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The air humidity

Memory flash ;)Please, give definitions to the following terms:Absolute humiditySpecific humiditySurface layerBoundary layer

Слайды и текст этой презентации

Слайд 1The air humidity
Lecture 20

The air humidityLecture 20

Слайд 2Memory flash ;)
Please, give definitions to the following terms:
Absolute humidity
Specific

humidity
Surface layer
Boundary layer

Memory flash ;)Please, give definitions to the following terms:Absolute humiditySpecific humiditySurface layerBoundary layer

Слайд 3Non stop rotation of water in the atmosphere http://www.meted.ucar.edu/mesoprim/mesodefn/index.htm
How much

is the amount of water
taking part in this rotation?

Non stop rotation of water in the atmosphere  http://www.meted.ucar.edu/mesoprim/mesodefn/index.htmHow much is the amount of water taking

Слайд 51 m2

1 m2
1 m2 = 10 000 cm2
Water density

= 1 g/ cm3


What is thickness of water layer?


1

000 g : 1 g/cm3 =
=1 000 cm3
1 000 cm3 : 10 000 cm2 =
=0.1 cm = 1 mm



1 kg of water per 1 m2 ? 1 mm of precipitated water

1 m21 m21 m2 = 10 000 cm2 Water density = 1 g/ cm3 What is thickness

Слайд 6Annual amount of precipitation
Spb 680 mm, Wien 300 mm, Amsterdam

1200 mm
Tropics 680 mm/ day !

Annual amount of precipitationSpb 680 mm, Wien 300 mm, Amsterdam 1200 mmTropics 680 mm/ day !

Слайд 71131 / 25.5=45 times or every 8 days
1.29 *10 13

t of water in the atmosphere (3 phases all together)
Equivalent

to 25.5 mm
Annual amount of precipitation is 1131 mm

How often is the water replaced in the atmosphere?



To evaporate 1131 mm of water we need
2.82* 10 5 J or 30% of solar radiation absorbed by the planet

1131 / 25.5=45 times or every 8 days

1131 / 25.5=45 times or every 8 days1.29 *10 13 t of water in the atmosphere (3

Слайд 8Equation of water transfer in the turbulent atmosphere





Only specific humidity

could be considered as a conservative characteristic of w.v.content of

a moving particle (no absolute or relative humidity, dew point, w.v.pressure
Equation of water transfer in the turbulent atmosphereOnly specific humidity could be considered as a conservative characteristic

Слайд 9Equation of water transfer in the turbulent atmosphere





1 m2
Amount of

the w.v.mass remained in the
air volume per a unit

of time
Equation of water transfer in the turbulent atmosphere1 m2Amount of the w.v.mass remained in the air volume

Слайд 10Advective terms could be neglected (too small)






Advective terms could be

neglected (too small)

Advective terms could be neglected (too small)Advective terms could be neglected (too small)

Слайд 11Eddy diffusion of w.v.







Eddy diffusion of w.v.
Horizontal transfer or advection
Convective

w.v. transfer
Only vertical eddy diffusion is represented here but it

could be both vertical and horizontal

The equation is true for non-saturated air

in/outflux of w.v. due to evap./condensation

Eddy diffusion of w.v.Eddy diffusion of w.v.Horizontal transfer or advectionConvective w.v. transferOnly vertical eddy diffusion is represented

Слайд 12Distribution of the humidity characteristics with height in the surface

layer








Let’s find S=S(z) in the surface layer ? integrate (20.5)

from 0 to Z

With the accuracy 10 % :

Is the w.v.flux at z=0, i.e. the rate of evaporation from the Earth’s surface:

Distribution of the humidity characteristics with height in the surface layerLet’s find S=S(z) in the surface layer

Слайд 13(20.8) shows that the w.v. eddy flux in the surface

layer
can be regarded as approximately unchangeable
with height (

as well as a heat flux).

Similarly to the heat flux :









(20.8) shows that the w.v. eddy flux in the surface layer
can be regarded as approximately unchangeable
with height ( as well as a heat flux).

Similarly to the heat flux :

“S” decreases at Q’0 < 0 with height proportionally to ln z

(20.8) shows that the w.v. eddy flux in the surface layer can be regarded as approximately unchangeable

Слайд 14Humidity distribution above the surface layer







Comparision of calculated and observed

w.v. pressure values shows that the observed values decrease with

height much more rapidly than calculated ones.

Suring’s formula
( empirical)

Z in km
True within the boundary layer above the surface layer

Humidity distribution above the surface layerComparision of calculated and observed w.v. pressure values shows that the observed

Слайд 15Diurnal variation of the humidity characteristics

Near sunrise
7 a.m.
3-5 p.m.
7-10 p.m.
Diurnal

variation is better pronounced over land in the warm season
w.v.pressure
Absolute

humidity
Diurnal variation of the humidity characteristicsNear sunrise7 a.m.3-5 p.m.7-10 p.m.Diurnal variation is better pronounced over land in

Слайд 16Diurnal variation of the humidity characteristics

In the night
when T air

drops
3 p.m.
RH=100% *e/E
e decreases near noon (summer)
E sharply increases (account

for T rise)

relative humidity


In winter/over water surfaces:
One min, usually before sunrise.
Weak max, supposed before noon.
Reasons:
Eddy exchange is weak
Eddy transfer of the w.v. is compensated by evaporation

Diurnal variation of the humidity characteristicsIn the nightwhen T air drops3 p.m.RH=100% *e/Ee decreases near noon (summer)E

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