2020
DOI: 10.1016/j.ces.2019.115441
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Large–eddy simulation in a Sonolator high–pressure homogeniser

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Cited by 4 publications
(9 citation statements)
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“…For given k , ε , trueu1*2¯ and the above assumptions about trueκ1¯ and σ 1 , Equation ) returns a spectrum shape which mimics the 1‐D spectra observed in our LES of a high‐pressure homogenizer 47 . This is achieved by redistributing energy from across the full spectrum to the wave numbers local to the vortex shedding frequency.…”
Section: Energy Spectrum—structure Function Model Based On Turbulencementioning
confidence: 52%
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“…For given k , ε , trueu1*2¯ and the above assumptions about trueκ1¯ and σ 1 , Equation ) returns a spectrum shape which mimics the 1‐D spectra observed in our LES of a high‐pressure homogenizer 47 . This is achieved by redistributing energy from across the full spectrum to the wave numbers local to the vortex shedding frequency.…”
Section: Energy Spectrum—structure Function Model Based On Turbulencementioning
confidence: 52%
“…The authors in Reference 48 concluded that the deviations between the measured spectra and the model spectra are consistent with finite Reynolds number effects (with Re L ∼ 1000 − 3000). In the high‐pressure homogenizer study, 47 Re L was also moderate 50 ranging from ∼10 3 − 10 4 .…”
Section: Deviations From Homogeneous Isotropic Turbulencementioning
confidence: 93%
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“…However, there is of yet no consensus on which of these that are most suitable for modelling industrially relevant breakup processes. Moreover, the turbulence found in high-pressure homogenizers, rotor-stators mixers and similar systems deviates substantially from the ideal isotropic, homogenous turbulence assumed in deriving these models [21][22][23].…”
Section: Introductionmentioning
confidence: 89%