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Existence of Weak Solutions for a Nonlinear Elliptic System
Boundary Value Problems volume 2009, Article number: 708389 (2009)
Abstract
We investigate the existence of weak solutions to the following Dirichlet boundary value problem, which occurs when modeling an injection molding process with a partial slip condition on the boundary. We have in
;
in
;
, and
on
.
1. Introduction
Injection molding is a manufacturing process for producing parts from both thermoplastic and thermosetting plastic materials. When the material is in contact with the mold wall surface, one has three choices: (i) no slip (which implies that the material sticks to the surface) (ii) partial slip, and (iii) complete slip [1–5]. Navier [6] in 1827 first proposed a partial slip condition for rough surfaces, relating the tangential velocity to the local tangential shear stress

where indicates the amount of slip. When
, (1.1) reduces to the no-slip boundary condition. A nonzero
implies partial slip. As
, the solid surface tends to full slip.
There is a full description of the injection molding process in [3] and in our paper [7]. The formulation of this process as an elliptic system is given here in after.
Problem 1.
Find functions and
defined in
such that



Here we assume that is a bounded domain in
with a
boundary. We assume also that
,
,
,
, and
are given functions, while
is a given positive constant related to the power law index;
is the pressure of the flow, and
is the temperature. The leading order term
of the PDE (1.3) is derived from a nonlinear slip condition of Navier type. Similar derivations based on the Navier slip condition occur elsewhere, for example, [8, 9], [10, equation (
)] .
The mathematical model for this system was established in [7]. Some related papers, both rigorous and formal, are [3, 11–13]. In [11, 13], existence results in no-slip surface, , are obtained, while in [3, 7], Navier's slip conditions,
and
, are investigated, and numerical, existence, uniqueness, and regularity results are given. Although the physical models are two dimensional, we shall carry out our proofs in the case of
dimension.
In Section 2, we introduce some notations and lemmas needed in later sections. In Section 3, we investigate the existence, uniqueness, stability, and continuity of solution to the nonlinear equation (1.3). In Section 4, we study the existence of weak solutions to Problem 1.
Using Rothe's method of time discretization and an existence result for Problem 1, one can establish existence of week solutions to the following time-dependent problem.
Problem 2.
Find functions and
defined in
such that

The proof is only a slight modification of the proofs given in [11, 13] and is omitted here.
2. Notations and Preliminaries
2.1. Notations
In this paper, for let
and
denote the usual Sobolev space equipped with the standard norm. Let

where . The conjugate exponent of
is

We assume that the boundary values and
for Problem 1 can be extended to functions defined on
such that

We further assume that there exist positive numbers and
such that

Finally, we assume that for ,
a.e. in
indicates

For the convenience of exposition, we assume that

Next, we recall some previous results which will be needed in the rest of the paper.
2.2. Preliminaries
An important inequality (e.g., see [11, page 550] ) in the study of -Laplacian is as follows:

where and
are certain constants.
To establish coercivity condition, we will use the following inequality:

where ,
, and
.
Using the Sobolev Embedding Theorem and Hölder's Inequality, we can derive the following results (for more details, see [11, Lemma 3.4] and [13, Lemma 4.2]).
Lemma 2.1.
The following statements hold
() For any positive numbers
and
, if
and
then

moreover,
() If
and
, then
moreover,

() If
and
, then
, where

and denotes the conjugate of r, namely,
for
moreover,

() If
and
, then

where and
. Moreover

The existence proof will use the following general result of monotone operators [14, Corollary III.1.8, page 87] and [15, Proposition 17.2].
Proposition 2.2.
Let be a closed convex set (
), and let
be monotone, coercive, and weakly continuous on
. Then there exists

The uniqueness proof is based on a supersolution argument (similar definition can be found in [15, Chapter 3]).
Definition 2.3.
A function is a weak supersolution of the equation

in if

whenever is nonnegative.
3. A Dirichlet Boundary Value Problem
We study the following Dirichlet boundary value problem:

Definition 3.1.
We say that is a weak solution to (3.1) if

for all and a given
.
Theorem 3.2.
Assume that conditions (2.1)–(2.6) are satisfied. Then there exists a unique weak solution to the Dirichlet boundary value problem (3.1) in the sense of Definition 3.1. In addition, the solution
satisfies the following properties.
we have

where is a constant independent of
and
;
if
a.e. in
, then

The idea behind the existence proof is related to [15, 16]. We will first consider the following Obstacle Problem.
Problem 3.
Find a function in
such that

for all . Here

Lemma 3.3.
If is nonempty, then there is a unique solution p to the Problem 3 in
.
Proof of Lemma 3.3.
Our proof will use Proposition 2.2.
Let and write

It follows from the proof in [15, Proposition 17.2] that is a closed convex set.
Next we define a mapping by

By Hölder's inequality,

Here we used Assumption (2.6), that is, . Therefore we have
whenever
. Moreover, it follows from inequality (2.7) that
is monotone.
To show that is coercive on
, fix
. Then

Inequality (2.8) is used to arrive at the last step. This implies that is coercive on
.
Finally, we show that is weakly continuous on
. Let
be a sequence that converges to an element
in
. Select a subsequence {
} such that
a.e. in
. Then it follows that

a.e. in . Moreover,

Thus we have that

weakly in . Since the weak limit is independent of the choice of the subsequence, it follows that

weakly in . Hence
is weakly continuous on
. We may apply Proposition 2.2 to obtain the existence of
.
Our uniqueness proof is inspired by [15, Lemmas ,
, and Theorem
]. Since
does not satisfy condition (3.4) of
operator in [15], we need to prove the following lemma, which is equivalent to [15, Lemma 3.11]. Then uniqueness can follow immediately from [15, Lemma 3.22].
Lemma 3.4.
If is a supersolution of (2.16) in
, then

for all nonnegative .
Proof.
Let and choose nonnegative sequence
such that
in
. Equation (2.6) and Hölder inequality imply that

Because , we obtain

and the lemma follows.
Similar to [15, Corollary 17.3, page 335], one can also obtain the following Corollary.
Corollary 3.5.
Let be bounded and
. There is a weak solution
to (3.1) in the sense of Definition 3.1.
Proof of Theorem 3.2.
The existence result is given in Corollary 3.5, and we now turn to proof of uniqueness. For a given , assume that there exists another solution
Then we have that

for all . If we take
in above equation, from inequality (2.7), we have the following.
() when
,

where is a positive constant;
() when
,

Here the Hölder inequality for , namely,

is applied to the last inequality.
Poincaré's inequality implies that a.e. We complete the uniqueness proof.
Next we prove (3.3). Taking in (3.2), we have

From (2.4), and the Hölder inequality, we obtain

Young's inequality with implies

and (3.3) follows immediately from (2.3) and (2.6).
Finally, we prove (3.4). From weak solution definition (3.2), we know that

Setting and subtracting
from both sides, we obtain that

Denote the right-hand side by . Similar to arguments in the uniqueness proof, we arrive at the folloing:
() when
,

() when
,

Egorov's Theorem implies that for all , there is a closed subset
of
such that
and
uniformly on
. Application of the absolute continuity of the Lebesgue Integral implies

Theorem 3.2 is proved.
4. Nonlinear Elliptic Dirichlet System
Definition 4.1.
We say that is a weak solution to Problem 1 if

and for all

and for all

Theorem 4.2.
Assume that (2.1)–(2.6) hold. Then there exists a weak solution to Problem 1 in the sense of Definition 4.1.
We shall bound the critical growth, , on the right-hand side of (4.2).
Lemma 4.3.
Suppose that and
satisfy

and (4.3). Then, under the conditions of Theorem 4.2, for all

Moreover, there exists a polynomial that is independent of
and
such that

Proof.
We first show (4.5). Letting in (4.3), we obtain

After some straightforward computations this yields exactly (4.5).
We now show (4.6). We denote the four terms on the right-hand side of equation (4.5) by I, II, III, and IV, respectively. Under the conditions of Lemma 4.3, we have

Part (iii) of Lemma 2.1 and Sobolev's imbedding theorems indicate

where satisfies
.
According to Sobolev's imbedding theorems, the integrability of depends on
. We estimate II in three different cases.
Case 1 ().

Case 2 ().

Case 3 ().
is a bounded continuous function, so

We next estimate III:

The estimate of the first term used Hölder inequality and Sobolev's imbedding theorems. The argument of the second estimate is similar to that of I.
Recall that . Similar to II, we estimate IV in three different cases.
Case 1 ().

Since , we have

Case 2 ().

Since , we have

Case 3 ().

These estimates lead to

for some polynomial .
Proof of Theorem 4.2.
Using Theorem 3.2, let then for (3.2) there exists a unique solution
satisfying

Moreover, if a.e. in
, then

Next, using Lemma 4.3, we can define a linear functional determined by

for all By virtue of (4.6),
is well defined, and there exists a constant
independent of
such that

We notice that (4.2) is the same as [11, equation ()]. Therefore, arguments after [11, equation (
)] can be used to complete the proof of Theorem 4.2.
References
Barone MR, Caulk DA: The effect of deformation and thermoset cure on heat conduction in a chopped-fiber reinforced polyester during compression molding. International Journal of Heat and Mass Transfer 1979, 22(7):1021–1032. 10.1016/0017-9310(79)90175-3
Laun HM, Rady M, Hassager O: Analytical solutions for squeeze flow with partial wall slip. Journal of Non-Newtonian Fluid Mechanics 1999, 81: 1–15. 10.1016/S0377-0257(98)00083-4
Advani SG, Sozer EM: Process Modeling in Composites Manufacturing. Marcel Dekker, New York, NY, USA; 2003.
Engmann J, Servais C, Burbidge AS: Squeeze flow theory and applications to rheometry: a review. Journal of Non-Newtonian Fluid Mechanics 2005, 132: 1–27. 10.1016/j.jnnfm.2005.08.007
Arda DR, Mackley MR: Shark skin instabilities and the effect of slip from gas-assisted extrusion. Rheologica Acta 2005, 44(4):352–359. 10.1007/s00397-004-0416-1
Navier CLM: Sur les lois du mouvement des fluides. Comptes Rendus de l'Académie des Sciences 1827, 6: 389–440.
Fang M, Gilbert R: Squeeze flow with Navier's slip conditions. preprint
Greenspan HP: On the motion of a small viscous droplet that wets a surface. Journal of Fluid Mechanics 1978, 84: 125–143. 10.1017/S0022112078000075
Münch A, Wagner BA: Numerical and asymptotic results on the linear stability of a thin film spreading down a slope of small inclination. European Journal of Applied Mathematics 1999, 10(3):297–318. 10.1017/S0956792599003769
Buckingham R, Shearer M, Bertozzi A: Thin film traveling waves and the Navier slip condition. SIAM Journal on Applied Mathematics 2002, 63(2):722–744.
Gilbert RP, Shi P: Nonisothermal, non-Newtonian Hele-Shaw flows—II: asymptotics and existence of weak solutions. Nonlinear Analysis: Theory, Methods & Applications 1996, 27(5):539–559. 10.1016/0362-546X(95)00022-N
Aronsson G, Evans LC: An asymptotic model for compression molding. Indiana University Mathematics Journal 2002, 51(1):1–36.
Gilbert RP, Fang M: Nonlinear systems arising from nonisothermal, non-Newtonian Hele-Shaw flows in the presence of body forces and sources. Mathematical and Computer Modelling 2002, 35(13):1425–1444. 10.1016/S0895-7177(02)00094-8
Kinderlehrer D, Stampacchia G: An Introduction to Variational Inequalities and Their Applications, Pure and Applied Mathematics. Volume 88. Academic Press, New York, NY, USA; 1980:xiv+313.
Heinonen J, Kilpeläinen T, Martio O: Nonlinear Potential Theory of Degenerate Elliptic Equations, Oxford Mathematical Monographs. The Clarendon Press, Oxford University Press, New York, NY, USA; 1993:vi+363.
Gilbert RP, Fang M: An obstacle problem in non-isothermal and non-Newtonian Hele-Shaw flows. Communications in Applied Analysis 2004, 8(4):459–489.
Acknowledgments
The project is partially supported by NSF/STARS Grant (NSF-0207971) and Research Initiation Awards at the Norfolk State University. The second author's work has been supported in part by NSF Grants OISE-0438765 and DMS-0920850. The project is also partially supported by a grant at Fudan University.
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Fang, M., Gilbert, R.P. Existence of Weak Solutions for a Nonlinear Elliptic System. Bound Value Probl 2009, 708389 (2009). https://doi.org/10.1155/2009/708389
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DOI: https://doi.org/10.1155/2009/708389
Keywords
- Weak Solution
- Elliptic System
- Slip Condition
- Obstacle Problem
- Existence Proof