An experimental and theoretical study of the mixing produced by a plum
e rising in a confined stratified environment is presented. As a resul
t of the pre-existing stable stratification, the plume penetrates only
part way into the region; at an intermediate level it intrudes latera
lly forming a horizontal layer. As time evolves, this layer of mixed f
luid is observed to increase in thickness. The bottom front advects do
wnward in a way analogous to the first front in the filling box of Bai
nes & Turner (1969), while the lateral spreading of the plume occurs a
t an ever-increasing level and an ascending top front results. We deve
lop a model of this stratified filling box; the model predicts the rat
e at which the two fronts advance into the environment. It is found th
at stratification in the environment, when smooth, has no significant
influence on the dynamics of the descending front. We show that the ra
te of rise of the ascending front is determined by the turbulent mixin
g occurring at the spreading level. Entrainment of environmental fluid
from above into the overshooting plume is significant; as a result, a
density interface develops at this level. Asymptotically, the system
reaches a state in which a bottom convecting layer, with an almost hom
ogeneous density, deepens in a stratified background. The model propos
ed for this large-time behaviour is based on the simple energetic form
ulation that a constant fraction of the kinetic energy supplied by the
plume, for mixing across the interface, is converted into potential e
nergy of the convective layer. Our experimental results suggest an eff
iciency of approximately 50 % for this conversion. We discuss our resu
lts in the light of previous studies on turbulent penetrative convecti
on and conclude that the theory developed should be valid for an inter
mediate range of values of the Richardson number characterizing the dy
namic conditions at the interface. The model is applied quantitatively
to the process of cooling of a room wherein stratification is relevan
t. The geological problem of replenishment of a magma chamber by a lig
ht input of magma is also analysed.