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Some characteristics of the surface layer Surface layer (SL) is greatly

Some characteristics of the surface layer

Surface layer (SL) is greatly influenced

by the underlying surface. The latter supplies the SL with heat, water vapor, and admixtures and here the air currents experience the friction effect.
Meteorological parameters experience variations with time and altitude that are much stronger than in the rest of the atmosphere.
Inversions are frequent phenomena in the surface layer.
The most important process in the surface layer is EDDY MIXING.
Слайд 3

For more clear reasoning, let’s assume the following conditions: no advection

For more clear reasoning, let’s assume the following conditions:
no advection
vertical

motion close to zero
εr=0, fair weather (no water phase transfer)

Q0

Q

Слайд 4

Let’s define the altitude z=h, up to which the ratio remains

Let’s define the altitude z=h, up to which the ratio remains

very small.

For instance ε=0,1

“h” is altitude of SL

According to measurements, Q0=40…250 w/m².

Suppose, temperature variation is 5°C for 12 hours

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From the previous discussion we know The layer 0 – Z

From the previous discussion we know

The layer 0 – Z is

relatively small. Therefore, within this layer temperature variation has the same sign at any altitude. It means that Z increase results in increase the integral too, and at Z

Thus, within the layer 0 – h Q≈Q0. The error will not be more than 10%

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Temperature profiles in the surface layer the New Bridge, Bratislava, Slovakia;

Temperature profiles in the surface layer

the New Bridge, Bratislava, Slovakia; Temperature

inversion; 11 Nov 2005
Author: --Ondrejk 23:33, 21 Mar 2005 (UTC)
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eddy coefficient k grows up with z in the surface layer

eddy coefficient k grows up with z in the surface layer
assume

there’s linear growth of k:
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Let’s multiply both parts of (13.4) by dz

Let’s multiply both parts of (13.4) by dz

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Let’s integrate (13.6) from z=0 ( ) to arbitrary chosen z

Let’s integrate (13.6) from z=0 ( ) to arbitrary chosen z
we

adopted that
(13.7) is a logarithmic law of air temperature distribution in the surface layer.
As known
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(13.7) can be rewritten as T0 is measured just at the

(13.7) can be rewritten as

T0 is measured just at the surface

(significant inaccuracy). Let’s reduce such errors (13.8 for z=z1 ):
substitute in (13.8)
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sign of temperature variation with height depends on sign of heat

sign of temperature variation with height depends on sign of heat

flux Q0
the air temperature decreases with height at
the air temperature increases with height at
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Some empirical studies have shown that logarithmic law describes T(z) more

Some empirical studies have shown that logarithmic law describes T(z) more

or less correctly at neutral stratification when

coefficient k0 can be expressed with roughness parameter z00
substituting (13.11) into (13.10):

order of magnitude Z0 (snow,grass,water,desert) 10-2m, (forest,town,broken terrain) 100…10-1 m.
We may neglect Z0 at z,z1 > 1 m.