Abstract:Abstract. We study the interaction of small-scale internal wave packets with a large-scale internal solitary wave using high-resolution direct numerical simulations in two dimensions. A key finding is that for wave packets whose constituent waves are short in comparison to the solitary wave width, the interaction leads to an almost complete destruction of the short waves. For mode-1 short waves in the packet, as the wavelength increases, a cutoff is reached, and for larger wavelengths the waves in the packet a… Show more
“…The propagation and instability of internal waves in such regions, where the background stratification varies strongly, is far different to the case of uniform stratification (Sutherland 2016). Nevertheless, the fundamental mechanism of shear refracting small-scale internal waves seems relevant at sharp density interfaces, at least in situations with large internal solitary waves as considered by Xu & Stastna (2018). Understanding how generic the mixing properties of this shear–wave interaction are for arbitrary is vital for the general application of our results.…”
“…The propagation and instability of internal waves in such regions, where the background stratification varies strongly, is far different to the case of uniform stratification (Sutherland 2016). Nevertheless, the fundamental mechanism of shear refracting small-scale internal waves seems relevant at sharp density interfaces, at least in situations with large internal solitary waves as considered by Xu & Stastna (2018). Understanding how generic the mixing properties of this shear–wave interaction are for arbitrary is vital for the general application of our results.…”
“…Interaction of small internal wave packets with a large internal wave was studied in [9]. The main result was that the indicated interaction with a single wave leads to a complete destruction of the packet which consists of waves having small length in comparison with the length of single waves.…”
Section: Literature Review and Problem Statementmentioning
confidence: 99%
“…According to (9) and (10), the wave motion on the lower and upper contact surfaces can be represented in the first approximation as: (1) (2) 11 11…”
Section: Analysis Of Wave Motion On the Contact Surfacesmentioning
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