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PreprintCC BY 4.0HAL

Asymptotics of Laplace and Stokes solutions in the gap between a sharp tip and a smooth boundary

Abstract

We derive an explicit description of the asymptotic singular behavior of 2D Laplace and Stokes solutions as the distance between a Lipschitz sharp tip and a smooth boundary vanishes. While classical lubrication theory for smoother boundaries relies on the anisotropy of the gap to perform dimensional reduction, the isotropic scaling imposed by a corner singularity requires a different approach. We introduce a stability-based method that allows us to construct the leading-order asymptotics of these solutions in the gap. As an application, we determine the asymptotic behavior of the Stokes resistance matrix and the pressure field.

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BibTeX
@misc{roblet2026asymptotics,
  title = {{Asymptotics of Laplace and Stokes solutions in the gap between a sharp tip and a smooth boundary}},
  author = {Nicolas Roblet},
  howpublished = {HAL},
  year = {2026},
  month = sep,
  doi = {10.48550/arxiv.2609.17377},
  eprint = {2609.17377},
  archivePrefix = {arXiv},
  url = {https://hal.science/hal-05747044v1},
  note = {CC BY 4.0},
}
RIS
TY  - UNPB
TI  - Asymptotics of Laplace and Stokes solutions in the gap between a sharp tip and a smooth boundary
AU  - Nicolas Roblet
PY  - 2026
DA  - 2026/09/11
PB  - HAL
DO  - 10.48550/arxiv.2609.17377
UR  - https://hal.science/hal-05747044v1
AB  - We derive an explicit description of the asymptotic singular behavior of 2D Laplace and Stokes solutions as the distance between a Lipschitz sharp tip and a smooth boundary vanishes. While classical lubrication theory for smoother boundaries relies on the anisotropy of the gap to perform dimensional reduction, the isotropic scaling imposed by a corner singularity requires a different approach. We introduce a stability-based method that allows us to construct the leading-order asymptotics of these solutions in the gap. As an application, we determine the asymptotic behavior of the Stokes resistance matrix and the pressure field.
ER  -