scholarly journals 3-D Micro-PIV Using High-speed 3-D Confocal Imaging Technique

2006 ◽  
Vol 26 (Supplement2) ◽  
pp. 233-236
Author(s):  
Haruyuki KINOSHITA ◽  
Marie OSHIMA ◽  
Shohei KANEDA ◽  
Teruo FUJII
2006 ◽  
Vol 17 (7) ◽  
pp. 1639-1646 ◽  
Author(s):  
K P Angele ◽  
Y Suzuki ◽  
J Miwa ◽  
N Kasagi
Keyword(s):  

2005 ◽  
Vol 295-296 ◽  
pp. 477-482
Author(s):  
K.W. Wang ◽  
Z.J. Cai ◽  
Li Jiang Zeng

A two-dimensional surface profile imaging technique based on heterodyne interferometer is proposed. A piezo translator vibrated grating is used to generate a heterodyne signal. A high speed CCD camera is used to extract the interference signal using a five step method. The uncertainty in the displacement measurement is approximately 0.035 µm within a measurement range of 1.7 µm, confirming the two dimensional heterodyne interferometer is valid for measuring the surface profile. The method is also available for low coherence heterodyne interferometer due to the optical frequency shifts caused by the vibration of grating independent on the wavelength.


2002 ◽  
Author(s):  
Christel Rousseau ◽  
John M. Girkin ◽  
Shilpa Vaidya ◽  
Andrew F. Hall ◽  
C. J. Whitters ◽  
...  

2011 ◽  
Vol 100 (3) ◽  
pp. 558a
Author(s):  
Vyacheslav M. Shkryl ◽  
Joshua T. Maxwell ◽  
Lothar A. Blatter

2000 ◽  
Vol 6 (S2) ◽  
pp. 814-815
Author(s):  
Rudolf E. Großkopf

CCD sensors are able to image a few megapixels within one frame. The image is scanned electronically within the semiconductor chip (instead of mechanical-optical scanning with moving mirrors, Nipkow discs or acousto-optical devices). Through parallelization. the novel concept yields speed at an unprecedented degree for confocal imaging Routine applications requiring high speed and low costs will profit from this principle. Thus, confocal imaging technology will take the same path television technology has taken—from mechanical scanning to the broadest possible application of electronicsIn order to go this way, a pinhole matrix is used on the illumination side. It has as many pinholes and the same pitch as the pitch and number of pixels of the CCD (Figure 1). In front of the receiver, a second pinhole matrix with the same pitch and number of pinholes is used All pinholes of both matrices and the pixels of the CCD are in confocal position.


2016 ◽  
Vol 110 (3) ◽  
pp. 165a ◽  
Author(s):  
Simon P. Poland ◽  
James A. Levitt ◽  
Nikola Krstajić ◽  
Ahmet Erdogen ◽  
Richard J. Walker ◽  
...  

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