Super cooled water in the atmosphere and water

Слайд 2

Lecture 21 Metastable state In some cases the relaxation time is

Lecture 21

Metastable state

In some cases the relaxation time is rather long.

It happens as the initial state is not really unstable. We say: “the system is in metastable state”.

A

B

C

A. Unstable state

B. Metastable state

C. Stable state

H

h

Super saturated water vapor and super cooled water in the atmosphere are metastable thermodynamic systems.

To start condensation or freezing, some nuclei of the new state are needed

Слайд 3

Lecture 21 Super saturated water vapor or/and supercooled water droplets Metastable

Lecture 21

Super saturated water vapor or/and supercooled water droplets

Metastable state

No condensation

(crystallization) nuclei

The nuclei can appear due to density fluctuation (random molecules approach each other)

Random molecular condensation (crystallization)

Energy released due to random condensation (crystallization), Er

Condensation (crystallization) on some larger nuclei releases additional energy EL.n.

Growth the nuclei requires some additional energy EN. It may come from condensation (crystallization)

Process will not go due to energetic disadvantage

There are condensation (crystallization) nuclei

Condensation will proceed, and the energy released will be scarified for formation of larger nuclei

Heterophased nuclei

Слайд 4

Lecture 21 Water droplet freezing process At the temperature below 0°C,

Lecture 21

Water droplet freezing process

At the temperature below 0°C, water droplets

may freeze becoming ice particles. For the ice phase to appear a nucleus of the ice must be formed inside of the droplet.

Such process is called homogenous phase transfer

The new phase can appear on foreign body (heterogeneous nucleus). Such kind of bodies are called crystallization nuclei. Accordingly this process is called heterogeneous phase transfer

In the atmosphere both homogenous and heterogeneous phase transfer may take place

Слайд 5

Lecture 21 Heterogeneous ice formation assumes existence of special crystallization nuclei.

Lecture 21

Heterogeneous ice formation assumes existence of special crystallization nuclei. At

present, meteorologists believe that condensation nuclei become (at least partly) crystallization ones as the air temperature grows down below 0°C

Crystallization start

No crystallization

Crystallization nuclei are present.
Heterogeneous phase transfer

Crystallization nuclei are not present.
Homogenous phase transfer

It is believed that amount of crystallization nuclei in the atmosphere is rather small. Therefore, the major role in crystallization process is played the homogenous phase transfer. This conclusion is supported by the observed facts of super cooled water droplet clouds (T=-12…-20°C) existence for a long time.

Слайд 6

Lecture 21 Distillation Suppose there is a super cooled clouds consisting

Lecture 21

Distillation

Suppose there is a super cooled clouds consisting of water

drops and ice crystals

Initial time

W.V. sublimates on ice crystal

Next time

Drops evaporate

And so on until all drops become evaporated. However this process is quite long, practically, it is infinite.

Слайд 7

Lecture 21 Theory of distillation The following equation set is to

Lecture 21

Theory of distillation

The following equation set is to be solved

to obtain unknown quantities r1 and r2 and a at a given moment of time.

D denotes diffusion of the water molecules

Слайд 8

Lecture 21 Low Temperature Scanning Electron Microscope (LT-SEM) http://emu.arsusda.gov/snowsite/default.html

Lecture 21

Low Temperature Scanning Electron Microscope (LT-SEM)

http://emu.arsusda.gov/snowsite/default.html

Слайд 9

Lecture 21 http://emu.arsusda.gov/snowsite/default.html http://emu.arsusda.gov/snowsite/default.html

Lecture 21

http://emu.arsusda.gov/snowsite/default.html

http://emu.arsusda.gov/snowsite/default.html

Слайд 10

Lecture 21 http://emu.arsusda.gov/snowsite/default.html http://emu.arsusda.gov/snowsite/default.html

Lecture 21

http://emu.arsusda.gov/snowsite/default.html

http://emu.arsusda.gov/snowsite/default.html

Слайд 11

Lecture 21 http://emu.arsusda.gov/snowsite/default.html http://emu.arsusda.gov/snowsite/default.html

Lecture 21

http://emu.arsusda.gov/snowsite/default.html

http://emu.arsusda.gov/snowsite/default.html