Large structure convection velocity measurements in compressible transverse injection flowfields

1996 ◽  
Author(s):  
M. Gruber ◽  
A. Nejad ◽  
T. Chen ◽  
J. Dutton
1997 ◽  
Vol 22 (5) ◽  
pp. 397-407 ◽  
Author(s):  
M. R. Gruber ◽  
A. S. Nejad ◽  
T. H. Chen ◽  
J. C. Dutton

1997 ◽  
Vol 119 (1) ◽  
pp. 50-55 ◽  
Author(s):  
W. L. Keith ◽  
B. M. Abraham

Cross-spectral and cross-correlation data from experiments and numerical simulations have shown the turbulent wall pressure convection velocity to vary with the streamwise sensor spatial separation. This variation is due to the spatial decay rates of turbulent structures in the inner and outer regions of the boundary layer. Its effect is shown to have a significant impact on the distribution of energy in the wavenumber-frequency spectrum Φ (k1, ω). The standard Corcos model is known to over predict the wavenumber-frequency spectrum at low wavenumbers. This is shown to result from its constant convection velocity assumption. The spectral levels at sub convective and lower wavenumbers are shown to be directly influenced by the spatial variation in convection velocity. Convection velocity measurements from past investigations that cover the range 285 ≤ Rθ ≤ 29,000 are compared, and an outer variable scaling is shown to effectively collapse the data.


2014 ◽  
Vol 15 (3) ◽  
pp. 175-178
Author(s):  
V. Carvalho ◽  
M. Barthes ◽  
V. Lepiller ◽  
Y. Bailly

1994 ◽  
Vol 12 (5) ◽  
pp. 481-495 ◽  
Author(s):  
R.D. Flack ◽  
K. Brun ◽  
J.B. Radford

Previous to this study, research has shown that small air veloci ties can strongly influence the ignition propensity of a cigarette on upholstered furniture simulations. However, data were not available to determine if such velocities existed in practice. The two objectives of the current effort were to de termine (1) the typical steady velocities near the cushion of a warm chair due strictly to free convection and (2) the typical unsteady velocities near the crev ice of a warm chair due to a combination of free convection and forced convec tion as a result of a person vacating the chair. Typical steady velocities were 40 mm/s. Typical velocities in the unsteady conditions were 15 mm/s. For the unsteady conditions large velocities remained long after the chair cooled to room temperature due to large vortices in the flow with long time constants.


1992 ◽  
Vol 13 (1) ◽  
pp. 63-70 ◽  
Author(s):  
Y. Zhou ◽  
R. A. Antonia

AIAA Journal ◽  
1968 ◽  
Vol 6 (4) ◽  
pp. 750-752 ◽  
Author(s):  
D. HECKMAN ◽  
A. CANTIN ◽  
A. EMOND ◽  
A. KIRKPATRICK

Author(s):  
Fan Hai-fu ◽  
Hao Quan ◽  
M. M. Woolfson

AbstractConventional direct methods, which work so well for small structures, are less successful for macromolecules. Where it has been demonstrated that a solution might be found using direct methods it is then found that the usual figures of merit are unable to distinguish the few good sets of phases from the large number of sets generated. The reasons for the difficulties with very large structures are considered from a first-principles approach taking into account both the factors of having a large number of atoms and low resolution data. A proposal is made for trying to recognize good phase sets by taking a large structure as a sum of a number of smaller structures for each of which a conventional figure of merit can be applied.


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