Evidence of electric-field-accelerated growth of tin whiskers

2015 ◽  
Vol 5 (4) ◽  
pp. 619-622 ◽  
Author(s):  
Anthony C. Vasko ◽  
Corey R. Grice ◽  
Andrew D. Kostic ◽  
Victor G. Karpov

Abstract

2018 ◽  
Vol 9 (01) ◽  
pp. 14-26 ◽  
Author(s):  
Qilai Chen ◽  
Gang Liu ◽  
Shuang Gao ◽  
Xiaohui Yi ◽  
Wuhong Xue ◽  
...  

Abstract


2013 ◽  
Vol 28 (10) ◽  
pp. 1349-1355 ◽  
Author(s):  
Zbigniew Rozynek ◽  
René C. Castberg ◽  
Alexander Mikkelsen ◽  
Jon Otto Fossum

Abstract


2013 ◽  
Vol 5 (6) ◽  
pp. 623-627
Author(s):  
P. Žák ◽  
I. Kudláček ◽  
J. Urbánek

1930 ◽  
Vol 26 (1) ◽  
pp. 117-121 ◽  
Author(s):  
R. J. Clark ◽  
W. H. Watson

If a light quantum has an electric moment, we should expect its axis to coincide with the direction of the electric vector, and therefore to be perpendicular to the plane of polarisation. Now an electric doublet of moment μ on entering a uniform electric field E with its doubletaxis parallel or antiparallel to the field will have its energy changed by an amount ∓ μE. For a light quantum this is equivalent to a change in wave-lengthwhen in the field. The method adopted to detect this change was to set up a grating with a strong electric field normal to its surface, and then have a plane polarised parallel beam of light fall on the ruled surface with the electric vector parallel to the direction of the field. The spectra formed near the normal to the grating were then examined both in the presence and absence of the field.


2011 ◽  
Vol 26 (2) ◽  
pp. 254-261 ◽  
Author(s):  
Rita Toth ◽  
Mateusz Schabikowski ◽  
Jakob Heier ◽  
Artur Braun ◽  
Dariusz Kata ◽  
...  

Abstract


1970 ◽  
Vol 4 (1) ◽  
pp. 143-144
Author(s):  
G. J. Lewak

In a previous paper [Lewak (1969), see also Pflrsch (1966) for related treatment], it was shown that the Vlasov equation in the Semi-Lagrangian (S.L.) formulation, may be written in a form resembling the fluid equations.plus Maxwell's equations with the source terms given bywhere n is the determinant of the tensor Tij = ∂gi/∂ζj, and N is the constant mean number density of electrons. The averaging notation < > here is defined bywhere f(σ) is the electron distribution function to be specified. The equations assume for simplicity a uniform fixed ion background, although this is not a necessary restriction and equations (1) and (2) need only an obvious modification to account for ions. The force fields in (1) are related to the electric field E and magnetic field B in the plasma by .


2016 ◽  
Vol 31 (22) ◽  
pp. 3580-3587
Author(s):  
Chunxiang Zhang ◽  
Limin Wang ◽  
Riping Liu ◽  
Bojun Zhao ◽  
Junting Luo

Abstract


2011 ◽  
Vol 26 (2) ◽  
pp. 215-222 ◽  
Author(s):  
Manish Mittal ◽  
Raul F. Lobo ◽  
Eric M. Furst

Abstract


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