Intrusive gravity currents arise when a fluid of intermediate density
intrudes into an ambient fluid. These intrusions may occur in both nat
ural and human-made settings and may be the result of a sudden release
of a fixed volume of fluid or the steady or time-dependent injection
of such a fluid. In this article we analytically and numerically analy
ze intrusive gravity currents arising both from the sudden release of
a fixed volume and the steady injection of fluid having a density that
is intermediate between the densities of an upper layer bounded by a
free surface and a heavier lower layer resting on a flat bottom. For t
he physical problems of interest we assume that the dynamics of the fl
ow are dominated by a balance between inertial and buoyancy forces wit
h viscous forces being negligible. The three-layer shallow-water equat
ions used to model the two-dimensional flow regime include the effects
of the surrounding fluid on the intrusive gravity current. These effe
cts become more pronounced as the fraction of the total depth occupied
by the intrusive current increases, To obtain some analytical informa
tion concerning the factors effecting bore formation we further reduce
the complexity of our three-layer model by assuming small density dif
ferences among the different layers. This reduces the model equations
from a 6 x 6 to a 4 x 4 system. The limit of applicability of this wea
kly stratified model for various ranges of density differences is exam
ined numerically. Numerical results, in most instances, are obtained u
sing MacCormack's method. It is found that the intrusive gravity curre
nt displays a wide range of flow behavior and that this behavior is a
strong function of the fractional depth occupied by the release volume
and any asymmetries in the density differences among the various laye
rs. For example: in the initially symmetric sudden release problem it
is found that an interior bore does not form when the fractional depth
of the release volume is equal to or less than 50% of the total depth
. The numerical simulations of fixed-volume releases of the intermedia
te layer for various density and initial depth ratios demonstrate that
the intermediate layer quickly slumps from any isostatically uncompen
sated state to its Archimedean level thereby creating a wave of opposi
te sign ahead of the intrusion on the interface between the upper and
lower layers. Similarity solutions are obtained for several cases that
include both steady injection and sudden releases and these are in ag
reement with the numerical solutions of the shallow-water equations. T
he 4 x 4 weak stratification system is also subjected to a wavefront a
nalysis to determine conditions for the initiation of leading-edge bor
es. These results also appear to be in agreement with numerical soluti
ons of the shallow-water equations.