Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media - - PowerPoint PPT Presentation
Existence of the free boundary in a diffusive ow in porous media - - PowerPoint PPT Presentation
Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy Existence of the free boundary in a diffusive ow in porous media Gabriela Marinoschi Institute of Mathematical Statistics and Applied Mathematics of the Romanian
Existence of the free boundary in a diffusive ow in porous media 2
1 Problem presentation
Prove the existence of the solution to a two phase ow in a porous medium Compute the solution and the diffusive interface evolution G.M., J. Optimiz. Theory Appl., 2012
Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 3
Problem presentation
R3; open bounded, = @ sufciently smooth
Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 4
Problem presentation
Q = (0; T) ; T < 1; = (0; T) Qs = f(t; x) 2 Q; y(t; x) = ysg Qu = f(t; x) 2 Q; y(t; x) < ysg
Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 5
Problem presentation
Q = (0; T) ; T < 1; = (0; T) Qs = f(t; x) 2 Q; y(t; x) = ysg Qu = f(t; x) 2 Q; y(t; x) < ysg
Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 6
Problem presentation
@y @t (t; x; y) 3 f
in Q
@(t; x; y) @ + (t; x; y) 3 0
- n ; > 0
(NE)
y(0; x) = y0
in :
: Q (1; ys] ! R; (t; x; ) 2 C1(1; ys); lim
r%ys (t; x; r) = K s; a.e. (t; x) 2 Q:
Fast diffusion in porous media (G.M. Springer, 2006; A. Favini, G.M. Springer 2012)
Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 7
Problem presentation
@y @t (t; x; y) 3 f
in Q
@(t; x; y) @ + (t; x; y) 3 0
- n ; > 0;
(NE)
y(0; x) = y0
in :
: Q (1; ys] ! R; (t; x; ) 2 C1(1; ys); lim
r%ys (t; x; r) = K s; a.e. (t; x) 2 Q:
Fast diffusion in porous media (G.M. Springer, 2006; A. Favini, G.M. Springer 2012)
Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 8
Problem presentation
j : Q R ! (1; 1]; j(t; x; r) = ( R r
- (t; x; s)ds; r ys;
+1;
- therwise
(t; x) ! j(t; x; r) is measurable on Q for all r 2 (1; ys] j(t; x; ) proper convex l.s.c. a.e. (t; x) 2 Q @j(t; x; ) = (t; x; ) a.e. (t; x) 2 Q j(t; x; r) K
s jrj ; for any r ys; a.e. (t; x) 2 Q
Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 9
Problem presentation Conjugate of j
j(t; x; !) = sup
r2R
(!r j(t; x; r)) a.e. (t; x) 2 Q
Legendre-Fenchel relations
j(t; x; r) + j(t; x; !) r! for all r 2 R; ! 2 R; a.e. (t; x) 2 Q; j(t; x; r) + j(t; x; !) = r! if and only if ! 2 @j(t; x; r), a.e. (t; x) 2 Q: C3 j!j + C0
3 j(t; x; !) for any ! 2 R; a.e. (t; x) 2 Q:
Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 10
Problem presentation Conjugate of j
j(t; x; !) = sup
r2R
(!r j(t; x; r)) a.e. (t; x) 2 Q
Legendre-Fenchel relations
j(t; x; r) + j(t; x; !) r! for all r 2 R; ! 2 R; a.e. (t; x) 2 Q; j(t; x; r) + j(t; x; !) = r! if and only if ! 2 @j(t; x; r), a.e. (t; x) 2 Q: C3 j!j + C0
3 j(t; x; !) for any ! 2 R; a.e. (t; x) 2 Q; C3 > 0:
Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 11
Problem presentation
@y @t (t; x; y) 3 f
in Q;
@(t; x; y) @ + (t; x; y) 3 0
- n ;
(NE)
y(0; x) = y0
in :
j singular potential, j minimal growth conditions, no time and space regularity m
Minimize J(y; w) for all (y; w) 2 U (P) connected with (NE) by j and j
Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 12
Problem presentation
@y @t (t; x; y) 3 f
in Q
@(t; x; y) @ + (t; x; y) 3 0
- n
(NE)
y(0; x) = y0
in :
j singular potential, j minimal growth conditions, no time and space regularity m
Minimize J(y; w) for all (y; w) 2 U (P) connected with (NE) by j and j
1
1
- H. Brezis, I. Ekeland, C.R. Acad. Sci. Paris, 282, 971–974, 1197–1198, 1976
Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 13
Problem presentation
I H. Brezis, I. Ekeland (C.R. Acad. Sci. Paris, 1976) I G. Auchmuty (NA, 1988) I N. Ghoussoub, L. Tzou ( Math. Ann. 2004) I N. Ghoussoub (Springer, 2009) I A. Visintin ( Adv. Math. Sci. Appl. 2008) I U. Stefanelli (SICON 2008, J. Convex Analysis 2009) I V. Barbu (JMAA 2011) I G. M. (JOTA 2012, 2013)
Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 14
Problem presentation
- Denition. Let f 2 L1(Q);
y0 2 L1(); y0 ys a.e. on :
A weak solution to (NE) is a pair (y; w)
y 2 L1(Q); w 2 (L1(Q))0; (w = wa + ws; wa 2 L1(Q)) wa(t; x) 2 @j(t; x; y) = (t; x; y) a.e. on Q; ws 2 ND(')(y)
- Z
Q
yd dt dxdt + Z
- y0 (0) + hw; A0;1 i(L1(Q))0;L1(Q) =
Z
Q
f dxdt
() for any 2 W 1;1([0; T]; L1()) \ L1(0; T; D(A0;1)); (T) = 0:
A0;1 = ; A0;1 : D(A0;1) L1() ! L1(); D(A0;1) = f 2 W 2;1(); @ @ + = 0 on g:
Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 15
Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 16
2 A duality approach
Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 17
A duality approach
J : L1(Q) L1(Q)
Min
(y;w)2U
Z
Q
(j(t; x; y(t; x)) + j(t; x; w(t; x))dxdt y(t; x)w(t; x)) dxdt
- U =
- (y; w); y 2 L1(Q); y(t; x) ys a.e., w 2 L1(Q); dy
dt w = f; y(0) = y0
- Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 18
A duality approach
J : L1(Q) (L1(Q))0 J(y; w) = Z
Q
j(t; x; y(t; x))dxdt + '(t; x; w) w(y)
Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 19
A duality approach
w 2 (L1(Q))0; w = wa + ws L1(Q) 3 wa = "absolutely continuous component", ws = singular component ' : L1(Q) ! (1; 1]; '(y) = Z
Q
j(t; x; y(t; x))dxdt proper, convex, lsc ' : (L1(Q))0 ! (1; 1]; '(w) = Z
Q
j(t; x; wa(t; x))dxdt +
D(')(ws);
- D(')(v) = supfv( ); 2 D(')g = conjugate of the indicator function of D(')
D(') = fy 2 L1(Q); '(y) < +1g = fy 2 L1(Q); y(t; x) ys a.e. g:
Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 20
A duality approach2
' : L1(Q) ! (1; 1] '(y) = R
Q j(t; x; y(t; x))dxdt proper, convex, lsc
' : (L1(Q))0 ! (1; 1] '(w) = R
Q j(t; x; wa(t; x))dxdt + D(')(ws)
- D(')(v) = supfv( ); 2 D(')g = conjugate of the indicator function of D(')
D(') = fy 2 L1(Q); '(y) < +1g = fy 2 L1(Q); y(t; x) ys a.e.g:
2 R.T. Rockafeller, Pacic J. Math. J, 39, 2, 1971 Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 21
A duality approach3
' : L1(Q) ! (1; 1] '(y) = R
Q j(t; x; y(t; x))dxdt proper, convex, lsc
' : (L1(Q))0 ! (1; 1] '(w) = R
Q j(t; x; wa(t; x))dxdt + D(')(ws)
- D(')(v) = supfv( ); 2 D(')g = conjugate of the indicator function of D(')
D(') = fy 2 L1(Q); '(y) < +1g = fy 2 L1(Q); y(t; x) ys a.e.g:
3 R.T. Rockafeller, Pacic J. Math. J, 39, 2, 1971 Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 22
A duality approach
J : L1(Q) (L1(Q))0 J(y; w) = Z
Q
j(t; x; y(t; x))dxdt + Z
Q
j(t; x; wa)dxdt +
D(')(ws) w(y)
In some good cases we have a Lemma of integration by parts:
w(y) = 1 2 ky(T)k2
(H1())0 1
2 ky0k2
(H1())0
Z
Q
fA1
0;1ydxdt
(**)
Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 23
A duality approach
J : L1(Q) (L1(Q))0 J(y; w) = Z
Q
j(t; x; y(t; x))dxdt + Z
Q
j(t; x; wa)dxdt +
D(')(ws) w(y)
In some good cases we have a Lemma of integration by parts:
w(y) = 1 2 ky(T)k2
(H1())0 1
2 ky0k2
(H1())0
Z
Q
fA1
0;1ydxdt
(**)
Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 24
A duality approach
J : L1(Q) (L1(Q))0 J(y; w) = Z
Q
j(t; x; y(t; x))dxdt + Z
Q
j(t; x; wa)dxdt +
D(')(ws) w(y)
In some good cases we have a Lemma of integration by parts:
dy dt w = f
- 1y
(**)
Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 25
A duality approach Minimize (J) for all (y; w) 2 U (P)
J(y; w) = 8 > < > : R
Q j(t; x; y(t; x))dxdt +
R
Q j(t; x; wa(t; x))dxdt + D(')(ws)
+1
2 ky(T)k2 (H1())0 1 2 ky0k2 (H1())0
R
Q fA1 0;1ydxdt
if (y; w) 2 U;
U =
- (y; w); y 2 L1(Q); y(t; x) 2 [0; ys] a.e., y(T) 2 (H1())0; w 2 (L1(Q))0;
(y; w) veries ()g
- Z
Q
yd dt dxdt + Z
- y0 (0) + hw; A0;1 i(L1(Q))0;L1(Q) =
Z
Q
f dxdt
for any 2 W 1;1([0; T]; L1()) \ L1(0; T; D(A0;1)); (T) = 0:
Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 26
A duality approach Minimize (J) for all (y; w) 2 U (P)
J(y; w) = 8 > < > : R
Q j(t; x; y(t; x))dxdt +
R
Q j(t; x; wa(t; x))dxdt + D(')(ws)
+1
2 ky(T)k2 (H1())0 1 2 ky0k2 (H1())0
R
Q fA1 0;1ydxdt
if (y; w) 2 U;
U =
- (y; w); y 2 L1(Q); y(t; x) 2 [0; ys] a.e., y(T) 2 (H1())0; w 2 (L1(Q))0;
(y; w) veries ()g
- Z
Q
yd dt dxdt + Z
- y0 (0) + hw; A0;1 i(L1(Q))0;L1(Q) =
Z
Q
f dxdt
() for any 2 W 1;1([0; T]; L1()) \ L1(0; T; D(A0;1)); (T) = 0:
Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 27
A duality approach Theorem
J is proper, convex, l.s.c. on L1(Q) (L1(Q))0:
Problem (P) has at least a solution (y; w):
4
A solution to (P) is called a generalized solution to (NE)
4
Alaoglu theorem
Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 28
A duality approach Theorem
J is proper, convex, l.s.c. on L1(Q) (L1(Q))0:
Problem (P) has at least a solution (y; w):
5
A solution to (P) is called a generalized solution to (NE)
5
Alaoglu theorem
Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 29
A duality approach Theorem Let (y; w) be the null minimizer in (P); i:e:; J(y; w) = 0: Assume that
1 2 ky(T)k2
(H1())0 1
2 ky0k2
(H1())0
Z
Q
fA1
0;1ydxdt = w(y):
(**) Then, (y; w) is the weak solution to (NE); i.e.,
wa(t; x) 2 (t; x; y(t; x)) a.e. (t; x) 2 Q
and
ws 2 ND(')(y):
Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 30
A duality approach Proof sketch
J(y; w) = Z
Q
j(t; x; y)dxdt + Z
Q
j(t; x; wa)dxdt +
D(')(ws)
+1 2 ky(T)k2
(H1())0 1
2 ky0k2
(H1())0
Z
Q
fA1
0;1ydxdt = 0
- D(')(ws) = supfws(z); z 2 D(')g ws(y)
Z
Q
j(t; x; y)dxdt + Z
Q
j(t; x; wa)dxdt Z
Q
waydxdt 0 ws(y) +
D(')(ws) = 0:
ws(y) ws(z) for any z 2 D(') = ) ws 2 ND(')(y):
Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 31
A duality approach Proof sketch
J(y; w) = Z
Q
j(t; x; y)dxdt + Z
Q
j(t; x; wa)dxdt +
D(')(ws)
- Z
Q
waydxdt ws(y) = 0
- D(')(ws) = supfws(z); z 2 D(')g ws(y)
Z
Q
(j(t; x; y) + j(t; x; wa) way)dxdt = 0 = ) wa(t; x) 2 (t; x; y(t; x)) a.e. (t; x) 2 Q ws(y) +
D(')(ws) = 0:
ws(y) ws(z) for any z 2 D(') = ) ws 2 ND(')(y):
Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 32
A duality approach Proof sketch
J(y; w) = Z
Q
j(t; x; y)dxdt + Z
Q
j(t; x; wa)dxdt +
D(')(ws)
- Z
Q
waydxdt ws(y) = 0
- D(')(ws) = supfws(z); z 2 D(')g ws(y)
Z
Q
(j(t; x; y) + j(t; x; wa) way)dxdt = 0 = ) wa(t; x) 2 (t; x; y(t; x)) a.e. (t; x) 2 Q ws(y) +
D(')(ws) = 0:
ws(y) ws(z) for any z 2 D(') = ) ws 2 ND(')(y):
Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 33
A duality approach
dy dt( ) + wa(A0;1 ) + ws(A0;1 ) = f( );
for any 2 W 1;1([0; T]; L1()) \ L1(0; T; D(A0;1)); (T) = 0: If dy
dt 2 (L1(Q))0
dy dt
- a
( ) + dy dt
- s
( ) + wa(A0;1 ) + ws(A0;1 ) = f( ):
Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 34
A duality approach If
y 2 intD(') = fy 2 L1(Q); ess sup y(t; x) < ysg = ) ND(')(y) = f0g = ) ws = 0 dy dt (t; x; y) = f; a.e. on Q
with initial condition and b.c.
Q = Qu = f(t; x); y(t; x) < ysg
unsaturated ow
Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 35
A duality approach If
y 2 @D(') = fy 2 L1(Q); ess sup y(t; x) = ysg = ) Qs = f(t; x); y(t; x) = ysg Qu = f(t; x); y(t; x) < ysg
- dy
dt
- s ws 3 0; in D0(
- Qs)
- dy
dt
- a (t; x; y) = f; a.e. on Qu
saturated unsaturated
Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 36
A duality approach If
y 2 @D(') = fy 2 L1(Q); ess sup y(t; x) = ysg = ) Qs = f(t; x); y(t; x) = ysg Qu = f(t; x); y(t; x) < ysg
- dy
dt
- s ws 3 0; in D0(
- Qs)
- dy
dt
- a (t; x; y) = f; a.e. on Qu
saturated unsaturated
Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 37
Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 38
3 A direct approach
Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 39
A direct approach: regularity for (t; x; r)
@y @t (t; x; y) + r K0(t; x; y) 3 f
in Q
@(t; x; y) @ + (t; x; y) 3 0
- n
(NE)
y(0; x) = y0
in :
(; ; r) 2 W 2;1(Q); for any r 2 (1; ys]; ((t; x; r) (t; x; r))(r r) (r r)2; for any r; r 2 (1; ys]; > 0 K0(t; x; y) = a(t; x)K(y); aj 2 W 1;1(Q); K Lipschitz and bounded.
Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 40
A direct approach: regularity for (t; x; r)
- Denition. Let f 2 L2(0; T; V 0); y0 2 L1(); y0 ys a.e.
We call a solution to (NE) a pair (y; w) such that
y 2 C([0; T]; L2()) \ L2(0; T; V ) \ W 1;2([0; T]; V 0) w 2 L2(0; T; V ); w(t; x) 2 (t; x; y(t; x)) a.e. on Q; y ys; a.e. (t; x) 2 Q;
which satises the equation
Z T dy dt(t); (t)
- V 0;V
dt + Z
Q
(rw K0(t; x; y)) rdxdt = Z T hf(t); (t)iV 0;V dt
for any 2 L2(0; T; V ); and the condition y(0) = y0:
V = H1(); V 0 = (H1())0
Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 41
A direct approach: regularity for (t; x; r) For each t
A(t) : D(A(t)) (H1())0 ! (H1())0; D(A(t)) =
- z 2 L2(); 9w 2 V; w(x) 2 (t; x; z)) a.e. x 2
- ;
by the relation
hA(t)z; iV 0;V := Z
- (rw K0(t; x; y)) r dx; for any 2 V:
dy dt(t) + A(t)y(t) 3 f(t); a.e. t 2 (0; T); y(0) = y0:
Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 42
A direct approach: regularity for (t; x; r)
- Step. 1 Prove the existence to the regularized Cauchy problem6
dy dt(t) + A"(t)y(t) = f(t); a.e. t 2 (0; T); y(0) = y0:
(a) The domain of A"(t) is independent of t and D(A"(t)) = D(A"(0)) = V: (b) For each " > 0 and t 2 [0; T] xed, the operator A"(t) is quasi m-accretive on V 0: (c) For 2 V and 0 s; t T we have
kA"(t) A"(s)kV 0 jt sj g (kkV 0) (kA(t)kV 0 + 1);
where g : [0; 1) ! [0; 1) is a nondecreasing function. Step 2. passing to the limit.
6 M.G. Crandall, A. Pazy, Proceedings of The American Mathematical Society, 1979
- C. Dafermos, M. Slemrod, J. Functional Anal.,1973
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Existence of the free boundary in a diffusive ow in porous media 43
4 Numerical results
Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 44
Numerical results
dy dt(t) + Ay(t) = f(t); a.e. t 2 (0; T); y(0) = y0: yh
i+1 yh i
h + Ayh
i+1 = f h i+1; i = 1; :::; n 1
yh
0 = y0
Stability and convergence Algorithm based on the proof of the m-accretivity of Ah = A + 1
hI
1 hI + Ah
- = g
for any g 2 V 0; has a solution 2 D(A):
Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 45
Numerical results
= f(x; y); x 2 (0; 5); y 2 (0; 5)g; T = 20 (r) = (
(c1)r (cr) ; r 2 [0; 1);
[1; 1) ; r = 1: ; K(r) = (c 1)r2 c r ; r 2 [0; 1] 0(x; y) = 0:01; f = 0; = 108; rain = exp(30 x2)= exp(30); c = 1:02 " " " " rain
Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy
Existence of the free boundary in a diffusive ow in porous media 46
Numerical results
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Diffuse Interface Models - DIMO2013, September 10-13, 2013, Levico Terme, Italy