A Flat Interface and its Unfolding Bifurcations

1991 ◽  
pp. 119-129
Author(s):  
A. Libchaber ◽  
A. J. Simon ◽  
J.-M. Flesselles
Keyword(s):  
Flat Interface

scholarly journals Force distribution on a slender body close to an interface

1981 ◽  
Vol 24 (1) ◽  
pp. 27-36 ◽  
Author(s):  
J.R. Blake ◽  
G.R. Fulford
Keyword(s):  
Reynolds Numbers ◽  
Plane Wall ◽  
Slender Body ◽  
Force Distribution ◽  
Immiscible Liquids ◽  
Flat Interface ◽  
Small Reynolds Numbers ◽  
Rigid Plane ◽  
Limiting Case ◽  
Analytical Expressions

The motion of a slender body parallel and very close to a flat interface which separates two immiscible liquids of differing density and viscosity is considered for very small Reynolds numbers. Approximate analytical expressions are obtained for the distribution of forces acting on the slender body. The limiting case of a rigid plane wall yields results obtained previously.

Depth migration from irregular surfaces with depth extrapolation methods

Geophysics ◽  
1991 ◽  
Vol 56 (1) ◽  
pp. 119-122 ◽  
Author(s):  
Moshe Reshef
Keyword(s):  
Wave Equation ◽  
Surface Topography ◽  
Time Shift ◽  
Extrapolation Methods ◽  
Irregular Surfaces ◽  
Depth Migration ◽  
Numerical Problem ◽  
Flat Interface ◽  
Interface Wave ◽  
Computationally Expensive

Nonflat surface topography introduces a numerical problem for migration algorithms that are based on depth extrapolation. Since the numerically efficient migration schemes start at a flat interface, wave‐equation datuming is required (Berryhill, 1979) prior to the migration. The computationally expensive datuming procedure is often replaced by a simple time shift for the elevation to datum correction. For nonvertically traveling energy this correction is inaccurate. Subsequent migration wrongly positions the reflectors in depth.

scholarly journals Fabrication of High Contact-Density, Flat-Interface Nerve Electrodes for Recording and Stimulation Applications

10.3791/54388 ◽  
2016 ◽  
Author(s):  
Yazan M. Dweiri ◽  
Matthew A. Stone ◽  
Dustin J. Tyler ◽  
Grant A. McCallum ◽  
Dominique M. Durand
Keyword(s):  
Contact Density ◽  
Flat Interface ◽  
Nerve Electrodes

SH wave propagation by discrete wavenumber boundary integral modeling in transversely isotropic medium

1996 ◽  
Vol 86 (2) ◽  
pp. 524-529
Author(s):  
Hayrullah Karabulut ◽  
John F. Ferguson
Keyword(s):  
Transversely Isotropic ◽  
Boundary Integral ◽  
Boundary Integral Method ◽  
Interface Problem ◽  
Seismic Profiles ◽  
Sh Waves ◽  
Vertical Seismic Profiles ◽  
Flat Interface ◽  
Transversely Isotropic Media ◽  
Isotropic Media

Abstract An extension of the boundary integral method for SH waves is given for transversely isotropic media. The accuracy of the method is demonstrated for a simple flat interface problem by comparison to the Cagniard-de Hoop solution. The method is further demonstrated for a case with interface topography for both surface and vertical seismic profiles. The new method is found to be both accurate and effective.

Chronic Response of the Rat Sciatic Nerve to the Flat Interface Nerve Electrode

2003 ◽  
Vol 31 (6) ◽  
pp. 633-642 ◽  
Author(s):  
Dustin J. Tyler ◽  
Dominique M. Durand
Keyword(s):  
Sciatic Nerve ◽  
Rat Sciatic Nerve ◽  
Flat Interface ◽  
Flat Interface Nerve Electrode

scholarly journals Entropic self-assembly of freely rotating polyhedral particles confined to a flat interface

Soft Matter ◽  
2015 ◽  
Vol 11 (8) ◽  
pp. 1481-1491 ◽  
Author(s):  
V. Thapar ◽  
T. Hanrath ◽  
F. A. Escobedo
Keyword(s):  
Self Assembly ◽  
Polyhedral Particles ◽  
Flat Interface

The 2D entropic packing of hard polyhedral nanoparticles into diverse phases lays a foundation to understand interfacial self-assembly.

Growth and Evaluation of [AFeOx/REFeO3] (A=Ca, Sr, RE=La, Bi) Superlattices by Pulsed Laser Deposition Method Using High Density Targets Prepared by Pechini Method

2012 ◽  
Vol 1454 ◽  
pp. 161-166 ◽  
Author(s):  
Nobuyuki Iwata ◽  
Yuta Watabe ◽  
Yoshito Tsuchiya ◽  
Kento. Norota ◽  
Takuya Hashimoto ◽  
...  
Keyword(s):  
Growth Rate ◽  
Flat Surface ◽  
Pechini Method ◽  
Laser Deposition ◽  
Growth Constant ◽  
Constant Growth Rate ◽  
X Ray ◽  
Flat Interface ◽  
Reference Layer ◽  
Constant Growth

ABSTRACTThe LaFeO3 and CaFeOX layers are grown using highly dense target prepared by Pechini method, with which accurate growth rate is achieved. Since the LaFeO3demonstrates the obvious RHEED oscillation until the end of growth, constant growth rate, and the step-terraces structure, the LFO is employed as a buffer and/or reference layer to determine the required pulses to deposit the thickness we desire in the superlattice. Superlattices show the clear satellite peaks and Laue oscillation in the XRD spectra as well as the oscillations caused by the film thickness with a flat surface and superstructure with a flat interface in the x-ray reflection spectrum. The streaky RHEED patterns and step-terraces surface are consistent with the results of spectra using x-ray.

Spectral‐domain solution to the electromagnetic scattering of a two‐dimensional beam by cylinders buried below a flat interface

2015 ◽  
Vol 13 (3) ◽  
pp. 219-225 ◽  
Author(s):  
Muhammad Arshad Fiaz ◽  
Fabrizio Frezza ◽  
Lara Pajewski ◽  
Cristina Ponti ◽  
Giuseppe Schettini
Keyword(s):  
Electromagnetic Scattering ◽  
Spectral Domain ◽  
Two Dimensional ◽  
Flat Interface
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