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Doppler velocimetry

This system produces a steady laminar flow with a flat velocity profile at the burner exit for mean flow velocities up to 5m/s. Velocity fluctuations at the burner outlet are reduced to low levels as v /v< 0.01 on the central axis for free jet injection conditions. The burner is fed with a mixture of methane and air. Experiments-described in what follows are carried out at fixed equivalence ratios. Flow perturbations are produced by the loudspeaker driven by an amplifier, which is fed by a sinusoidal signal s)mthesizer. Velocity perturbations measured by laser doppler velocimetry (LDV) on the burner symmetry axis above the nozzle exit plane are also purely sinusoidal and their spectral... [Pg.82]

There are many nonintrusive experimental tools available that can help scientists to develop a good picture of fluid dynamics and transport in chemical reactors. Laser Doppler velocimetry (LDV), particle image velocimetry (PIV) and sonar Doppler for velocity measurement, planar laser induced fluorescence (PLIF) for mixing studies, and high-speed cameras and tomography are very useful for multiphase studies. These experimental methods combined with computational fluid dynamics (CFDs) provide very good tools to understand what is happening in chemical reactors. [Pg.331]

Ultrasonic Doppler velocimetry is a nonintrusive technique that has been developed into a very useful technique for opaque liquid flows [3]. This technique provides good measurement of velocity new high-frequency techniques give a space resolution on the millimeter level, and even the large turbulent scales can be resolved. [Pg.333]

Davies, R. and Prcece, A.W. (1983). The electrophoretic mobilities of minerals determined by laser Doppler velocimetry and their relationship with the biological effects of dusts towards macrophages. Clin. Phys. Physiol. Meas. 4, 129-140,... [Pg.257]

LCR Locus control region LDH Lactate dehydro nase LDL Low-density lipoprotein LDV Laser Doppler velocimetry Le (Lewis X) leucocyte ligand for selectin... [Pg.283]

The discussion above that led to Eqs. (4.2.6 and 4.2.7) assumes that the no-slip condition at the wall of the pipe holds. There is no such assumption in the theory for the spatially resolved measurements. We have recently used a different technique for spatially resolved measurements, ultrasonic pulsed Doppler velocimetry, to determine both the viscosity and wall slip velocity in a food suspension [2]. From a rheological standpoint, the theoretical underpinnings of the ultrasonic technique are the same as for the MRI technique. Flence, there is no reason in principle why MRI can not be used for similar measurements. [Pg.389]

J. Bouillard, B. Alban, P. Jacques, C. Xuereb 2001, (Liquid flow velocity measurements in stirred tanks by ultrasound doppler velocimetry), Chem. Eng. Sci. 56, 747. [Pg.455]

See also Planar cavity surface-emitting laser (PCSEL) diodes Vertical cavity surface-emitting laser (VCSEL) diodes compound semiconductor-based, 22 179 Laser Doppler velocimetry (LDV), 11 784 Laser Doppler velocimeters, 11 675 Laser-drilled surgical needles, 24 206 Laser dye energy levels, 14 702-703 Laser fabrication techniques, titanium, 24 857... [Pg.510]

In homogeneous turbulence, the one-point joint velocity PDF can be written as /u(V t), and can be readily measured using hot-wire anemometry or laser Doppler velocimetry (LDV). [Pg.49]

The zeta potential of the formulations was determined by Doppler velocimetry and PCS on a Zetasizer 4 (Malvern Instruments, U.K.), without further dilution. The zeta potential of LC-AmB under these conditions was —44 mV, slightly lower than that measured for the same lipid composition without AmB, —55 mV, but remaining consistent with colloidal stability. This reduction in the absolute value of the zeta potential could be due to the presence of AmB at the surface, because free AmB dispersed in water under the same conditions had a less negative zeta potential about —27 mV. [Pg.98]

In an earlier phase of this work [9] the intensities of axial and circumferential components of velocity fluctuation were measured in the TC annulus, using Laser Doppler Velocimetry (LDV), for a wide range of cylinder rotation speeds. On average, the intensities of axial velocity fluctuations were found to be within 25% of the intensities of circumferential velocity fluctuations [9]. As in Ronney et al. [5], turbulence intensities were found to be nearly homogeneous along the axial direction and over most of the annulus width, and to be linearly proportional... [Pg.244]

Campbell and Hanratty (1982) used Lau s (1980) measurements with some special optics on a laser Doppler velocimetry system to calculate /3(f) near a fixed interface, in this case, the inside of a clear pipe. They determined w(z,t) from equation (8.52), and solved equations (8.49) and (8.50) numerically for / l(0- Finally, they applied equation (8.51) to determine Kl, which has been the goal all along. The end results (Kl) may then be related to the other, independent parameters that are important to the transfer process, such as diffusivity, viscosity, and turbulence parameters. Campbell and Hanratty performed this operation and found the following correlation ... [Pg.220]

Bickel, W. S., J. F. Davidson, D. R. Huffman, and R. Kilkson, 1976. Application of polarization effects in light scattering a new biophysical tool, Proc. Natl. Acad. Sci. USA, 73, 486-490. Bilbro, J. W., 1980. Atmospheric laser Doppler velocimetry an overview, Opt. Eng., 19, 533-542. Blanchard, D. C., 1967. From Raindrops to Volcanoes Adventure with Sea Surface Meteorology, Doubleday, New York. [Pg.501]

Rotmensch S, Liberati M, Celentano C, Efrat Z, Bar-Hava I, Kovo M, Golan A, Moravski G, Ben-Rafael Z. The effect of betamethasone on fetal biophysical activities and Doppler velocimetry of umbilical and middle cerebral arteries. Acta Obstet Gynecol Scand 1999 78(9) 768-73. [Pg.66]

The methods described in this book are primarily concerned with the measurement of the microstructure of complex fluids subject to the application of external, orienting fields. In the case of flow, it is also of interest to measure the kinematics of the fluid motion. This chapter describes two experimental techniques that can be used for this purpose laser Doppler velocimetry for the measurement of fluid velocities, and dynamic light scattering (or photon correlation spectroscopy) for the determination of velocity gradients. [Pg.100]

Laser Doppler velocimetry is a powerful technique for the in situ measurement of fluid velocities. The basic optical configuration for the measurement is shown in Figure 6.1. The velocity measurement is made at the intersection of two laser beams that are focused to a point in the flow. The use of laser radiation is essential since the light must be monochromatic and coherent. This is required since the intersection of the two beams must create an interference pattern within the fluid. Such a pattern is shown in Figure 6.2, where two plane waves intersect at an angle 2(J). The two waves will have the following form [55] ... [Pg.100]

Laser Doppler Velocimetry and Dynamic Light Scattering... [Pg.102]

Figure 6.3 Two-component laser Doppler velocimetry beam arrangement. Figure 6.3 Two-component laser Doppler velocimetry beam arrangement.

See other pages where Doppler velocimetry is mentioned: [Pg.127]    [Pg.4]    [Pg.38]    [Pg.97]    [Pg.339]    [Pg.250]    [Pg.125]    [Pg.386]    [Pg.433]    [Pg.434]    [Pg.222]    [Pg.309]    [Pg.7]    [Pg.655]    [Pg.43]    [Pg.302]    [Pg.100]    [Pg.101]    [Pg.102]    [Pg.225]    [Pg.225]   
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See also in sourсe #XX -- [ Pg.2 ]

See also in sourсe #XX -- [ Pg.404 , Pg.406 ]




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Doppler

Laser Doppler Velocimetry and Dynamic Light Scattering

Laser Doppler velocimetry

Laser Doppler velocimetry (LDV)

Laser Doppler velocimetry measurements

Laser-Doppler Velocimetry and Computational Fluid Dynamics

Micro Laser Doppler Velocimetry

Optical Doppler Velocimetry

Phase doppler velocimetry

Ultrasonic Doppler velocimetry

Ultrasound Doppler velocimetry

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