Abstract
In this paper, we mainly consider global well-posedness and long time behavior of compressible Navier–Stokes equations without heat conduction in \(L^p\)-framework. This is a generalization of Peng and Zhai (SIMA 55(2):1439–1463, 2023), where they obtained the corresponding result in \(L^2\)-framework. Based on the key observation that we can release the regularity of non-dissipative entropy S in high frequency in Peng and Zhai (2023), we ultimately achieve the desired \(L^p\) estimate in the high frequency via complicated calculations on the nonlinear terms. In addition, we get the \(L^p\)-decay rate of the solution.
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The research was supported by National Natural Science Foundation of China (11971100) and Natural Science Foundation of Shanghai (22ZR1402300).
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Cai and Liu wrote the main manuscript text, and Wu provided the idea and revised the manuscript text. All authors reviewed the manuscript.
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Appendix
Appendix
We will state several important lemmas and propositions on the homogeneous Besov space \(\dot{B}^{s}_{p,r}\). First, let \(\mathcal {S}(\mathbb {R}^{n})\) be the Schwartz class of rapidly decreasing function. Given \(f\in \mathcal {S}(\mathbb {R}^{n})\), its Fourier transform \(\mathcal {F}f=\widehat{f}\) is defined by
Let \((\chi , \varphi )\) be a couple of smooth functions valued in [0, 1] such that \(\chi \) is supported in the ball \(\{\xi \in \mathbb {R}^{n}: \ |\xi |\le \frac{4}{3}\}\), \(\varphi \) is supported in the shell \(\{\xi \in \mathbb {R}^{n}: \ \frac{3}{4}\le |\xi |\le \frac{8}{3}\}\), \(\varphi (\xi ):=\chi (\xi /2)-\chi (\xi )\) and
For \(f\in \mathcal {S}'\), the homogeneous frequency localization operators \(\dot{\Delta }_j\) and \(\dot{S}_j\) are defined by
We denote the space \(\mathcal {S}'_{h}(\mathbb {R}^n)\) by the dual space of \(\mathcal {S}'(\mathbb {R}^n)=\{f\in \mathcal {S}(\mathbb {R}^n):\,D^\alpha \hat{f}(0)=0\}\), which can also be identified by the quotient space of \(\mathcal {S}'(\mathbb {R}^n)/{\mathbb {P}}\) with the polynomial space \({\mathbb {P}}\). The formal equality
holds true for \(f\in \mathcal {S}'_{h}(\mathbb {R}^n)\) and is called the homogeneous Littlewood-Paley decomposition, and then we have the fact that
One easily verifies that with our choice of \(\varphi \),
Definition 3.1
(Homogeneous Besov space) For \(s\in \mathbb {R}\) and \(1\le p,r\le \infty \), the homogeneous Besov space \(\dot{B}^{s}_{p,r}\) is defined by
where
Definition 3.2
(Chemin-Lerner spaces) Let \(T>0\), \(s\in \mathbb {R}\), \(1<r,p,q\le \infty \). The space \(\widetilde{L}^q_{T}(\dot{B}^s_{p,r})\) is defined by
where
Remark 3.1
It holds that
Restricting the above norms (4.2), (4.3) to the low or high frequencies parts of distributions will be crucial in our approach. For example, let us fix some integer \(j_0\) and set
Lemma 3.1
(Bernstein inequalities) Let \(\mathscr {B}\) be a ball and \(\mathscr {C}\) be a ring of \(\mathbb {R}^n\). For \(\lambda >0\), integer \(k\ge 0\), \(1\le p\le q\le \infty \) and a smooth homogeneous function \(\sigma \) in \(\mathbb {R}^n\backslash \{0\}\) of degree m, then there holds
Proposition 3.2
[1](Embedding for Besov space on \(\mathbb {R}^n\))
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For any \(p\in [1,\infty ]\), we have the continuous embedding \(\dot{B}^{0}_{p,1}\hookrightarrow L^p\hookrightarrow \dot{B}^{0}_{p,\infty }\).
-
If \(s\in \mathbb {R}\), \(1\le p_1\le p_2\le \infty \), and \(1\le r_1\le r_2\le \infty \) then \(\dot{B}^{s}_{p_1,r_1}\hookrightarrow \dot{B}^{s-n(\frac{1}{p_1}-\frac{1}{p_2})}_{p_2,r_2}\).
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The space \(\dot{B}^{\frac{n}{p}}_{p,1}\) is continuously embedded in the set of bounded continuous function (going to zero at infinity if, additionally, \(p<\infty \)).
Proposition 3.3
[16] If supp\(\mathcal {F}f\subset \left\{ \xi \in \mathbb {R}^n:R_1\lambda \le |\xi |\le R_2\lambda \right\} \), then there exists C depending only on d, \(R_1\), \(R_2\) so that for all \(1<p<\infty \),
Proposition 3.4
[1](Interpolation inequality) Let \(1\le p,r,r_1,r_2\le \infty \), if \(f\in \dot{B}^{s_1}_{p,r_1}\cap \dot{B}^{s_2}_{p,r_2}\) and \(s_1\ne s_2\), then \(f\in \dot{B}^{\theta s_1+(1-\theta )s_2}_{p,r}\) for all \(\theta \in (0,1)\) and
with \(\frac{1}{r}=\frac{\theta }{r_1}+\frac{1-\theta }{r_2}\).
Proposition 3.5
[1, 13] Let \(s>0\), \(1\le p\), \(r\le \infty \), then \(\dot{B}^{s}_{p,r}\cap L^\infty \) is an algerbra and
Let \(s_1+s_2>0\), \(s_1 \le \frac{n}{p_1}\), \(s_2 \le \frac{n}{p_2}\), \(s_1\ge s_2\), \(\frac{1}{p_1}+\frac{1}{p_2}\le 1\). Then, it holds that
where \(\frac{1}{q} = \frac{1}{p_1} + \frac{1}{p_2} - \frac{s_1}{n}\).
Proposition 3.6
[41] Let the real numbers \(s_1,\ s_2,\ p_1\) and \(p_2\) be such that
Then, it holds that
Corollary 3.1
Let the real numbers \(1-\frac{n}{2}<\sigma _1\le \frac{2n}{p}-\frac{n}{2}\) and p satisfy (1.7). The following two inequalities hold true:
as well as
Proposition 3.7
[42] Let \(j_0\in \mathbb {Z}\), and denote \(z^l\triangleq \dot{S}_{j_0}z,\ z^h\triangleq z-z^l\) and, for any \(s\in \mathbb {R}\),
There exists a universal integer \(N_0\) such that for any \(2\le p\le 4\) and \(s>0\), we have
where \(\sigma _0\triangleq \frac{2n}{p}-\frac{n}{2}\), \(\frac{1}{p^*}+\frac{1}{p}=\frac{1}{2}\), C depends only on \(k_0,\ n,\ s\).
Additionally, for exponents \(s>0\), \(1 \le p_1,p_2,q \le \infty \) satisfying
Then, it holds that
Proposition 3.8
[11] Let \((s,r)\in \mathbb {R}\times [1,\infty ]\) and \(1\le p,p_1,p_2\le \infty \) with \(1/p=1/p_1+1/p_2\): For the paraproduct, the following continuity properties hold true
and
If \(s_1+s_2>0\) and \(1/r=1/r_1+1/r_2\le 1\), then
If \(s_1+s_2=0\) and \(1/r_1+1/r_2\ge 1\), then
From Proposition 3.8, we easily deduce the following proposition:
Proposition 3.9
[42] The Bony decomposition satisfies that
where \(\frac{1}{p'}+\frac{1}{p}=\frac{1}{2}\).
Lemma 3.2
[13] Let \(n\ge 2\), \(1\le p, q\le \infty \), \(v\in \dot{B}^{s}_{q,1}(\mathbb {R}^n)\) and \(\nabla u \in \dot{B}^{\frac{n}{p}}_{p,1}\).
Asumme that
Then, it holds the commutator estimate
In the limit case \(s=-n\min \left( \frac{1}{p}, 1-\frac{1}{q}\right) \), we have
Proposition 3.10
[42] Let \(F: \mathbb {R} \mapsto \mathbb {R}\) be a smooth function with \(F(0)=0\), \(1\le p, r\le \infty \) and \(s>0\). Then, \(F: \dot{B}^{s}_{p,r}(\mathbb {R}^n)\cap (L^\infty (\mathbb {R}^n))\) and
with C a constant depending only on \(|||u||_{L^\infty }\), s, p, n and derivatives of F.
If \(s>-\min (\frac{n}{p}, \frac{n}{p'})\), then \(F: \dot{B}^{s}_{p,r}(\mathbb {R}^n)\cap \dot{B}^{\frac{n}{p}}_{p,1}(\mathbb {R}^n) \mapsto \dot{B}^{s}_{p,r}(\mathbb {R}^n)\cap \dot{B}^{\frac{n}{p}}_{p,1}(\mathbb {R}^n)\), and
where \(\frac{1}{p}+\frac{1}{p'}=\frac{1}{2}\).
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Cai, J., Wu, Z. & Liu, M. Compressible Navier–Stokes equations without heat conduction in \(L^p\)-framework. Z. Angew. Math. Phys. 75, 101 (2024). https://doi.org/10.1007/s00033-024-02250-7
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DOI: https://doi.org/10.1007/s00033-024-02250-7