Because of the variation in the temperature of maximum density with de
pth, it is known that the upper (above 250 m) and lower water columns
circulate separately in deep temperate lakes. While near-surface water
overturns twice per year, the deep waters often mix only partially du
ring a complete annual cycle. It is believed that deep convection is t
riggered by storm surge, forcing of some of the relatively cold upper
water column downward through its compensation depth, so that it becom
es unstable and sinks. The scale and intensity of the resulting deep w
ater forming plumes are studied numerically. A high-resolution model b
ased on the nonhydrostatic Boussinesq equations is used. Deep water fo
rmation is initiated by applying a statically unstable, initial temper
ature profile over various regions of the domain at depths below 300 m
. The grid spacing is small enough to resolve individual plumes which
carry surface water to the lake bottom. The domain of study is also la
rge enough that the geostrophic Eady (1949) wave breakup of newly form
ed deep water can be observed. It is found that when the initial insta
bility is applied in midbasin, remote from the solid sidewalls, relati
vely little fresh deep water is formed and the fluid quickly reaches a
geostrophic and hydrostatic balance. Vigorous vertical mixing ceases
after 4 days, and the resulting baroclinic fluid has a well-defined an
d predictable scale. In contrast, when the initial instability is appl
ied immediately adjacent to a solid boundary, vigorous plume motion co
ntinues for the duration of the numerical simulations (12 days), produ
cing a much greater volume of fresh deep water. A parametric study inv
estigates the scale and intensity of this boundary mixing. It is found
that reduced surface water temperature, Coriolis acceleration, or hig
her horizontal diffusion coefficients increase the rate of deep water
renewal.