Wir danken Susantha Wijesinghe, die entworfen und konstruiert, um das Bildkompressionssystem, das wir verwenden. Wir danken für die Unterstützung von der NSF Zuschuss DMR-1208990.

<ol>
	<li>Marcus, G., Parsa, S., Kramel, S., Ni, R., Voth, G. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Measurements+of+the+Solid-body+Rotation+of+Anisotropic+Particles+in+3D+Turbulence.">Measurements of the Solid-body Rotation of Anisotropic Particles in 3D Turbulence.</a> New J. Phys. 16, 102001 (2014).</li><li>Bretherton, F. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=The+motion+of+rigid+particles+in+a+shear+flow+at+low+Reynolds+number.">The motion of rigid particles in a shear flow at low Reynolds number.</a> J. Fluid Mech. 14 (02), 284-304 (1962).</li><li>Oullette, N., Xu, H., Bodenschatz, E. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=A+quantitative+study+of+three-dimensional+Lagrangian+particle+tracking+algorithms.">A quantitative study of three-dimensional Lagrangian particle tracking algorithms.</a> Exp. in Fluids. 40 (2), 301-313 (2006).</li><li>Parsa, S., Calzavarini, E., Toschi, F., Voth, G. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Rotation+Rate+of+Rods+in+Turbulent+Fluid.">Rotation Rate of Rods in Turbulent Fluid.</a> Phys. Rev. Lett. 109 (13), 134501 (2012).</li><li>Parsa, S., Voth, G. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Inertial+Range+Scaling+in+Rotations+of+Long+Rods+in+Turbulence.">Inertial Range Scaling in Rotations of Long Rods in Turbulence.</a> Phys. Rev. Lett. 112 (2), 024501 (2014).</li><li>Tsai, R. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=A+versatile+camera+calibration+technique+for+high-accuracy+3d+machine+vision+metrology+using+off-the-shelf+tv+cameras+and+lenses.">A versatile camera calibration technique for high-accuracy 3d machine vision metrology using off-the-shelf tv cameras and lenses.</a> IEEE Journal of Robotics and Automation. 3 (4), 323-344 (1987).</li><li>Blum, D., Kunwar, S., Johnson, J., Voth, G. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Effects+of+nonuniversal+large+scales+on+conditional+structure+functions+in+turbulence.">Effects of nonuniversal large scales on conditional structure functions in turbulence.</a> Phys. Fluids. 22 (1), 015107 (2010).</li><li>Mann, J., Ott, S., Andersen, J. S. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Experimental+study+of+relative,+turbulent+diffusion.">Experimental study of relative, turbulent diffusion.</a> RISO Internal Report. , (1999).</li><li>Chan, K., Stich, D., Voth, G. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Real-time+image+compression+for+high-speed+particle+tracking.">Real-time image compression for high-speed particle tracking.</a> Rev. Sci. 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Rev. Fluid Mech. 27, 469-514 (1995).</li><li>Su, L., Dahm, W. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Scalar+imaging+velocimetry+measurements+of+the+velocity+gradient+tensor+field+in+turbulent+flows.+I.+Assessment+of+errors.">Scalar imaging velocimetry measurements of the velocity gradient tensor field in turbulent flows. I. Assessment of errors.</a> Phys. Fluids. 8, 1869-1882 (1996).</li><li>L&#252;thi, B., Tsinober, A., Kinzelbach, W. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Lagrangian+measurement+of+vorticity+dynamics+in+turbulent+flow.">Lagrangian measurement of vorticity dynamics in turbulent flow.</a> J. Fluid Mech. 528, 87-118 (2005).</li><li>Frish, M., Webb, W. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Direct+measurement+of+vorticity+by+optical+probe.">Direct measurement of vorticity by optical probe.</a> J. Fluid Mech. 107, 173-200 (1981).</li><li>Zimmerman, R., et al. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Tracking+the+dynamics+of+translation+and+absolute+orientation+of+a+sphere+in+a+turbulent+flow.">Tracking the dynamics of translation and absolute orientation of a sphere in a turbulent flow.</a> Rev. Sci. Instrum. 82 (3), 033906 (2011).</li><li>Zimmerman, R., et al. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Rotational+Intermittency+and+Turbulence+Induced+Lift+Experienced+by+Large+Particles+in+a+Turbulent+Flow.">Rotational Intermittency and Turbulence Induced Lift Experienced by Large Particles in a Turbulent Flow.</a> Phys. Rev. Lett. 106 (15), 154501 (2011).</li><li>Klein, S., Gibert, M. a. t. h. i. e. u., B&#233;rut, A., Bodenschatz, E. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Simultaneous+3D+measurement+of+the+translation+and+rotation+of+finite-size+particles+and+the+flow+field+in+a+fully+developed+turbulent+water+flow.">Simultaneous 3D measurement of the translation and rotation of finite-size particles and the flow field in a fully developed turbulent water flow.</a> Meas. Sci. Technol. 24 (2), 1-10 (2013).</li><li>Bellani, G., Byron, M., Collignon, A., Meyer, C., Variano, E. <a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?db=PubMed&cmd=Search&doptcmdl=Citation&defaultField=Title+Word&term=Shape+effects+on+turbulent+modulation+by+large+nearly+neutrally+buoyant+particles.">Shape effects on turbulent modulation by large nearly neutrally buoyant particles.</a> J. Fluid Mech. 712, 41-60 (2012).</li></ol>

Die Autoren haben keine konkurrierenden finanziellen Interessen offen zu legen.

Die Messungen der Verwirbelung und die Rotation der Partikel in turbulenten Fluidstrom sind seit langem als wichtige Ziele in der experimentellen Strömungsmechanik erkannt worden. Der Festkörperdrehung von kleinen Kugeln in Turbulenzen ist gleich der Hälfte der Flüssigkeit Verwirbelung, aber die Rotationssymmetrie von Kugeln hat eine direkte Messung ihrer Festkörperrotation erschwert. Traditionell wurde die Flüssigkeit vorticity gemessen unter Verwendung komplexer, Multisensor, Hitzdraht-Sonden 14. Aber...

In einer kürzlich erschienenen Publikation haben wir die Verwendung von Partikeln aus mehreren schlanken Arme zur Messung von Drehbewegung von Teilchen in Turbulenzen 1 gemacht. Diese Partikel können mit Hilfe von 3D-Druckern hergestellt werden, und es ist möglich, genau ihre Position messen, Ausrichtung und Drehrate unter Verwendung mehrerer Kameras. Verwendung von Werkzeugen aus schlanken Körper Theorie kann gezeigt werden , dass diese Partikel zu denen ihrer jeweiligen wirksamen Ellipsoide wirksamen Ellipsoide 2 und die Drehbewegungen dieser Partikel sind identisch haben entspricht. Teilchen mit symmetrischen Armen gleicher Länge drehen wie Kugeln. Ein solches Teilchen ist eine Buchse, die drei zueinander senkrechten Armen hat in seiner Mitte angebracht ist. Einstellen der relativen Längen der Arme des Hebers kann ein Teilchen entspricht jeder dreiachsigen Ellipsoid bilden. Wenn die Länge eines Armes gleich Null gesetzt wird, entsteht ein Kreuz, dessen äquivalente Ellipsoid ist eine Scheibe. Teilchen aus slenderArme nehmen einen kleinen Teil des festen Volumen ihrer festen Ellipsoid-Pendants nach oben. Als Ergebnis sedimentieren sie langsamer, sie leichter zu Dichte Spiel zu machen. Dies ermöglicht die Untersuchung der viel größeren Teilchen als bei festen ellipsoidale Teilchen bequem ist. Zusätzlich können Bildgebung bei viel höheren Partikelkonzentrationen durchgeführt werden, da die Teilchen einen kleineren Bruchteil des Lichts von anderen Partikeln zu blockieren. In diesem Dokument werden Verfahren zur Herstellung und Verfolgung von 3D-gedruckten Teilchen dokumentiert. Werkzeuge für die Translationsbewegung von sphärischen Teilchen aus Partikelpositionen Verfolgungs wie durch mehrere Kameras gesehen wurden von mehreren Gruppen 3,4 entwickelt. Parsa et al. 5 erweitert diesen Ansatz Stangen der von mehreren Kameras gesehen Stangen unter Verwendung der Position und Orientierung zu verfolgen. Hier stellen wir Verfahren zur Partikel einer Vielzahl von Formen Herstellung und ihre 3D-Orientierungen zu rekonstruieren. Dies bietet the Möglichkeit 3D-Tracking von Partikeln mit komplexen Formen zu einer Vielzahl von neuen Anwendungen zu erweitern. Diese Technik hat ein großes Potenzial für die weitere Entwicklung aufgrund der Vielzahl von Partikelformen, die entworfen werden können. Viele dieser Formen haben direkte Anwendungen in der Umwelt fließt, wo Plankton, Samen und Eiskristalle von Formen in einem breiten Spektrum kommen. Die Verbindungen zwischen Partikel Drehungen und Grundklein Eigenschaften turbulenter Strömungen 6 deuten darauf hin , dass das Studium der Umdrehungen dieser Teilchen , neue Wege bei der turbulenten Kaskadenprozess zu suchen zur Verfügung stellt.

<table border="1" fo:keep-together.within-page="1" fo:keep-with-next.within-page="always">
	<tbody>
		<tr>
			<td>Condor Nd:YAG 50W laser</td>
			<td>Quantronics</td>
			<td>532-30-M</td>
			<td></td>
		</tr>
		<tr>
			<td>High speed camera</td>
			<td>Basler</td>
			<td>A504k</td>
			<td></td>
		</tr>
		<tr>
			<td>High speed camera</td>
			<td>Mikrotron</td>
			<td>EoSens Mc1362</td>
			<td></td>
		</tr>
		<tr>
			<td>Rhodamine-B</td>
			<td>ScienceLab.com</td>
			<td>SLR1465</td>
			<td></td>
		</tr>
		<tr>
			<td>Sodium Hydroxide</td>
			<td>Macron</td>
			<td>7708</td>
			<td>Pellets.</td>
		</tr>
		<tr>
			<td>500 Connex 3D printer</td>
			<td>Objet</td>
			<td></td>
			<td>Used to make smaller particles. Particles ordered from RP+M (rapid prototyping plus manufacturing).</td>
		</tr>
		<tr>
			<td>VeroClear</td>
			<td>Stratasys</td>
			<td>RGD810</td>
			<td>Objet build material.</td>
		</tr>
		<tr>
			<td>Form 1+ 3D printer</td>
			<td>Formlabs</td>
			<td></td>
			<td>Used to make larger particles.</td>
		</tr>
		<tr>
			<td>Clear Form 1 Photopolymer Resin</td>
			<td>Formlabs</td>
			<td></td>
			<td></td>
		</tr>
		<tr>
			<td>Cylindrical and spherical lenses</td>
			<td></td>
			<td></td>
			<td></td>
		</tr>
		<tr>
			<td>200, 100, 50 mm macro camera lenses</td>
			<td></td>
			<td></td>
			<td>F-mount.</td>
		</tr>
		<tr>
			<td>Ultrasonic bath</td>
			<td>Sonicator</td>
			<td></td>
			<td></td>
		</tr>
		<tr>
			<td>Calcium Chloride</td>
			<td>Spectrum Chemical Mfg. Corp.</td>
			<td>CAS 10043-52-2</td>
			<td>Pellets.</td>
		</tr>
		<tr>
			<td>LabVIEW System Design Software</td>
			<td>National Instruments</td>
			<td></td>
			<td>Used to trigger cameras, control grid, and trigger laser.</td>
		</tr>
		<tr>
			<td>XCAP Software</td>
			<td>EPIX</td>
			<td></td>
			<td>Used with LabVIEW to trigger cameras.</td>
		</tr>
		<tr>
			<td>MATLAB</td>
			<td>Mathworks</td>
			<td></td>
			<td>Used for all image and data analysis. Programs for extracting 3D orientations from multiple images are included with this publication.</td>
		</tr>
		<tr>
			<td>OpenPTV: Open Source Particle Tracking Velocimetry</td>
			<td>OpenPTV Consortium</td>
			<td></td>
			<td></td>
		</tr>
		<tr>
			<td>ParaView</td>
			<td>Kitware</td>
			<td></td>
			<td></td>
		</tr>
		<tr>
			<td>AutoCAD</td>
			<td>AutoDesk</td>
			<td></td>
			<td>Used to design all particles. Screenshots of particle designs are all of AutoCAD.</td>
		</tr>
		<tr>
			<td>Mesh with 0.040 x 0.053 inch holes</td>
			<td>Industrial Netting</td>
			<td>XN5170&#8211;43.5</td>
			<td></td>
		</tr>
		<tr>
			<td>Camera filters</td>
			<td>Schneider Optics</td>
			<td>B+W 040M</td>
			<td></td>
		</tr>
	</tbody>
</table>

methods for measuring the orientation and rotation rate of 3d-printed particles in turbulence

Experimentelle Methoden zur Messung der Rotations- und Translationsbewegung der anisotropen Teilchen in turbulenten Fluidströmen dargestellt. 3D-Drucktechnologie wird verwendet, Partikel mit schlanken Arme an einem gemeinsamen Zentrum verbunden herzustellen. Formen erforscht sind Kreuze (zwei senkrechten Stangen), Buchsen (drei senkrechten Stangen), Triaden (drei Stäbe in dreieckigen planaren Symmetrie) und Tetraden (vier Arme in tetraedrischer Symmetrie). Verfahren zum in der Größenordnung von 10.000 fluoreszenzgefärbten Partikeln werden beschrieben. Die zeitaufgelöste Messungen von ihrer Ausrichtung und Festkörperdrehrate von vier synchronisierten Videos ihrer Bewegung in einer turbulenten Strömung erhalten werden zwischen den Gittern mit R λ = 91. In diesem relativ niedriger Reynolds - Zahl Fluss oszilliert, sind die advektiert Partikel klein genug dass sie ellipsenförmigen Tracerpartikel nähern. Wir präsentieren Ergebnisse der zeitaufgelösten 3D Trajektorien von Position und Orientierung der Partikel alsund Messungen ihrer Drehraten.

3a zeigt ein Bild eines tetrad von einem unserer Kameras über ein Grundstück von der Euler aus einem Abschnitt seiner Bahn erhalten Winkel (Abbildung 3c). In 3b Algorithmus die Ergebnisse der Ausrichtung Findungs, beschrieben in Protokoll 5-5,3, auf dem Bild überlagert Tetrade. Die Arme der tetrad in 3a folgen nicht den einfachen Intensitätsverteilungen, die das Modell (Protokoll 5.1.3.1) verwendet werden , zu erstel...

Watch this Scientific Journal Video about Methods for Measuring the Orientation and Rotation Rate of 3D-printed Particles in Turbulence at JoVE.com

Methods for Measuring the Orientation and Rotation Rate of 3D-printed Particles in Turbulence

We use 3D printing to fabricate anisotropic particles in the shapes of jacks, crosses, tetrads, and triads, whose alignments and rotations in turbulent fluid flow can be measured from multiple simultaneous video images.

Verfahren zur Messung der Neigung und Drehrate von 3D-gedruckten Particles in Turbulence

Experimental methods are presented for measuring the rotational and translational motion of anisotropic particles in turbulent fluid flows. 3D printing ...

methods-for-measuring-orientation-rotation-rate-3d-printed-particles

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3-Dimensional Kinetics of a Rigid Body

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Dynamics of Rotational Motions

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10.0K Aufrufe.  Wesleyan University. We use 3D printing to fabricate anisotropic particles in the shapes of jacks, crosses, tetrads, and triads, whose alignments and rotations in turbulent fluid flow can be measured from multiple simultaneous video images.

Serie: Methods for Measuring the Orientation and Rotation Rate of 3D-printed Particles in Turbulence

Encapsulation and Permeability Characteristics of Plasma Polymerized Hollow Particles

In this protocol, core-shell nanostructures are synthesized by plasma enhanced chemical vapor deposition. We produce an amorphous barrier by plasma polymerization of isopropanol on various solid substrates, including silica and potassium chloride. This versatile technique is used to treat nanoparticles and nanopowders with sizes ranging from 37 nm to 1 micron, by depositing films whose thickness can be anywhere from 1 nm to upwards of 100 nm. Dissolution of the core allows us to study the rate of permeation through the film. In these experiments, we determine the diffusion coefficient of KCl through the barrier film by coating KCL nanocrystals and subsequently monitoring the ionic conductivity of the coated particles suspended in water. The primary interest in this process is the encapsulation and delayed release of solutes. The thickness of the shell is one of the independent variables by which we control the rate of release. It has a strong effect on the rate of release, which increases from a six-hour release (shell thickness is 20 nm) to a long-term release over 30 days (shell thickness is 95 nm). The release profile shows a characteristic behavior: a fast release (35% of the final materials) during the first five minutes after the beginning of the dissolution, and a slower release till all of the core materials come out.

We have used plasma enhanced chemical vapor deposition to deposit thin films ranging from a few nm to several 100 nm on nano-sized particles of various materials. We subsequently etch the core material to produce hollow nanoshells whose permeability is controlled by the thickness of the shell. We characterize the permeability of these coatings to small solutes and demonstrate that these barriers can provide sustained release of the core material over several days.

Encapsulation und Permeabilitätseigenschaften von plasmapolymerisierten Hohlteilchen

In this protocol, core-shell nanostructures are synthesized by plasma enhanced chemical vapor deposition. We produce an amorphous barrier by plasma ...

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Ingenieurwesen

Experimental Measurement of Settling Velocity of Spherical Particles in Unconfined and Confined Surfactant-based Shear Thinning Viscoelastic Fluids

An experimental study is performed to measure the terminal settling velocities of spherical particles in surfactant based shear thinning viscoelastic (VES) fluids. The measurements are made for particles settling in unbounded fluids&#160;and fluids between parallel walls. VES fluids over a wide range of rheological properties are prepared and rheologically characterized. The rheological characterization involves steady shear-viscosity and dynamic oscillatory-shear measurements to quantify the viscous and elastic properties respectively. The settling velocities under unbounded conditions are measured in beakers having diameters at least 25x the diameter of particles. For measuring settling velocities between parallel walls, two experimental cells with different wall spacing are constructed. Spherical particles of varying sizes are gently dropped in the fluids and allowed to settle. The process is recorded with a high resolution video camera and the trajectory of the particle is recorded using image analysis software. Terminal settling velocities are calculated from the data.
The impact of elasticity on settling velocity in unbounded fluids is quantified by comparing the experimental settling velocity to the settling velocity calculated by the inelastic drag predictions of Renaud et al.1&#160;Results show that elasticity of fluids can increase or decrease the settling velocity. The magnitude of reduction/increase is a function of the rheological properties of the fluids and properties of particles. Confining walls are observed to cause a retardation effect on settling and the retardation is measured in terms of wall factors.

This paper demonstrates the experimental procedure to measure terminal settling velocities of spherical particles in surfactant-based shear thinning viscoelastic fluids. Fluids over a wide range of rheological properties are prepared and settling velocities are measured for a range of particle sizes in unbounded fluids and fluids between parallel walls.

Experimentelle Messung der Settling Velocity von sphärischen Partikeln in unbeschränkten und geschlossenen Tensid-basierten Scherdünnungsviskoelastischen Flüssigkeiten

An experimental study is performed to measure the terminal settling velocities of spherical particles in surfactant based shear thinning viscoelastic ...

Automation of Mode Locking in a Nonlinear Polarization Rotation Fiber Laser through Output Polarization Measurements

When a laser is mode-locked, it emits a train of ultra-short pulses at a repetition rate determined by the laser cavity length. This article outlines a new and inexpensive procedure to force mode locking in a pre-adjusted nonlinear polarization rotation fiber laser. This procedure is based on the detection of a sudden change in the output polarization state when mode locking occurs. This change is used to command the alignment of the intra-cavity polarization controller in order to find mode-locking conditions. More specifically, the value of the first Stokes parameter varies when the angle of the polarization controller is swept and, moreover, it undergoes an abrupt variation when the laser enters the mode-locked state. Monitoring this abrupt variation provides a practical easy-to-detect signal that can be used to command the alignment of the polarization controller and drive the laser towards mode locking. This monitoring is achieved by feeding a small portion of the signal to a polarization analyzer measuring the first Stokes parameter. A sudden change in the read out of this parameter from the analyzer will occur when the laser enters the mode-locked state. At this moment, the required angle of the polarization controller is kept fixed. The alignment is completed. This procedure provides an alternate way to existing automating procedures that use equipment such as an optical spectrum analyzer, an RF spectrum analyzer, a photodiode connected to an electronic pulse-counter or a nonlinear detecting scheme based on two-photon absorption or second harmonic generation. It is suitable for lasers mode locked by nonlinear polarization rotation. It is relatively easy to implement, it requires inexpensive means, especially at a wavelength of 1550 nm, and it lowers the production and operation costs incurred in comparison to the above-mentioned techniques.

A protocol to detect and automate mode locking in a pre-adjusted nonlinear polarization rotation fiber laser is presented. The detection of a sudden change in the output polarization state when mode locking occurs is used to command the alignment of an intra-cavity polarization controller in order to find mode-locking conditions.

Automatisierung der Modenkopplung in einem nicht-linearen Polarisationsdrehung Faserlaser durch Ausgabe Polarisationsmessungen

When a laser is mode-locked, it emits a train of ultra-short pulses at a repetition rate determined by the laser cavity length. This article outlines a ...

Three-dimensional Particle Tracking Velocimetry for Turbulence Applications: Case of a Jet Flow

3D-PTV is a quantitative flow measurement technique that aims to track the Lagrangian paths of a set of particles in three dimensions using stereoscopic recording of image sequences. The basic components, features, constraints and optimization tips of a 3D-PTV topology consisting of a high-speed camera with a four-view splitter are described and discussed in this article. The technique is applied to the intermediate flow field (5 &#60;x/d &#60;25) of a circular jet at Re &#8776; 7,000. Lagrangian flow features and turbulence quantities in an Eulerian frame are estimated around ten diameters downstream of the jet origin and at various radial distances from the jet core. Lagrangian properties include trajectory, velocity and acceleration of selected particles as well as curvature of the flow path, which are obtained from the Frenet-Serret equation. Estimation of the 3D velocity and turbulence fields around the jet core axis at a cross-plane located at ten diameters downstream of the jet is compared with literature, and the power spectrum of the large-scale streamwise velocity motions is obtained at various radial distances from the jet core.

A three-dimensional particle tracking velocimetry (3D-PTV) system based on a high-speed camera with a four-view splitter is described here. The technique is applied to a jet flow from a circular pipe in the vicinity of ten diameters downstream at Reynolds number Re &#8776; 7,000.

Dreidimensionale Particle Tracking Velocimetry für Turbulence Anwendungen: Fall eines Jet Fluss

3D-PTV is a quantitative flow measurement technique that aims to track the Lagrangian paths of a set of particles in three dimensions using stereoscopic ...

Subsurface Defect Localization by Structured Heating Using Laser Projected Photothermal Thermography

The presented method is used to locate subsurface defects oriented perpendicularly to the surface. To achieve this, we create destructively interfering thermal wave fields that are disturbed by the defect. This effect is measured and used to locate the defect. We form the destructively interfering wave fields by using a modified projector. The original light engine of the projector is replaced with a fiber-coupled high-power diode laser. Its beam is shaped and aligned to the projector&#39;s spatial light modulator and optimized for optimal optical throughput and homogeneous projection by first characterizing the beam profile, and, second, correcting it mechanically and numerically. A high-performance infrared (IR) camera is set up according to the tight geometrical situation (including corrections of the geometrical image distortions) and the requirement to detect weak temperature oscillations at the sample surface. Data acquisition can be performed once a synchronization between the individual thermal wave field sources, the scanning stage, and the IR camera is established by using a dedicated experimental setup which needs to be tuned to the specific material being investigated. During data post-processing, the relevant information on the presence of a defect below the surface of the sample is extracted. It is retrieved from the oscillating part of the acquired thermal radiation coming from the so-called depletion line of the sample surface. The exact location of the defect is deduced from the analysis of the spatial-temporal shape of these oscillations in a final step. The method is reference-free and very sensitive to changes within the thermal wave field. So far, the method has been tested with steel samples but is applicable to different materials as well, in particular to temperature sensitive materials.

This method aims at locating vertical subsurface defects. Here, we couple a laser with a spatial light modulator and trigger its video input to heat a sample surface deterministically with two anti-phased modulated lines while acquiring highly resolved thermal images. The defect position is retrieved from evaluating thermal wave interference minima.

Untergrundfehler-Lokalisierung durch strukturierte Erwärmung mittels laserprojektierter photothermischer Thermografie

The presented method is used to locate subsurface defects oriented perpendicularly to the surface. To achieve this, we create destructively interfering ...

A 3D-printed Chamber for Organic Optoelectronic Device Degradation Testing

In this manuscript, we outline the manufacture of a small, portable, easy-to-use atmospheric chamber for organic and perovskite optoelectronic devices, using 3D-printing. As these types of devices are sensitive to moisture and oxygen, such a chamber can aid researchers in characterizing the electronic and stability properties. The chamber is intended to be used as a temporary, reusable, and stable environment with controlled properties (including humidity, gas introduction, and temperature). It can be used to protect air-sensitive materials or to expose them to contaminants in a controlled way for degradation studies. To characterize the properties of the chamber, we outline a simple procedure to determine the water vapor transmission rate (WVTR) using relative humidity as measured by a standard humidity sensor. This standard operating procedure, using a 50% infill density of polylactic acid (PLA), results in a chamber that can be used for weeks without any significant loss of device properties. The versatility and ease of use of the chamber allows it to be adapted to any characterization condition that requires a compact-controlled atmosphere.

Here, we present a protocol for the design, manufacture, and use of a simple, versatile 3D-printed and controlled atmospheric chamber for the optical and electrical characterization of air-sensitive organic optoelectronic devices.

Ein 3D-gedruckten Kammer für organische opto-elektronischen Gerät Abbau testen

In this manuscript, we outline the manufacture of a small, portable, easy-to-use atmospheric chamber for organic and perovskite optoelectronic devices, ...

Methods of Ex Situ and In Situ Investigations of Structural Transformations: The Case of Crystallization of Metallic Glasses

We demonstrate the use of two nuclear-based analytical methods that can follow the modifications of microstructural arrangement of iron-based metallic glasses (MGs). Despite their amorphous nature, the identification of hyperfine interactions unveils faint structural modifications. For this purpose, we have employed two techniques that utilize nuclear resonance among nuclear levels of a stable 57Fe isotope, namely M&#246;ssbauer spectrometry and nuclear forward scattering (NFS) of synchrotron radiation. The effects of heat treatment upon (Fe2.85Co1)77Mo8Cu1B14 MG are discussed using the results of ex situ and in situ experiments, respectively. As both methods are sensitive to hyperfine interactions, information on structural arrangement as well as on magnetic microstructure is readily available. M&#246;ssbauer spectrometry performed ex situ describes how the structural arrangement and magnetic microstructure appears at room temperature after the annealing under certain conditions (temperature, time), and thus this technique inspects steady states. On the other hand, NFS data are recorded in situ during dynamically changing temperature and NFS examines transient states. The use of both techniques provides complementary information. In general, they can be applied to any suitable system in which it is important to know its steady state but also transient states.

Methods of Ex Situ and In Situ Investigations of Structural Transformations: The Case of Crystallization of Metallic Glasses

Here, we present a protocol to describe ex situ and in situ investigations of structural transformations in metallic glasses. We employed nuclear-based analytical methods which inspect hyperfine interactions. We demonstrate the applicability of M&#246;ssbauer spectrometry and nuclear forward scattering of synchrotron radiation during temperature-driven experiments.

Methoden der Ex-Situ und In Situ Untersuchungen zu strukturellen Veränderungen: der Fall der Kristallisation von metallischen Gläsern

We demonstrate the use of two nuclear-based analytical methods that can follow the modifications of microstructural arrangement of iron-based metallic ...

Applicability Analysis of Assessment Methods for Morphological Parameters of Corroded Steel Bars

The irregular and uneven residual sections along the length of a corroded steel bar substantially change its mechanical properties and significantly dominate the safety and performance of an existing concrete structure. As a result, it is important to measure the geometry and amount of corrosion of a steel bar in a structure properly to assess the residual bearing capacity and service life of the structure. This paper introduces and compares five different methods for measuring the geometry and amount of corrosion of a steel bar. A single 500 mm long and 14 mm diameter steel bar is the specimen that is subjected to accelerated corrosion in this protocol. Its morphology and the amount of corrosion were carefully measured before and after using mass loss measurements, a Vernier caliper, drainage measurements, 3D scanning, and X-ray micro-computed tomography (XCT). The applicability and suitability of these different methods were then evaluated. The results show that the Vernier caliper is the best choice for measuring the morphology of a non-corroded bar, while 3D scanning is the most suitable for quantifying the morphology of a corroded bar.

This paper measures the geometry and the amount of corrosion of a steel bar using different methods: mass loss, calipers, drainage measurements, 3D scanning, and X-ray micro-computed tomography (XCT).

Anwendbarkeit Analyse der Bewertungsmethoden für morphologische Parameter der korrodierten Stabstahl

The irregular and uneven residual sections along the length of a corroded steel bar substantially change its mechanical properties and significantly ...

Simultaneous Measurement of Turbulence and Particle Kinematics Using Flow Imaging Techniques

Numerous problems in scientific and engineering fields involve understanding the kinematics of particles in turbulent flows, such as contaminants, marine micro-organisms, and/or sediments in the ocean, or fluidized bed reactors and combustion processes in engineered systems. In order to study the effect of turbulence on the kinematics of particles in such flows, simultaneous measurements of both the flow and particle kinematics are required. Non-intrusive, optical flow measurement techniques for measuring turbulence, or for tracking particles, exist but measuring both simultaneously can be challenging due to interference between the techniques. The method presented herein provides a low cost and relatively simple method to make simultaneous measurements of the flow and particle kinematics. A cross section of the flow is measured using a particle image velocimetry (PIV) technique, which provides two components of velocity in the measurement plane. This technique utilizes a pulsed-laser for illumination of the seeded flow field that is imaged by a digital camera. The particle kinematics are simultaneously imaged using a light emitting diode (LED) line light that illuminates a planar cross section of the flow that overlaps with the PIV field-of-view (FOV). The line light is of low enough power that it does not affect the PIV measurements, but powerful enough to illuminate the larger particles of interest imaged using the high-speed camera. High-speed images that contain the laser pulses from the PIV technique are easily filtered by examining the summed intensity level of each high-speed image. By making the frame rate of the high-speed camera incommensurate with that of the PIV camera frame rate, the number of contaminated frames in the high-speed time series can be minimized. The technique is suitable for mean flows that are predominantly two-dimensional, contain particles that are at least 5 times the mean diameter of the PIV seeding tracers, and are low in concentration.

The technique described herein offers a low cost and relatively simple method to simultaneously measure particle kinematics and turbulence in flows with low particle concentrations. The turbulence is measured using particle image velocimetry (PIV), and particle kinematics are calculated from images obtained with a high-speed camera in an overlapping field-of-view.

Gleichzeitige Messung von Turbulenzen und Partikel-Kinematik mit bildgebenden Verfahren

Numerous problems in scientific and engineering fields involve understanding the kinematics of particles in turbulent flows, such as contaminants, marine ...

Measurement of Dynamic Force Acted on Water Strider Leg Jumping Upward by the PVDF Film Sensor

This study aimed to make an explanation for the phenomenon in nature that water strider usually jumps or glides on the water surface easily but quickly, with its peak locomotion speed reaching 150 cm/s. First of all, we observed the microstructure and hierarchy of water strider legs using the scanning electron microscope. On the basis of the observed morphology of the legs, a theoretical model of the detachment from water surface was established, which explained water striders' capability to slide on water surface effortlessly in terms of energy reduction. Secondly, a dynamic force measurement system was devised using the PVDF film sensor with excellent sensitivity, which could detect the whole interaction process. Subsequently, a single leg in contact with water was pulled upward at different speeds, and the adhesion force was measured at the same time. The results of the departing experiment suggested a deep understanding of the fast jumping of water striders.

The protocol here is dedicated to investigating the free and quick maneuvering of water strider on water surface. The protocol includes observing the microstructure of legs and measuring the adhesion force when departing from water surface at different speeds.

Messung der dynamischen Kraft gehandelt auf Wasser Strider Bein nach oben springen, indem Sie die PVDF Film Sensor

This study aimed to make an explanation for the phenomenon in nature that water strider usually jumps or glides on the water surface easily but quickly, ...