. In the present embodiments, processing in accordance with one or more algorithms described herein is applied to model this motion and recognize the frequency of rotation, or of reciprocation. Once the frequency of rotation or reciprocation has been determined in accordance with the present embodiments, the repeating patterns of motion which occur in the video data allow a user to direct or use the methods herein to capture recordings with negligible time delay to be synchronized with the measured frequency with high confidence that the machine or component speed has not changed. If the duration of the measurement is large, then it may be desirable to measure the frequency of operation a second time as soon as the data recording is complete. If both speed measurements are the same, it is unlikely that there have been large speed deviations during the data recording, and the measurements afforded by multiple embodiments and alternatives herein provides a reliable measurement of the speed of the asset with no contact of the moving component needed to analyze motion in a scene. In an alternate embodiment, the speed measurement may be performed on the same recording used to measure the orthogonal vibrations in the field of view if the frame acquisition rate of the recording is sufficient to resolve the frequency of rotation or reciprocation.
The drawings, schematics, figures, and descriptions contained in this application are to be understood as illustrative of steps, structures, features and aspects of the present embodiments. Accordingly, the scope of embodiments is not limited to features, dimensions, scales, and arrangements shown in the figures.
In some aspects of the present disclosure, in accordance with multiple embodiments and alternatives, a user in the operation of present embodiments measures the speed of rotation or reciprocation of an element on a mechanical structure, a machine or machine component without contacting the structure using the same camera that will be employed to investigate the dynamic motion of the mechanical structure.
In
Machines often present a complex picture on a video recording that represents the operating speed of the machine itself, as well as potentially different operating speeds of components of the machine as they undergo periodic movements (rotational or reciprocating). By way of simple and non-limiting illustration, a machine might include a motor with components captured on the video rotating at first frequency, operatively connected to a rotating shaft that drives one or more gears through a series of rotations at a second frequency. Therefore, it is extremely important to know the exact frequency of rotation or reciprocation associated with the current operation of a machine. This allows an analyst to identify other frequencies present in the vibration measured on the mechanical structure. When diagnosing a specific fault condition, it is important to know which frequencies on a mechanical structure are sub-synchronous, synchronous, or non-synchronous with respect to the operation speed. A synchronous peak which occurs at 12 times the running speed might be associated with a 12-tooth gear; however, a nonsynchronous peak occurring at 12.08 times running speed may be associated with a defect in an anti-friction bearing. The ability to measure the rate of rotation or reciprocation using the same non-contacting camera that will make the vibration measurements on the structure is very cost effective and efficient for the analyst.
In one or more exemplary embodiments, the user follows the typical steps necessary to obtain good recordings of a machine or portion of machine having a rotating or reciprocating component:
1. Position the camera to acquire the perspective of the equipment of interest, containing at least a portion of the rotating or reciprocating component,
2. Focus the camera, and
3. Adjust the aperture; this may require the addition of external light or shielding the field of view in the presence of bright light conditions to achieve acceptable lighting conditions for recording.
After the camera is set up as desired or needed (
The system software in some embodiments can automatically adjust the exposure to improve the asset speed measurement by modifying the brightness and gain settings on the camera. One embodiment providing an automated exposure adjustment method is outlined in the flowchart provided in
1. Gain is initialized to 0 (
2. A frame is acquired and the percentage of pixels above half intensity (i.e. 2048 for 12-bit data) is computed.
3. If less than 10% of pixels are above half intensity (
a. If Brightness is <95%, then Brightness is increased by 20% (limited to 100%) and then repeat from “2” above (
b. Otherwise, if Gain is <95%, then Gain is increased by 10% (limited to 100%) and then repeat from “2” above (
4. If more than 10% of pixels are above half intensity, then exposure is accepted (
Automated adjustment of the exposure minimizes user interaction and the time required to perform the speed measurement. Any other algorithms which result in an acceptable exposure could be employed in alternate embodiments and would remain in the scope of the embodiments described herein. If the system cannot successfully make the speed measurement, then the user will need to select another location on the shaft or manually adjust the exposure.
In some embodiments, after the exposure has been automatically adjusted, then a recording is acquired which will provide waveforms with approximately 12 revolutions of the shaft (128-1024 samples per waveform). For a set of N pixels (camera pixels or virtual pixels) (
1. Intensity waveforms are formed, and “DC” is removed from them (
2. The autocorrelation waveform is computed (
3. The largest peaks in the autocorrelation waveform are located (
4. The peaks are sorted in time order and statistics of their spacing computed. If the coefficient of variance of the peaks is >−5.0, the pixel is discarded (
5. The average peak spacing yields the speed from that pixel (
6. The asset speed is average of the retained pixel speeds ((
The resulting asset speed is displayed to the user who then accepts or rejects it. A flowchart of this algorithm is shown in
In an alternate embodiment, the practice of which is described below in exemplary fashion, the asset speed is determined by locating the peaks in FFT frequency spectrum of the waveforms with approximately 12 revolutions of the shaft (128-1024 samples per waveform). For a set of N pixels (camera pixels or virtual pixels) (
1. Intensity waveforms are formed, and “DC” is removed from them (
2. The FFT frequency spectrum of the intensity waveform is computed (
3. The largest 5 peaks in the FFT spectrum are located accurately using FFT windowing parameters (
4. The peaks are tested to find harmonically related peaks and the fundamental frequency of the family is calculated (
5. The mean value of the retained fundamental harmonic frequency values is formed and any pixels whose value fundamental frequency differs by more than 1 Hz is discarded from the set,
6. The asset speed is average of the fundamental harmonic frequencies for the retained pixels (
The resulting asset speed is displayed to the user who then accepts or rejects it. An exemplary flowchart of this algorithm is shown in
This process is improved by using located peak values rather than the nominal peak value which is identified by the frequency line in the spectrum with the highest amplitude. In a spectrum calculated with 1 Hz resolution, the nominal peak value might be 22 Hz because the frequency line at 22 Hz has the highest amplitude of 2. The amplitude value at 21 Hz might be 0.05 and the line at 23 Hz might be 1.90 indicating that the true peak frequency lies between 22 Hz and 23 Hz. It is well known in signal processing art, that the true frequency value can be estimated more accurately by applying formulas that consider the windowing function used when calculating the FFT frequency spectrum. In the case above, the true value would be about halfway between the two lines giving a located peak frequency of 22.4 Hz. The FFT could be constructed using any number of windows such as the Uniform, Hanning, Hamming, Blackman-Harris, Kaiser-Bessel, or others. More accurate frequency estimates of the peak location can be calculated using the parameters that are characteristic of the respective windows. An improved location of the peak frequency can also be accomplished by applying any number of well-known fitting algorithms to the center line in the peak and the 2 lines on either side. The generic fitting algorithms are generally not as accurate as using the algorithm that takes into account the FFT windowing functions. Demonstrating the broad nature of the descriptions herein, alternative embodiments could use any of the methods discussed or those obtaining equivalent improvements in locating the peak frequency values. Nominal peak frequency values can also be used but would not provide as reliable results in some cases. When calculating the ratio of the frequency of two peaks to determine if they are harmonically related (integer multiples of the fundamental frequency), located peak values will result in a closer match to integer values and thus correctly identify harmonic family members.
The intensity waveform from one of the pixels in the region of interest located on the rotating or reciprocating component is shown in
In an alternate embodiment, the algorithms described above could be applied to the regular video recording which are captured to measure the orthogonal vibration in the field of view. In the situation where the rotating or reciprocating element is in the field of view and the data acquisition parameters are sufficient to enable resolving the rate of rotational or reciprocation, the rate of repetition could be measured for a ROI identified by the user.
In other aspects of the present disclosure, in accordance with multiple embodiments and alternatives, a user in the operation of present embodiments measures the instantaneous speed of rotation of an element on a mechanical structure, a machine or machine component without contacting the structure using the same camera that will be employed to investigate the dynamic motion of the mechanical structure. Measurement of the instantaneous speed at various points during each revolution of the shaft allows the user to investigate the angular or torsional vibration characteristics of the mechanical system. This measurement requires access to a gear wheel which is integral or attached to the shaft of interest or the application of a patterned or graduated tape to a visible position on the shaft.
When using a video camera to make torsional measurements, the tape applied could have graduated lines or a repeating pattern, such as shown in
In a use case shown in
1. On a selected frame, the user optionally identifies the edge of component by drawing a reference line (212 in
2. On the selected frame, the user identifies the region where the torsional motion will be measured by drawing the reference rectangle (identified as 211 in
3. The system software can optionally match the references to the side of the disk and the closest lines of the selected division to achieve a finer resolution in the position of user selected references.
4. Count number of whole divisions (N) and measure fraction division (F), visually or from video,
5. Determine circumference (C) and diameter (D) of component being monitored,
6. Set the sampling rate to be the larger of:
a. 1.5*N·F*RPS or
b. 2.5 times the number of orders of interest,
7. Collect the number of samples or frames equal to 3 times the reciprocal of the lowest sub order (1/M) of interest times the sampling rate: Total Samples=3*SR*M,
8. Determine change in arc for the division passing through the reference rectangle for each frame (sample) recorded:
a. Use the fractional movement of the lines across this reference zone if processing a full tape division,
b. If a partial division (tape overlap) enters the zone, then move to preceding full tape division to determine distance moved in the interval or the arc of the motion,
9. Movement of the wheel due to vibration can be removed by measuring the motion at the reference line (212 in
Further, in accordance with the embodiments herein,
It will be appreciated that this embodiment describes the use of targets or markings affixed to the shaft. In some instance measurements may be possible on pre-existing markings on the shaft. These marking may be from but not limited to normal wear on the shaft, damage to the shaft, scuff or scratches or marking made on the shaft by an individual.
In some instances, the displacements of a marking on the shaft will be made directly from the apparent distance traveled by the mark as seen by the camera. It will be appreciated that a shaft measurement can be corrected for the curvature of the shaft such that apparent motion on the horizon of the shaft can be compared to the motion at the nearest point of the shaft to the camera. When a mark is moving near the horizon of the shaft a given angular displacement will appear to travel a shorter distance as viewed from the camera as compared to the same angular displacement moving at the nearest point of the shaft to the camera. By accounting for this curvature, the angular displacement can be normalized and compared across the entire shaft. The radius of the shaft may be entered into the software to make this correction or the camera may make the measurement of the shaft radius from the image itself if the shaft is visible and the scale of the image is known.
Several exemplary claims are set forth herein but are not intended to place boundaries on the full range of embodiments and alternatives described and provided for herein, nor are these intended to waive or otherwise circumscribe any potential claims that could be pursued in a later application claiming the benefit of the teachings and disclosures herein. A claim expressed in this filing as a method also could represents a system that performs such a method or other methods, and a system claim if recited also could represent a method of operation executed by said system.
It will be understood that the embodiments described herein are not limited in their application to the details of the teachings and descriptions set forth, or as illustrated in the accompanying figures. Rather, it will be understood that the present embodiments and alternatives, as described and claimed herein, are capable of being practiced or carried out in various ways. Also, it is to be understood that words and phrases used herein are for the purpose of description and should not be regarded as limiting. The use herein of such words and phrases as “including,” “such as,” “comprising,” “e.g.,” “containing,” or “having” and variations of those words is meant to encompass the items listed thereafter, and equivalents of those, as well as additional items.
Accordingly, the foregoing descriptions of embodiments and alternatives are meant to illustrate, rather than to serve as limits on the scope of what has been disclosed herein. The descriptions herein are not meant to limit the understanding of the embodiments to the precise forms disclosed. It will be understood by those having ordinary skill in the art that modifications and variations of these embodiments are reasonably possible in light of the above teachings and descriptions.
This patent application claims the benefit of priority to U.S. Provisional Patent Application Ser. No. 62/965,382, with a filing date of Jan. 24, 2020, the contents of which are fully incorporated by reference herein.
Number | Name | Date | Kind |
---|---|---|---|
5517251 | Rector et al. | May 1996 | A |
5666157 | Aviv | Sep 1997 | A |
6028626 | Aviv | Feb 2000 | A |
6295383 | Smitt et al. | Sep 2001 | B1 |
6422741 | Murphy et al. | Jul 2002 | B2 |
6456296 | Cataudella | Sep 2002 | B1 |
6727725 | Devaney et al. | Apr 2004 | B2 |
6774601 | Schwartz et al. | Apr 2004 | B2 |
6792811 | Argento et al. | Sep 2004 | B2 |
7622715 | Ignatowicz | Nov 2009 | B2 |
7627369 | Hunt | Dec 2009 | B2 |
7672369 | Garakani et al. | Mar 2010 | B2 |
7710280 | McLellan | May 2010 | B2 |
7862188 | Luty et al. | Jan 2011 | B2 |
7903156 | Nobori et al. | Mar 2011 | B2 |
8119986 | Garvey, III et al. | Feb 2012 | B1 |
8149273 | Liu et al. | Apr 2012 | B2 |
8170109 | Gaude et al. | May 2012 | B2 |
8242445 | Scanlon et al. | Aug 2012 | B1 |
8351571 | Brinks et al. | Jan 2013 | B2 |
8374498 | Pastore | Feb 2013 | B2 |
8475390 | Heaton et al. | Jul 2013 | B2 |
8483456 | Nagatsuka et al. | Jul 2013 | B2 |
8502821 | Louise et al. | Aug 2013 | B2 |
8515711 | Mitchell et al. | Aug 2013 | B2 |
8523674 | Patti | Sep 2013 | B2 |
8537203 | Seibel et al. | Sep 2013 | B2 |
8693735 | Keilkopf et al. | Apr 2014 | B2 |
8720781 | Wang et al. | May 2014 | B2 |
8731241 | Johnson et al. | May 2014 | B2 |
8765121 | Maslowski et al. | Jul 2014 | B2 |
8774280 | Tourapis et al. | Jul 2014 | B2 |
8797439 | Coley et al. | Aug 2014 | B1 |
8803977 | Uchima et al. | Aug 2014 | B2 |
8811708 | Fischer et al. | Aug 2014 | B2 |
8823813 | Manzel et al. | Sep 2014 | B2 |
8831370 | Archer | Sep 2014 | B2 |
8874374 | Bogucki | Oct 2014 | B2 |
8879789 | Figov et al. | Nov 2014 | B1 |
8879894 | Neuman et al. | Nov 2014 | B2 |
8884741 | Cavallaro et al. | Nov 2014 | B2 |
8897491 | Ambrus et al. | Nov 2014 | B2 |
8924163 | Hudson et al. | Dec 2014 | B2 |
9006617 | Mullen | Apr 2015 | B2 |
9075136 | Joao | Jul 2015 | B1 |
9805475 | Rubinstein et al. | Oct 2017 | B2 |
20040032924 | Judge, Jr. | Feb 2004 | A1 |
20040081369 | Gindele et al. | Apr 2004 | A1 |
20040160336 | Hoch et al. | Aug 2004 | A1 |
20040184529 | Henocq et al. | Sep 2004 | A1 |
20060009700 | Brumfield et al. | Jan 2006 | A1 |
20060049707 | Vuyyuru | Mar 2006 | A1 |
20060147116 | Le Clerc et al. | Jul 2006 | A1 |
20060251170 | Ali | Nov 2006 | A1 |
20070061043 | Ermakov et al. | Mar 2007 | A1 |
20070276270 | Tran | Nov 2007 | A1 |
20090010570 | Yamada et al. | Jan 2009 | A1 |
20100033579 | Yokohata et al. | Feb 2010 | A1 |
20100042000 | Schuhrke et al. | Feb 2010 | A1 |
20100091181 | Capps | Apr 2010 | A1 |
20100110100 | Anandasivam | May 2010 | A1 |
20100324423 | El-Aklouk et al. | Dec 2010 | A1 |
20100328352 | Shamier et al. | Dec 2010 | A1 |
20110019027 | Fujita et al. | Jan 2011 | A1 |
20110152729 | Oohashi et al. | Jun 2011 | A1 |
20120207218 | Asamura et al. | Aug 2012 | A1 |
20130060571 | Soemo et al. | Mar 2013 | A1 |
20130176424 | Weil | Jul 2013 | A1 |
20130201316 | Binder et al. | Aug 2013 | A1 |
20130342691 | Lewis et al. | Dec 2013 | A1 |
20140002667 | Cheben et al. | Jan 2014 | A1 |
20140072190 | Wu et al. | Mar 2014 | A1 |
20140072228 | Rubinstein et al. | Mar 2014 | A1 |
20140072229 | Wadhwa et al. | Mar 2014 | A1 |
20140112537 | Frank et al. | Apr 2014 | A1 |
20140169763 | Nayak et al. | Jun 2014 | A1 |
20140205175 | Tanaka et al. | Jul 2014 | A1 |
20140236036 | de Haan et al. | Aug 2014 | A1 |
20140341470 | Lee et al. | Nov 2014 | A1 |
20140368528 | Konnola | Dec 2014 | A1 |
20150134545 | Mann et al. | May 2015 | A1 |
20150221534 | van der Meulen | Aug 2015 | A1 |
20160171309 | Hay | Jun 2016 | A1 |
20160217587 | Hay | Jul 2016 | A1 |
20160217588 | Hay | Jul 2016 | A1 |
20160232686 | Park et al. | Aug 2016 | A1 |
20160300341 | Hay | Oct 2016 | A1 |
20170000356 | Smith, Sr. | Jan 2017 | A1 |
20170000392 | Smith | Jan 2017 | A1 |
20170119258 | Kotanko | May 2017 | A1 |
20170135626 | Singer | May 2017 | A1 |
20170221216 | Chen | Aug 2017 | A1 |
20180061063 | Buyukozturk | Mar 2018 | A1 |
20180177464 | DeBusschere | Jun 2018 | A1 |
20180225803 | Elgharib | Aug 2018 | A1 |
20180276823 | Barral | Sep 2018 | A1 |
20180296075 | Meglan | Oct 2018 | A1 |
20180335366 | Qiao | Nov 2018 | A1 |
20190206068 | Stark | Jul 2019 | A1 |
20200029891 | Swisher | Jan 2020 | A1 |
20200065957 | Hay | Feb 2020 | A1 |
Entry |
---|
Hay, J.R. “High Dynamic Range Imaging for the Detection of Motion”\pp. 18-141; dissertation University of Louisville (Kentucky); May 2011. |
Liu et al., “Motion magnification”, ACM Transactions on Graphics (TOG)—Proceedings of ACM SIGGRAPH 2005 TOG Homepage, vol. 24 Issue 3, Jul. 2005. |
Mazen, et al.; A vision-based approach for the direct measurement of displacements in vibrating systems; article from Smart Materials and Structures; 2003; 12; pp. 735-794; IOP Publishing LTD; UK. |
Meyer S., Sorkine-Homung A., Gross M. (2016) Phase-Based Modification Transfer for Video. In: Leibe B., Matas J., Sebe N., Welling M. (eds) Computer Vision—ECCV 2016. ECCV 201 6. Lecture Notes in Computer Science, vol. 9907. Springer, Cham. (Year: 2016). |
Miyatake K, Yamagishi M, Tanaka N, Uematsu M, Yamazaki N, Mine Y, Sano A, Hirama M. New method for evaluating left ventricular wall motion by color-coded tissue Doppler imaging: in vitro and in vivo studies. J Am Coll Cardiel. Mar. 1, 1995 ;25(3):717-24 (Year: 1995). |
Nobuo Yamazaki et al “Analysis of Ventricular Wall Motion Using Color-Coded Tissue Doppler Imaging System” 1994 Jpn. J. Appl. Phys. 33 3141 (Year: 1994). |
“Rubinstein et al. (“Revealing Invisible Changes in The World (YouTube)”, YouTube https://www.youtube.com/watch?v=e9ASH8IBJ2U, 2012”. |
“Wadhwa et al., “Phase-based Video Motion Processing”, also see YouTube https://www.youtube.com/watch? v=W7ZQFG7Nvw, SIGGRAPH 2013”. |
Wu et al., “Eulerian Video Magnification for Revealing Subtle Changes in the World”, ACM Transactions on Graphics (TOG)—Proceedings of ACM SIGGRAPH 2012 TOG Homepage, vol. 31 Issue 4, Jul. 2012, Article No. 65. |
Number | Date | Country | |
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62965382 | Jan 2020 | US |