Se. Belcher et N. Wood, FORM AND WAVE DRAG DUE TO STABLY STRATIFIED TURBULENT-FLOW OVER LOW RIDGES, Quarterly Journal of the Royal Meteorological Society, 122(532), 1996, pp. 863-902
We investigate how stable stratification affects the aerodynamic force
, or form drag, induced by turbulent boundary-layer now over two-dimen
sional hills. Both analytical and numerical models are used to calcula
te the now and thence the form drag on the hill. In the analytical mod
el we use a two-layer, truncated mixing-length, turbulence model, whic
h is consistent with scaling arguments and which produces reliable est
imates of the form drag for the neutral now. The form drag is also cal
culated analytically using an eddy-viscosity model, and the results co
mpare well with values computed with the nonlinear numerical model tha
t uses a similar turbulence model. The leading-order contribution to t
he form drag is from a non-separated sheltering mechanism, which is si
milar to the mechanism in neutral flow. Stable stratification changes
the magnitude of this mechanism through several effects. For weak stra
tification the predominant effect is an increase in shear in the upstr
eam wind profile across a middle layer, which increases the form drag
by a factor of two or more. There is indirect experimental evidence to
support this finding. If the stratification is more stable, then the
shear across the middle layer becomes limited because the boundary lay
er has a finite depth. Then the dynamical effect of buoyancy on the pr
essure perturbation becomes important and reduces the form drag, event
ually to zero. For still more stable stratification, gravity waves and
associated wave drag are produced. The analysis shows that the approp
riate scaling velocity for wave drag is the approach-flow wind speed e
valuated at the middle-layer height. The relationship between the form
and wave drag components is investigated by evaluating the analytical
formula for the drag on isolated hills of two idealized shapes. For w
eak stratification the form drag dominates, but as the stratification
becomes more stable the wave drag increases and first equals the form
drag, at a value that depends on the hill shape, and then dominates.