Undulatiform clouds

Содержание

Слайд 2

Undulatiform clouds Wave-like motion in the atmosphere is rather often phenomena.

Undulatiform clouds

Wave-like motion in the atmosphere is rather often phenomena. This

motion, at certain conditions, are responsible for undulatiform cloud formation.

The undulatiform clouds are seen as long banks, bands, streets, and plates. The sizes of these formations are: 10³-10² km in horizontal directions, and 101-10² meters in vertical, rarely up to 2 km.

Слайд 3

Conditions for undulatiform clouds to arise Wave-like motion Stable stratification of

Conditions for undulatiform clouds to arise

Wave-like motion
Stable stratification of the

atmosphere
The air involved into the cloud formation should be humid enough to become saturated at a small ascent.

Reasons for the wave-like motion to arise

Two layers ( one above another) with different density and speed of motion.
Inversion (barrier layer) must exist to prevent the layer to mix up.

According to Helmholtz formula, the waves spread with the speed

Слайд 4

The wave can be stable or unstable. Stable wave amplitude does

The wave can be stable or unstable. Stable wave amplitude does

not change its value. Unstable wave amplitude value increases.
The wave stability depends on the wave length at a given conditions, i. e. on the radicand value in the Helmholtz’ formula.

Setting this value to zero, we obtain

Critical wavelength

Value varies from a few meter up to 8 km

The waves are stable. Clouds may appear, but not develop

The waves are unstable. Clouds appear and develop

Слайд 5

An example of the critical wavelength determination If at these conditions

An example of the critical wavelength determination

If at these conditions the

observed wave , this wave is stable.
If at these conditions the observed wave , this wave is unstable.
Слайд 6

Another reason for wave formation is air flowing over mountains. These

Another reason for wave formation is air flowing over mountains. These

wave arise on the lee side of mountains. That is why they are known as lee waves

Lee wave structure depends on:
Velocity of air currents
Stratification of the atmosphere (unstable stratification results in formation of lee vortexes and chaotic cloudiness appearance)
Size of the mountains.

Слайд 7

Terrain-related lifting mechanisms (Whiteman ppt) Whiteman (2000)

Terrain-related lifting mechanisms (Whiteman ppt)

Whiteman (2000)

Слайд 8

Lee waves (Whiteman ppt) Stull (1995) Lift

Lee waves (Whiteman ppt)

Stull (1995)

Lift

Слайд 9

Amplification and cancellation of lee waves (Whiteman ppt) Bérenger & Gerbier (1956)

Amplification and cancellation of lee waves (Whiteman ppt)

Bérenger & Gerbier (1956)

Слайд 10

© Jeff Grandy www.pbs.org/wgbh/nova/ denali/extremes/speak.html Lenticular clouds (Whiteman ppt)

© Jeff Grandy

www.pbs.org/wgbh/nova/ denali/extremes/speak.html

Lenticular clouds (Whiteman ppt)

Слайд 11

Lenticular and wave clouds (Whiteman ppt) Whiteman (2000) a, b, & g: Brooks Martner photos

Lenticular and wave clouds (Whiteman ppt)

Whiteman (2000)

a, b, & g:
Brooks

Martner photos
Слайд 12

Smith et al. (1997) http://www.wrh.noaa.gov/spokane/pix_month/waves.htm MODIS satellite Leewave clouds, wakes (Whiteman

Smith et al. (1997)

http://www.wrh.noaa.gov/spokane/pix_month/waves.htm

MODIS satellite

Leewave clouds, wakes (Whiteman ppt)

Wave clouds over

Cascades and Rocky Mtns of MT and Alberta
Wave clouds induced by South Sandwich Islands on 27 January 2004, MODIS satellite
Слайд 13

Wakes -турбулентный след (Whiteman ppt) Orgill (1981)

Wakes -турбулентный след (Whiteman ppt)

Orgill (1981)

Слайд 14

Wake (Whiteman ppt) From Erick Brenstrum

Wake (Whiteman ppt)

From Erick Brenstrum

Слайд 15

© Rick Dunn 1995 www.RJDphoto.com Kelvin-Helmholz instability (Whiteman ppt)

© Rick Dunn 1995
www.RJDphoto.com

Kelvin-Helmholz instability

(Whiteman ppt)

Слайд 16

© Amy Flygare (Whiteman ppt)

© Amy Flygare

(Whiteman ppt)

Слайд 17

Matterhorn banner cloud (Whiteman ppt) Whiteman (2000)

Matterhorn banner cloud (Whiteman ppt)

Whiteman (2000)

Слайд 18

Blocked flow - New Zealand (Whiteman ppt) Whiteman photo

Blocked flow - New Zealand (Whiteman ppt)

Whiteman photo

Слайд 19

Notion on cloud cells Observation (including satellite ones) show that clouds

Notion on cloud cells

Observation (including satellite ones) show that clouds often

exist in form of mesoscale objects that are called cloud cells. These cells have a form of not fully regular systems – hexagons. The cells are not the only systems; there are also bands and banks of clouds.
Benar (1900) and Rayleigh (1916) were the first to discover this kind of cloud field structure. According to Rayleigh’s investigations, regime of motion causing waves and cloud formation depends on non-dimensional number (Rayleigh’s number)

Depth of convective layer

Molecular viscosity

Temperature conductivity

Open cell

Closed cell

Over warm surface

Over cold surface

Wavelike motion of the cell type; unstable waves

Any type of motion; waves (if any) are stable

Слайд 20

Open cells which resembles a honeycomb

Open cells which resembles a honeycomb

Слайд 21

open- and closed-cell in South Atlantic Credit Jacques Descloitres, MODIS Rapid

open- and closed-cell in South Atlantic

Credit Jacques Descloitres, MODIS Rapid Response

Team, NASA/GSFC
http://visibleearth.nasa.gov/view_rec.php?id=6394

In "closed" cells, seen primarily in the top right corner of the image, warm air is rising in the center, and sinking around the edges, so clouds appear in cell centers, but evaporate around cell edges.
Closed and open cell convection represent two stable atmospheric configurations—two sides of the convection coin.

Слайд 22

Closed Cell Convection near the Azores (NASA MODIS Terra Satellite –

Closed Cell Convection near the Azores (NASA MODIS Terra Satellite –

12 April 2006

12:30 UTC - resolution 1 km; Image courtesy of MODIS Rapid Response Project at NASA/GSFC,
[Van Delden, A., 1998, On the flow-pattern of shallow atmospheric convection,
Beitr.Phys.Atmos., 61, 169-186])