|
|
|
|
|
|
|
|
|
|
|
SUMMARY OF ENERGY FLOW
|
|
|
|
|
|
|
|
|
|
|
|
|
|
APE or Heat Flow
| |
KE or Momentum Flow
|
|
1. Latitudinal distribution of radiative heating & cooling (especially
when a P average is taken) has excess heating in tropics, deficit at high
latitudes.
| |
1. Westerly momentum is introduced in the tropics (i.e. an "excess") and
is removed by friction in mid lats. (a "deficit") Recall O&P 1983 fig.
13 or fig. 4.6
|
2. Result of item 1. is a poleward heat flux (fig. 3.9) which includes
v*theta as well as vLq.
| |
2. Result of item 1. is a poleward flux of angular momentum (fig. 4.12)
and of KE
(see O&P 1983 fig. 36) |
3. In middle latitudes: eddies are the main mechanism for heat transport,
all else is seondary.
| |
3. In middle latitudes: eddies are the main process for momentum
transport, all else is seondary.
|
4. The CA and CE conversions show us that the v'theta' and W'theta'
fluxes are how
eddies gain energy (fig 4.30) v'Lq' may also be an energy source. (p.
133) for eddies.
| |
4. Eddy momentum fluxes also provide sources & sinks of
eddy momentum (or eddy kinetic energy from CK
conversion). Since global average CK>0 eddies must loose KE
to the mean flow in the net.
|
5. The net radiation being >0 causes the heat flux to increase with
latitude in the
subtropics (Compare figs 3.8c, 3.9) (More and more heat must be
transported poleward to maintain quasi-steady T.)
| |
5. The flux of [KE] keeps increasing with latitude in
subtropics where CK > 0. (See
O&P 1983 fig. 36 and text's fig. 4.32) (More and more momentum must be
transported poleward to maintain quasi-steady [KE].)
|
6. Eddy heat flux is DOWN the T gradient.
| |
6. Eddy momentum flux is UP the gradient of [u]/R in subtropics.
|
7. The heat flux is a maximum where net radiation is zero
(no more heat is added
to that already coming from lower latitudes so that which
must be transported poleward is a maximum there.)
| |
7. The flux of [KE] reaches a maximum where CK=0. (no additional
[KE] is being created by the CK conversion, so no more KE must
be added to the KE that is already being
transported poleward)
|
8. Poleward of the heat flux maximum there is cooling by net radiation
| |
8. Poleward of that (angular velocity) jetstream maximum
the eddies remove energy from [KE] in the net.
|
|
|