Published online by Cambridge University Press: 21 October 2013
Through theory and numerical simulations in an axisymmetric geometry, we examine evolution of a symmetric intrusion released from a cylindrical lock in stratified fluid as it depends upon the ambient interface thickness, $h$, and the lock aspect ratio
${R}_{c} / H$, in which
${R}_{c} $ is the lock radius and
$H$ is the ambient depth. Whereas self-similarity and shallow-water theory predicts that intrusions, once established, should decelerate shortly after release from the lock, we find that the intrusions rapidly accelerate and then enter a constant-speed regime that extend between
$2{R}_{c} $ and
$5{R}_{c} $ from the gate, depending upon the relative interface thickness
${\delta }_{h} \equiv h/ H$. This result is consistent with previously performed laboratory experiments. Scaling arguments predict that the distance,
${R}_{a} $, over which the lock fluid first accelerates increases linearly with
${R}_{c} $ if
${R}_{c} / H\ll 1$ and
${R}_{a} / H$ approaches a constant for high aspect ratios. Likewise in the constant-speed regime, the speed relative to the rectilinear speed,
$U/ {U}_{\infty } $, increases linearly with
${R}_{c} / H$ if the aspect ratio is small and is of order unity if
${R}_{c} / H\gg 1$. Beyond the constant-speed regime, the intrusion front decelerates rapidly, with power-law exponent as large as
$0. 7$ if the relative ambient interface thickness,
${\delta }_{h} \lesssim 0. 2$. For intrusions in uniformly stratified fluid (
${\delta }_{h} = 1$), the power-law exponent is close to
$0. 2$. Except in special cases, the exponents differ significantly from the
$1/ 2$ power predicted from self-similarity and the
$1/ 3$ power predicted for intrusions from partial-depth lock releases.