2009
DOI: 10.1007/s00162-009-0101-1
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Decaying homogeneous turbulence under strong density stratification at low-Prandtl number

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Cited by 8 publications
(8 citation statements)
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“…Even for Fr −1 10 2 , the turbulence is not quenched, if Re is sufficiently large. Turbulence persists for Re Fr −2 or equivalently R 2 (∆Ω) 3 νN 2 , where ν is the kinematic viscosity (Iida et al 2009;Lasky et al 2013). Neutron stars lie near the boundary defined by the above condition in the Fr −1 -Re plane.…”
Section: Superfluid Turbulencementioning
confidence: 93%
“…Even for Fr −1 10 2 , the turbulence is not quenched, if Re is sufficiently large. Turbulence persists for Re Fr −2 or equivalently R 2 (∆Ω) 3 νN 2 , where ν is the kinematic viscosity (Iida et al 2009;Lasky et al 2013). Neutron stars lie near the boundary defined by the above condition in the Fr −1 -Re plane.…”
Section: Superfluid Turbulencementioning
confidence: 93%
“…Even for Fr −1 10 2 , the turbulence is not quenched, if Re is sufficiently large. Turbulence persists for Re Fr −2 or equivalently R 2 (ΔΩ) 3 νN 2 , where ν is the kinematic viscosity (Iida et al 2009;Lasky et al 2013). Neutron stars lie near the boundary defined by the above condition in the Fr −1 -Re plane.…”
Section: Superfluid Turbulencementioning
confidence: 96%
“…spherical shells) only when the activity parameter Ro 3 S −1 E −1 drops below ≈ 7, which condition is avoided for Ro 10 −2 , i.e. throughout much of Figure 1 [see Iida et al (2009) and§2 in Melatos &Peralta (2010)]. Stochastic gravitational radiation from hydrodynamic turbulence imposes a fundamental noise floor on gravitational-wave observations of fossil rotators with Ro 1 even with the current generation of long-baseline interferometers (Melatos & Peralta 2010).…”
Section: Observational Signaturesmentioning
confidence: 99%