a reduced model for internal waves interacting with submarine ...
a reduced model for internal waves interacting with submarine ...
a reduced model for internal waves interacting with submarine ...
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assumption was made on the wave amplitude up to now, the <strong>model</strong> derived is<br />
strongly nonlinear. It involves a Hilbert trans<strong>for</strong>m on the strip characterizing the<br />
presence of harmonic functions (hence the potential flow) below the interface.<br />
System (2.27) is a reduction of the original Euler equations constituted by<br />
a pair of 2D-systems of PDEs to a single 1D-system of PDEs at the interface.<br />
Instead of the integration of the Euler equations in the presence of a free interface,<br />
a single 1D-system of PDEs is to be solved. Efficient computational methods can<br />
be produced <strong>for</strong> this accurate <strong>reduced</strong> <strong>model</strong> which governs, to leading order, a<br />
complex two-dimensional problem.<br />
Remarks:<br />
1. If the bottom is flat, M(ξ)=1 and the same system derived in [8] is recovered,<br />
which is a nice consistency check.<br />
2. When the lower depth tends to infinity (h 2 →∞) the limit <strong>for</strong> this <strong>model</strong><br />
is the same one obtained in [8] because the bottom is not seen anymore<br />
(M(ξ)→1 and x(˜ξ, 0)→ ˜ξ). There<strong>for</strong>e<br />
φ xt (x, 0, t)→ 1 π<br />
( ) ( )<br />
(1−η)u1<br />
xt ˜x, t<br />
˜x− x<br />
[ ((1−η)u1 )<br />
]<br />
d ˜x=H<br />
xt<br />
(x),<br />
whereH is the usual Hilbert trans<strong>for</strong>m defined as<br />
H[ f ](x)= 1 π<br />
f ( ˜x)<br />
˜x− x d ˜x.<br />
In this (shallow upper layer) infinite lower layer regime, system (2.26) be-<br />
26