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ginzburg-landau theory

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Series: ASM Handbook
Volume: 22A
Publisher: ASM International
Published: 01 December 2009
DOI: 10.31399/asm.hb.v22a.a0005435
EISBN: 978-1-62708-196-2
... Abstract This article assesses the evolution of martensite modeling in the changing materials engineering environment. It describes the physics of displacive transformations using Ginzburg-Landau theory, microstructure representation, dynamics and simulations, density functional theory...
Series: ASM Handbook
Volume: 2
Publisher: ASM International
Published: 01 January 1990
DOI: 10.31399/asm.hb.v02.a0001109
EISBN: 978-1-62708-162-7
... ( T ) − G s ( T ) = μ 0 [ H c ( T ) ] 2 / 2 Application of a magnetic field larger than H c will destroy the superconducting state. Theoretical Background of Superconductivity In 1950, Ginzburg and Landau developed a phenomenological theory...
Series: ASM Handbook
Volume: 22A
Publisher: ASM International
Published: 01 December 2009
DOI: 10.31399/asm.hb.v22a.a0005415
EISBN: 978-1-62708-196-2
... conservation law the way mass and concentration do, and they follow a different type of kinetic equation, known as the time-dependent Ginzburg-Landau equation or the Allen-Cahn equation: (Eq 12) ∂ η ∂ t = − L δ E chem δ η Here, the unit of the kinetic coefficient L...
Series: ASM Handbook
Volume: 22B
Publisher: ASM International
Published: 01 November 2010
DOI: 10.31399/asm.hb.v22b.a0005511
EISBN: 978-1-62708-197-9
... potential gradient and chemical mobility and the time-dependent Ginzburg-Landau equation ( Ref 67 ) that characterizes structural changes accompanying a phase transformation and other materials processes. The phase-field method is well known for its ability to handle arbitrary microstructures consisting...
Series: ASM Handbook
Volume: 22A
Publisher: ASM International
Published: 01 December 2009
DOI: 10.31399/asm.hb.v22a.a0005409
EISBN: 978-1-62708-196-2
... LSW theory predicts the following for the variation of the average radius of the particles ( r ¯ α ) as a function of time, t : (Eq 13a) r ¯ α 3 − r ¯ α o 3 = [ 8 D β γ α β C β V M 9 R g T ] ( t − t o...
Series: ASM Handbook
Volume: 22A
Publisher: ASM International
Published: 01 December 2009
DOI: 10.31399/asm.hb.v22a.9781627081962
EISBN: 978-1-62708-196-2
Series: ASM Handbook
Volume: 4E
Publisher: ASM International
Published: 01 June 2016
DOI: 10.31399/asm.hb.v04e.a0006277
EISBN: 978-1-62708-169-6
... methods. For example, the use of field description, gradient thermodynamics, phase transformation crystallography, and microelasticity theory of nonuniform systems allows the method to account self-consistently for an arbitrarily complex multiphase microstructure with strong shape anisotropy and well...