What maintains the subtropical jet?
In observations, the zonal mean winter jet is
subtropical – at the edge of the Hadley cell, while the zonal mean summer jet
is eddy driven or merged- in midlatitudes in the Ferrel cell (Figure 1 below).
Thus the bserved subtropical jet occurs during times when the waves are strong.
Figure
1: The climatological zonal mean zonal winds (shading) and the meridional
stream function (contours) using NCEP reanalysis.
In the MQG model, a subtropical jet forms when the eddies are weak.
This is because the eddy momentum flux convergence is zero at the edge of the
Hadley cell, thus the eddies necessarily act to shift the subtropical jet
poleward. If the eddies are strong
enough they succeed, and the jet shifts to the peak in eddy momentum flux
convergence, inside the Ferrel cell.
Why are
eddies weak in the subtropical jet regime even though the vertical shear of the
jet is strong?
Because at subtropical latitudes, β is strong
enough to make the lower level PV gradients positive. Baroclinic instability is
thus between midlatitude lower level waves and upper level subtropical waves
and is inefficient. In fact, the most unstable waves in the subtropical jet
regime are high latitude, slowly westward propagating planetary scale waves.
For these waves the eddy momentum flux convergence maximizes too poleward to
strongly affect the subtropical jet.
What
happens in observations?
A closer
look at the zonally varying flow (figure 2 below) shows that eddies are
strongest at longitudes where the jet is in midlatitudes, while they are
weakest where the jet is subtropical.
The
observations are thus consistent with the MQG model in localized zonal sectors:
a subtropical jet forms when the eddies are weak enough to allow it to be
sustained.
Figure
2: Climatological Jun-Aug mean 300hPa zonal wind (contours) and synoptic 850hPa
poleward heat flux (shading, m/sec K) using NCEP reanalysis for years
1969–2011.