cirrostratus, may be observed in the lower stratosphere
above the polar tropopause, but mainly below the level
of the jetstream core. The cirrus clouds of the equatorial
zone also generally extend to the tropopause. There is
a general tendency for the mean height of the bases to
increase from high to low latitudes more or less
paralleling the mean tropopause height, ranging from
24,000 feet at 70°to 80°atitude to 35,000 to 4,000 feet
or higher in the vicinity of the equator. The thickness of
individual cirrus cloud layers are generally about 800
feet in the midlatitudes. The mean thickness of cirrus
clouds tends to increase from high to low latitudes. In
polar continental regions in winter, cirrus clouds are
virtually based at the surface. In the midlatitudes and in
the tropics, there is little seasonal variation.
Cirrus Clouds in Relation to the Jetstream
A discussion of cloud types associated with the
jetstream is contained in the AG2 TRAMAN, volume 1.
In addition to this information, we will discuss a few
studies pertaining to cloud types. All of these studies
agree that most of the more extensive and dense clouds
clouds are on the equatorward of the jet axis. The
observed frequency of high clouds poleward of the jet
axis can be accounted for as the upper reaches of a cold
front, or cold lows, not directly related to the jetstream.
In some parts of a trough, these high clouds may tend to
be dense, and in other areas thin.
PREDICTION OF SNOW
VS RAIN
LEARNING OBJECTIVES: Evaluate the
surface and upper-level synoptic situations in
determining the form of precipitation in your
forecast.
Typically, an inch or so of precipitation in the form
of rain will cause no serious inconvenience. On the
other hand the same amount of precipitation in the form
of snow, sleet, or freezing rain can seriously interfere
with naval operations. In such cases, the snow versus
rain problem may become a factor of operational
significance.
Sleet and freezing rain, which often may occur in
the intermediate period between snow and rain, are
generally grouped with snow in our discussion. Any
decision arrived at for the snow versus rain problem
would, naturally, have to be modified, dependant on
your geographical location. This should be easily
accomplished through a local study of the optimum
conditions. The various techniques and systems
presented here will often complement each other. The
approach used here is a discussion of the general
synoptic patterns and the thermal relationship; that is,
the use of temperatures at the surface and aloft, and the
presentation of an objective technique to distinguish the
types of precipitation.
GEOGRAPHICAL AND SEASONAL
CONSIDERATIONS
The forecasting problem of snow versus rain arises,
naturally, during the colder months of the year. In
midwinter when the problem is most serious in the
northern states, the southern states may not be
concerned.
PHYSICAL NATURE OF THE PROBLEM
The type of precipitation that reaches the ground in
a borderline situation is essentially dependent on two
conditions. There must be a stratum of above-freezing
temperatures between the ground and the level at which
precipitation is forming, and this stratum must be
sufficiently deep to melt all of the falling snow prior to
striking the surface. Thus, a correct prediction of rain
or snow at a given location depends largely on the
accuracy with which the vertical distribution of the
temperature, especially the height of the freezing level,
can be predicted.
On the average, it is generally
satisfactory to assume that the freezing level must be at
least 1,200 feet above the surface to ensure that most of
the snow will melt before reaching the surface.
Effects of Advection
In the lower troposphere, above the surface,
horizontal advection is usually the dominant factor
affecting local temperature changes. In most
precipitation situations, particularly in borderline
situations, warm air advection and upward motion are
occurring simultaneously, giving rise to the fact that
warming generally accompanies precipitation.
However, this effect is frequently offset when there is
weak warm advection, or even cold advection, in the
cold air mass in the lower layers.
In situations where precipitation is occurring in
association with a cold upper low, upward motion is
accompanied by little, if any, warm advection. In such
borderline cases, precipitation may persist as snow, or
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