M. Gloor et al., Dynamics of mixed bottom boundary layers and its implications for diapycnal transport in a stratified, natural water basin, J GEO RES-O, 105(C4), 2000, pp. 8629-8646
Here we report on two field experiments from Lake Alpnach (surface area: 4.
8 km(2); maximum depth: 34 m) that were designed to study the process of bo
undary mixing and to estimate its efficiency, the ratio between the turbule
nt kinetic energy converted into potential energy and dissipated into heat,
for diapycnal tracer transport. Lake Alpnach is particularly suited for th
is purpose because it is known from earlier experiments that (1) its curren
ts follow a regular oscillatory pattern, associated with basin-wide standin
g internal waves (seiches, period similar to 0.5 days and 1 day, respective
ly), and (2) diapycnal tracer transport is mainly caused by boundary mixing
. During one of the experiments reported here, strong seiches were excited
regularly and damped on a timescale of the order of 3 days; during the othe
r experiment seiching motion was comparably weak. If seiching is excited re
gularly, we find a persistent well-mixed bottom layer of 4-5 m height at th
e deepest part of the lake. In the absence of regular seiching the layer di
sappears within 10-20 days. On the sloping bottom boundaries the well-mixed
layers (1) are of much more transient nature, (2) exhibit different therma
l structure, and (3) decrease in thickness toward shallower depth inversely
proportionally to the stability at the same depth in the lake interior. Th
eir reduced thickness is possibly the result of repeatedly occurring intrus
ions of boundary mixed water masses that are observed to extend horizontall
y similar to 100-200 m into the lake interior. As a consequence of repeated
generation of intrusions, mixing on the sloping boundaries is expected to
be considerably more efficient compared to mixing over flat bottom boundari
es. The observed mixing efficiency, the ratio of the rate of change of pote
ntial energy below depth z caused by turbulence to the energy loss by botto
m friction below depth z, increases indeed from 0.01 +/- 0.01 in the deepes
t well-mixed layers to 0.15 +/- 0.04 in the upper pycnocline.