Representation of effectivity functions by acceptable game forms: a complete characterization

2004 ◽  
Vol 47 (3) ◽  
pp. 275-287 ◽  
Author(s):  
Bezalel Peleg
Keyword(s):  
Complete Characterization ◽  
Effectivity Functions ◽  
Game Forms

Effectivity functions, game forms, games, and rights

1997 ◽  
Vol 15 (1) ◽  
pp. 67-80 ◽  
Author(s):  
Bezalel Peleg
Keyword(s):  
Effectivity Functions ◽  
Game Forms

Effectivity Functions and Acceptable Game Forms

Econometrica ◽  
1984 ◽  
Vol 52 (5) ◽  
pp. 1151 ◽  
Author(s):  
Bhaskar Dutta
Keyword(s):  
Effectivity Functions ◽  
Game Forms

On effectivity functions of game forms

2010 ◽  
Vol 68 (2) ◽  
pp. 512-531 ◽  
Author(s):  
Endre Boros ◽  
Khaled Elbassioni ◽  
Vladimir Gurvich ◽  
Kazuhisa Makino
Keyword(s):  
Effectivity Functions ◽  
Game Forms

Diffraction contrast of dislocations in icosahedral quasicrystals

1990 ◽  
Vol 48 (4) ◽  
pp. 454-455
Author(s):  
K. Urban ◽  
Z. Zhang ◽  
M. Wollgarten ◽  
D. Gratias
Keyword(s):  
Dimensional Space ◽  
Three Dimensional ◽  
Complete Characterization ◽  
Extinction Condition ◽  
Burgers Vector ◽  
Diffraction Contrast ◽  
Lattice Geometry ◽  
Reference Space ◽  
Icosahedral Quasicrystals ◽  
The One

Recently dislocations have been observed by electron microscopy in the icosahedral quasicrystalline (IQ) phase of Al65Cu20Fe15. These dislocations exhibit diffraction contrast similar to that known for dislocations in conventional crystals. The contrast becomes extinct for certain diffraction vectors g. In the following the basis of electron diffraction contrast of dislocations in the IQ phase is described. Taking account of the six-dimensional nature of the Burgers vector a “strong” and a “weak” extinction condition are found.Dislocations in quasicrystals canot be described on the basis of simple shear or insertion of a lattice plane only. In order to achieve a complete characterization of these dislocations it is advantageous to make use of the one to one correspondence of the lattice geometry in our three-dimensional space (R3) and that in the six-dimensional reference space (R6) where full periodicity is recovered . Therefore the contrast extinction condition has to be written as gpbp + gobo = 0 (1). The diffraction vector g and the Burgers vector b decompose into two vectors gp, bp and go, bo in, respectively, the physical and the orthogonal three-dimensional sub-spaces of R6.

Experimental Characterization of Mechanical Behavior of Cord-Rubber Composites

1982 ◽  
Vol 10 (1) ◽  
pp. 37-54 ◽  
Author(s):  
M. Kumar ◽  
C. W. Bert
Keyword(s):  
Response Characteristic ◽  
Cord Compression ◽  
Complete Characterization ◽  
Strain Response ◽  
Strain Gages ◽  
Experimental Characterization ◽  
Rubber Composites ◽  
Stress Strain ◽  
Strain Data

Abstract Unidirectional cord-rubber specimens in the form of tensile coupons and sandwich beams were used. Using specimens with the cords oriented at 0°, 45°, and 90° to the loading direction and appropriate data reduction, we were able to obtain complete characterization for the in-plane stress-strain response of single-ply, unidirectional cord-rubber composites. All strains were measured by means of liquid mercury strain gages, for which the nonlinear strain response characteristic was obtained by calibration. Stress-strain data were obtained for the cases of both cord tension and cord compression. Materials investigated were aramid-rubber, polyester-rubber, and steel-rubber.

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