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Sea Ice Growth and Formation Organization Tree

This is a clickable image.  Point your mouse at a topic you would like to further explore and it will take you to a short description of the ice type of concern.  Also see the interpretation below the chart.

This chart describes the sea ice formation and growth process.  Time increases from left to right; and first order categories are expanded vertically.  In all cases ice formation begins with frazil ice production, but depending on surface water conditions, the nature of ice growth varies.  Under calm conditions, nilas ice growth is favored (little convective mixing of frazil crystals), while under, windy, rough conditions frazil ice production is enhanced (lots of convective mixing) leading to slush, grease ice, and pancake ice as  surface roughness increases.  New ice grows through a transition layer, then becoming young ice.  Categories of more mature ice (thicker than 30 cm.)  are not discussed in detail.

It is interesting to ponder how long each ice type can exist in nature, based on the thickness classifications as described by the WMO nomenclature system.  The surface energy balance can be used to investigate growth rates of ice of varying thicknesses.  Values for terms in the surface energy balance were taken from Maykut (1978) "Energy Exchange Over Young Sea Ice in the Central Arctic" . To come up with a range in growth rates, I calculated growth rates for both September and January, with hopes of capturing growth rates in early season when young ice first appears as well as growth rates during the depths of winter when they are at their maximum values.  A growth rate expression was taken from Carol Pease's 1987 paper "The Size of Wind-Driven Coastal Polynyas".
 

dH/dT= -[(1-a)Qr+Qld-Qlu+Qs+Qe]/rhoice*L

where

dH/dT=ice growth rate

(1-a)Qr= incoming shortwave radiation considering albedo

Qld=downward longwave radiation

Qlu=upward longwave radiation

Qs=sensible heat flux

Qe=latent heat of evaporation

rhoice=density of ice=0.95 X103 kg m-3

L=latent heat of fusion for saltwater=3.34 X 105 j kg-1

The results of the exercise are tabled below, giving a back of the envelope idea of how long one can expect various ice types to exist under conditions common to the arctic in both September and January.
 

Ice
thickness

Class

dH/dt

Existence time
(September)

Existence time
(January)

open water

frazil

0.01-0.23 m/d

~few days

hours to days

0.05 m

dark nilas
0-0.05 m

0.01-0.12 m/d

<5 days

<12 hours

0.10 m

light nilas
0.05-0.10 m

0.0075-0.175 m/d

<6.6 days

<7 hours

0.20 m

grey-white
0.10-0.30 m

0.005- 0.05 m/d

<40 days

<4 days

0.40 m

Thin first year
0.30-0.70 m

0.003-0.03 m/d

~130 days

~13 days

0.80 m

Med. first year
0.70- 1.2 m

0.001-0.02 m/d

~500 days

~25 days

3.0 m

multi-year

0.003-0.004 m/d

indefinite

indefinite

Ice type existence time from surface energy balance 

See References

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