Riming Growth of Hailstones
Consider a cylindrical hailstone of radius
falling with velocity
relative to the air. The air temperature is
and the liquid water density in the cloud is
.
Supercooled drops (originally at
) land on the hailstone
and freeze in two stages.
Stage 1: Ice is nucleated inside the drop. The drop temperature rises
to
(
K) as a result of partial freezing.
- Find
, the fraction of the drop that freezes without heat loss
to the hailstone or the air, in terms of
,
the latent heat of freezing/melting, and the specific heats of ice
and water
and
. (Note: dLf/dT = cw-ci:
Kirchoff's Law).
Stage 2: The rest of the drop freezes, losing heat via conduction
to the ice substrate and to the air, and losing latent heat via evaporation.
The following equation (Maclin and Payne (1967), QJRMS) uses five
terms to parameterize the heat balance at the hailstone surface.
where
is a numerical constant,
is the steady state
hailstone surface temperature,
the Reynolds number,
the Prandtl number, where
is the thermal diffusivity,
the Schmidt number which is approximately unity for air,
the
latent heat of evaporation, and
and
the densities of water vapor at the hailstone surface and the environment.
Assume
(note liquid vapor pressure)
and
(note ice vapor pressure),
where the mass of a water vapor molecule =
and the Boltzmann
constant =
- Explain in words the physical significance of each of the five terms
(three on the left and two on the right) in this equation.
- Find the relationship between
and
that produces
the transition from dry to wet growth
- Find the relationship between
and
that give the
transition between evaporation and vapor growth.