Energy dissipation mechanisms in hollow metallic microlattices

2014 ◽  
Vol 29 (16) ◽  
pp. 1755-1770 ◽  
Author(s):  
Ladan Salari-Sharif ◽  
Tobias A. Schaedler ◽  
Lorenzo Valdevit
Keyword(s):  
Energy Dissipation ◽  
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Abstract

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 ◽  
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Scaling of the turbulent energy dissipation correlation function

2020 ◽  
Vol 891 ◽  
Author(s):  
S. L. Tang ◽  
R. A. Antonia ◽  
L. Djenidi ◽  
Y. Zhou
Keyword(s):  
Correlation Function ◽  
Energy Dissipation ◽  
Turbulent Energy ◽  
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On the measurement of energy dissipation using nanoindentation and the continuous stiffness measurement technique

2013 ◽  
Vol 28 (21) ◽  
pp. 3029-3042 ◽  
Author(s):  
Erik G. Herbert ◽  
Kurt E. Johanns ◽  
Robert S. Singleton ◽  
George M. Pharr
Keyword(s):  
Energy Dissipation ◽  
Measurement Technique ◽  
Stiffness Measurement ◽  
Continuous Stiffness Measurement ◽  
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Abstract

scholarly journals Influence of chemical disorder on energy dissipation and defect evolution in advanced alloys

2016 ◽  
Vol 31 (16) ◽  
pp. 2363-2375 ◽  
Author(s):  
Yanwen Zhang ◽  
Ke Jin ◽  
Haizhou Xue ◽  
Chenyang Lu ◽  
Raina J. Olsen ◽  
...  
Keyword(s):  
Energy Dissipation ◽  
Chemical Disorder ◽  
Defect Evolution ◽  
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Abstract

Hidden energy dissipation mechanism in nacre

2014 ◽  
Vol 29 (14) ◽  
pp. 1573-1578 ◽  
Author(s):  
Zaiwang Huang ◽  
Zhiliang Pan ◽  
Haoze Li ◽  
Qiuming Wei ◽  
Xiaodong Li
Keyword(s):  
Energy Dissipation ◽  
Energy Dissipation Mechanism ◽  
Dissipation Mechanism ◽  
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Abstract

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 ◽  
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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

A Magnetic Spectrometer for a Scanning Transmission Electron Microscope

1974 ◽  
Vol 32 ◽  
pp. 436-437
Author(s):  
A. Kosiara ◽  
J. W. Wiggins ◽  
M. Beer
Keyword(s):  
Scanning Transmission Electron Microscope ◽  
Magnetic Spectrometer ◽  
Fringe Field ◽  
Curvature Radius ◽  
Magnetic Pole ◽  
Quadrupole Field ◽  
Transmission Electron ◽  
Scanning Transmission ◽  
Under Construction ◽  
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A magnetic spectrometer to be attached to the Johns Hopkins S. T. E. M. is under construction. Its main purpose will be to investigate electron interactions with biological molecules in the energy range of 40 KeV to 100 KeV. The spectrometer is of the type described by Kerwin and by Crewe Its magnetic pole boundary is given by the equationwhere R is the electron curvature radius. In our case, R = 15 cm. The electron beam will be deflected by an angle of 90°. The distance between the electron source and the pole boundary will be 30 cm. A linear fringe field will be generated by a quadrupole field arrangement. This is accomplished by a grounded mirror plate and a 45° taper of the magnetic pole.

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