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The Inviscid Limit of Viscous Burgers through Shock Formation and Development

Abstract

We study the inviscid limit of the one-dimensional viscous Burgers equation from smooth initial data through nondegenerate shock formation and subsequent shock development. Chaturvedi and Graham \cite{CG} obtained sharp estimates of order ν1/4 up to the shock-formation time. We extend their analysis beyond this time, comparing the viscous solution with the inviscid entropy solution evolving from the same initial data. With the shock-formation time normalized to t=0, we prove a pointwise error bound on a fixed interval 0≤ t ≤ ε̅, where ε̅>0 is independent of the viscosity ν. The bound consists of a term of order ν1/4 and an exponentially localized contribution originating from the viscous shock layer. The proof is based on matching an outer expansion, an inner expansion near the formation point, and a viscous shock-profile expansion. Combined with the results of Chaturvedi and Graham, this yields a quantitative description of the inviscid limit from the initial time through the development of the young shock.

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BibTeX
@misc{wang2026inviscid,
  title = {{The Inviscid Limit of Viscous Burgers through Shock Formation and Development}},
  author = {Chao Wang and Yueyi Yang and Zhifei Zhang},
  howpublished = {arXiv},
  year = {2026},
  month = oct,
  doi = {10.48550/arxiv.2610.16420},
  eprint = {2610.16420},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2610.16420},
}
RIS
TY  - UNPB
TI  - The Inviscid Limit of Viscous Burgers through Shock Formation and Development
AU  - Chao Wang
AU  - Yueyi Yang
AU  - Zhifei Zhang
PY  - 2026
DA  - 2026/10/12
PB  - arXiv
DO  - 10.48550/arxiv.2610.16420
UR  - https://arxiv.org/abs/2610.16420
AB  - We study the inviscid limit of the one-dimensional viscous Burgers equation from smooth initial data through nondegenerate shock formation and subsequent shock development. Chaturvedi and Graham \cite{CG} obtained sharp estimates of order ν^1/4 up to the shock-formation time. We extend their analysis beyond this time, comparing the viscous solution with the inviscid entropy solution evolving from the same initial data. With the shock-formation time normalized to t=0, we prove a pointwise error bound on a fixed interval 0≤ t ≤ ε̅, where ε̅>0 is independent of the viscosity ν. The bound consists of a term of order ν^1/4 and an exponentially localized contribution originating from the viscous shock layer. The proof is based on matching an outer expansion, an inner expansion near the formation point, and a viscous shock-profile expansion. Combined with the results of Chaturvedi and Graham, this yields a quantitative description of the inviscid limit from the initial time through the development of the young shock.
ER  -