Free Energy Functions

2012 ◽  
pp. 97-110
Keyword(s):  
2013 ◽  
Vol 29 (6) ◽  
pp. 763-772 ◽  
Author(s):  
Samuel Forest ◽  
Nicolas Guéninchault

Author(s):  
Lallit Anand ◽  
Sanjay Govindjee

This chapter presents several technologically important constitutive relations for elastomeric materials. In particular, the Neo-Hookean, Mooney-Rivlin, Ogden, Arruda-Boyce, and Gent free energy functions are discussed in the context of incompressible response. Extensions to the slightly compressible case are also detailed, this includes a presentation of a number of possible volumetric response relations and their properties.


1997 ◽  
Vol 192 (1) ◽  
pp. 29-44 ◽  
Author(s):  
V. A. Stephanovich
Keyword(s):  

1990 ◽  
Vol 205 ◽  
Author(s):  
Kwang-Ryeol Lee ◽  
Jeffrey A. West ◽  
Patrick M. Smith ◽  
M. J. Aziz ◽  
J. A. Knapp

AbstractThe congruent melting point, or To curve, of crystalline Si-As alloys has been measured in the range of 1.6 to 18.1 at. % arsenic by line source electron beam annealing. Alloys were created by ion implantation of As into 0.1mm Si-on-sapphire and crystallized by pulsed laser melting. To temperatures decrease from 1673±10K at 2.0 at.% As to 1516±30K at 18.1 at.% As. The results of these measurements are significantly higher than the previous results of studies using pulsed laser melting techniques. Advantages of the e-beam technique over previous techniques are discussed. Chemical free energy functions of the solid and liquid phases were calculated from existing thermodynamic data. The calculated To curve agrees with the measured values only in low concentration region (less than 8 at.%).


1986 ◽  
Vol 64 (12) ◽  
pp. 1581-1583 ◽  
Author(s):  
Robert Cleary

The critical temperature of a clean, normal (n) and superconducting (s) material is calculated and found to differ very slightly from its bulk value. The order parameter at 0°, Δ(0), is found to be modified much more than its bulk value for periodic structures of various cell widths, superconducting-to-normal metal length ratios, and Fermi-velocity differences in the normal and superconducting regions. At intermediate temperatures, an expression for Δ(T)/Δ(0) as a function of T/Tc and Δ(0)/Tc is given. The free-energy functional Fs − Fn is calculated. As in the case of Δ(T)/Δ(0), numerical calculations are necessary. These integrands are carried out to the point where numerical quadrature is simple and straightforward. Because of the great number of parameters describing our system, we do not perform any numerical calculation. These are left to the interested experimentalist for his particular structure.


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