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The Stokes type equations are the linearized form of the stationary case of flow (describing by the Navier–Stokes equations) around a rotating body (see equations ( 1.25 ) and ( 1.26 ) from the Introduction, with \({\mathbf {u}}_{\infty }=\mathbf {0}\) and \( \operatorname {\mathrm {div}} \mathbf {u} = 0\) ).

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The Steady Stokes Type Problem

  • 章节

  • 发表日期：

    2025年

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  • Šárka Nečasová,
  • Stanislav Kračmar,
  • Jiří Neustupa,
  • Patrick Penel

摘要

The Stokes type equations are the linearized form of the stationary case of flow (describing by the Navier–Stokes equations) around a rotating body (see equations ( 1.25 ) and ( 1.26 ) from the Introduction, with \({\mathbf {u}}_{\infty }=\mathbf {0}\) and \( \operatorname {\mathrm {div}} \mathbf {u} = 0\) ).