scholarly journals Axisymmetric internal wave transmission and resonant interference in nonlinear stratifications

2020 ◽  
Vol 886 ◽  
Author(s):  
S. Boury ◽  
P. Odier ◽  
T. Peacock
Keyword(s):  
Internal Wave ◽  
Wave Transmission ◽  
Image Position

scholarly journals Water wave transmission and energy dissipation by a floating plate in the presence of overwash

2020 ◽  
Vol 889 ◽  
Author(s):  
Filippo Nelli ◽  
Luke G. Bennetts ◽  
David M. Skene ◽  
Alessandro Toffoli
Keyword(s):  
Energy Dissipation ◽  
Water Wave ◽  
Wave Transmission ◽  
Floating Plate ◽  
Image Position

Internal wave transmission in nonuniform flows

2007 ◽  
Vol 19 (1) ◽  
pp. 016601 ◽  
Author(s):  
J. T. Nault ◽  
B. R. Sutherland
Keyword(s):  
Internal Wave ◽  
Wave Transmission ◽  
Nonuniform Flows

Simple Identification of Electron Diffraction Ring Patterns

1969 ◽  
Vol 27 ◽  
pp. 160-161
Author(s):  
Carolyn Nohr ◽  
Ann Ayres
Keyword(s):  
Electron Microscope ◽  
Electron Diffraction ◽  
Diffraction Ring ◽  
Image Position

Texts on electron diffraction recommend that the camera constant of the electron microscope be determine d by calibration with a standard crystalline specimen, using the equation

Atomic orientation effects in proton stopping at low velocity

1983 ◽  
Vol 41 ◽  
pp. 708-709
Author(s):  
Kin Lam
Keyword(s):  
Polycrystalline Material ◽  
Charged Particles ◽  
Target Material ◽  
Stopping Power ◽  
Low Velocity ◽  
Electronic Density ◽  
Interatomic Distances ◽  
Frame Work ◽  
Image Position ◽  
Atomic Orientation

The energy of moving ions in solid is dependent on the electronic density as well as the atomic structural properties of the target material. These factors contribute to the observable effects in polycrystalline material using the scanning ion microscope. Here we outline a method to investigate the dependence of low velocity proton stopping on interatomic distances and orientations.The interaction of charged particles with atoms in the frame work of the Fermi gas model was proposed by Lindhard. For a system of atoms, the electronic Lindhard stopping power can be generalized to the formwhere the stopping power function is defined as

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