Finite element approximation of a phase field model arising in nanostructure patterning
We consider a fully practical finite element approximation of the nonlinear parabolic Cahn–Hilliard system γ ∂ u ∂ t − ∇ _ · ( ∇ _ w ) = 0 , w = − γ Δ u + γ − 1 Ψ ′ ( u ) − 1 2 α c ′ ( · , u ) | ∇ _ ϕ | 2 , ∇ _ · ( c ( · , u ) ∇ _ ϕ ) = 0 , subject to an initial condition u 0 ( . )...
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Published in: | Numerical methods for partial differential equations Vol. 31; no. 6; pp. 1890 - 1924 |
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Main Authors: | , |
Format: | Journal Article |
Language: | English |
Published: |
New York
Blackwell Publishing Ltd
01-11-2015
Wiley Subscription Services, Inc |
Subjects: | |
Online Access: | Get full text |
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Summary: | We consider a fully practical finite element approximation of the nonlinear parabolic Cahn–Hilliard system
γ
∂
u
∂
t
−
∇
_
·
(
∇
_
w
)
=
0
,
w
=
−
γ
Δ
u
+
γ
−
1
Ψ
′
(
u
)
−
1
2
α
c
′
(
·
,
u
)
|
∇
_
ϕ
|
2
,
∇
_
·
(
c
(
·
,
u
)
∇
_
ϕ
)
=
0
,
subject to an initial condition
u
0
(
.
)
∈
[
−
1
,
1
]
on the conserved order parameter
u
∈
[
−
1
,
1
]
, and mixed boundary conditions. Here,
γ
∈
ℝ
>
0
is the interfacial parameter,
α
∈
ℝ
≥
0
is the field strength parameter,
Ψ
is the obstacle potential,
c
(
·
,
u
)
is the diffusion coefficient, and
c
′
(
·
,
u
)
denotes differentiation with respect to the second argument. Furthermore, w is the chemical potential and
ϕ
is the electrostatic potential. The system, in the context of nanostructure patterning, has been proposed to model the manipulation of morphologies in organic solar cells with the help of an applied electric field. In the limit
γ
→
0
, it reduces to a sharp interface problem that models the evolution of an unstable interface between two dielectric media in the presence of a quasistatic electric field. On introducing a finite element approximation for the above Cahn–Hilliard system, we prove existence and stability of a discrete solution. Moreover, in the case of two space dimensions, we are able to prove convergence and hence existence of a solution to the considered system of partial differential equations. We demonstrate the practicality of our finite element approximation with several numerical simulations in two and three space dimensions. © 2015 Wiley Periodicals, Inc. Numer Methods Partial Differential Eq 31: 1890–1924, 2015 |
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Bibliography: | ark:/67375/WNG-TPZJ38F3-6 ArticleID:NUM21972 istex:572B1AFFE7EF70BE1DBEDA279B32A3053B9DEF99 ObjectType-Article-1 SourceType-Scholarly Journals-1 ObjectType-Feature-2 content type line 23 |
ISSN: | 0749-159X 1098-2426 |
DOI: | 10.1002/num.21972 |