Reduced Wettability of Solids by a Liquid Ga–In–Sn Alloy in a Steady Magnetic Field

2018 ◽  
Vol 122 (48) ◽  
pp. 27451-27455 ◽  
Author(s):  
Chuanjun Li ◽  
Yang Cao ◽  
Stephanie Lippmann ◽  
Zhongming Ren ◽  
Markus Rettenmayr
Keyword(s):  
Magnetic Field ◽  
Steady Magnetic Field

Graded Coating Produced by Laser Melt Injection Under Steady Magnetic Field

2016 ◽  
Vol 43 (5) ◽  
pp. 0503005
Author(s):  
宋诗英 Song Shiying ◽  
王梁 Wang Liang ◽  
胡勇 Hu Yong ◽  
姚建华 Yao Jianhua
Keyword(s):  
Magnetic Field ◽  
Graded Coating ◽  
Steady Magnetic Field

Oscillatory Flow of a Magnetic Fluid in a Pipe at Low Frequency Range Under a Magnetic Field: Phase Difference of Pressure

2003 ◽  
Author(s):  
Kunio Shimada ◽  
Shigemitsu Shuchi ◽  
Shinichi Kamiyama
Keyword(s):  
Magnetic Field ◽  
Experimental Data ◽  
Phase Difference ◽  
Mass Concentration ◽  
Oscillatory Flow ◽  
Low Frequency ◽  
Nonuniform Distribution ◽  
Straight Pipe ◽  
Number Range ◽  
Steady Magnetic Field

We made on numerical analysis of phase difference between pressure along the pipe axis and given oscillatory flow velocity in an straight pipe under a nonuniform steady magnetic field. In the analysis, a few cases under the assumption of numerical condition were conducted on: the first is taking into account the least compressibility of the fluid with using the obtained experimental data of the bulk modulus, the second taking into account the nonuniform distribution of mass concentration of particles, and the thrid taking into account the aggregation with the number of aggregated particles proposing as a prorate spheroid. By considering the three effects of the least compressibility and the nonuniform distribution of mass concentration, the aggregation as a prorate spheroid, the phase difference varies quantitatively at the lowest Womersley number range. And then, the numerical results were compared with the experimental data.

Excitation of surface-type X modes by charged-particle beams

1998 ◽  
Vol 60 (2) ◽  
pp. 413-420 ◽  
Author(s):  
V. O. GIRKA
Keyword(s):  
Magnetic Field ◽  
Charged Particle ◽  
Structural Parameters ◽  
Particle Beam ◽  
Charged Particle Beam ◽  
Surface Type ◽  
Charged Particle Beams ◽  
Steady Magnetic Field ◽  
Polarized Surface ◽  
Oriented Parallel

A theoretical investigation of extraordinary polarized surface waves at the second harmonics of ion and electron cyclotron frequencies propagating across an external steady magnetic field is carried out in the case of weak plasma spatial dispersion when the thermal velocities of plasma particles are much less than the phase velocities of the considered waves. These waves are eigenmodes of a planar plasma–vacuum waveguide structure that is situated in a steady magnetic field oriented parallel to the plasma surface. A cold charged-particle beam is assumed to propagate over the plasma interface. Excitation of surface X modes at the second harmonics of electron and ion cyclotron frequencies due to the beam–plasma interaction is studied analytically. The dependence of surface-type X-mode (STXM) growth rates on the considered waveguide structural parameters is also studied.

Steady magnetic field generation due to transient field ionization in ultrashort laser-solid interaction

1999 ◽  
Vol 59 (1) ◽  
pp. R36-R39 ◽  
Author(s):  
Andrea Macchi ◽  
Enrique Conejero Jarque ◽  
Dieter Bauer ◽  
Fulvio Cornolti ◽  
Luis Plaja
Keyword(s):  
Magnetic Field ◽  
Field Ionization ◽  
Transient Field ◽  
Magnetic Field Generation ◽  
Field Generation ◽  
Steady Magnetic Field ◽  
Ultrashort Laser

Modulated Beams in a Plasma with a Magnetic Field

1961 ◽  
Vol 16 (12) ◽  
pp. 1313-1319
Author(s):  
E. Canobbio ◽  
R. Croci
Keyword(s):  
Magnetic Field ◽  
External Magnetic Field ◽  
Energy Loss ◽  
Single Particle ◽  
Linear Density ◽  
Energy Output ◽  
Straight Beam ◽  
Resonance Frequencies ◽  
Steady Magnetic Field ◽  
Cerenkov Effect

The radiation emitted by a linear density-modulated beam of ions parallel to a steady magnetic field and by a straight beam perpendicular to the field into a non dissipative plasma is investigated. In both cases the energy output becomes infinite at the “ion” and “electron resonance frequencies”.From the expression for the radiation of the beam which is parallel to the external magnetic field the energy loss of a single particle by ČERENKOV effect is also derived.

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