2016
DOI: 10.1016/j.ultsonch.2016.01.025
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Numerical 3D flow simulation of ultrasonic horns with attached cavitation structures and assessment of flow aggressiveness and cavitation erosion sensitive wall zones

Abstract: As a contribution to a better understanding of cavitation erosion mechanisms, a compressible inviscid finite volume flow solver with barotropic homogeneous liquid-vapor mixture cavitation model is applied to ultrasonic horn set-ups with and without stationary specimen, that exhibit attached cavitation at the horn tip. Void collapses and shock waves, which are closely related to cavitation erosion, are resolved. The computational results are compared to hydrophone, shadowgraphy and erosion test data. At the hor… Show more

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Cited by 57 publications
(36 citation statements)
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“…5 (a): this is in good agreement with practical experience as well as topographic measurements, as reprinted in Fig. 5 (b) from [13], where the erosion depth for the stationary specimen and horn tip is shown.…”
Section: Fig 5 (A): Radial Erosion Probability ( ) Distribution On Tsupporting
confidence: 85%
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“…5 (a): this is in good agreement with practical experience as well as topographic measurements, as reprinted in Fig. 5 (b) from [13], where the erosion depth for the stationary specimen and horn tip is shown.…”
Section: Fig 5 (A): Radial Erosion Probability ( ) Distribution On Tsupporting
confidence: 85%
“…Loading of the stationary specimen is dominated by subharmonic collapse, i.e. the collapse of large vapor structures which form over a multiple of the horn driving period [13]. The weak grid dependence of numerical sensor signals presented here is attributed to the large sensor size: while numerical pressure in a single cell strongly depends on grid size, cell-face area weighted integration across a large number of cells to obtain a sensor force diminishes grid dependency.…”
Section: Grid Quality and Grid Independencymentioning
confidence: 83%
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