Research Article | Open Access

E. Ortega-Torres, E. J. Villamizar-Roa, M. A. Rojas-Medar, "Micropolar Fluids with Vanishing Viscosity", *Abstract and Applied Analysis*, vol. 2010, Article ID 843692, 18 pages, 2010. https://doi.org/10.1155/2010/843692

# Micropolar Fluids with Vanishing Viscosity

**Academic Editor:**Nobuyuki Kenmochi

#### Abstract

A study of the convergence of weak solutions of the nonstationary micropolar fluids, in bounded domains of , when the viscosities tend to zero, is established. In the limit, a fluid governed by an Euler-like system is found.

#### 1. Introduction

The aim of this work is to analyze the convergence of the evolution equations for the motion of incompressible micropolar fluids, when the viscosities related to the physical properties of the fluid tend to zero. The equations that describe the motion of a viscous incompressible micropolar fluid express the balance of mass, momentum, and angular momentum. In a bounded domain and in a time interval , this model is given by the following system of differential equations: with , where the unknowns are , and which denote, respectively, the velocity of the fluid, the microrotational velocity, and the hydrostatic pressure of the fluid, at a point , and are positive constants which satisfy with where represent viscosity coefficients. In particular, is the usual Newtonian viscosity, is called the viscosity of microrotation and are new viscosities related to the asymmetry of the stress tensor. The fields and are given and denote external sources of linear and angular momentum, respectively.

With (1.1)–(1.3) the following initial and boundary conditions are prescribed where, for the simplicity in this exposition, homogeneous boundary conditions have been taken. The initial data is also assumed to be equal to zero due to the nature of the solutions of the Euler-like system (1.6)–(1.10) below.

Theory of micropolar fluids was proposed by Eringen [1] and describes flows of fluids whose particles undergo translations androtations as well. In this sense, micropolar fluids permit to consider some physical phenomena that cannot be treated by the classical Navier-Stokes equations for viscous incompressible fluids. Indeed, if in system (1.1)–(1.3), the equations are decoupled and (1.1) reduces to the incompressible Navier-Stokes equations (see [2]). For the derivation and physical discussion of system (1.1)–(1.3), see the references [1, 3, 4].

There is extensive literature related to the solutions of micropolar fluids. In a hilbertian context, in [4–6] and some references therein, results of existence, uniqueness and regularity of weak solutions were found. On the other hand, in [7, 8], by using semigroups approach, some recent results related to the initial value problem (1.1)–(1.5) with initial data in - spaces, including the stability of strong steady solutions, were performed.

This work is concerned with the behavior of the micropolar fluids, in a bounded domain , with boundary smooth enough, when the viscosities tend to zero. We will prove that there is a subspace of such that, for external sources in the weak solutions of the micropolar fluid system (1.1)–(1.3) converge in when the viscosities in (1.1)–(1.3) tend to zero, to the solution of the following Euler-like system: As far as it is known, the analysis of convergence of the evolution equations for the motion of incompressible micropolar fluids, when the viscosities tend to zero, in an open set with being a bounded domain of is still unknown. In [9] a nonhomogeneous, viscous incompressible asymmetric fluid in was considered, and the existence of a small time interval where the fluid variables converge uniformly as the viscosities tend to zero was proved. However, the results of [9] are not applicable in our case, that is, when is a bounded domain of . Indeed, the analysis of our situation is still more difficult. The difficulties arise from the lack of smoothness of the weak solution. To overcome this difficulty a penalization argument is needed. This argument generalizes the penalization method given in [10], for the Navier-Stokes equations, to this case of micropolar fluids. In fact, if we take the viscosity of microrotation our results imply the other ones in [10], where the analysis of the convergence in an appropriate sense, of solutions of Navier-Stokes equations to the solutions of the Euler equations on a small time interval, is given. It is worthwhile to remark that [10] has been the unique work where the convergence of nonstationary Navier-Stokes equations, with vanishing viscosity, to the Euler equations, in a bounded domain of has been considered. In the whole space the authors of [11–13] analyzed the convergence, as the viscosity tends to zero, of the Navier-Stokes equations to the solution of the Euler equations on a small time interval. The two-dimensional case is more usual in the literature. In fact, the book [14] presents a result where the fundamental argument involves the stream formulation for the Navier-Stokes equations, which is not applicable in the three-dimensional case.

This paper is organized as follows. In Section 2 the basic notation is stated and the main results are formulated. In Section 3, the analysis of convergence of solutions of the initial value problem (1.1)–(1.5), when the viscosities tend to zero, is done. This analysis is based on the ideas of [10] for Navier-Stokes equations in bounded domains.

#### 2. Statements and Notations

Let be a bounded domain of with smooth enough boundary We consider the usual Sobolev spaces with norm denoted by . is the closure in the norm In order to distinguish the scalar-value functions to vector-value functions, bold characters will be used; for instance, and so on. The solenoidal functional spaces and , will be also used. Here the Helmholtz decomposition of the space where is recalled. Throughout the paper, denotes the orthogonal projection from onto The norm in the -spaces will be denoted by In particular, the norm in and its scalar product will be denoted by and , respectively. Moreover will denote some duality products. We remark that, in the rest of this paper, the letter denotes inessential positive constants which may vary from line to line.

In order to study the behavior of system (1.1)–(1.5), when the viscosities tend to zero, the initial value problem (1.6)–(1.10) is required to study. An immediate question related to the system (1.6)–(1.10) is to know about the existence of its solution. In the following lemma a partial result about the existence and uniqueness of solution of problem (1.6)–(1.10) is given. For that, let us consider the following functional space: Thus we have the following lemma.

Lemma 2.1. *Let . Then there is a unique solution of problem (1.6)–(1.10).*

*Proof. * The proof follows by using the arguments of [10, Lemma ]. Indeed, with being an element of , we consider and define
Note that the pair satisfies conditions (1.4) and (1.5). Moreover, and thus, . Then, and . Hence
with . Therefore the proof of the existence is finished.

In order to prove the uniqueness, we consider and two solutions of (1.6)–(1.10) and define , . Then, from (1.6) and (1.8), we have
Taking the inner product of (2.4) with the function we obtain
Since and , we get
Integrating the last inequality from to , we have , which implies Consequently .

Similarly, by taking the inner product of (2.5) with the function we find
Then, by integrating the last equality from to , we have and thus .

In the next theorem our main result is stated.

Theorem 2.2. *Let be in . Then one has the following.**(1) Existence*

There is a weak solution of problem (1.1)–(1.5) verifying
where and are dependent on *(2) Convergence*

If is the unique solution of problem (1.6)–(1.10) given by Lemma 2.1, then
Moreover, if for some constant , as one has

*Remark 2.3. *() Due to that we are interested in the convergence of system (1.1)–(1.5) when go to zero, the assumptions in item () of Theorem 2.2 are verified. Moreover, since if , system (1.1)–(1.5) decouples and therefore, if tends to zero, the known results for the Navier-Stokes equations are recovered.

() Note that although in Theorem 2.2 the external sources and are assumed in the class the case of constant external sources is covered.

#### 3. Vanishing Viscosity: Proof of Theorem 2.2

The aim of this section is to prove Theorem 2.2. For this the following auxiliary result is needed.

Lemma 3.1. *Let and for real constants consider the operator defined by Then for all the following inequality holds
*

*Proof. * Using the equality and the definition of , we obtain
Hence the proof of lemma is finished.

The next theorem is crucial in the proof of our main result.

Theorem 3.2. *Let be in and . Then, for each with there is a unique solution of the problem
*

*Proof. * In order to prove the existence of solutions of system (3.3)–(3.7), the Galerkin method is used. Let the subspace of spanned by and be the subspace of spanned by . For each , the following approximations and of and , are defined:
for , where the coefficients and are calculated such that and solve the following system:
for all and .

Then, by multiplying (3.9) by and , respectively, summing over from to and taking into account (3.8), we have
Now, by applying Hölder's and Young's inequalities we get
Then, summing (3.10), with the help of last inequalities, we obtain
and hence, by integrating (3.12) from to we find
Applying Gronwall's inequality in (3.13) we get
Thus, from (3.14) we conclude that there is such that as
Now, since and, from (3.14) we have that consequently and , with and being the topological duals of and respectively. Therefore
Since is compact and is continuous, as well as is compact and is continuous, then as , we obtain

In order to pass to the limit in (3.9) we take into account (3.15) and (3.17). Indeed, the convergence in the linear terms follows directly. Moreover, as in [2, page 289], we can prove that as
for all and all Finally, from (3.15) we have
and hence, by taking in (3.19), and then, as we get
Moreover, as
we conclude that

Now the uniqueness of solution will be analyzed. Let and be two solutions of (3.3)–(3.7). We denote , and . Then we have
Taking the inner product of (3.23) with of (3.25) with by using (3.24), we obtain
Hence, by using Lemma 3.1 we get
Consequently
Now, by using Hölder's and Young's inequalities we have
Then, by summing (3.28), and taking into account the last inequalities, we obtain
where .

Since , by integrating (3.30) from to and then applying Gronwall's inequality, we conclude that
which implies and Consequently the uniqueness of solution is proved.

Proposition 3.3. *Under the assumptions of Lemma 2.1 and Theorem 3.2, if and are the solutions of problems (3.3)–(3.7) and (1.6)–(1.10), respectively, then
*

*Proof. * Considering the differences between (1.6) and (3.3), as well as between (1.8) and (3.5) and then by taking the inner product with and **,** respectively, we have
Recalling the notation we get
Using Hölder's and Young's inequalities we bound the right hand of (3.34) and (3.35) as follows:
Carrying (3.36)–(3.39) in (3.34) and (3.40)–(3.45) in (3.35), we have

Now, by using the equality the definition of and Lemma 3.1, from (3.46) we get
which implies

Since and , by integrating (3.48) from to and then applying Gronwall's inequality, we obtain
and hence the proof of estimates (3.32) is concluded.

Proposition 3.4. *Under the assumptions of Theorem 3.2 and considering , then as the solution of (3.3)–(3.7) verifies the following convergences:
**
where is a solution of problem (1.1)–(1.3).*

*Proof. * Let be as in Theorem 3.2. Then from (3.14) we have
where is a constant which does not depend on , and .

Then, since and , we have that Consequently and , with and being the topological dual of and , respectively.

Now, since from (3.3) and (3.5) we obtain
Then, by using and (3.51), from the last inequalities we get
Integrating the last inequalities from to we conclude
Using Hölder's inequality and (3.51), since we obtain
Hence, from (3.54)–(3.55) and (3.51) we get
Thus, since , from last two inequalities we have
where the constant is independent of , and .

From (3.51) and (3.57), taking subsequences if necessary, we deduce that, as
Similarly, as
Since is compact and is continuous, as well as is compact and is continuous, then as we have

We can verify that is a weak solution of (1.1)–(1.3). Indeed, we need to verify that satisfies the following variational system:
for all

Note that the before convergence results enable us to pass to the limit in the linear terms of (3.3)–(3.7), obtaining the linear term in (3.61). Furthermore, through standard arguments one can obtain
Moreover it is not difficult to check that
Finally, it is clear that for all , as it holds

*Proof. *The existence of a solution of (1.1)–(1.5) is given by using Proposition 3.4 as the limit of the sequence .

Now the second part of the Theorem 2.2 will be proved. Let be solution of problem (1.6)–(1.10). From (3.58)-(3.59) we have
Consequently
Hence, from the last inequalities and taking into account (3.32) we conclude that
Therefore, since , with the additional condition for some positive constant from (3.67) we get