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References in periodicals archive ?
In this study, the direction of a magnet that can be oriented along the 3 axes of X, Y, and Z is expressed by 3 bit variables, and the magnetic flux density generated is formulated using the variable and Bio-Savart's law, one of the laws of electromagnetism, and an objective function (function whose value should be maximized) as a combinatorial optimization problem in which the magnetic flux density is maximized for a specific part.
Magnetic flux density created by the surface current flowing over the toroidal current surface has only an azimuthal component and is concentrated inside the toroidal volume, in other words, there is no field of scattering in the idealized model.
Therefore, core protuberance length d1 near the magnetic corners was adjusted to raise permeance, and a magnetic flux path was formed with the objectives of changing magneto-resistance.
It was observed that in model 1 the magnetic flux through the steel platform to the steel plate is a small value, 0.01 T.
In case of using the lower energy density magnets, like ferrite or AlNiCo, there are still various possibilities to improve the magnetic flux density in the air-gap.
All these observations stimulated the modeling of KH instability in moving twisted magnetic flux tubes in nonmagnetic environment [62], in magnetic tubes of partially ionized plasma [63], in spicules [64-66], in photospheric tubes [67], in high-temperature and cool surges [68, 69], in dark mottles [70], at the boundary of rising coronal mass ejections [60, 61, 71, 72], in rotating, tornado-like magnetized jets [49], and in a chromospheric jet (fast disappearance of rapid red-shifted and blue-shifted excursions alongside a larger scale H[alpha] jet) [73].
Caption: FIGURE 9: Calculated magnetic flux lines by finite element method ANSYS code [9] for three-layer stacked tape conductors (a) without FMs and (b) with FMs at the edges under the same-direction ([up arrow][up arrow][up arrow]) current feeding mode.
From these differential relations, the magnetization M and the magnetic field H can be determined by the value and variation of the magnetic flux B.
Magnetic core is steel 175.4mm in length and 40.5mm in width with high saturation magnetic flux density (over 2.2 Tl), NdFeB permanent magnets with remanent flux density 1.32 Tl, tube is steel 1020 wall thickness 9mm, cooper coil with 5 mm in length and 2 mm in width with a lift-off distance 3mm to the tube.
The stator resistance becomes higher, increasing Joule losses, but it is compensated by the reduction of iron losses due to the magnetic flux density reduction.