A mechanism of cadmium poisoning: The cross effect of calcium and cadmium in the calmodulin-dependent system

1990 ◽  
Vol 64 (2) ◽  
pp. 161-164 ◽  
Author(s):  
Den'etsu Sutoo ◽  
Kayo Akiyama ◽  
Shunichiro Imamiya
Keyword(s):  
Cross Effect ◽  
Cadmium Poisoning ◽  
The Cross

Static 1H dynamic nuclear polarization with the biradical TOTAPOL: a transition between the solid effect and the cross effect

2014 ◽  
Vol 16 (14) ◽  
pp. 6687-6699 ◽  
Author(s):  
Daphna Shimon ◽  
Akiva Feintuch ◽  
Daniella Goldfarb ◽  
Shimon Vega
Keyword(s):  
High Temperatures ◽  
Dynamic Nuclear Polarization ◽  
Low Temperatures ◽  
Nuclear Polarization ◽  
Cross Effect ◽  
Solid Effect ◽  
The Cross

Static 1H-DNP with TOTAPOL: the solid effect (SE) dominant at low temperatures; the cross effect (CE) dominant at high temperatures; and DNP-buildup: Tbu(SE) < Tbu(CE).

On the Overhung Rigid Rotor Balancing

2000 ◽  
Author(s):  
José A. Méndez-Adriani
Keyword(s):  
Efficient Technique ◽  
Influence Coefficient ◽  
Rigid Rotor ◽  
Cross Effect ◽  
Calibration Process ◽  
The Third ◽  
Influence Coefficient Method ◽  
The Cross ◽  
Rotor Balancing ◽  
Coefficient Method

Abstract This article develops a more efficient technique for the balancing of the overhung rigid rotor, which is a variation of the exact influence coefficient method, that gives directly the correction weights for both balancing planes. During the calibration process, one trial weight is used for the second run and, to reduce the cross effect, only one trial weight to form a couple is used for the third run, improving the field balancing method for maintenance works.

Probing the cross-effect of strains in non-linear elasticity of nearly regular polymer networks by pure shear deformation

2015 ◽  
Vol 142 (17) ◽  
pp. 174908 ◽  
Author(s):  
Takuya Katashima ◽  
Kenji Urayama ◽  
Ung-il Chung ◽  
Takamasa Sakai
Keyword(s):  
Shear Deformation ◽  
Linear Elasticity ◽  
Pure Shear ◽  
Polymer Networks ◽  
Cross Effect ◽  
Non Linear ◽  
The Cross

The Anisotropic Yield, Flow and Creep Behaviour of Pre-Strained En24 Steel

1975 ◽  
Vol 17 (2) ◽  
pp. 93-104 ◽  
Author(s):  
S. N. Shahabi ◽  
A. Shelton
Keyword(s):  
Internal Pressure ◽  
Creep Behaviour ◽  
Strain Ratio ◽  
Stress Axis ◽  
Cross Effect ◽  
Plastic Strain Ratio ◽  
Strain Components ◽  
Yield Behaviour ◽  
Yield Loci ◽  
The Cross

Tests under combinations of tension, torsion and internal pressure have been performed at constant stress ratio on En24 steel, previously annealed, and then subjected to a pre-stress in either axial or circumferential tension or torsion. Post-yield behaviour showed marked room-temperature creep by all strain components in the logarithmic form ε = a In t + c. The initial direction of the incremental plastic strain-ratio vector was markedly different from isotropic behaviour and remained constant in direction with time. Increased loading resulted in a progressive rotation towards the isotropic direction. Anisotropic yield loci were established from the normality rule and from the backward extrapolation of curves of creep coefficient versus stress and stress versus ‘long-time’ strain. The yield locus was translated to the pre-stress point and this local work-hardening was accompanied by softening in both the transverse and reverse directions, i.e. the cross-effect and Bauschinger effect respectively. Yield loci in planes not containing the pre-stress axis showed softening in all directions and under axial tension-internal pressure the cross-effect caused a rotation of the locus. All yield loci were smooth and continuous. Yield criteria derived from the theories of Edelman and Drucker and also Williams and Svensson were in good agreement with experiment over the whole locus. Hill's theory was thought to be more appropriate to material behaviour following large deformations.

Interference Effect between Electron and Ion Flows in Semiconducting Fe3−δO4

2000 ◽  
Vol 658 ◽  
Author(s):  
Jeong-Oh Hong ◽  
Han-Ill Yoo
Keyword(s):  
Electrical Conductivity ◽  
Interference Effect ◽  
Elevated Temperatures ◽  
Cross Effect ◽  
Fixed Temperature ◽  
Total Electrical Conductivity ◽  
A Value ◽  
Effective Valence ◽  
The Cross ◽  
Fe Ions

ABSTRACTThe effective valence, zFe–αFe*, of mobile Fe-ions (Fe2+, Fe3+) in semiconducting Fe3O4was determined at elevated temperatures via the electrotransport experiment in association with the literature data on the cation diffusivity and total electrical conductivity. It has been found that the value for zFe–αFe* varies systematically from below 2 up to 3 with oxygen partial pressure at a fixed temperature. The effective valence is determined not only by the mobility difference of Fe2+and Fe3+ions (zFe), but also by the cross effect between the cations and electrons upon their transfer (αFe*). A value of zFe–αFe* between 2 and 3 may be attributed to the mobility difference between Fe2+and Fe3+ions even in the absence of the cross effect, but the values of zFe–αFe* < 2 clearly indicate that the cross effect is in play in Fe3O4.

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