On the sharp critical mass threshold for the 3D Patlak-Keller-Segel-Navier-Stokes system via Couette flow
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arXiv
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| Autores principales: | , , , |
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| Formato: | Preprint |
| Publicado: |
2025
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| _version_ | 1866918056899379200 |
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| author | Cui, Shikun Wang, Lili Wang, Wendong Wei, Juncheng |
| author_facet | Cui, Shikun Wang, Lili Wang, Wendong Wei, Juncheng |
| contents | As is well-known, the solution of the Patlak-Keller-Segel system in 3D may blow up in finite time regardless of any initial cell mass. In this paper, we are interested in the suppression of blow-up and the critical mass threshold for the 3D Patlak-Keller-Segel-Navier-Stokes system via the Couette flow $(Ay, 0, 0)$. It is proved that if the Couette flow is sufficiently strong ($A$ is large enough), then the solutions for the system are global in time in the periodic domain $(x,y,z)\in\mathbb{T}^{3}$ as long as the initial cell mass is less than $16π^{2}$. This result seems to be sharp, since the zero-mode function (the mean value in $x-$direction) of the three dimensional density is a complication of the two-dimensional Keller-Segel equations, whose critical mass in 2D is $8π$. One new observation is the dissipative decay of $(\widetilde{u}_{2,0},\widetilde{u}_{3,0})$ (see Lemma 4.3 for more details), then we combine the quasi-linear method proposed by Wei-Zhang (Comm. Pure Appl. Math., 2021) with the zero-mode estimate of the density by the logarithmic Hardy-Littlewood-Sobolev inequality as Bedrossian-He (SIAM J. Math. Anal., 2017) or He (Nonlinearity, 2025) to obtain the bounded-ness of the density and the velocity. |
| format | Preprint |
| id |
arxiv_https___arxiv_org_abs_2506_10578 |
| institution | arXiv |
| publishDate | 2025 |
| record_format | arxiv |
| spellingShingle | On the sharp critical mass threshold for the 3D Patlak-Keller-Segel-Navier-Stokes system via Couette flow Cui, Shikun Wang, Lili Wang, Wendong Wei, Juncheng Analysis of PDEs As is well-known, the solution of the Patlak-Keller-Segel system in 3D may blow up in finite time regardless of any initial cell mass. In this paper, we are interested in the suppression of blow-up and the critical mass threshold for the 3D Patlak-Keller-Segel-Navier-Stokes system via the Couette flow $(Ay, 0, 0)$. It is proved that if the Couette flow is sufficiently strong ($A$ is large enough), then the solutions for the system are global in time in the periodic domain $(x,y,z)\in\mathbb{T}^{3}$ as long as the initial cell mass is less than $16π^{2}$. This result seems to be sharp, since the zero-mode function (the mean value in $x-$direction) of the three dimensional density is a complication of the two-dimensional Keller-Segel equations, whose critical mass in 2D is $8π$. One new observation is the dissipative decay of $(\widetilde{u}_{2,0},\widetilde{u}_{3,0})$ (see Lemma 4.3 for more details), then we combine the quasi-linear method proposed by Wei-Zhang (Comm. Pure Appl. Math., 2021) with the zero-mode estimate of the density by the logarithmic Hardy-Littlewood-Sobolev inequality as Bedrossian-He (SIAM J. Math. Anal., 2017) or He (Nonlinearity, 2025) to obtain the bounded-ness of the density and the velocity. |
| title | On the sharp critical mass threshold for the 3D Patlak-Keller-Segel-Navier-Stokes system via Couette flow |
| topic | Analysis of PDEs |
| url | https://arxiv.org/abs/2506.10578 |