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digital particle image velocimetry tool pivlab  (MathWorks Inc)


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    MathWorks Inc digital particle image velocimetry tool pivlab
    Digital Particle Image Velocimetry Tool Pivlab, supplied by MathWorks Inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
    https://www.bioz.com/product/particle+image+velocimetry+pivlab/pmc12269425-158-12-20
    Average 90 stars, based on 1 article reviews
    digital particle image velocimetry tool pivlab - by Bioz Stars, 2026-09
    90/100 stars

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    Related Articles

    other:

    Article Title: Loss of E-cadherin is causal to pathologic changes in chronic lung disease
    Article Snippet: Cellular velocity was quantified by performing Particle Image Velocimetry (PIVlab) on Matlab (R2020a), using multi-pass cross-correlation analysis with decreasing interrogation window size on image pairs to obtain the spatial velocity as described previously by us .

    Article Title: Acoustophoresis of monodisperse oil droplets in water: Effect of symmetry breaking and non-resonance operation on oil trapping behavior
    Article Snippet: To get the localized velocity field around the trapping location, particle image velocimetry (PIV) was performed using the MATLAB tool PIVlab (see section “Particle image velocimetry results” in the supplementary material for details of PIV analysis). shows the snapshots of the 5 th time frame (2.5 s) of the PIV movie for SO droplets in SDS100 solution (see Movies S6 and S7 in the supplementary material for the combined zoomed-in videos with the PIV results of SO and HD droplets in SDS100, respectively).

    Article Title: Loss of E-cadherin is causal to pathologic changes in chronic lung disease.
    Article Snippet: Cellular velocity was quantified by performing Particle Image Velocimetry (PIVlab) on Matlab (R2020a), using multi-pass cross-correlation analysis with decreasing interrogation window size on image pairs to obtain the spatial velocity as described previously by us48.

    Article Title: Regulation of collective cell polarity and migration using dynamically adhesive micropatterned substrates.
    Article Snippet: Collective cell migration is a fundamental biological process in which groups of cells move together in a coordinated manner, and it is essential for tissue development and wound repair.. However, the underlying mechanisms that orchestrate directionality in collectively migrating cells remain poorly understood.. In this study, we employed dynamically adhesive micropatterned substrates to investigate the role of adhesive cues in directing epithelial migration.

    Article Title: Periodic splay Fréedericksz transitions in a ferroelectric nematic.
    Article Snippet: In (a–d), d= (3.0 ±0.1)μm; applied voltage from the source Urms=30V, 200kHz sinusoidal waveform; 120 °C. e Particle image velocimetry (PIVlab, Matlab) integrated trajectories of fluorescent spherical flow tracers of the diameter 300nm in the square lattice of +1/−1 defects; d= (4.8 ±0.1)μm cell; sinusoidal wave of voltage 4.5 V and frequency f= 200kHz; 115 °C. f the same cell, in-plane velocity field of the tracers.

    Bacteria:

    Article Title: Pattern formation along signaling gradients driven by active droplet behaviour of cell groups
    Article Snippet: .. To estimate the flow field of bacteria , particle image velocimetry (using PIVlab, Matlab) was applied to the bacteria (green) and cell nuclei (red) channels of each 2D plane (parallel to the direction of swarm travel) and then averaged (500μm) at each time point. ..

    Shear:

    Article Title: High-speed ultrasound imaging of bubbly flows and shear waves in soft matter.
    Article Snippet: .. The high-speed optical videos obtained for both the jetting dynamics and the propagation of the resultant shear waves, were analyzed by implementing particle image velocimetry (PIV) using an open source code MATLAB named PIVlab.36,37 The generation of the US high-speed images requires subsequent processing of the scattered acoustic signals captured by the ultrasound transducer. ..

    Migration:

    Article Title: Effect of sub-chronic exposure to cigarette smoke, electronic cigarette and waterpipe on human lung epithelial barrier function
    Article Snippet: .. Cell migration was quantified by performing Particle Image Velocimetry (PIVlab) on Matlab using multi-pass cross-correlation analysis with decreasing interrogation window size on image pairs to obtain the spatial velocity field as described previously [ ]. .. Total RNA was isolated from cultured primary bronchial epithelial cells and purified using a column kit supplemented with the Proteinase K and RNase-Free Dnase Set, and cDNA of 1000 ng·μL − 1 was obtained using a cDNA Reverse Transcription Kit (Qiagen).



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    a PolScope Microimager texture of the in-plane splay and bend for the normal incidence of light; wavelength 535 nm. b Polarizing microscopy of square lattice of +1/−1 defects. c Potential difference measured at the N F cell electrodes; the generated voltage. d Transmitted intensity as a function of time at locations L1’–L4’. \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${{\bf{P}}}$$\end{document} P oscillates with the frequency of the applied field. Incident laser beam makes an angle \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\beta=$$\end{document} β = 15° with the normal \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\hat{{{\bf{z}}}}$$\end{document} z ^ to the cell. Dashed line corresponds to zero voltage. In ( a – d ), \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$d$$\end{document} d = (3.0 ± 0.1) μm; applied voltage from the source U rms = 30 V, 200 kHz sinusoidal waveform; 120 °C. e Particle image <t>velocimetry</t> <t>(PIVlab,</t> Matlab) integrated trajectories of fluorescent spherical flow tracers of the diameter 300 nm in the square lattice of +1/−1 defects; d = (4.8 ± 0.1) μm cell; sinusoidal wave of voltage 4.5 V and frequency f = 200 kHz; 115 °C. f the same cell, in-plane velocity field of the tracers.
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    a PolScope Microimager texture of the in-plane splay and bend for the normal incidence of light; wavelength 535 nm. b Polarizing microscopy of square lattice of +1/−1 defects. c Potential difference measured at the N F cell electrodes; the generated voltage. d Transmitted intensity as a function of time at locations L1’–L4’. \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${{\bf{P}}}$$\end{document} P oscillates with the frequency of the applied field. Incident laser beam makes an angle \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\beta=$$\end{document} β = 15° with the normal \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\hat{{{\bf{z}}}}$$\end{document} z ^ to the cell. Dashed line corresponds to zero voltage. In ( a – d ), \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$d$$\end{document} d = (3.0 ± 0.1) μm; applied voltage from the source U rms = 30 V, 200 kHz sinusoidal waveform; 120 °C. e Particle image <t>velocimetry</t> <t>(PIVlab,</t> Matlab) integrated trajectories of fluorescent spherical flow tracers of the diameter 300 nm in the square lattice of +1/−1 defects; d = (4.8 ± 0.1) μm cell; sinusoidal wave of voltage 4.5 V and frequency f = 200 kHz; 115 °C. f the same cell, in-plane velocity field of the tracers.
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    a PolScope Microimager texture of the in-plane splay and bend for the normal incidence of light; wavelength 535 nm. b Polarizing microscopy of square lattice of +1/−1 defects. c Potential difference measured at the N F cell electrodes; the generated voltage. d Transmitted intensity as a function of time at locations L1’–L4’. \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${{\bf{P}}}$$\end{document} P oscillates with the frequency of the applied field. Incident laser beam makes an angle \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\beta=$$\end{document} β = 15° with the normal \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\hat{{{\bf{z}}}}$$\end{document} z ^ to the cell. Dashed line corresponds to zero voltage. In ( a – d ), \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$d$$\end{document} d = (3.0 ± 0.1) μm; applied voltage from the source U rms = 30 V, 200 kHz sinusoidal waveform; 120 °C. e Particle image <t>velocimetry</t> <t>(PIVlab,</t> Matlab) integrated trajectories of fluorescent spherical flow tracers of the diameter 300 nm in the square lattice of +1/−1 defects; d = (4.8 ± 0.1) μm cell; sinusoidal wave of voltage 4.5 V and frequency f = 200 kHz; 115 °C. f the same cell, in-plane velocity field of the tracers.
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    a PolScope Microimager texture of the in-plane splay and bend for the normal incidence of light; wavelength 535 nm. b Polarizing microscopy of square lattice of +1/−1 defects. c Potential difference measured at the N F cell electrodes; the generated voltage. d Transmitted intensity as a function of time at locations L1’–L4’. \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${{\bf{P}}}$$\end{document} P oscillates with the frequency of the applied field. Incident laser beam makes an angle \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\beta=$$\end{document} β = 15° with the normal \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\hat{{{\bf{z}}}}$$\end{document} z ^ to the cell. Dashed line corresponds to zero voltage. In ( a – d ), \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$d$$\end{document} d = (3.0 ± 0.1) μm; applied voltage from the source U rms = 30 V, 200 kHz sinusoidal waveform; 120 °C. e Particle image <t>velocimetry</t> <t>(PIVlab,</t> Matlab) integrated trajectories of fluorescent spherical flow tracers of the diameter 300 nm in the square lattice of +1/−1 defects; d = (4.8 ± 0.1) μm cell; sinusoidal wave of voltage 4.5 V and frequency f = 200 kHz; 115 °C. f the same cell, in-plane velocity field of the tracers.
    Particle Image Velocimetry Tool Pivlab, supplied by MathWorks Inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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    a PolScope Microimager texture of the in-plane splay and bend for the normal incidence of light; wavelength 535 nm. b Polarizing microscopy of square lattice of +1/−1 defects. c Potential difference measured at the N F cell electrodes; the generated voltage. d Transmitted intensity as a function of time at locations L1’–L4’. \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${{\bf{P}}}$$\end{document} P oscillates with the frequency of the applied field. Incident laser beam makes an angle \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\beta=$$\end{document} β = 15° with the normal \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\hat{{{\bf{z}}}}$$\end{document} z ^ to the cell. Dashed line corresponds to zero voltage. In ( a – d ), \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$d$$\end{document} d = (3.0 ± 0.1) μm; applied voltage from the source U rms = 30 V, 200 kHz sinusoidal waveform; 120 °C. e Particle image <t>velocimetry</t> <t>(PIVlab,</t> Matlab) integrated trajectories of fluorescent spherical flow tracers of the diameter 300 nm in the square lattice of +1/−1 defects; d = (4.8 ± 0.1) μm cell; sinusoidal wave of voltage 4.5 V and frequency f = 200 kHz; 115 °C. f the same cell, in-plane velocity field of the tracers.
    Particle Image Velocimetry Pivlab Plugin, supplied by MathWorks Inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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    MathWorks Inc particle image velocimetry pivlab package
    a PolScope Microimager texture of the in-plane splay and bend for the normal incidence of light; wavelength 535 nm. b Polarizing microscopy of square lattice of +1/−1 defects. c Potential difference measured at the N F cell electrodes; the generated voltage. d Transmitted intensity as a function of time at locations L1’–L4’. \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${{\bf{P}}}$$\end{document} P oscillates with the frequency of the applied field. Incident laser beam makes an angle \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\beta=$$\end{document} β = 15° with the normal \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\hat{{{\bf{z}}}}$$\end{document} z ^ to the cell. Dashed line corresponds to zero voltage. In ( a – d ), \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$d$$\end{document} d = (3.0 ± 0.1) μm; applied voltage from the source U rms = 30 V, 200 kHz sinusoidal waveform; 120 °C. e Particle image <t>velocimetry</t> <t>(PIVlab,</t> Matlab) integrated trajectories of fluorescent spherical flow tracers of the diameter 300 nm in the square lattice of +1/−1 defects; d = (4.8 ± 0.1) μm cell; sinusoidal wave of voltage 4.5 V and frequency f = 200 kHz; 115 °C. f the same cell, in-plane velocity field of the tracers.
    Particle Image Velocimetry Pivlab Package, supplied by MathWorks Inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
    https://www.bioz.com/product/particle+image+velocimetry+pivlab/pmc11717197-253-13-16
    Average 90 stars, based on 1 article reviews
    particle image velocimetry pivlab package - by Bioz Stars, 2026-09
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    Image Search Results


    a PolScope Microimager texture of the in-plane splay and bend for the normal incidence of light; wavelength 535 nm. b Polarizing microscopy of square lattice of +1/−1 defects. c Potential difference measured at the N F cell electrodes; the generated voltage. d Transmitted intensity as a function of time at locations L1’–L4’. \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${{\bf{P}}}$$\end{document} P oscillates with the frequency of the applied field. Incident laser beam makes an angle \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\beta=$$\end{document} β = 15° with the normal \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\hat{{{\bf{z}}}}$$\end{document} z ^ to the cell. Dashed line corresponds to zero voltage. In ( a – d ), \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$d$$\end{document} d = (3.0 ± 0.1) μm; applied voltage from the source U rms = 30 V, 200 kHz sinusoidal waveform; 120 °C. e Particle image velocimetry (PIVlab, Matlab) integrated trajectories of fluorescent spherical flow tracers of the diameter 300 nm in the square lattice of +1/−1 defects; d = (4.8 ± 0.1) μm cell; sinusoidal wave of voltage 4.5 V and frequency f = 200 kHz; 115 °C. f the same cell, in-plane velocity field of the tracers.

    Journal: Nature Communications

    Article Title: Periodic splay Fréedericksz transitions in a ferroelectric nematic

    doi: 10.1038/s41467-025-55827-9

    Figure Lengend Snippet: a PolScope Microimager texture of the in-plane splay and bend for the normal incidence of light; wavelength 535 nm. b Polarizing microscopy of square lattice of +1/−1 defects. c Potential difference measured at the N F cell electrodes; the generated voltage. d Transmitted intensity as a function of time at locations L1’–L4’. \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${{\bf{P}}}$$\end{document} P oscillates with the frequency of the applied field. Incident laser beam makes an angle \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\beta=$$\end{document} β = 15° with the normal \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\hat{{{\bf{z}}}}$$\end{document} z ^ to the cell. Dashed line corresponds to zero voltage. In ( a – d ), \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$d$$\end{document} d = (3.0 ± 0.1) μm; applied voltage from the source U rms = 30 V, 200 kHz sinusoidal waveform; 120 °C. e Particle image velocimetry (PIVlab, Matlab) integrated trajectories of fluorescent spherical flow tracers of the diameter 300 nm in the square lattice of +1/−1 defects; d = (4.8 ± 0.1) μm cell; sinusoidal wave of voltage 4.5 V and frequency f = 200 kHz; 115 °C. f the same cell, in-plane velocity field of the tracers.

    Article Snippet: Their trajectories are uncovered by particle image velocimetry package PIVLab in Matlab.

    Techniques: Microscopy, Generated