Effect of Tension on Change of Resistance and Thermoelectromotive Force by Transverse Magnetization

1923 ◽  
Vol 22 (1) ◽  
pp. 58-65 ◽  
Author(s):  
Alpheus W. Smith
Keyword(s):  
Transverse Magnetization ◽  
Thermoelectromotive Force

A duplex commutator and key of small thermoelectromotive force

1934 ◽  
Vol 11 (4) ◽  
pp. 116-118
Author(s):  
N R Campbell ◽  
O Kantorowicz
Keyword(s):  
Thermoelectromotive Force

scholarly journals Thermoelectromotive Force of Some Redox Couples in an Amide-type Room-temperature Ionic Liquid

2009 ◽  
Vol 77 (8) ◽  
pp. 639-641 ◽  
Author(s):  
Tsubasa MIGITA ◽  
Naoki TACHIKAWA ◽  
Yasushi KATAYAMA ◽  
Takashi MIURA
Keyword(s):  
Ionic Liquid ◽  
Room Temperature ◽  
Room Temperature Ionic Liquid ◽  
Thermoelectromotive Force ◽  
Redox Couples

Transmission of Transverse Magnetization in Spin-Exchange Collisions of Alkali Metal Atoms

2018 ◽  
Vol 44 (10) ◽  
pp. 860-861 ◽  
Author(s):  
S. P. Dmitriev ◽  
N. A. Dovator ◽  
E. N. Pestov ◽  
V. A. Kartoshkin ◽  
A. I. Okunevich
Keyword(s):  
Alkali Metal ◽  
Spin Exchange ◽  
Transverse Magnetization ◽  
Metal Atoms

Effect of Transverse Magnetization on the Resistance of Nickel at High Temperatures

1906 ◽  
Vol 25 (1) ◽  
pp. 292-294
Author(s):  
C. G. Knott
Keyword(s):  
Transverse Magnetization ◽  
Nickel Wire ◽  
Great Care ◽  
Final Temperature ◽  
Longitudinal Magnetization ◽  
Resistance Change ◽  
Considerable Difficulty ◽  
Magnetic Action ◽  
Remarkable Result ◽  
The Wire

AbstractIn a previous communication it was pointed out that the effect of transverse magnetization on the resistance of nickel wire was inappreciable in fields below 500 C.G.S. units, thereby differing from the case of longitudinal magnetization, in which the effect was easily measurable in fields below 20. The reason of this is no doubt to be referred to the thinness of the wire in the direction of the magetizing force. To measure the effect of transverse magnetization it was necessary to form a fiat coil and insert it between the poles of a powerful electro-magnet. Considerable difficulty was experienced in winding this coil with interwound asbestos insulation, for great care had to be taken that no part of the wire cut the lines of force obliquely, otherwise there would be a resolved component of longitudinal effect, which in certain cases might altogether mask the effect looked for. The coil used in the final experiments was suitable in all respects. It was coiled between glass plates, the successive coils being separated by threads of asbestos. Round the coil another coil (of Beacon wire) was wound anti-inductively, so that any current passing through it would have no magnetic action upon the nickel wire inside. By varying the current in this external coil I was able to heat the nickel to any desired temperature up to 400° C. In any one experiment the final temperature came to a steady state, and not till this state was reached was it possible to begin the observations on the resistance change. This was measured in the manner already described in my paper on the effect of longitudinal magnetization, and it will suffice meanwhile to call attention to a remarkable result obtained when the temperature approached that at which nickel ceases to be strongly magnetic.

The Thermoelectromotive Force of Copper-Manganese Alloys

1922 ◽  
Vol 20 (5) ◽  
pp. 441-451 ◽  
Author(s):  
Skezug Kimura ◽  
Zunehachi Isawa
Keyword(s):  
Thermoelectromotive Force ◽  
Manganese Alloys ◽  
Copper Manganese

Excitation magnetic flux losses in acyclic motors with transverse magnetization

2007 ◽  
Vol 78 (2) ◽  
pp. 70-78
Author(s):  
O. K. Epifanov ◽  
I. A. Salova ◽  
V. V. Khrushchev ◽  
M. M. Fillipov
Keyword(s):  
Magnetic Flux ◽  
Transverse Magnetization

On the critical behaviour of the two dimensional spin XY model

1982 ◽  
Vol 60 (3) ◽  
pp. 368-372 ◽  
Author(s):  
Jos Rogiers
Keyword(s):  
Critical Point ◽  
Triangular Lattice ◽  
Second Order ◽  
Critical Behaviour ◽  
Transverse Magnetization ◽  
Xy Model ◽  
Two Dimensional ◽  
Exponential Behaviour ◽  
Transformation Methods

Transformation methods are used to analyse the series for the second order fluctuation of the transverse magnetization for the triangular and square lattices. For the triangular lattice some evidence is found for an exponential behaviour of this quantity near the critical point with a tentative estimate for the exponent [Formula: see text].

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