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At any one time, about one half of the earth's surface is covered by clouds. Clouds can occur at altitudes from the surface of the earth up to about 20 km ... – PowerPoint PPT presentation

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Title: Todays lecture objectives:


1
ATMS 455 Physical Meteorology
  • Todays lecture objectives
  • Cloud Morphology (WH 5.1)
  • How do microscopic processes impact weather
    phenomena on the mesoscale?

http//www.artcyclopedia.com/feature-2001-08.html
2
ATMS 455 Physical Meteorology
  • Todays lecture topics
  • Cloud Morphology (WH 5.1)
  • Mechanisms of formation
  • Types of clouds
  • Convective clouds
  • Layer clouds
  • Orographic clouds

3
Introduction
  • At any one time, about one half of the earths
    surface is covered by clouds
  • Clouds can occur at altitudes from the surface of
    the earth up to about 20 km
  • Nacreous (mother-of-pearl) clouds occur at
    heights up to 30 km and noctilucent clouds occur
    at about 80 km exact compositions of these
    clouds are unknown

http//www.carlwozniak.com/clouds/Graphics/New20P
ix/clouds14.jpg
4
Mechanisms of formation
  • Clouds form in air which has become
    supersaturated with respect to liquid water or
    ice happens most commonly through ascent
    accompanied by adiabatic expansion and cooling

http//www.carlwozniak.com/clouds/Graphics/New20P
ix/clouds03.jpg
5
Mechanisms of formation
  • A brief review of environmental stability
  • Absolute stability (G
  • Conditional instability (Gd
  • Absolute instability (Gd

Gd g/cp 9.8 oC/km
http//weather.uwyo.edu/upperair/sounding.html
6
Mechanisms of formation
  • Principal types of ascent
  • Local ascent of warm buoyant air parcels in a
    conditionally unstable environment produces
    convective clouds
  • Vertical velocities 3 m s-1
  • Cloud lifetimes range from minutes to hours

http//www.carlwozniak.com/clouds/Graphics/New20P
ix/clouds36.jpg
7
Mechanisms of formation
  • Principal types of ascent
  • Forced lifting of stable air which produces layer
    clouds
  • Vertical velocities range from 3-10 cm s-1
  • Cloud lifetimes are in the range of tens of hours

http//www.carlwozniak.com/clouds/Graphics/New20P
ix/clouds39.jpg
8
Mechanisms of formation
  • Principal types of ascent
  • Forced lifting of air as it passes over hills or
    mountains produces orographic clouds
  • Vertical velocities several m s-1
  • Cloud lifetimes depend on wind direction steady
    winds means long lifetimes

http//www.cartage.org.lb/en/themes/Sciences/Earth
science/Hydrology/Meteorology/Clouds/CloudDescript
ions/Lenticular2/Lenticular2.htm
9
Mechanisms of formation
  • Clouds may also form by the cooling of air below
    its dew point when it comes into contact with a
    cold surface (e.g. radiation fog, advection fog)

http//asd-www.larc.nasa.gov/SCOOL/New_Clouds/Fog/
fog6.jpg
10
Mechanisms of formation
  • The mixing of two parcels of air with different
    temperatures (e.g. steam fog)

http//www.pbase.com/clickaway/image/34671223
11
Mechanisms of formation
  • Adiabatic expansion and cooling due to a rapid
    local reduction in pressure (e.g. funnel clouds)

http//hms.pnl.gov/funnels.htm
12
Types of clouds
  • Currently used cloud classification scheme was
    first proposed back in 1803

13
Types of clouds
  • Currently used cloud classification scheme was
    first proposed back in 1803 by Howard (not Moe,
    Curly, Larry, or Shemp) - Luke
  • Cumulus (heap or pile)
  • Stratus (a layer)
  • Cirrus (filament of hair)
  • Nimbus (rain clouds)

14
Types of clouds
  • Other names for the classification scheme
  • alto (mid-level)
  • lenticularis (lens-shaped clouds)
  • castellanus (turrets)
  • Main characteristics for classifying clouds are
    depth and altitude

15
Types of clouds
16
Convective clouds
55 minute period
17
Convective clouds
  • Physical mechanisms
  • Well-defined cloud bases indicates
  • that the air at lower levels is well mixed
    due convective stirring (a)
  • Boundaries of young clouds are sharp, giving them
    the cauliflower appearance due to the clouds
    consisting mainly of liquid water (a)
  • Cumulus congestus in (a) likely due to growth
    above a particularly hot spot on the ground

18
Convective clouds
  • Physical mechanisms (cont.)
  • As clouds age, their outlines become
  • more ragged due to decrease buoyancy and due
    to the increasing presence of ice particles
    (b)-(e)
  • Anvil begins to form as upper regions of the
    cloud are starting to spread out horizontally by
    the wind at this level (b). Largest cloud in (b)
    has transformed into a cumulonimbus.
  • due to (1) growth of ice at expense of liquid
    droplets and (2) ice particles evaporate slower
    than water droplets at the edges of the cloud
    see WH Fig. 2.7

19
Convective clouds
  • Physical mechanisms (cont.)
  • Regions on the right of the largest
  • cloud in (c) and (d) have become increasingly
    diffuse as the concentrations of ice particles
    increase and the anvil becomes larger
  • The upper regions of the cumulonimbus have
    glaciated (become dominated by ice particles) in
    (e)
  • Both anvil cirrus and stratocumulus clouds can
    restrict the heating of the ground and thereby
    inhibit the formation of new convective clouds

20
Convective clouds
  • Cloud towers are produced by elements of rising
    buoyant air called thermals

21
Convective clouds
  • As a thermal rises, it pushes environmental air
    away from its upper boundary
  • At the same time, environmental air is entrained
    into the turbulent wake beneath the thermal (a)
    and (b)
  • Some environmental air is entrained through the
    sides and top of the thermal due to turbulent
    mixing
  • As a result of entrainment, the diameter of a
    thermal initially increases as it rises (a)

22
Convective clouds
  • Thermal widening ceases above the LCL due to the
    entrainment of cool, dry air
  • Some cloud water evaporates and the thermal
    buoyancy is reduced
  • Buoyancy is completely destroyed once the thermal
    has been thoroughly turned inside out
  • Evaporation at the cloud boundary causes cooling
    and sinking motions which help to keep the
    boundaries well defined

23
Convective clouds
  • Net upward movement of air in convective clouds
    is compensated by slower subsidence of air over
    the much larger area between the clouds
  • This subsidence produces warming and drying and
    hinders the growth of thermals in the regions
    between clouds
  • There is a tendency for thermals to feed
    previously formed clouds regions that have been
    moistened by earlier thermals have new thermals
    form that have reduced evaporation

Parameterize a thermal
24
Convective clouds
  • In situ aircraft measurements of a convective
    cloud

25
Convective clouds
  • Within the cloud the air is generally moving
    upward
  • Larger liquid water contents are generally
    associated with the higher updraft velocities
  • Three droplet spectra measured 100 m apart in the
    cloud
  • Bimodal droplet distribution with peak
    concentrations at droplet radii of 6 and 11 mm
  • Bimodal distribution is often observed in clouds
    growing in an unstable environment- may be
    produced by the mixing of cloudy air and drier
    environmental air at the growing cloud top

26
Convective clouds
  • The weight of falling precipitation can influence
    convective overturning through downward motions
    influenced by evaporation downdrafts are
    visible as large protuberances called mamma

Often forms under the anvil associated with
severe convective storms
http//www.invectis.co.uk/cloud/cloud.htmlpic
27
Layer clouds
  • Widespread ascent of air
  • associated with the
  • development of cyclones
  • Cirrus often the first sign of
  • an approaching warm front.

http//www.stormeyes.org/tornado/SkyPix/dngeness.h
tm
28
Layer clouds
  • Cirrus (cont.)
  • High level ( 9 km)
  • Composed of ice particles
  • Large in size
  • Low concentrations

http//www.stormeyes.org/tornado/SkyPix/dngeness.h
tm
29
Layer clouds
  • Cirrus - fallstreaks
  • Due to the large sizes of ice particles in cirrus
    and the low saturation vapor pressure of ice, ice
    particles often fall through distances of a
    kilometer or more before evaporating

http//ww2010.atmos.uiuc.edu/guides/mtr/cld/cldtyp
/hgh/gifs/crs1.gif
30
Layer clouds
  • Cirrostratus
  • As a warm front moves closer to the observer, the
    cirrus clouds give way to cirrostratus. Thin
    forms of cirrostratus often give rise to a bright
    halo (22o and 46o halos)

http//www.invectis.co.uk/cloud/cloud.html
31
Layer clouds
  • 22o and 46o halo
  • Produced by refraction of sunlight in hexagonal
    prisms of ice

32
Layer clouds
  • 22o and 46o halo
  • Inner edge of 22o halo is sharp and colored red
  • Outer edge of 22o halo is colored blue
  • Sky immediately inside the 22o halo is always
    darker than the outside
  • Halos with an angular radius 46o of can also be
    produced by refraction of ice crystals but they
    are less common and less bright than the 22o halo

33
Layer clouds
  • As warm front continues to approach, clouds
    thicken and lower in the form of altostratus
    sometimes the sun and/or moon are visible through
    altostratus

http//www.stormeyes.org/tornado/SkyPix/asundula.h
tm
34
Layer clouds
  • altostratus corona
  • Produced by the diffraction of light in small
    water droplets
  • If the droplets are uniform in size, rings may be
    seen (inside ring is blue
  • or violet, outside ring
  • is red)

http//www.du.edu/jcalvert/astro/corona.htm
http//www.planetterragen.com/clouds/
35
Layer clouds
  • Multiple cloud layers
  • Ice particles from an upper cloud layer may fall
    into lower cloud layers where they grow into snow
    particles, melt as they pass through the 0oC
    level, and reach the ground as rain
  • Melting level can often be seen looking toward
    the horizon in the direction of sun
  • Snow scatters more light than rain cloud is much
    darker just above the melting layer than below it
  • As the air is moistened by rain, fragments of
    low-level cloud (pannus or scud) often form

36
Layer clouds
  • Distribution of liquid water in warm layer clouds
    (fog)
  • Radius of droplets ranges from a few micrometers
    up to 30 40 mm
  • LWC ranges from 0.05 to 0.1 g m-3
  • Average droplet radius is about 5 mm and
    increases with height into the cloud

37
Layer clouds
  • Other types cirrocumulus (shown below),
    altocumulus, and stratocumulus
  • Two types of motions that break them up into
    small cumulus-type elements
  • Rayleigh convection
  • Shear instability

http//www.stormeyes.org/tornado/SkyPix/ccvirga.ht
m
38
Layer clouds
  • Rayleigh convection vertical shear of
    horizontal flow

39
Layer clouds
  • Rayleigh convection
  • Small convective cells warmed by radiation from
    the ground (aided at times by convective heat
    transfer) while cloud tops are cooled as they
    radiate to space a related phenomena was first
    observed in a pub!
  • Critical rate of differential heating above which
    cellular motion occurs (Benard cells)

40
Layer clouds
  • Rayleigh convection vertical shear of
    horizontal wind
  • Benard cells give way to cloud streets or rolls
  • Winds stronger than 6 m s-1
  • Lapse rate is neutrally stable
  • Align along mean direction of the wind
  • Horizontal spacing on order of 10 km
  • Ratio of horizontal wavelength to depth of the
    convective layer is 101

41
Layer clouds
  • Shear instability
  • Vertical wind shear exceeds some critical value
    within a stably stratified atmosphere

http//amath.colorado.edu/student/petersem/header.
html
42
Orographic clouds
  • Formation due to the lifting of moist air above
    LCL as streamlines are perturbed by orography
    (mountains or hills)
  • Mountain wave first wave in streamlines that
    forms over the barrier can produce mountain
    wave clouds

flow
43
Orographic clouds
flow
  • Mountain wave cloud particle distribution
  • LWC a peak value over the windward slopes (a)
  • For cold cloud, ice content peak is on downwind
    of crest (b)
  • Cloud base differences

44
Orographic clouds
  • Mountain wave clouds
  • Moisture layers ? layered (stacked) clouds
  • Can be extensive and important
  • Augment clouds in cyclonic storm systems
    producing heavy precipitation on windward slopes
  • Rain shadow areas on leeward (downwind) slopes
  • A train of lee waves (lee-wave clouds) downwind
    of a mountain (Fig. 5.15)

45
Orographic clouds
  • Moisture layers

The first modern sighting of a flying saucer
(1947) was made over Mt. Rainier, WA, where
disk-shaped wave clouds are very common.
http//www.invectis.co.uk/cloud/cloud.htmlci
Photo credit Jenny Roye
46
Orographic clouds
  • Moisture layers

http//www.invectis.co.uk/cloud/cloud.htmlci Phot
o credit Dave Appel
47
Orographic clouds
  • Mountain wave clouds
  • Within 25o of the sun are often tinted with
    brilliant (iridescent green, purple-red, blue)
    colors
  • Common in newly formed wave clouds when the cloud
    droplets tend to be uniform in size (WH 4.4.1)
  • Billow clouds are sometimes confused with wave
    clouds and rarely exhibit iridescence because
    their droplet size distributions are broader

48
Orographic clouds
  • Lee wave clouds
  • Steepest slopes of streamlines (vertical air
    velocity maxima) are a few kilometers downwind of
    the barrier
  • Sailplane records, waves can extend to 30 km,
    nacreous clouds

49
Orographic clouds
  • Leeward (downwind) winds
  • Fohn winds in Alps, Chinooks in North America
  • Rotor and rotor cloud winds may reverse
    direction near the ground due to the formation of
    a vortex. Very turbulent!

50
Orographic clouds
  • A train of lee waves (lee-wave clouds) downwind
    of the Appalachian Mountains (Fig. 5.18)

51
Orographic clouds
  • Orographic wave phenomena
  • Vertical profiles of wind and temperature play an
    important role
  • Increase in wind speed and decrease in static
    stability from the lower to the upper troposphere
  • If the width of the mountain range is comparable
    to the natural wavelength of the waves, the
    amplitude of the waves is increased by the
    resonance effect.
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