Asymptotic behavior of solutions to the compressible Navier-Stokes equations on the half space
Asymptotic behavior of solutions to the compressible Navier-Stokes equations on the half space
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DOI:
10.4064/bc70-0-8
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发表时间:
2005
期刊:
影响因子:
--
通讯作者:
Y. Kagei;Takayuki Kobayashi
中科院分区:
文献类型:
--
作者:
Y. Kagei;Takayuki Kobayashi
(0.2) m|xn=0 = 0, ρ(0, x) = ρ0(x), m(0, x) = m0(x). Here R+ = {x = T ( x, xn) ; x ′ = T (x1, · · · , xn−1) ∈ R , xn > 0}, n ≥ 2, and the superscript T · stands for the transposition; ρ = ρ(t, x) and m = T (m1(t, x), . . . , mn(t, x)) denote the unknown density and momentum at time t ≥ 0 and position x ∈ R+, respectively; P = P (ρ) is the pressure; ν and ν̃ are the viscosity coefficients that satisfy ν > 0, 2 nν + ν̃ ≥ 0; div m denotes the usual divergence in x of m; and ∇f denotes the usual gradient in x of a scalar function f . (e.g., j-th component of ∇P (ρ) is ∂xj P (ρ).) The notation div ( m⊗m ρ ) means that its j-th component is given by div ( mjm ρ ).