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CHAPTER 35
TROPICAL CYCLONES
DESCRIPTION AND CAUSES
3500. Introduction
closed isobars and a distinct rotary circulation. The highest
sustained (1-minute mean) surface wind speed is 34 to 63
knots.
When fully developed, a
hurricane
or
typhoon
has
closed isobars, a strong and very pronounced rotary
circulation, and a sustained (1-minute mean) surface wind
speed of 64 knots or higher.
A
tropical cyclone
is a cyclone originating in the
tropics or subtropics. Although it generally resembles the
extratropical cyclone of higher latitudes, there are
important differences, the principal one being the concen-
tration of a large amount of energy into a relatively small
area. Tropical cyclones are infrequent in comparison with
middle and high latitude storms, but they have a record of
destruction far exceeding that of any other type of storm.
Because of their fury, and because they are predominantly
oceanic, they merit special attention by mariners.
A tropical storm may have a deceptively small size,
and beautiful weather may be experienced only a few
hundred miles from the center. The rapidity with which the
weather can deteriorate with approach of the storm, and the
violence
3502. Areas of Occurrence
Tropical cyclones occur almost entirely in six distinct
areas, four in the Northern Hemisphere and two in the
Southern Hemisphere, as shown in
Figure 3502.
The name
by which the tropical cyclone is commonly known varies
somewhat with the locality.
of
the
fully
developed
tropical
cyclone,
are
1.
North Atlantic. A tropical cyclone with winds of 64
knots or greater is called a
hurricane
.
difficult to imagine if they have not been experienced.
On his second voyage to the New World, Columbus
encountered a tropical storm. Although his vessels suffered
no damage, this experience proved valuable during his
fourth voyage when his ships were threatened by a fully
developed hurricane. Columbus read the signs of an
approaching storm from the appearance of a southeasterly
swell, the direction of the high cirrus clouds, and the hazy
appearance of the atmosphere. He directed his vessels to
shelter. The commander of another group, who did not heed
the signs, lost most of his ships and more than 500 men
perished.
2.
Eastern North Pacific. The name
hurricane
is used
as in the North Atlantic.
3.
Western North Pacific. A fully developed storm
with winds of 64 knots or greater is called a
typhoon
or, locally in the Philippines, a
baguio
.
4.
North Indian Ocean. A tropical cyclone with winds
of 34 knots or greater is called a
cyclonic storm
.
5.
South Indian Ocean. A tropical cyclone with winds
of 34 knots or greater is called a
cyclone
.
6.
Southwest Pacific and Australian Area. The name
cyclone
is used as in the South Indian Ocean. A
severe tropical cyclone originating in the Timor Sea
and moving southwest and then southeast across the
interior of northwestern Australia is called a
willy-
willy
.
3501. Definitions
Tropical cyclones are classified by form and intensity
as they increase in size.
A
tropical disturbance
is a discrete system of
apparently organized convection, generally 100 to 300
miles in diameter, having a nonfrontal migratory character,
and having maintained its identity for 24 hours or more. It
may or may not be associated with a detectable disturbance
of the wind field. It has no strong winds and no closed
isobars i.e., isobars that completely enclose the low.
At its next stage of development it becomes a
tropical
depression
. A tropical depression has one or more closed
isobars and some rotary circulation at the surface. The highest
sustained (1-minute mean) surface wind speed is 33 knots.
The next stage is
tropical storm
. A tropical storm has
Tropical cyclones have not been observed in the South
Atlantic or in the South Pacific east of 140
°
W.
3503. Origin, Season and Frequency
See
Figure 3503a
and
Figure 3503b
. Origin, season,
and frequency of occurrence of the tropical cyclones in the
six areas are as follows:
North Atlantic:
Tropical cyclones can affect the
entire North Atlantic Ocean in any month. However, they
are mostly a threat south of about 35
°
N from June through
November;
August,
September,
and
October
are
the
503
504
TROPICAL CYCLONES
Figure 3502. Areas in which tropical cyclones occur. The average number of tropical cyclones per 5˚ square has been
analyzed for this figure. The main season for intense tropical storm activity is also shown for each major basin.
months of highest incidence. See
Figure 3503b
. About 9
or 10 tropical cyclones (tropical storms and hurricanes)
form each season; 5 or 6 reach hurricane intensity (winds
of 64 knots and higher). A few hurricanes have generated
winds estimated as high as 200 knots. Early and late
season storms usually develop west of 50
September are the months of highest incidence. These
storms differ from their North Atlantic counterparts in that
they are usually smaller in size. However, they can be just
as intense.
Western North Pacific:
More tropical cyclones form
in the tropical western North Pacific than anywhere else in
the world. More than 25 tropical storms develop each year,
and about 18 become typhoons. These typhoons are the larg-
est and most intense tropical cyclones in the world. Each
year an average of five generate maximum winds over 130
knots; circulations covering more than 600 miles in diameter
are not uncommon. Most of these storms form east of the
Philippines, and move across the Pacific toward the Philip-
pines, Japan, and China; a few storms form in the South
China Sea. The season extends from April through Decem-
ber. However, tropical cyclones are more common in the
off-season months in this area than anywhere else. The peak
of the season is July through October, when nearly 70 per-
cent of all typhoons develop. There is a noticeable seasonal
shift in storm tracks in this region. From July through Sep-
tember, storms move north of the Philippines and recurve,
while early- and late-season typhoons move on a more west-
erly track through the Philippines before recurving.
W; during
August and September, this spawning ground extends to
the Cape Verde Islands. These storms usually move
westward or west northwestward at speeds of less than 15
knots in the lower latitudes. After moving into the
northern Caribbean or Greater Antilles regions, they
usually either move toward the Gulf of Mexico or recurve
and accelerate in the North Atlantic. Some will recurve
after reaching the Gulf of Mexico, while others will
continue westward to a landfall in Texas or Mexico.
Eastern North Pacific:
The season is from June
through October, although a storm can form in any month.
An average of 15 tropical cyclones form each year with
about 6 reaching hurricane strength. The most intense
storms are often the early- and late-season ones; these form
close to the coast and far south. Mid season storms form
anywhere
°
in
a
wide
band
from
the
Mexican-Central
American
coast
to
the
Hawaiian
Islands.
August
and
TROPICAL CYCLONES
505
Figure 3503a. Storm tracks.The width of the arrow indicates the approximate frequency of storms; the wider the arrow
the higher the frequency. Isolines on the base map show the resultant direction toward which storms moved. Data for the
entire year has been summarized for this figure.
AREA AND STAGE
JAN
FEB
MAR
APR
MAY
JUN
JUL
AUG
SEP
OCT
NOV
DEC
ANNUAL
NORTH ATLANTIC
TROPICAL STORMS
*
*
*
*
0.1
0.4
0.3
1.0
1.5
1.2
0.4
*
4.2
HURRICANES
*
*
*
*
*
0.3
0.4
1.5
2.7
1.3
0.3
*
5.2
TROPICAL STORMS AND HURRICANES
*
*
*
*
0.2
0.7
0.8
2.5
4.3
2.5
0.7
0.1
9.4
JAN
FEB
MAR
APR
MAY
JUN
JUL
AUG
SEP
OCT
NOV
DEC
ANNUAL
EASTERN NORTH PACIFIC
TROPICAL STORMS
*
*
*
*
*
1.5
2.8
2.3
2.3
1.2
0.3
*
9.3
HURRICANES
*
*
*
*
0.3
0.6
0.9
2.0
1.8
1.0
*
*
5.8
TROPICAL STORMS AND HURRICANES
*
*
*
*
0.3
2.0
3.6
4.5
4.1
2.2
0.3
*
15.2
JAN
FEB
MAR
APR
MAY
JUN
JUL
AUG
SEP
OCT
NOV
DEC
ANNUAL
WESTERN NORTH PACIFIC
TROPICAL STORMS
0.2
0.3
0.3
0.2
0.4
0.5
1.2
1.8
1.5
1.0
0.8
0.6
7.5
TYPHOONS
0.3
0.2
0.2
0.7
0.9
1.2
2.7
4.0
4.1
3.3
2.1
0.7
17.8
TROPICAL STORMS AND TYPHOONS
0.4
0.4
0.5
0.9
1.3
1.8
3.9
5.8
5.6
4.3
2.9
1.3
25.3
JAN
FEB
MAR
APR
MAY
JUN
JUL
AUG
SEP
OCT
NOV
DEC
ANNUAL
SOUTHWEST PACIFIC AND AUSTRALIAN AREA
TROPICAL STORMS
2.7
2.8
2.4
1.3
0.3
0.2
*
*
*
0.1
0.4
1.5
10.9
HURRICANES
0.7
1.1
1.3
0.3
*
*
0.1
0.1
*
*
0.3
0.5
3.8
TROPICAL STORMS AND HURRICANES
3.4
4.1
3.7
1.7
0.3
0.2
0.1
0.1
*
0.1
0.7
2.0
14.8
JAN
FEB
MAR
APR
MAY
JUN
JUL
AUG
SEP
OCT
NOV
DEC
ANNUAL
SOUTHWEST INDIAN OCEAN
TROPICAL STORMS
2.0
2.2
1.7
0.6
0.2
*
*
*
*
0.3
0.3
0.8
7.4
HURRICANES
1.3
1.1
0.8
0.4
*
*
*
*
*
*
*
0.5
3.8
TROPICAL STORMS AND HURRICANES
3.2
3.3
2.5
1.1
0.2
*
*
*
*
0.3
0.4
1.4
11.2
1
Winds
* Less than 0.05
48 Kts.
Monthly values cannot be combined because single storms overlapping two months were counted once in each month and once in the annual.
³
Figure 3503b. Monthly and annual average number of storms per year for each area.
506
TROPICAL CYCLONES
AREA AND STAGE
JAN
FEB
MAR
APR
MAY
JUN
JUL
AUG
SEP
OCT
NOV
DEC
ANNUAL
NORTH INDIAN OCEAN
TROPICAL STORMS
0.1
*
*
0.1
0.3
0.5
0.5
0.4
0.4
0.6
0.5
0.3
3.5
CYCLONES
1
*
*
*
0.1
0.5
0.2
0.1
*
0.1
0.4
0.6
0.2
2.2
0.1
*
0.1
0.3
0.7
0.7
0.6
0.4
0.5
1.0
1.1
0.5
5.7
TROPICAL STORMS AND CYCLONES
1
1
Winds
* Less than 0.05
48 Kts.
Monthly values cannot be combined because single storms overlapping two months were counted once in each month and once in the annual.
³
Figure 3503b. Monthly and annual average number of storms per year for each area.
North Indian Ocean—
Tropical cyclones develop in
the Bay of Bengal and Arabian Sea during the spring and
fall. Tropical cyclones in this area form between latitudes
8
(tropical storms and hurricanes) form each season, and
about 4 reach hurricane intensity. The season is from
December through March, although it is possible for a
storm to form in any month. Tropical cyclones in this
region
N, except from June through September, when
the little activity that does occur is confined north of about
15
°
N and 15
°
usually
form
south
of
10
°
S.
The
latitude
of
N. These storms are usually short-lived and weak;
however, winds of 130 knots have been encountered. They
often develop as disturbances along the Intertropical
Convergence Zone (ITCZ); this inhibits summertime
development, since the ITCZ is usually over land during
this monsoon season. However, it is sometimes displaced
southward, and when this occurs, storms will form over the
monsoon-flooded plains of Bengal. On the average, six
cyclonic storms form each year. These include two storms
that generate winds of 48 knots or greater. Another 10
tropical cyclones never develop beyond tropical
depressions. The Bay of Bengal is the area of highest
incidence. However, it is not unusual for a storm to move
across southern India and reintensify in the Arabian Sea.
This is particularly true during October, the month of
highest incidence during the tropical cyclone season. It is
also during this period that torrential rains from these
storms, dumped over already rain-soaked areas, cause
disastrous floods.
South Indian Ocean—
Over the waters west of 100
°
recurvature usually migrates from about 20
°
S in January to
around 15
S, these storms
sometimes become intense extratropical lows.
Southwest Pacific and Australian Area—
These
tropical waters spawn an annual average of 15 tropical
cyclones 4, of which reach hurricane intensity. The season
extends from about December through April, although
storms can form in any month. Activity is widespread in
January and February, and it is in these months that
tropical cyclones are most likely to affect Fiji, Samoa, and
the other eastern islands. Tropical cyclones usually form
in the waters from 105
°
S in April. After crossing 30
°
S.
Storms affecting northern and western Australia often
develop in the Timor or Arafura Sea, while those that
affect the east coast form in the Coral Sea. These storms
are often small, but can develop winds in excess of 130
knots. New Zealand is sometimes reached by decaying
Coral Sea storms, and occasionally by an intense
hurricane. In general, tropical cyclones in this region
move southwestward and then recurve southeastward.
°
E to 160
°
W, between 5
°
and 20
°
E,
to the east African coast, an average of 11 tropical cyclones
°
ANATOMY OF TROPICAL CYCLONES
3504. Formation
conditions needed to generate hurricane circulation, and the
relationships between large- and small-scale atmospheric
processes. But scientists today, treating the hurricane sys-
tem
Hurricane formation was once believed to result from
an intensification of convective forces which produce the
towering cumulonimbus clouds of the doldrums. This view
of hurricane generation held that surface heating caused
warm moist air to ascend convectively to levels where
condensation produced cumulonimbus clouds, which, after
an inexplicable drop in atmospheric pressure, coalesced
and were spun into a cyclonic motion by Coriolis force.
This hypothesis left much unexplained. Although some
hurricanes develop from disturbances beginning in the dol-
drums, very few reach maturity in that region. Also, the high
incidence of seemingly ideal convective situations does not
match the low incidence of Atlantic hurricanes. Finally, the
hypothesis did not explain the drop in atmospheric pressure,
so essential to development of hurricane-force winds.
There is still no exact understanding of the triggering
mechanism involved in hurricane generation, the balance of
as
an
atmospheric
heat
engine,
present
a
more
comprehensive and convincing view.
They begin with a starter mechanism in which either
internal or external forces intensify the initial disturbance.
The initial disturbance becomes a region into which low-
level air from the surrounding area begins to flow,
accelerating the convection already occurring inside the
disturbance. The vertical circulation becomes increasingly
well organized as water vapor in the ascending moist layer
is condensed (releasing large amounts of heat energy to
drive the wind system), and as the system is swept into a
counterclockwise cyclonic spiral. But this incipient
hurricane would soon fill up because of inflow at lower
levels, unless the chimney in which converging air surges
upward is provided the exhaust mechanism of high-altitude
winds.
TROPICAL CYCLONES
507
Figure 3504. Pumping action of high-altitude winds.
These high-altitude winds pump ascending air out of
the cyclonic system, into a high-altitude anticyclone, which
transports the air well away from the disturbance, before
sinking occurs. See
Figure 3504
. Thus, a large scale vertical
circulation is set up, in which low-level air is spiraled up the
cyclonic twisting of the disturbance, and, after a trajectory
over the sea, returned to lower altitudes some distance from
the storm. This pumping action-and the heat released by the
ascending air may account for the sudden drop of
atmospheric pressure at the surface, which produces the
steep pressure gradient along which winds reach hurricane
proportions.
It is believed that the interaction of low-level and high-
altitude wind systems determines the intensity the hurricane
will attain. If less air is pumped out than converges at low
levels, the system will fill and die out. If more is pumped out
than flows in, the circulation will be sustained and will
intensify.
Scientists have found that any process which increases
the rate of low-level inflow is favorable for hurricane
development, provided the inflowing air carries sufficient
heat and moisture to fuel the hurricane’s power system. It has
also been shown that air above the developing disturbance, at
altitudes between 20,000 and 40,000 feet, increases 1
3505. Portrait of a Hurricane
In the early life of the hurricane, the spiral covers an
area averaging 100 miles in diameter with winds of 64
knots and greater, and spreads gale-force winds over a 400-
mile diameter. The cyclonic spiral is marked by heavy
cloud bands from which torrential rains fall, separated by
areas of light rain or no rain at all. These spiral bands
ascend in decks of cumulus and cumulonimbus clouds to
the convective limit of cloud formation, where condensing
water vapor is swept off as ice-crystal wisps of cirrus
clouds. See
Figure 3505
. Thunderstorm electrical activity is
observed in these bands, both as lightning and as tiny
electrostatic discharges.
In the lower few thousand feet, air flows in through the cy-
clone, and is drawn upward through ascending columns of air
near the center. The size and intensity decrease with altitude,
the cyclonic circulation being gradually replaced above 40,000
feet by an anticyclonic circulation centered hundreds of miles
away, which is the exhaust system of the hurricane heat engine.
At lower levels, where the hurricane is more intense,
winds on the rim of the storm follow a wide pattern, like the
slower currents around the edge of a whirlpool; and, like
those currents, these winds accelerate as they approach the
center of the vortex. The outer band has light winds at the
rim of the storm, perhaps no more than 25 knots; within 30
miles of the center, winds may have velocities exceeding
130 knots. The inner band is the region of maximum wind
velocity, where the storm’s worst winds are felt, and where
ascending air is chimneyed upward, releasing heat to drive
the storm. In most hurricanes, these winds reach 85 knots,
and more than 170 knots in severe storms.
In the hurricane, winds flow toward the low pressure in
the warm, comparatively calm core. There, converging air
is whirled upward by convection, the mechanical thrusting
of other converging air, and the pumping action of high-
altitude circulations. This spiral is marked by the thick
F
in temperature about 24 hours before the disturbance
develops into a hurricane. But it is not known whether low-
level inflow and high-level warming cause hurricanes. They
could very well be measurable symptoms of another effect
which actually triggers the storm’s increase to hurricane
intensity.
The view of hurricanes as atmospheric engines is
necessarily a general one. The exact role of each contributor
is not completely understood. The engine seems to be both
inefficient and unreliable; a myriad of delicate conditions
must be satisfied for the atmosphere to produce a hurricane.
Their relative infrequency indicates that many potential
hurricanes dissipate before developing into storms.
°
to 3
°
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