Abstract:We establish the existence, uniqueness and L q estimates of weak solutions to the stationary Stokes equations with rotation effect both in the whole space and in exterior domains. The equation arises from the study of viscous incompressible flows around a body that is rotating with a constant angular velocity, and it involves an important drift operator with unbounded variable coefficient that causes some difficulties.
“…This result is regarded as a generalization of [4], [22], [30], [31] in the usual case o ¼ 0, since the restriction on the exponent q is the same. Since the case q ¼ 3=2ð¼ n=2Þ needed to estimate the nonlinearity u Á 'u is missing in [28], an L q theory does not help to solve the nonlinear problem (1.2), (1.3). Note that L 3=2 is too restrictive at infinity to expect 'u A L 3=2 for (1.8) even if f ¼ div F with F A C y 0 .…”
Section: ð1:7þmentioning
confidence: 99%
“…We refer to [3], [9], [10], [12], [13], [14], [15], [16], [18], [19], [20], [21], [23], [24], [25], [26], [27], [28], [33], [34] and [36]. Nevertheless, our mathematical understanding is still far from complete.…”
Section: Introductionmentioning
confidence: 99%
“…In [28], based on an idea from [14], one of the present authors has established the existence, uniqueness and L q estimate…”
Abstract. Consider a viscous incompressible fluid filling the whole 3-dimensional space exterior to a rotating body with constant angular velocity o. By using a coordinate system attached to the body, the problem is reduced to an equivalent one in a fixed exterior domain. The reduced equation involves the crucial drift operator ðo5xÞ Á ', which is not subordinate to the usual Stokes operator. This paper addresses stationary flows to the reduced problem with an external force f ¼ div F , that is, time-periodic flows to the original one. Generalizing previous results of G. P. Galdi [19] we show the existence of a unique solution ð'u; pÞ in the class L 3=2; y when both F A L 3=2; y and o are small enough; here L 3=2; y is the weak-L 3=2 space.
“…This result is regarded as a generalization of [4], [22], [30], [31] in the usual case o ¼ 0, since the restriction on the exponent q is the same. Since the case q ¼ 3=2ð¼ n=2Þ needed to estimate the nonlinearity u Á 'u is missing in [28], an L q theory does not help to solve the nonlinear problem (1.2), (1.3). Note that L 3=2 is too restrictive at infinity to expect 'u A L 3=2 for (1.8) even if f ¼ div F with F A C y 0 .…”
Section: ð1:7þmentioning
confidence: 99%
“…We refer to [3], [9], [10], [12], [13], [14], [15], [16], [18], [19], [20], [21], [23], [24], [25], [26], [27], [28], [33], [34] and [36]. Nevertheless, our mathematical understanding is still far from complete.…”
Section: Introductionmentioning
confidence: 99%
“…In [28], based on an idea from [14], one of the present authors has established the existence, uniqueness and L q estimate…”
Abstract. Consider a viscous incompressible fluid filling the whole 3-dimensional space exterior to a rotating body with constant angular velocity o. By using a coordinate system attached to the body, the problem is reduced to an equivalent one in a fixed exterior domain. The reduced equation involves the crucial drift operator ðo5xÞ Á ', which is not subordinate to the usual Stokes operator. This paper addresses stationary flows to the reduced problem with an external force f ¼ div F , that is, time-periodic flows to the original one. Generalizing previous results of G. P. Galdi [19] we show the existence of a unique solution ð'u; pÞ in the class L 3=2; y when both F A L 3=2; y and o are small enough; here L 3=2; y is the weak-L 3=2 space.
“…Similar estimates for weak solutions in the Oseen case (λ = 0) were established in [37] and [38] by Kračmar, Nečasová, and Penel. The results in [31] and [37], [38] were obtained using the same very technical approach that was used in [9] and [6] based on the Littlewood-Paley decomposition. Simple proofs of these estimates were recently made available by Galdi and Kyed in [22].…”
“…On the existence, uniqueness and regularity of solutions of (1), there are many papers, such as [1][2][3][4][5][6][7][8] and references therein. However, few results about the numerical analysis are developed.…”
Abstract. In this paper, we apply the boundary integral method to the steady rotating Navier-Stokes equations in exterior domain. Introducing some open ball which decomposes the exterior domain into a finite domain and a infinite domain, we obtain a coupled problem by the steady rotating Navier-Stokes equations in finite domain and a boundary integral equation without using the artificial boundary condition. For the coupled problem, we show the existence of solution in a convex set. Mathematics Subject Classification (2000). 76M15, 76U05.
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