high velocity gradient
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2021 ◽  
Author(s):  
Richard Hobbs ◽  
Christine Peirce

<p>The transition zone between the more porous upper extrusive layer (2A) and the less porous lower dyke layer (2B) within the oceanic crust is characterised by a high velocity gradient based on inversion of controlled-source, long-offset refraction data. In these data the phase associated with this high velocity gradient, termed the 2A Event, has an anomalously high amplitude over a limited range of offsets and appears to form a triplication with refractions from layer 2A above and 2B below. These characteristics fit the accepted model that this event is a caustic or retrograde phase, generated by a distinct layer whose thickness and velocity gradient can be determined by ray-trace modelling. Hence, a velocity model for Layer 2 (derived from seismic data acquired near ODP 504B) consists of a ~500 m-thick 2A with a velocity gradient of ~1.0 s<sup>-1</sup>; a ~200 m-thick transition zone with a high velocity gradient of ~4.0 s<sup>-1</sup>; and a ~1300 m-thick 2B with a velocity gradient of ~0.3 s<sup>-1</sup>. However, this model is at odds with observation of Layer 2 lithology obtained from coring and ophiolites where the 2A is composed of a mixture of higher velocity basalt flows and lower velocity pillow lavas and breccia, with the transition zone represented by an increasing number of dykes which eventually make up 100% of the section in layer 2B combined and the effects of high-temperature alteration. Starting with a simplified but plausible geologically-based model, we show that it is possible to synthetically generate the observed 2A Event, and gain insight into what controls its visibility and variability in refraction data. Our primary findings show that the 2A Event will only form and propagate in the base of layer 2A, above the level where the higher velocities dominate. We also show that the amplitude of the 2A Event is sensitive to the local velocity structure of the extrusive layer and is most visible when seismic energy is focused by a low velocity layer. Hence, we conclude that the 2A Event is not a simple caustic, as defined by geometrical optics, but instead caused by the incident seismic energy being briefly concentrated in a leaky waveguide close to, but above, the mean depth of the dykes and the onset of high temperature alteration.</p>



2020 ◽  
Vol 10 (1) ◽  
Author(s):  
Ali Koohandaz ◽  
Ehsan Khavasi ◽  
Arameh Eyvazian ◽  
Hamid Yousefi

Abstract A gravity current in a channel at the presence of a triangular obstacle was investigated using LES simulation and the Eulerian approach. The Saffman–Mei equation was also applied to examine the effect of shear-induced lift force on particle deposition. To this end, particles were considered as Lagrangian markers and injected into gravity current. It is important to keep in mind that the interaction between the gravity current and particles was treated as a one-way coupling. The results show that shear-induced lift force prevents particles to deposit at the entrance of channel, where the velocity gradient is high. Furthermore, a reduction in the rate of sediment deposition can be seen again in the vicinity of obstacle due to high velocity gradient. The important result is that the shear-induced lift force has an important role in the cases with considerable velocity gradient in quasi-steady flows and this force can affect the pattern of sedimentation over time. Q criterion is utilized to depict the vortical structures of flow. Vortical structures with larger diameter, that indicate stronger vortexes, has been seen in various sections of channel, especially in the region near the obstacle due to the presence of obstacle.



2020 ◽  
Vol 47 (1) ◽  
pp. 38-40
Author(s):  
Prerna B. Bansal ◽  
Hari P. Chaliki ◽  
Kantha R. Kolla ◽  
Roger L. Click ◽  
Alberto Pochettino

A high-velocity gradient across the left ventricular outflow tract is most often caused by aortic valve stenosis. We describe the unusual case of a high-velocity gradient caused by a kinked ascending aortic graft in a 69-year-old man who had Marfan syndrome. The patient had a history of ascending aortic aneurysm and had previously undergone replacement of the aortic root and ascending aorta with use of a bioprosthetic valved graft. The kinking was caused by dilation of the native aortic arch. The patient underwent successful hemi-arch replacement and repair of the kinked graft. Late complications and reoperation after proximal aortic surgery in patients with Marfan syndrome are rare, and a high-velocity left ventricular outflow tract gradient caused by the kinking of the aorta is unusual.



2016 ◽  
Vol 590 ◽  
pp. A5 ◽  
Author(s):  
Claudia P. Gutiérrez ◽  
Santiago González-Gaitán ◽  
Gastón Folatelli ◽  
Giuliano Pignata ◽  
Joseph P. Anderson ◽  
...  


2016 ◽  
Vol 25 (1) ◽  
pp. 017102 ◽  
Author(s):  
An-Min He ◽  
Pei Wang ◽  
Jian-Li Shao


2009 ◽  
Vol 131 (9) ◽  
Author(s):  
Bu-Geun Paik ◽  
Kyung-Youl Kim ◽  
Jong-Woo Ahn

The objective of the present study is to investigate propeller wake using particle image velocimetry (PIV) technique with bubble type of tracers, naturally generated by the decrease in the static pressure in a cavitation tunnel. The bubble can be grown from the nuclei melted in the water tunnel and the size of bubbles is changed by varying the tunnel pressure. A series of experiments are conducted in the conditions of the uniform and high velocity gradient flows to find out the characteristics of bubble tracers and compared the measurement results using bubbles with those using solid particles. Bubbles showed good trace ability in the region of 15<ReS<75; however, some discrepancies showed at high velocity gradient region of ReS≈1000. The fitted vorticity reduction rate would give reference for the prediction in a real flow when bubble tracers are utilized in PIV measurements of a vortical flow. In addition, the characteristics of bubble slip velocity can provide information on the vortex core center and the reduction in the Reynolds shear stress caused by bubble’s deformability.



2007 ◽  
Vol 18 (07) ◽  
pp. 1119-1131 ◽  
Author(s):  
ZHEN-HUA CHAI ◽  
BAO-CHANG SHI ◽  
LIN ZHENG

In this paper, the effects of viscous dissipation in electro-osmotic flow in microchannels are numerically analyzed with lattice Boltzmann method (LBM), and three different lattice Boltzmann models that can recover the macroscopic governing equations for electro-osmotic flow (EOF) are proposed. As the dimensions of the channels approach the microlevel, viscous dissipation could be significant due to a high velocity gradient in electric double layer (EDL). Numerical results show that viscous dissipation plays an important role in EOF in microchannels.



2006 ◽  
Vol 2006 ◽  
pp. 1-7 ◽  
Author(s):  
K. S. Adegbie ◽  
F. I. Alao

This paper discusses the effect of viscosity and viscous dissipation (due to a high velocity gradient) on the steady flow of a viscous liquid in a symmetrically heated channel. The coupled nonlinear differential equations arising in the planar Poiseuille flow are not amendable to analytical solutions. Therefore, numerical solutions based on finite-difference scheme are presented. The effects of various flow controlling parameters such as temperature differenceα, dimensionless pressure gradient, and the dimensionless viscous heating parameterδon the dimensionless velocity and temperature are analyzed. The analysis reveals that when viscous heating parameterδ=0, we obtained zero solution for the dimensionless temperature.





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