2017
DOI: 10.1080/00036811.2016.1269321
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On singular solutions of time-periodic and steady Stokes problems in a power cusp domain

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Cited by 7 publications
(9 citation statements)
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“…Then we can pass to the limit as k m → ∞ in integral identity (31) taking any test function η ∈ J ∞ 0 (Ω). For the limit function v ∈ H(Ω) we obtain the integral identity (29). Obviously, the limit function v obeys estimate (48).…”
Section: Existence and Uniqueness Of Weak Solutionmentioning
confidence: 99%
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“…Then we can pass to the limit as k m → ∞ in integral identity (31) taking any test function η ∈ J ∞ 0 (Ω). For the limit function v ∈ H(Ω) we obtain the integral identity (29). Obviously, the limit function v obeys estimate (48).…”
Section: Existence and Uniqueness Of Weak Solutionmentioning
confidence: 99%
“…Proof. Suppose problem (1) has two solutions u 1 and u 2 admitting representation (28), i.e., u 1 = A + v 1 , u 2 = A + v 2 , where v 1 , v 2 ∈ H(Ω) and satisfy integral identity (29). Denote v = u 1 − u 2 = v 1 − v 2 ∈ H(Ω).…”
Section: Existence and Uniqueness Of Weak Solutionmentioning
confidence: 99%
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“…The existence of singular solutions to the time-periodic and the non-stationary Stokes problem in the domain with a cusp point was studied in [2,3]. We can also mention the recent paper [4] where the Dirichlet problem for the non-stationary Stokes system is studied in a three-dimensional cone.…”
Section: Introductionmentioning
confidence: 99%
“…In recent papers the authors have studied existence of singular solutions to the time-periodic and initial boundary value problems for the linear Stokes equations [3,4] and an initial boundary value problem for the Navier-Stokes equations [28,29] in domains having a power-cusp (peak type) singular point on the boundary. The case when the flux of the boundary value is nonzero was considered.…”
Section: Introductionmentioning
confidence: 99%