2019
DOI: 10.1016/j.nonrwa.2018.08.002
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On the large time decay of global solutions for the micropolar dynamics inL2(Rn)

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Cited by 12 publications
(4 citation statements)
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“…for every m ≥ 0, see e.g. [15,16]. The extra factor t 1/2 in (1.5b) as compared to (1.5a) seems to have been first obtained in the incompressible case in [14,23] (for compressible flows, see [20]), as a consequence of the damping term in the equation (1.1c).…”
Section: Introductionmentioning
confidence: 88%
See 1 more Smart Citation
“…for every m ≥ 0, see e.g. [15,16]. The extra factor t 1/2 in (1.5b) as compared to (1.5a) seems to have been first obtained in the incompressible case in [14,23] (for compressible flows, see [20]), as a consequence of the damping term in the equation (1.1c).…”
Section: Introductionmentioning
confidence: 88%
“…[24]). Since (2.4) is also valid for n = 2, it follows that [14,16,23]), this condition is satisfied for suitable t * * , which depends on how fast z(•, t) L 2 (R 2 ) becomes small for t 1.…”
Section: Mathematical Preliminariesmentioning
confidence: 99%
“…[38]). Since (2.4) is also valid for n = 2, it follows that [23]), this condition is satisfied for suitable t * * , which depends on how fast z(•, t) L 2 (R 2 ) becomes small for t 1.…”
Section: Mathematical Preliminariesmentioning
confidence: 94%
“…for every m ≥ 0, see [21,23,32]. The extra factor t 1/2 in (1.5b) as compared to (1.5a) seems to have been first obtained in the incompressible case in [21,23] (for compressible flows, see [30]), as a consequence of the damping term in the equation (1.1c).…”
Section: Introductionmentioning
confidence: 91%