Answer to the Question 10/98
FALLING CLOUDS
The question was:
Clouds are made of water droplets, and water is about 800 times denser than
air. Why don't clouds fall like a rock to the ground?
(11/98) The problem has been solved with varying
degrees of accuracy and completness, by
Oren Melinger (e-mail
melinger@internet-zahav.net),
Kerry MacArthur (e-mail
MacArthu@firsttrust.com),
Dmitriji Podolsky from Ukraine,
and
William Chess (e-mail chess@kennett.net).
Short solution of the problem is presented below.
The answer: The clouds do fall, but they fall very slowly...
The solution:
A falling drop feels a frictional force
from the air's viscosity that opposes gravity (the
drop has to push its way through the air), the drop
reaches a constant terminal velocity, and this
terminal velocity is smaller the smaller the radius
of a fluid particle or ice crystal. It turns out that
this terminal velocity is quite small for drops the
size of a few millimeters and so, although the drops
in a cloud fall, they fall so slowly that only
careful measurements would reveal this fact.
More quantitatively we can say the following:
The weight of a drop of air of radius R is
4{pi}R3{rho}g/3
where {rho} is the density of the water
(=103 kg/m3,
and g (=9.8 m/sec2) free-fall acceleration.
If the drop is falling through air with velocity v, the viscosity
of the air n (=1.75*10-5 N*sec/m2)
will cause friction (Stokes law) 6{pi}nRv. [Here we neglect
the density of the air and assume that the viscosity of the drop is
much larger than viscosity of the air; we also asume that the drop
is approximately spherical.]
The terminal velocity of the falling drop is obtained by equating
the weight and the friction force, and is given by
v=2{rho}gR2/9n .
Thus 1 micron drop will have velocity of 0.13 mm/sec, or 11 m/day.
Larger, 10 micron drops will still fall slowly, - 1.1km/day.
Such fall rates can be neglected, especially since the motion of
the air itself can be faster than that.
Drops significantly smaller than 1 micron are not visible and will not
be percieved as clouds, while 0.1 mm drops will fall with velocity of
about 1 m/sec, i.e. it will rain. Larger drops will fall with even larger
velocities; however, the air-friction starts increasing faster than
than v, i.e. the velocity will not increase as fast with
increasing drop size. At such large speeds the weight of the drop is
balanced by the drag force
(1/2){rho}airC{pi}R2v2, where
{rho}air is the density of the air
(=1.2kg/m3) and C=1.2 is the
drag coefficient for sphere. According to this equation 1 mm drop will fall
with velocity of 4.3 m/sec and 10 mm drop will fall with velocity of
13.6 m/sec. However, drops larger than 5 mm are usually broken into smaller
drops that fall more slowly.
Comment 1: This problem is related to
the Milliken oil-drop experiment in which the
absolute magnitude of the electric charge was
measured for the first time.
Comment 2: There is a nice book that discusses
the question of
falling clouds and other meteorological phenomena:
W. E. Knowles Middleton, A History of the Theories of Rain and
Other Forms of Precipitation, Franklin Watts, Inc. (NY), 1965.
We thank Henry S. Greenside for his help in formulation
of this solution.
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