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Algorithm particle tracking

The particle-tracking algorithm is tested for the rigid body rotation of fluid in a circular channel as shown in Fig. 8. The radius of the outer boundary and the width of the channel are set to = 1 and = 0.2, respectively. The velocity field is specified as u =yo y and v = x -Xo where x andy are the two-dimensional Cartesian coordinates and and... [Pg.214]

Jacobs, G. B., D. A. Kopriva, and F. Mashayek. 2001. A particle tracking algorithm for the multidomain staggered-grid spectral method. AIAA Paper No. 2001-0630. [Pg.29]

A sample particle is immobilized on a slide and the measurement noise (X easCO) is calculated with the help of a particle-tracking algorithm. [Pg.216]

In a separate experiment, a sample particle is allowed to freely diffuse in the fluid, while its center of mass is estimated at regular time intervals (30 ms suffices for a micron-sized particle in water at room temperature) using the particle-tracking algorithm. [Pg.216]

Particle tracking algorithms have also been used successfully in measurements of two- and three-dimensional diffusion [9], slip velocity [10], and colloidal electrokinetics [11]. In the context of experimental fluid mechanics studies, researchers found that the Brownian, thermal motion of sub-micron-sized particles suspended in a fluid is significant and may mask the... [Pg.1057]

Cross Correlation Displacement of particles in PIV image pairs is calculated based on correlation approach in contrast to the particle tracking algorithm, where particle path is followed. Here, the average motion of a small group of particles contained in the interrogation spot is calculated by spatial autocorrelation or cross correlation. Autocorrelation is performed when images for both laser pulses are recorded on the same sensor, while in cross correlation, each pulse is collected into separate frames. Cross-correlation calculation can be carried out faster... [Pg.418]

Coupled methods (transport model coupled with hydrogeochemical code) For coupled models solving the transport equation can be done by means of the finite-difference method (and finite volumes) and of the finite-elements method. Algorithms based on the principle of particle tracking (or random walk), as for instance the method of characteristics (MOC), have the advantage of not being prone to numerical dispersion (see 1.3.3.4.1). [Pg.63]

Rodrfguez-Rodrfguez J, Martmez-Bazan C, Montaiies JL (2003) A novel particle tracking and break-up detection algorithm application to the turbulent break-up of bubbles. Meas Sci Technol 14(8) 1328-1340... [Pg.864]

Ishikawa M, Murai Y, Wada A, Iguchi M, Okamoto K, Yamamoto F (2000) A novel algorithm for particle tracking velocimetry using the velocity gradient tensor. Exp Fluids 29 519-531... [Pg.2086]

The variable is defined with respect to the axis of the fragmentation jet which is reconstructed from charged particle tracks only. The tracks are clustered by a jet algorithm (TrackJets) and a combined transverse energy of > 1 GeV is required. In order to facilitate the comparison between the measurement and the theory predictions, the TrackJet is not included in the cross section definition. The extrapolation of the measured cross-section amounts to 10%. [Pg.42]

TrackJets are obtained when using only charged particle tracks as input to the jet algorithm. They are expected to give a better result when reconstructing low... [Pg.46]

The qualitative increase stems from the need to perform particle tracking, a task which has no equivalent in one dimension, since particles never leave the element in which they are initially located as they are carried by the velocity field. The generic term particle tracking actually involves a number of nontrivial individual subtasks, which must be tackled efficiently if CONNFFESSIT is to be viable. The key to practicable micro/macro computations is the invention of efficient schemes of reduced algorithmic complexity. [Pg.518]

A further increase to three spatial dimensions brings about another increase in the size of the problem. The tracking techniques are, however, not more complex than in the two-dimensional case. Furthermore, some of the algorithms to be presented perform proportionally better than classical continuum-mechanical tools the larger a problem is. For this reason, the two-dimensional case is especially critical it involves particle tracking in its full complexity, yet typical 2D problem sizes are not yet in the range where the CONNFFESSIT approach can even remotely compete with traditional methods. [Pg.518]

The optimal order of the tracking algorithm is thus determined by the ratio of particle tracking to particle simulation. [Pg.533]

FIG. 7 Effect of order of tracking algorithm on particle trajectories close to impenetrable boundaries (a) first-order Euler, (b) trapezoidal rule, (c) 12th-order Adams-Bashforth PC. [Pg.536]


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See also in sourсe #XX -- [ Pg.214 ]




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