Review: Relative Isentropic Flow
in a WCB (Chap. 12.3)
Page Last modified: 9 December 1998
- Purpose: to illustrate how following the motion on constant
surfaces of or
W explains
cloud patterns, precipitation, and other features that may be
hard to deduce from a conventional isobaric analysis.
- The different examples illustrate
somewhat different aspects of motion for cloud bands
formed in relatively warmer air.
- First example: a cloud band, such as the "cloud leaf"
stage (fig. 12.7a)
- from thermal wind relation, jet tends to lie above a strong
horizontal T gradient. Such a gradient would form at the
boundary between 2 distinctly different airmasses.
- sharp cloud edge near axis of the max upper level winds
- air in the cloud band has a subtropical or tropical
origin
- clear air to the west has a polar origin.
- Note: long thin arrows are streamlines: trajectories would not
necessarily cross the cloud bands because
- the whole band is
also moving towards the east.
- these are geostrophic streamlines, not actual trajectories
based on the total wind
- there are sinking and rising motions not included in the
streamlines shown.
- cloud band called a "warm conveyor belt" (WCB)
- sharp edge to the cloud lines up well with a "limiting
streamline" (LSW) for the WCB.
- Second example: fig. 12.7b is similar to figure 12.7a
except that the cloud band has an west-east orientation.
Such bands are common in the North Pacific and often
provide an indicator of a jet streak on a satellite image.
- Third example: fig. 12.8
- WCB with poleward then eastward streamlines
- dashed contours ()
and even more so (W)
indicate that parcels moving through the WCB must rise considerably.
(In going from point A, near New Orleans, to B, to C; a parcel
goes from the lower to the upper troposphere.)
- note how clouds seen in this visible image become more
glaciated (appear fuzzy due to composition as ice crystals) the
further north on the cloud band.
- Fourth example: fig. 12.9
- compares conventional analysis (fig. 12.9a) with isentropic
views (esp. 12.9b).
- where there is strong T advection, there is likely to be
the biggest differences in the analysis. (Isentropic depiction
will follow the vertical motion implied by T advection,
isobaric depiction will not.)
- fig. 12.9c: relatively sharp cloud edge matches LSW well.
- fig. 12.9e: shows
- layer of high humidity air rising dramatically as head N
(hatched). This is WCB.
- gradient in W
below and N of WCB suggests transition to colder, drier air mass
- arrows cross lines
consistent with latent heating, though
W is conserved.
- W increases
with height at most stations (not south end) indicates
air is potentially stable.
- fig. 12.9d shows how you might spot this on a single
sounding (Pittsburg).
- Fifth example: fig. 12.10 (emphasize 12.10c)
- fig 12.10c shows a cross section perpendicular to the WCB
- surfaces bend up
and over the cold air
- tropopause is lowered ("x" symbols) where the upper
trough is located
- strong contrast in RH (dashed contours) reveals air
masses of contrasting properties
- Sixth example, fig. 12.12:
- precipitation present far away from location of
the surface front (fig 12.12a).
However, since the 500 mb winds strongest further
north (fig. 12.12b big arrow), the T gradient at 700 mb (say) may be
strongest well north of the surface front. So, there might
be some midlevel WAA that might not be easily
deduced from a conventional SLP and h map. I mention this
because eqn
analysis must still apply, the WAA might not be obvious.
- there is a broad region of PVA over much of the Great
Lakes and extending to the east coast (fig. 12.12b).
- however, the precipitation has a well defined western
edge over Ohio and Kentucky.
- relative wind analysis explains these features, specifically
the sharp edge of the precipitation contained within the
region of PVA. The edge lies on another LSW (fig. 12.12c).
Back to
ATM 111 homepage