“…[1,3,6,7,12,13,16,20] and references therein). Here, we are mainly interested in the results of [13], where the following improvement in time of (2) is provided.…”
Section: Earlier Resultsmentioning
confidence: 99%
“…The purpose of this article is to establish a novel regularity criterion in terms of the pressure gradient, valid either when Ω is bounded or Ω = R 3 , and in presence of an external force φ ∈ L 2 (0 T ; L 2 ). This is done in the spirit of Theorem 1.2, yielding an improved (in time) version of (3).…”
Section: Resultsmentioning
confidence: 99%
“…Let Ω ⊂ R 3 be either the whole space or a bounded domain with smooth boundary ∂Ω. For an arbitrarily fixed T > 0, we consider the dimensionless form of the Navier-Stokes equations in the space-time cylinder Ω T = Ω × (0 T )…”
The incompressible three-dimensional Navier-Stokes equations are considered. A new regularity criterion for weak solutions is established in terms of the pressure gradient.
MSC:35Q30, 76D03, 76D05
“…[1,3,6,7,12,13,16,20] and references therein). Here, we are mainly interested in the results of [13], where the following improvement in time of (2) is provided.…”
Section: Earlier Resultsmentioning
confidence: 99%
“…The purpose of this article is to establish a novel regularity criterion in terms of the pressure gradient, valid either when Ω is bounded or Ω = R 3 , and in presence of an external force φ ∈ L 2 (0 T ; L 2 ). This is done in the spirit of Theorem 1.2, yielding an improved (in time) version of (3).…”
Section: Resultsmentioning
confidence: 99%
“…Let Ω ⊂ R 3 be either the whole space or a bounded domain with smooth boundary ∂Ω. For an arbitrarily fixed T > 0, we consider the dimensionless form of the Navier-Stokes equations in the space-time cylinder Ω T = Ω × (0 T )…”
The incompressible three-dimensional Navier-Stokes equations are considered. A new regularity criterion for weak solutions is established in terms of the pressure gradient.
MSC:35Q30, 76D03, 76D05
“…Theorem 1.1 in the whole space Ω = R 3 can be found in [1], whereas Theorem 1.2 is proved in [9] for a small constant c > 0, although the value of this constant is not explicit. On the contrary, in our proof the value of c can be in principle explicitly calculated.…”
Section: Theorem 12 For Every Prodi-serrin Pairmentioning
We give simple proofs that a weak solution u of the Navier-Stokes equations with H 1 initial data remains strong on the time interval [0, T ] if it satisfies the Prodi-Serrin type condition u ∈ L s (0, T ; L r,∞ (Ω)) or if its L s,∞ (0, T ; L r,∞ (Ω)) norm is sufficiently small, where 3 < r ≤ ∞ and (3/r) + (2/s) = 1.Mathematics Subject Classification. 35Q30, 76D03, 76D05.
“…Before formulating our results, we mention that, as (1.8), regularity criteria in terms of pressure Π or gradient of pressure ∇Π with only space direction belonging to Lorentz spaces can be found in [7,33]. As for other regularity criteria involving Lorentz spaces, see [5,10,13,21,22,31]. Now our first result is stated as follows.…”
In this paper, we derive regular criteria via pressure or gradient of the velocity in Lorentz spaces to the 3D Navier-Stokes equations. It is shown that a Leray-Hopf weak solution is regular on (0, T ] provided that either the norm Π L p,∞ (0,T ;L q,∞ (R 3 )) with 2/p + 3/q = 2 (3/2 < q < ∞) or ∇Π L p,∞ (0,T ;L q,∞ (R 3 )) with 2/p + 3/q = 3 (1 < q < ∞) is small. This gives an affirmative answer to a question proposed by Suzuki in [26, Remark 2.4, p.3850]. Moreover, regular conditions in terms of ∇u obtained here generalize known ones to allow the time direction to belong to Lorentz spaces. MSC(2000): 76D03, 76D05, 35B33, 35Q35
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