Erythrocytes Sedimentation Profiles Under Gravitational Field as Determined by He-Ne Laser: VIII - Effect of Inhomogeneous Magnetic Field

1983 ◽  
Vol BME-30 (1) ◽  
pp. 70-73 ◽  
Author(s):  
Megha Singh ◽  
S. Swarnamani
2018 ◽  
Vol 1 (1) ◽  
pp. 30-34 ◽  
Author(s):  
Alexey Chernogor ◽  
Igor Blinkov ◽  
Alexey Volkhonskiy

The flow, energy distribution and concentrations profiles of Ti ions in cathodic arc are studied by test particle Monte Carlo simulations with considering the mass transfer through the macro-particles filters with inhomogeneous magnetic field. The loss of ions due to their deposition on filter walls was calculated as a function of electric current and number of turns in the coil. The magnetic field concentrator that arises in the bending region of the filters leads to increase the loss of the ions component of cathodic arc. The ions loss up to 80 % of their energy resulted by the paired elastic collisions which correspond to the experimental results. The ion fluxes arriving at the surface of the substrates during planetary rotating of them opposite the evaporators mounted to each other at an angle of 120° characterized by the wide range of mutual overlapping.


1967 ◽  
Vol 45 (4) ◽  
pp. 1481-1495 ◽  
Author(s):  
Myer Bloom ◽  
Eric Enga ◽  
Hin Lew

A successful transverse Stern–Gerlach experiment has been performed, using a beam of neutral potassium atoms and an inhomogeneous time-dependent magnetic field of the form[Formula: see text]A classical analysis of the Stern–Gerlach experiment is given for a rotating inhomogeneous magnetic field. In general, when space quantization is achieved, the spins are quantized along the effective magnetic field in the reference frame rotating with angular velocity ω about the z axis. For ω = 0, the direction of quantization is the z axis (conventional Stern–Gerlach experiment), while at resonance (ω = −γH0) the direction of quantization is the x axis in the rotating reference frame (transverse Stern–Gerlach experiment). The experiment, which was performed at 7.2 Mc, is described in detail.


2010 ◽  
Vol 53 (6) ◽  
pp. 1053-1058 ◽  
Author(s):  
Chen Tao ◽  
Shan Chuan-Jia ◽  
Li Jin-Xing ◽  
Liu Ji-Bing ◽  
Liu Tang-Kun ◽  
...  

2005 ◽  
Vol 14 (03n04) ◽  
pp. 687-695 ◽  
Author(s):  
B. J. AHMEDOV ◽  
A. V. KHUGAEV ◽  
N. I. RAKHMATOV

We present analytic solutions of Maxwell equations for infinitely long cylindrical conductors with nonvanishing electric charge and currents in the external background spacetime of a line gravitomagnetic monopole. It has been shown that vertical magnetic field arising around cylindrical conducting shell carrying azimuthal current will be modified by the gravitational field of NUT source. We obtain that the purely general relativistic magnetic field which has no Newtonian analog will be produced around charged gravitomagnetic monopole.


2016 ◽  
Vol 23 (11) ◽  
pp. 112101 ◽  
Author(s):  
V. A. Svidzinski ◽  
J. S. Kim ◽  
J. A. Spencer ◽  
L. Zhao ◽  
S. A. Galkin ◽  
...  

2022 ◽  
Author(s):  
Andrey Starikovskiy ◽  
Nickolay Aleksandrov ◽  
Mikhail N. Shneider

Sign in / Sign up

Export Citation Format

Share Document