Abstract
The compressible Navier-Stokes-Smoluchowski equations under investigation concern the behavior of the mixture of fluid and particles at a macroscopic scale. We devote to the existence of the global classical solution near the stationary solution based on the energy method under weaker conditions imposed on the external potential compared with Chen et al. (Global existence and time–decay estimates of solutions to the compressible Navier-Stokes-Smoluchowski equations, Discrete Contin. Dyn. Syst. 36 (2016), no. 10, 5287–5307). Under further assumptions that the stationary solution
1 Introduction
The compressible Navier-Stokes-Smoluchowski system can be comprehended as a fluid–particles interaction model, which has broad applications in hemodynamics [20,38], sprays and aerosols [28,43], and sedimentation [4]. The particles in the system are assumed to be light compared with the fluid and will tend to bubble upward due to buoyancy effects [15]. In the condition of high concentration of particles, the interaction between the particles can be described by a potential. The particles are transported by a fluid and described by a probability distribution that is responsible for the Smoluchowski equation [10]. Mathematically, the evolution of disperse suspensions of the particles in the viscous compressible fluid can be described by the Navier-Stokes equations coupled to the Smoluchowski equation via a drag force, which take the following form [2,7,15]:
The fluid density
In case the particle density
For the Navier-Stokes equations with a potential external force in three-dimensional space, Matsumura and Nishida [41] investigated the initial boundary value problem with small external force and initial perturbation on the exterior domain and the half space, and the global classical solution was proved to exist uniquely. Duan et al. [16,17] obtained the optimal convergence rates under the smallness conditions on the initial perturbation of the stationary solution and the potential force in
We take a brief review on the researches about the Navier-Stokes-Smoluchowski equations which have come into people’s note in recent years. Neglecting the viscosity terms in equation (1.1), this system was derived from a Vlasov-Fokker-Planck equation by formal hydrodynamic limit [5]. Ballew and Trivisa [3] analyzed the local existence of the weakly dissipative solutions to the Navier-Stokes-Smoluchowski equations in
This article is devoted to considering the Cauchy problem of the Navier-Stokes-Smoluchowski equations (1.1) in
for the positive constant
which implies
and the stationary solution
We define the perturbation by
then problem (1.1) can be reformulated into the perturbed form of
with
where
By Taylor expansion, we have
with
Notation. We use the notation
Our first result in this article is concerned with the global existence of the classical solution near the steady state
Theorem 1.1
Under the condition that
We want to complete the proof of Theorem 1.1 based on the energy method. Unfortunately, combined with the dissipation estimates of the solution
Remark 1.2
In Theorem 1.1, the conditions imposed on the initial perturbation and the external potential are weaker compared with the existence results in [7]. We only assume that the gradient of the external potential
Under the assumptions of Theorem 1.1, if further assumptions are imposed on
Theorem 1.3
Under the same conditions of Theorem
1.1, if further assume that
Remark 1.4
In Theorem 1.3, owing to the conditions imposed on the external potential
It’s difficult to obtain the decay rates of the system (1.7) which is an evolution one with variable coefficient
The structure of the article is as follows: in Section 2, some analysis tools are prepared, which will be helpful in establishing the energy estimates of the solution
2 Preliminaries
This section is mainly about the lemmas to be used in establishing the energy estimates in Sections 3 and 4. The Gagliardo-Nirenberg’s inequality, which is also called the interpolation inequality, will be stated in the following lemma.
Lemma 2.1
If the constants
with the superscript
Note that if
Proof
The proof of this lemma can be seen in the study by Nirenberg [42].□
Lemma 2.2
The commutator notation is defined as
for the integer
and the product estimates
hold. In the above,
Proof
See Lemma 3.1 in the study by Ju [29].□
Lemma 2.3
We have that for
and
Proof
One can see Lemma A.3 in the study by Tan et al. [48].□
The following lemma has been proved in the study by Tan et al. [47]. We recall the lemma as follows:
Lemma 2.4
Assume that
3 Global existence of the classical solution
It is well known that the global classical solution of the system (1.1) can follow from the existence and the uniform estimates of the local solution [40]. For the reason that the compressible Navier-Stokes-Smoluchowski equations (1.1) can be reduced to a symmetrizable hyperbolic-parabolic one, according to [30], the local existence of the classical solution is standard. In view of this, it suffices to establish the uniform energy estimates of the Navier-Stokes-Smoluchowski equations.
3.1 Energy estimates
In this subsection, we are devoted to establishing the energy estimates of the local solution
hold for sufficiently small
Lemma 3.1
Under the assumption of equation (3.1), it holds that
and for
Proof
Applying the operator
If
By Hölder’s inequality and the interpolation inequality, we can estimate
The following inequality is a simple consequence of the Hölder’s inequality and Young’s inequality
It follows from the integration by parts and the Hölder’s inequality that
Direct calculations lead to
Therefore, the inequality (3.2) follows from estimates (3.6)–(3.8).
It remains to deal with the case
We obtain after the Hölder’s inequality and the commutator estimates (2.3) that for
where the Young’s inequality is also used. It follows from the commutator estimates (2.3), the Gagliardo-Nirenberg’s inequality (2.1), and the Young’s inequality that for
and
In terms of estimates (3.9)–(3.11), it implies that
We can employ the integration by parts and the commutator notation (2.2) to rewrite
It infers from the Hölder’s inequality and the product estimates (2.4) that for
and
We employ the Hölder’s inequality, the commutator estimates (2.3) along with the Gagliardo-Nirenberg’s inequality (2.1), and the Young’s inequality to estimate, for
Combining the product estimates (2.4) and the Gagliardo-Nirenberg’s inequality (2.1), due to the Young’s inequality, for
and
In terms of estimates (3.13)–(3.17), it implies that
and, similarly,
From the product estimates (2.4), the Gagliardo-Nirenberg’s inequality (2.1), and the Young’s inequality, one can conclude that
Now, we turn to estimate the term
We use the commutator notation (2.2) to rewrite
It infers from the integration by parts and the Hölder’s inequality that
By the application of the interpolation inequality (2.1) and the commutator estimates (2.3), we can deduce that
It implies from the product estimates (2.4) that
In terms of estimates (3.21)–(3.23), the term
It is derived from the product estimates (2.4) along with the Young’s inequality that
We can deduce from equation (2.5) of Lemma 2.3 that
We should distinguish the order
If
If
From estimates (3.27) and (3.28), we have
Similarly to equation (3.29), it holds
One can deduce from the Hölder’s inequality and the product estimates (2.4) that
and
where the Young’s inequality is also be used. To this end, in light of estimate (3.12) and estimates (3.18)–(3.20), along with estimates (3.24)–(3.26) and estimates (3.29)–(3.32), we can prove estimates (3.3) to be true.□
Second, we derive the dissipation estimates for
Lemma 3.2
It holds for
and for
Proof
Taking the inner product of the third equation in equation (1.7) with
which implies equation (3.33), since
The energy estimates established in Lemmas 3.1–3.2 are not sufficient to close the energy estimates due to the lack of the dissipation estimates of
Lemma 3.3
Under the assumption of equation (3.1), we can deduce
Proof
Taking the inner product of the second equation in equation (1.7) with
For the first term of the inequality (3.36), by integrating by parts and making use of the first equation of (1.7), it is obvious to have
The combination of estimates (3.36) and (3.37) leads to equation (3.35).□
In a similar way, the dissipation estimates of
Lemma 3.4
For integer
Proof
Applying
We can take a similar approach to equation (3.37), using the Hölder’s inequality and the product estimates (2.4), to obtain
By the commutator estimates (2.3), it infers
With the help of the product estimates (2.4) and the Young’s inequality, we deduce
and
We can adopt a similar approach to equations (3.42) and (3.43) to have
Based on Lemmas 3.1–3.4, at this point, it is able to prove Theorem 1.1.
3.2 Proof of Theorem 1.1
The summation of equations (3.2) and (3.3) with
Summing up equation (3.35) in Lemma 3.3 and equation (3.38) in Lemma 3.4 from 1 to
It follows from equations (3.33) and (3.34) with
A suitable linear combination of equations (3.45) and (3.46) implies that
which combined with equation (3.47) gives
In order to obtain the uniform estimates of the solution
and claim that
which along with definition (3.49) gives
Since
With the help of equation (3.50) and taking the integration of equation (3.48) about the time variable
To this end, we have obtained the uniform estimates of the solution and finished the proof of Theorem 1.1.
4 Time decay rates of the solution
This section is devoted to the time decay rates of the solution
with the nonlinear terms
By the Duhamel principle, the solution
where
Based on the spectral analysis in the study by Chen et al. [7], the time decay property of the solution
Proposition 4.1
For
4.1 Energy estimates
We should make a little preparations for the later use in the proof of Theorem 1.3. From Theorem 1.1, it is known that
for some small
Lemma 4.2
Suppose that
Proof
We can apply the operator
The term
due to the commutator notation (2.2). It infers from the integration by parts that
We employ the commutator estimates (2.3) to derive
Employing the product estimates (2.4) leads to
and
Plugging equations (4.8)–(4.11) into equation (4.7), the term
It follows from the product estimates (2.4) and the interpolation inequality (2.1) of Lemma 2.1 that
and
We can use the product estimates (2.4) to deduce
by the fact (2.6) of Lemma 2.3. We can perform the similar approach to estimates (4.13)–(4.15) to conclude
and
It follows through direct calculation that
For
which together with equation (4.18) yields easily that
for
As a consequence of estimates (4.13)–(4.17) and estimate (4.19), it infers that
Next, under the assumptions of Theorem 1.3, we proceed to establish the dissipation estimates of
Lemma 4.3
For
Proof
Performing the operator
For the first term
We can take a similar approach to equation (3.40) to conclude
By the product estimates (2.4), one can arrive at
and similarly,
We can deal with the remaining nonlinear terms like equations (3.43) and (3.44), which combined with estimates (4.23)–(4.25) prove estimate (4.21).□
Finally, using the similar approach to equation (3.34) in Lemma 3.2, the energy estimates of
Lemma 4.4
Under the assumption of Theorem
1.3, for
Proof
Applying the operator
To this end, estimate (4.26) is proved.□
From Lemmas 4.2–4.4, we derive the following proposition.
Proposition 4.5
There exists an energy functional
Proof
Taking
It follows from estimate (4.21) of Lemma 4.3 that
provided the index
Combining the inequalities (4.29) and (4.28), since
We define
In order to obtain the decay rates of the solution
Lemma 4.6
It holds that for
For
Proof
Under the conditions of Theorem 1.3, we can use the Hölder’s inequality and the interpolation inequality (2.1) to deduce
and
Similar to equations (4.33) and (4.34), it is straightforward to obtain
and
In the same manner, the remaining nonlinear terms can also be estimated and estimate (4.31) will be obtained.
For
and
Adopting a similar approach, it can be obtained by direct calculation that
and
The remaining terms can be obtained in a similar way and estimate (4.32) is proved.□
4.2 Proof of Theorem 1.3
In this subsection, we will prove Theorem 1.3. Let
By the Gronwall inequality, it gives
For simplicity of notation, we denote
and define
The expression
where
In terms of equations (4.41)–(4.42), it follows from equation (4.40) with
where the notation
From the decay property in Proposition 4.1, together with estimates (4.31) and (4.32) of the nonlinear terms, we can obtain
Taking
We can take a similar approach to equation (4.48) to deduce
In terms of the decay estimates (4.47)–(4.49), it is evident that
which together with equation (4.45) gives
Therefore, by the definition of
which yields
since
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Funding information: The author was supported by the National Natural Science Foundation of China (Grant No. 12001077) and the Natural Science Foundation of Chongqing (Grant No. CSTB2023NSCQ-MSX0575).
-
Conflict of interest: The author states that there is no conflict of interest.
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