Physical uniqueness of higher-order Korteweg-de Vries theory for continuously stratified fluids without background shear
The 2nd-order Korteweg-de Vries (KdV) equation and the Gardner (or extended KdV) equation are often used to investigate internal solitary waves, commonly observed in oceans and lakes. However, application of these KdV-type equations for continuously stratified fluids to geophysical problems is hinde...
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Veröffentlicht in: | Physics of fluids (1994) 2017-10, Vol.29 (10) |
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Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | The 2nd-order Korteweg-de Vries (KdV) equation and the Gardner (or extended KdV) equation
are often used to investigate internal solitary waves, commonly observed in oceans and
lakes. However, application of these KdV-type equations for continuously stratified fluids
to geophysical problems is hindered by nonuniqueness of the higher-order coefficients and
the associated correction functions to the wave fields. This study proposes to reduce
arbitrariness of the higher-order KdV theory by considering its uniqueness in the
following three physical senses: (i) consistency of the nonlinear higher-order
coefficients and correction functions with the corresponding phase speeds, (ii)
wavenumber-independence of the vertically integrated available potential energy, and (iii)
its positive definiteness. The spectral (or generalized Fourier) approach based on
vertical modes in the isopycnal coordinate is shown to enable an alternative derivation of
the 2nd-order KdV equation, without encountering nonuniqueness. Comparison with previous
theories shows that Parseval’s theorem naturally yields a unique set of special conditions
for (ii) and (iii). Hydrostatic fully nonlinear solutions, derived by combining the
spectral approach and simple-wave analysis, reveal that both proposed and previous
2nd-order theories satisfy (i), provided that consistent definitions are used for the wave
amplitude and the nonlinear correction. This condition reduces the arbitrariness when
higher-order KdV-type theories are compared with observations or numerical simulations.
The coefficients and correction functions that satisfy (i)-(iii) are given by explicit
formulae to 2nd order and by algebraic recurrence relationships to arbitrary order for
hydrostatic fully nonlinear and linear fully nonhydrostatic effects. |
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ISSN: | 1070-6631 1089-7666 |
DOI: | 10.1063/1.5008767 |