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Lackmann , Chapter 1:. Basics of atmospheric motion. time scales of atmospheric variability. Lovejoy 2013, EOS . time scales of atmospheric variability. Lovejoy 2013, EOS . (1) Scales of atmospheric motion. Note two spectral extremes: (a) A maximum at about 2000 km - PowerPoint PPT Presentation
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Lackmann, Chapter 1:
Basics of atmospheric motion
time scales of atmospheric variability
Lovejoy 2013, EOS
Lovejoy 2013, EOS
time scales of atmospheric variability
Gage and Nastrom (1985)
[shifted x10 to right]Note two spectral extremes:
(a) A maximum at about 2000 km(b) A minimum at about 500 km
1100 101000wavelength [km]
(1) Scales of atmospheric motion
inertial subrange
35
kSD
FA=free atmos.BL=bound. layerL = long wavesWC = wave cyclonesTC=tropical cyclonescb=cumulonimbuscu=cumulusCAT=clear air turbulence
From Ludlam (1973)
Energy cascade
synoptic scale
Big whirls have little whirlsthat feed on their velocity;and little whirls have lesser whirls,and so on to viscosity. -Lewis Fry Richardson
Markowski & Richardson 2010, Fig. 1.1
Scales of atmospheric motion
Scales of atmospheric motion• Air motions at all scales from planetary-scale to microscale explain weather:
– planetary scale: low-frequency (10 days – intraseasonal) e.g. blocking highs (~10,000 km) – explains low-frequency anomalies
• size such that planetary vort adv > relative vort adv• hydrostatic balance applies
– synoptic scale: cyclonic storms and planetary-wave features: baroclinic instability (~3000 km) – deep stratiform clouds
• smaller features, whose relative vort adv > planetary vort adv• size controlled by b=df/dy• hydrostatic balance applies
– mesoscale: waves, fronts, thermal circulations, terrain interactions, mesoscale instabilities, upright convection & its mesoscale organization: various instabilities – synergies (100-500 km) – stratiform & convective clouds
• time scale between 2p/N and 2p/f• hydrostatic balance usually applies
– microscale: cumuli, thermals, K-H billows, turbulence: static instability (1-5 km) – convective clouds
• Size controlled by entrainment and perturbation pressures• no hydrostatic balance
b gg vv
2p/N ~ 2p/10-2 ~ 10 minutes2p/f = 12 hours/sin(latitude) = 12 hrs at 90°, 24 hrs at 30°
1.4 thermal wind balance
yT
pp
fRu
yT
fpR
ygp
RT
fg
pu
gpRT
pZ
yZ
fgu
g
g
g
)2(
)1( geostrophic wind
hypsometric eqn
plug (2) into (1)
finite difference expression:
this is the thermal wind: an increase in wind with height due to a temperature gradient
greater thickness
lower thickness
y
ug
ug
The thermal wind blows ccw around cold pools in the same way as the geostrophic wind blows ccw around lows. The thermal wind is proportional to the T gradient, while the geostrophic wind is proportional to the pressure (or height) gradient.
ug=0
Let’s verify qualitatively that climatological temperature and wind fields are roughly in thermal wind balance.
For instance, look at the meridional variation of temperature with height (in Jan)
Around 30-45 ºN, temperature drops northward, therefore westerly winds increase in strength with height.
The meridional temperature gradient is large between 30-50ºN and 1000-300
hPa
thermal wind
Therefore the zonal wind increases rapidly from 1000 hPa up to 300 hPa.
Question:
Why, if it is colder at higher latitude, doesn’t the wind continue to get stronger with altitude ?
There is definitively a jet ...
Answer: above 300 hPa, it is no longer colder at higher latitudes...
tropopause
Tp
Tp
Tp
Tp
Z500500500 ˆ Zk
fgv g
Z500-Z1000
ZkfgZZk
fgvvv
TkfpR
fpR
xT
yT
fpR
pv
pu
pv
ggT
ggg
ˆˆ
ˆ,,
100050010005001000,500
baroclinicity• The atmosphere is baroclinic if a horizontal temperature gradient is
present• The atmosphere is barotropic if NO horizontal temperature gradient
exists– the mid-latitude belt typically is baroclinic, the tropical belt barotropic
• The atmosphere is equivalent barotropic if the temperature gradient is aligned with the pressure (height Z) gradient– in this case, the wind increases in strength with height, but it does not
change direction equivalent barotropic
Z Theight
gradienttemperature gradient
warmcold
baroclinic
warm
cold
geostrophic wind at various levels
1gv
1gv
12 ggT vvv
1.4.2 Geostrophic T advection:cold air advection (CAA) & warm air advection
(WAA)
highlight areas of cold air advection (CAA) & warm air advection (WAA)
CAA
WAA
WAA & CAA
geostrophic temperature advection: the solenoid method
lower
heigh
t Z
greate
r Z
geostrophic wind: Z
fgv
xZ
yZ
fgZk
fgv
g
g
,ˆ
warm
cold
warm
cold
lower
Z
greate
r Z
fatter arrow: larger T gradient T
TZfgTv
Tv
g
g
geo. temperature advection is:
the magnitude is:
the smaller the box, the stronger the temp advection
Let us use the natural coordinate and choose the s direction along the thermal wind (along the isotherms) and n towards the cold air. Rotating the x-axis to the s direction, the advection equation is:
)0∂T∂ that (note ,
∂T∂
∂T∂
sn
Vt n
Thermal wind and geostrophic temperature advection
V nwhere is the average wind speed perpendicular to the thermal wind.
local T change T advection
The sign of
+ -
V n
VT VT
V n V n
12 ggT vvv
warm
coldwarm
cold
If the wind veers with height, is positive and there is warm advection. If the wind is back with height, is negative and there is cold advection.
V n V n
+ -
VTVT
V n V n
WARM
WARM
COLD
COLD
)0∂T∂ that (note ,
∂T∂
∂T∂
sn
Vt n
0>∂T∂t
WAA
0<∂T∂tCAA
Thermal wind and temperature advection
Procedure to estimate the temperature advection in a layer:
1. On the hodograph showing the upper- and low-level wind, draw the thermal wind vector.
2. Apply the rule that the thermal wind blows ccw around cold pools, to determine the temperature gradient, and the unit vector n (points to cold air)
3. Plot the mean wind , perpendicular to the thermal wind. Note that is positive if it points in the same direction as n. Then the wind veers with height, and you have warm air advection.
If there is warm advection in the lower layer, or cold advection in
the upper layer, or both, the environment will become less stable.
V n
V n
thermal wind and temperature advection
example
x
y
1000gv
850gv
1000850 ggT vvv
WARM
COLD
0>∂T∂t
n
V n
0 nV
veering wind warm air advectionbetween 1000-850 hPa
10°C
5°C
s
friction-inducednear-surfaceconvergence into lows/trofs
1.5 vorticity
shear and curvature vorticity
fa
? ora
a
av
Hovmoller diagrams (Fig. 1.20)