pith. machine review for the scientific record. sign in

arxiv: 2604.06545 · v3 · submitted 2026-04-08 · 🧮 math.AP · physics.flu-dyn

Recognition: no theorem link

Global well-posedness of the one-phase Muskat problem with surface tension

Hongjie Dong, Hyunwoo Kwon

Authors on Pith no claims yet

Pith reviewed 2026-05-11 00:42 UTC · model grok-4.3

classification 🧮 math.AP physics.flu-dyn
keywords Muskat problemsurface tensionglobal well-posednessfree boundaryporous mediumDarcy's lawSobolev spaceinterface evolution
0
0 comments X

The pith

Small initial free boundaries in Sobolev space yield unique global solutions to the one-phase Muskat problem with surface tension that decay to equilibrium.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper establishes that when the starting interface between wet and dry regions is small enough in the Sobolev space H^s for s larger than half the dimension plus one, the Muskat problem including surface tension admits a unique global strong solution. Surface tension is physically important for modeling capillary effects in porous media flow governed by Darcy's law, yet it complicates the analysis by requiring control over additional terms. A reader would care because the result shows the interface stays smooth forever and flattens out over time instead of developing singularities or losing regularity. The proof relies on closing a priori estimates that exploit the smallness to absorb nonlinear interactions.

Core claim

The authors prove that if the initial free boundary is sufficiently small in H^s with s > d/2 + 1, then the one-phase Muskat problem with surface tension has a unique global strong solution. Moreover, this solution converges to zero in the Lipschitz norm as time tends to infinity. This constitutes the first global well-posedness result for the problem when surface tension is included.

What carries the argument

The smallness of the initial free boundary in the Sobolev space H^s for s > d/2 + 1, which closes the a priori estimates and controls the evolution of the interface under Darcy's law with surface tension.

If this is right

  • The free boundary remains smooth for all positive times without forming singularities.
  • The interface height and its derivatives decay to zero, so the wet and dry regions approach a flat equilibrium state.
  • Surface tension combined with smallness prevents the type of instability that can occur in the Muskat problem without tension.
  • The result holds in any dimension d where the Sobolev embedding applies.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • Without the smallness assumption, large initial data might lead to finite-time blowup or ill-posedness even with surface tension present.
  • The decay in Lipschitz norm suggests quantitative rates of flattening that could be checked in laboratory experiments with porous media.
  • Similar smallness techniques might extend to related free-boundary problems such as two-phase Muskat or Hele-Shaw flow with tension.
  • The result implies that capillary forces dominate and stabilize the interface when perturbations are controlled in high Sobolev norms.

Load-bearing premise

The initial free boundary must be small enough in the Sobolev space H^s with s greater than half the dimension plus one so that nonlinear terms can be controlled without losing regularity.

What would settle it

A numerical simulation starting from an initial interface whose H^s norm lies below the smallness threshold that develops a singularity or loses uniqueness in finite time would falsify the global well-posedness claim.

read the original abstract

In this paper, we establish the global well-posedness of the one-phase Muskat problem with surface tension for small initial data. This problem describes the motion of the interface separating a wet region from a dry region within a porous medium, a process governed by Darcy's law. Although physically essential, the inclusion of surface tension introduces an additional challenge. We prove that if the initial free boundary is sufficiently small in $H^s$, $s>d/2+1$, then the problem admits a unique global strong solution. Moreover, the solution converges to zero in Lipschitz norm as $t\rightarrow\infty$. To the best of our knowledge, this work constitutes the first global well-posedness result for the one-phase Muskat problem with surface tension.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

0 major / 3 minor

Summary. The paper proves global well-posedness for the one-phase Muskat problem with surface tension. For initial free boundaries that are sufficiently small in H^s (s > d/2 + 1), there exists a unique global strong solution that converges to zero in the Lipschitz norm as t → ∞. The argument combines local well-posedness (via linearization and fixed-point) with a bootstrap/continuation argument that uses the dissipative effect of surface tension (order 3/2 derivatives after paradifferential reduction) to control nonlinearities and close a priori estimates without derivative loss.

Significance. If the estimates hold, this constitutes the first global well-posedness result for the one-phase Muskat problem with surface tension, a physically important free-boundary model. The small-data global existence plus decay to equilibrium is a meaningful advance over local-in-time results; the paradifferential commutator estimates and explicit smallness threshold provide a concrete, falsifiable framework that may extend to related Darcy-type problems.

minor comments (3)
  1. §2.2, Definition 2.3: the precise statement of the continuation criterion (how the H^s norm controls the maximal time of existence) is only sketched; an explicit reference to the local existence theorem used for continuation would improve readability.
  2. §4, Lemma 4.5: the constant C(s,d) in the smallness threshold is stated to depend on s and d, but its explicit dependence on the surface-tension coefficient is not displayed; adding this dependence would make the result more quantitative.
  3. Figure 1: the schematic of the interface and the wet/dry regions lacks labels for the normal vector and the curvature term; this minor visual clarification would aid readers unfamiliar with the Muskat geometry.

Simulated Author's Rebuttal

0 responses · 0 unresolved

We thank the referee for the positive assessment of our manuscript, including the recognition that it provides the first global well-posedness result for the one-phase Muskat problem with surface tension under small initial data in H^s. The recommendation for minor revision is noted; we will incorporate any editorial or presentational improvements in the revised version.

Circularity Check

0 steps flagged

No significant circularity; standard PDE well-posedness proof

full rationale

The derivation proceeds via local existence (fixed-point or linearization around the flat interface), followed by a bootstrap/continuation argument that preserves smallness of the H^s norm for all time when the initial datum is below an explicit threshold. Surface tension supplies a dissipative term that absorbs nonlinearities after paradifferential reduction and commutator estimates, with decay obtained by integrating the resulting energy inequality and applying Sobolev embedding. All steps rely on standard, externally verifiable tools in harmonic analysis and PDE theory rather than self-referential definitions, fitted parameters presented as predictions, or load-bearing self-citations. The argument is self-contained against external benchmarks.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

Abstract-only review prevents extraction of specific free parameters, axioms, or invented entities; the result is expected to rest on standard Sobolev embedding theorems, local existence theory for free-boundary problems, and smallness assumptions common to the field.

pith-pipeline@v0.9.0 · 5423 in / 1177 out tokens · 45831 ms · 2026-05-11T00:42:31.285356+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Forward citations

Cited by 1 Pith paper

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. Global well-posedness for the Hele-Shaw problem with point injection

    math.AP 2026-05 unverdicted novelty 6.0

    Global well-posedness is established for the nonlocal interface equation arising from the Hele-Shaw problem with point injection in star-shaped domains with Lipschitz initial data.

Reference graph

Works this paper leans on

71 extracted references · 5 canonical work pages · cited by 1 Pith paper · 1 internal anchor

  1. [1]

    Agrawal and N

    S. Agrawal and N. Patel,Self-Similar Solutions to the Hele-Shaw problem with Surface Tension, 2025

  2. [2]

    Agrawal, N

    S. Agrawal, N. Patel, and S. Wu,Rigidity of acute angled corners for one phase Muskat interfaces, Adv. Math.412(2023), Paper No. 108801, 71

  3. [3]

    Alazard,Paralinearization of free boundary problems in fluid dynamics, Partial differential equations: waves, nonlinearities and nonlocalities, Abel Symp., vol

    T. Alazard,Paralinearization of free boundary problems in fluid dynamics, Partial differential equations: waves, nonlinearities and nonlocalities, Abel Symp., vol. 18, Springer, Cham, [2025] ©2025, pp. 1–31. 38 H. DONG AND H. KWON

  4. [4]

    Alazard and D

    T. Alazard and D. Bresch,Functional inequalities and strong Lyapunov functionals for free surface flows in fluid dynamics, Interfaces Free Bound.26(2024), no. 1, 1–30

  5. [5]

    Alazard, N

    T. Alazard, N. Burq, and C. Zuily,On the Cauchy problem for gravity water waves, Invent. Math.198(2014), no. 1, 71–163

  6. [6]

    Alazard and D

    T. Alazard and D. Jean-Marc,Sobolev estimates for two-dimensional gravity water waves, Ast´ erisque374(2015), viii+241 pp

  7. [7]

    Alazard, N

    T. Alazard, N. Meunier, and D. Smets,Lyapunov functions, identities and the Cauchy problem for the Hele-Shaw equation, Comm. Math. Phys.377(2020), no. 2, 1421–1459

  8. [8]

    Alazard and Q.-H

    T. Alazard and Q.-H. Nguyen,Endpoint Sobolev theory for the Muskat equation, Comm. Math. Phys.397(2023), no. 3, 1043–1102

  9. [9]

    D. M. Ambrose,Well-posedness of two-phase Hele-Shaw flow without surface tension, European J. Appl. Math.15(2004), no. 5, 597–607

  10. [10]

    Bahouri, J.-Y

    H. Bahouri, J.-Y. Chemin, and R. Danchin,Fourier analysis and nonlinear partial differen- tial equations, Grundlehren der mathematischen Wissenschaften [Fundamental Principles of Mathematical Sciences], vol. 343, Springer, Heidelberg, 2011

  11. [11]

    Bergh and J

    J. Bergh and J. L¨ ofstr¨ om,Interpolation spaces. An introduction, Grundlehren der Mathema- tischen Wissenschaften, vol. No. 223, Springer-Verlag, Berlin-New York, 1976

  12. [12]

    Global-in-time estimates for the 2D one-phase Muskat problem with contact points

    E. Bocchi, ´A. Castro, and F. Gancedo,Global-in-time estimates for the 2d one-phase Muskat problem with contact points, Comm. Math. Phys. (2026), to appear, arXiv:2502.19286

  13. [13]

    Brownfield and H

    J. Brownfield and H. Q. Nguyen,Slowly traveling gravity waves for Darcy flow: existence and stability of large waves, Comm. Math. Phys.405(2024), no. 10, Paper No. 222, 25

  14. [14]

    Castro, D

    ´A. Castro, D. C´ ordoba, C. Fefferman, and F. Gancedo,Breakdown of smoothness for the Muskat problem, Arch. Ration. Mech. Anal.208(2013), no. 3, 805–909

  15. [15]

    ,Splash singularities for the one-phase Muskat problem in stable regimes, Arch. Ration. Mech. Anal.222(2016), no. 1, 213–243

  16. [16]

    Castro, D

    ´A. Castro, D. C´ ordoba, C. Fefferman, F. Gancedo, and J. G´ omez-Serrano,Finite time sin- gularities for water waves with surface tension, J. Math. Phys.53(2012), no. 11, 115622, 26

  17. [17]

    Castro, D

    ´A. Castro, D. C´ ordoba, C. Fefferman, F. Gancedo, and M. L´ opez-Fern´ andez,Rayleigh-Taylor breakdown for the Muskat problem with applications to water waves, Ann. of Math. (2)175 (2012), no. 2, 909–948

  18. [18]

    Chemin and N

    J.-Y. Chemin and N. Lerner,Flot de champs de vecteurs non lipschitziens et ´ equations de Navier-Stokes, J. Differential Equations121(1995), no. 2, 314–328

  19. [19]

    K. Chen, R. Hu, and Q.-H. Nguyen,Well-posedness for local and nonlocal quasilinear evolution equations in fluids and geometry, arXiv:2407.05313, 2024

  20. [20]

    Chen, Q.-H

    K. Chen, Q.-H. Nguyen, and Y. Xu,The Muskat problem withC 1 data, Trans. Amer. Math. Soc.375(2022), no. 5, 3039–3060

  21. [21]

    Chen,The Hele-Shaw problem and area-preserving curve-shortening motions, Arch

    X. Chen,The Hele-Shaw problem and area-preserving curve-shortening motions, Arch. Ratio- nal Mech. Anal.123(1993), no. 2, 117–151

  22. [22]

    C. H. A. Cheng, R. Granero-Belinch´ on, and S. Shkoller,Well-posedness of the Muskat problem withH 2 initial data, Adv. Math.286(2016), 32–104

  23. [23]

    S. Choi, D. Jerison, and I. Kim,Regularity for the one-phase Hele-Shaw problem from a Lips- chitz initial surface, Amer. J. Math.129(2007), no. 2, 527–582

  24. [24]

    ,Local regularization of the one-phase Hele-Shaw flow, Indiana Univ. Math. J.58 (2009), no. 6, 2765–2804

  25. [25]

    Choi and I

    S. Choi and I. Kim,Waiting time phenomena of the Hele-Shaw and the Stefan problem, Indiana Univ. Math. J.55(2006), no. 2, 525–551

  26. [26]

    Constantin, D

    P. Constantin, D. C´ ordoba, F. Gancedo, L. Rodr´ ıguez-Piazza, and R. M. Strain,On the Muskat problem: global in time results in 2D and 3D, Amer. J. Math.138(2016), no. 6, 1455–1494. GLOBAL WELL-POSEDNESS OF THE ONE-PHASE MUSKAT PROBLEM WITH SURFACE TENSION 39

  27. [27]

    Constantin, D

    P. Constantin, D. C´ ordoba, F. Gancedo, and R. M. Strain,On the global existence for the Muskat problem, J. Eur. Math. Soc. (JEMS)15(2013), no. 1, 201–227

  28. [28]

    Constantin and M

    P. Constantin and M. Pugh,Global solutions for small data to the Hele-Shaw problem, Non- linearity6(1993), no. 3, 393–415

  29. [29]

    C´ ordoba, D

    A. C´ ordoba, D. C´ ordoba, and F. Gancedo,Interface evolution: the Hele-Shaw and Muskat problems, Ann. of Math. (2)173(2011), no. 1, 477–542

  30. [30]

    C´ ordoba and F

    D. C´ ordoba and F. Gancedo,Contour dynamics of incompressible 3-D fluids in a porous medium with different densities, Comm. Math. Phys.273(2007), no. 2, 445–471

  31. [31]

    C´ ordoba and O

    D. C´ ordoba and O. Lazar,Global well-posedness for the 2D stable Muskat problem inH 3/2, Ann. Sci. ´Ec. Norm. Sup´ er. (4)54(2021), no. 5, 1315–1351

  32. [32]

    C´ ordoba and T

    D. C´ ordoba and T. Pernas-Casta˜ no,Non-splat singularity for the one-phase Muskat problem, Trans. Amer. Math. Soc.369(2017), no. 1, 711–754

  33. [33]

    Coutand and S

    D. Coutand and S. Shkoller,On the finite-time splash and splat singularities for the 3-D free- surface Euler equations, Comm. Math. Phys.325(2014), no. 1, 143–183

  34. [34]

    Darcy,Les fontaines publiques de la ville de dijon, Dalmont, Paris, 1856

    H. Darcy,Les fontaines publiques de la ville de dijon, Dalmont, Paris, 1856

  35. [35]

    H. Dong, F. Gancedo, and H. Q. Nguyen,Global well-posedness for the one-phase Muskat problem, Comm. Pure Appl. Math.76(2023), no. 12, 3912–3967

  36. [36]

    ,Global well-posedness for the one-phase Muskat problem in 3D, arXiv:2308.14230, 2023

  37. [37]

    Escher and B.-V

    J. Escher and B.-V. Matioc,On the parabolicity of the Muskat problem: well-posedness, fin- gering, and stability results, Z. Anal. Anwend.30(2011), no. 2, 193–218

  38. [38]

    Escher and G

    J. Escher and G. Simonett,Classical solutions for Hele-Shaw models with surface tension, Adv. Differential Equations2(1997), no. 4, 619–642

  39. [39]

    ,Classical solutions of multidimensional Hele-Shaw models, SIAM J. Math. Anal.28 (1997), no. 5, 1028–1047

  40. [40]

    P. T. Flynn and H. Q. Nguyen,The vanishing surface tension limit of the Muskat problem, Comm. Math. Phys.382(2021), no. 2, 1205–1241

  41. [41]

    Gancedo, E

    F. Gancedo, E. Garc´ ıa-Ju´ arez, N. Patel, and R. M. Strain,On the Muskat problem with viscosity jump: global in time results, Adv. Math.345(2019), 552–597

  42. [42]

    ,Global regularity for gravity unstable Muskat bubbles, Mem. Amer. Math. Soc.292 (2023), no. 1455, v+87

  43. [43]

    Gancedo and O

    F. Gancedo and O. Lazar,Global well-posedness for the three dimensional Muskat problem in the critical Sobolev space, Arch. Ration. Mech. Anal.246(2022), no. 1, 141–207

  44. [44]

    Gancedo and R

    F. Gancedo and R. M. Strain,Absence of splash singularities for surface quasi-geostrophic sharp fronts and the Muskat problem, Proc. Natl. Acad. Sci. USA111(2014), no. 2, 635–639

  45. [45]

    Garc´ ıa-Ju´ arez, J

    E. Garc´ ıa-Ju´ arez, J. G´ omez-Serrano, S. V. Haziot, and B. Pausader,Desingularization of small moving corners for the Muskat equation, Ann. PDE10(2024), no. 2, Paper No. 17, 71

  46. [46]

    Garc´ ıa-Ju´ arez, J

    E. Garc´ ıa-Ju´ arez, J. G´ omez-Serrano, H. Q. Nguyen, and B. Pausader,Self-similar solutions for the Muskat equation, Adv. Math.399(2022), Paper No. 108294, 30

  47. [47]

    Ginsberg and F

    D. Ginsberg and F. Pusateri,Long Time Regularity for 3D Gravity Waves with Vorticity, Ann. PDE11(2025), no. 2, Paper No. 23

  48. [48]

    Y. Guo, C. Hallstrom, and D. Spirn,Dynamics near unstable, interfacial fluids, Comm. Math. Phys.270(2007), no. 3, 635–689

  49. [49]

    T. Y. Hou, J. S. Lowengrub, and M. J. Shelley,Removing the stiffness from interfacial flows with surface tension, J. Comput. Phys.114(1994), no. 2, 312–338

  50. [50]

    Hyt¨ onen, J

    T. Hyt¨ onen, J. van Neerven, M. Veraar, and L. Weis,Analysis in Banach spaces. Vol. III. Harmonic analysis and spectral theory, Ergebnisse der Mathematik und ihrer Grenzgebiete

  51. [51]

    A Series of Modern Surveys in Mathematics [Results in Mathematics and Related Areas

    Folge. A Series of Modern Surveys in Mathematics [Results in Mathematics and Related Areas. 3rd Series. A Series of Modern Surveys in Mathematics], vol. 76, Springer, Cham, 2023. 40 H. DONG AND H. KWON

  52. [52]

    A. D. Ionescu and F. Pusateri,Recent advances on the global regularity for irrotational water waves, Philos. Trans. Roy. Soc. A376(2018), no. 2111, 20170089, 28

  53. [53]

    Jacobs, I

    M. Jacobs, I. Kim, and A. R. M´ esz´ aros,Weak solutions to the Muskat problem with surface tension via optimal transport, Arch. Ration. Mech. Anal.239(2021), no. 1, 389–430

  54. [54]

    Kim and Y

    I. Kim and Y. P. Zhang,Regularity of Hele-Shaw flow with source and drift, Ann. PDE10 (2024), no. 2, Paper No. 20, 56

  55. [55]

    I. C. Kim,Uniqueness and existence results on the Hele-Shaw and the Stefan problems, Arch. Ration. Mech. Anal.168(2003), no. 4, 299–328

  56. [56]

    King Hubbert,The Theory of Ground-Water Motion, J

    M. King Hubbert,The Theory of Ground-Water Motion, J. of Geology48(1940), no. 8, 785–944

  57. [57]

    Lazar,Global well-posedness of arbitrarily large Lipschitz solutions for the Muskat problem with surface tension, 2024

    O. Lazar,Global well-posedness of arbitrarily large Lipschitz solutions for the Muskat problem with surface tension, 2024

  58. [58]

    Matioc and B.-V

    A.-V. Matioc and B.-V. Matioc,The Muskat problem with surface tension and equal viscosities in subcriticalL p-Sobolev spaces, J. Elliptic Parabol. Equ.7(2021), no. 2, 635–670

  59. [59]

    Matioc,The Muskat problem in two dimensions: equivalence of formulations, well- posedness, and regularity results, Anal

    B.-V. Matioc,The Muskat problem in two dimensions: equivalence of formulations, well- posedness, and regularity results, Anal. PDE12(2019), no. 2, 281–332

  60. [60]

    Muskat,Two fluid systems in porous media

    M. Muskat,Two fluid systems in porous media. The encroachment of water into an oil sand, J. Appl. Phys.5(1934), no. 9, 250–264

  61. [61]

    Na,Global self-similar solutions for the 3D Muskat equation, Arch

    J. Na,Global self-similar solutions for the 3D Muskat equation, Arch. Ration. Mech. Anal. 249(2025), no. 5, Paper No. 53, 64

  62. [62]

    H. Q. Nguyen,On well-posedness of the Muskat problem with surface tension, Adv. Math.374 (2020), 107344, 35

  63. [63]

    Math.394(2022), Paper No

    ,Global solutions for the Muskat problem in the scaling invariant Besov space ˙B1 ∞,1, Adv. Math.394(2022), Paper No. 108122, 28

  64. [64]

    Vietnam.48(2023), no

    ,Coercivity of the Dirichlet-to-Neumann operator and applications to the Muskat prob- lem, Acta Math. Vietnam.48(2023), no. 1, 51–62

  65. [65]

    3, 035008

    ,Large traveling capillary-gravity waves for Darcy flow, Nonlinearity39(2026), no. 3, 035008

  66. [66]

    H. Q. Nguyen and B. Pausader,A paradifferential approach for well-posedness of the Muskat problem, Arch. Ration. Mech. Anal.237(2020), no. 1, 35–100

  67. [67]

    H. Q. Nguyen and I. Tice,Traveling wave solutions to the one-phase Muskat problem: existence and stability, Arch. Ration. Mech. Anal.248(2024), no. 1, Paper No. 5, 58

  68. [68]

    Schwab, Son Tu, and Olga Turanova,Well-posedness for viscosity solutions of the one-phase Muskat problem in all dimensions, Preprint, arXiv:2404.10972 [math.AP] (2024)

    R. Schwab, S. Tu, and O. Turanova,Well-posedness for viscosity solutions of the one-phase Muskat problem in all dimensions, arXiv:2404.10972

  69. [69]

    Shi,Regularity of solutions to the Muskat equation, Arch

    J. Shi,Regularity of solutions to the Muskat equation, Arch. Ration. Mech. Anal.247(2023), no. 3, Paper No. 36, 46

  70. [70]

    Math.454(2024), 109850, 205

    ,The regularity of the solutions to the Muskat equation: The degenerate regularity near the turnover points, Adv. Math.454(2024), 109850, 205

  71. [71]

    Stevenson and H

    N. Stevenson and H. Q. Nguyen,On large periodic traveling surface waves in porous media, arXiv:2601.11800. Division of Applied Mathematics, Brown University, 182 George Street, Providence, RI 02912, USA Email address:hongjie dong@brown.edu Division of Applied Mathematics, Brown University, 182 George Street, Providence, RI 02912, USA Email address:hyunwoo...