The dynamics of solid-solid phase transitions 2. Incoherent interfaces |
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Authors: | Paolo Cermelli Morton E Gurtin |
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Institution: | (1) Dipartimento di Matematica, Università di Torino, 10123 Torino;(2) Department of Mathematics, Carnegie Mellon University, 15213 Pittsburgh, Pennsylvania |
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Abstract: | Incoherent phase transitions are more difficult to treat than their coherent counterparts. The interface, which appears as a single surface in the deformed configuration, is represented in its undeformed state by a separate surface in each phase. This leads to a rich but detailed kinematics, one in which defects such as vacancies and dislocations are generated by the moving interface. In this paper we develop a complete theory of incoherent phase transitions in the presence of deformation and mass transport, with phase interface structured by energy and stress. The final results are a complete set of interface conditions for an evolving incoherent interface.Frequently used symbols Ai,Ci
generic subsurface of St
- Bi
undeformed phase-i region
- C
configurational bulk stress, Eshelby tensor
- F
deformation gradient
- G
inverse deformation gradient
- H
relative deformation gradient
- J
bulk Jacobian of the deformation
- ¯K, Ki
total (twice the mean) curvature of
and Si
- Lin (U, V)
linear transformations from U into V
- Lin+
linear transformations of 3 with positive determinant
- Orth+
rotations of 3
- Qa
external bulk mass supply of species a
- ¯S
bulk Cauchy stress tensor
- S
bulk Piola-Kirchhoff stress tensor
- Si
undeformed phase i interface
- Ui
relative velocity of Si
- Unim+
linear transformations of 3 with unit determinant
- ¯V, Vi
normal velocity of
and Si
-
intrinsic edge velocity of
S and A
i S
- Wi
volume flow across the phase-i interface
- X
material point
- b
external body force
- e
internal bulk configurational force
- fi
external interfacial force (configurational)
- ¯g
external interfacial force (deformational)
- grad, div
spatial gradient and divergence
-
gradient and divergence on
- h
relative deformation
- ha,
diffusive mass flux of species a and list of mass fluxes
- ¯m
outward unit normal to a spatial control volume
- ¯n, ni
unit normal to
and Si
- n
subspace of 3 orthogonal to n
- ¯qa
external interfacial mass supply of species a
- s
.........
- ¯v, vi
compatible velocity fields of
and Si
- ¯w, wi
compatible edge velocity fields for
and Ai
- x
spatial point
- yi
deformation or motion of phase i
- y.
material velocity
-
generic subsurfaces of
- , i
deformed body and deformed phase-i region
- ()
energy supplied to by mass transport
-
symmetry group of the lattice
- i,
surface jacobians
-
lattice
- ()
power expended on
-
spatial control volume
-
S
deformed phase interface
-
lattice point density
-
interfacial power density
- , A
total surface stress
- C
configurational surface stress for phase 1 (material)
- ¯Ci
configurational surface stress (spatial)
- Fi
tangential deformation gradient
- Gi
inverse tangential deformation gradient
- H
incoherency tensor
- ¯1(x), 1i(X)
inclusions of ¯n(x) and n
i
(X) into 3
- K
configurational surface stress for phase 2 (material)
- ¯L, li
curvature tensor of
and Si
- ¯P(x), Pi(X)
projections of 3 onto ¯n(x) and ni
(X)
- ¯S, S
deformational surface stress (spatial and material)
- ¯a, a
normal part of total surface stress
- c
normal part of configurational surface stress for phase 1 (material)
- ei
internal interfacial configurational force
- ¯v, vi
unit normal to
and A
i
- (x),i(X)
projections of 3 onto ¯n(x) and n
i
(X)
- i
normal internal force (material)
-
bulk free energy
-
slip velocity
- i=(–1)i i
.........
- a,
chemical potential of species a and list of potentials
- a,
bulk molar density of species a and list of molar densities
- i
normal internal force (spatial)
-
surface tension
- , i
effective shear
-
referential-to-spatial transform of field
-
interfacial energy
-
grand canonical potential
- l
unit tensor in 3
- x,
vector and tensor product in 3
- (...)., t(...)
material and spatial time derivative
- , Div
material gradient and divergence
-
gradient and divergence on Si
- (...), (...)
normal time derivative following
and Si
- (...)
limit of a bulk field asx
,xi
- ...],...>
jump and average of a bulk field across the interface
- (...)ext
extension of a surface tensor to 3
-
tangential part of a vector (tensor) on
and Si |
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Keywords: | |
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