A polar vortex is an upper-level low-pressure area lying near one of the Earth's poles. There are two polar vortices in the Earth's atmosphere, overlying the North and South Poles. Each polar vortex is a persistent, large-scale,
low-pressure zone less than 1,000 kilometers (620 miles) in diameter,
that rotates counter-clockwise at the North Pole and clockwise at the
South Pole (called a cyclone
in both cases), i.e., both polar vortices rotate eastward around the
poles. As with other cyclones, their rotation is driven by the Coriolis effect. The bases of the two polar vortices are located in the middle and upper troposphere and extend into the stratosphere. Beneath that lies a large mass of cold, dense Arctic air.
The interface between the cold dry air mass of the pole and the
warm moist air mass farther south defines the location of the polar
front. The polar front is centered, roughly at 60° latitude. A polar
vortex strengthens in the winter and weakens in the summer because of
its dependence on the temperature difference between the equator and the
poles.
The vortices weaken and strengthen from year to year. When the
vortex of the Arctic is strong, it is well defined, there is a single
vortex, and the Arctic air is well contained; when weaker, which it
generally is, it will break into two or more vortices; when very weak,
the flow of Arctic air becomes more disorganized, and masses of cold
Arctic air can push equatorward, bringing with them a rapid and sharp
temperature drop. When the polar vortex is strong, there is a single
vortex with a jet stream
that is "well constrained" near the polar front. When the northern
vortex weakens, it separates into two or more vortices, the strongest of
which are near Baffin Island, Canada, and the other over northeast Siberia.
The Antarctic vortex of the Southern Hemisphere is a single low-pressure zone that is found near the edge of the Ross ice shelf, near 160 west longitude. When the polar vortex is strong, the mid-latitude Westerlies
(winds at the surface level between 30° and 60° latitude from the west)
increase in strength and are persistent. When the polar vortex is weak,
high-pressure zones of the mid-latitudes may push poleward, moving the
polar vortex, jet stream,
and polar front equatorward. The jet stream is seen to "buckle" and
deviate south. This rapidly brings cold dry air into contact with the
warm, moist air of the mid-latitudes, resulting in a rapid and dramatic
change of weather known as a "cold snap".
Ozone depletion occurs within the polar vortices – particularly over the Southern Hemisphere – reaching a maximum depletion in the spring.
History
The polar vortex was first described as early as 1853. The phenomenon's sudden stratospheric warming (SSW) develops during the winter in the Northern Hemisphere and was discovered in 1952 with radiosonde observations at altitudes higher than 20 km.
The phenomenon was mentioned frequently in the news and weather media in the cold North American winter of 2013–2014, popularizing the term as an explanation of very cold temperatures.[6]
A deep freeze
that gripped much of the United States and Canada in late January 2019
has been blamed on a polar vortex. The US National Weather Service
warned that frostbite is possible within just 10 minutes of being
outside in such extreme temperatures, and hundreds of schools, colleges
and universities in the affected areas were closed. Around 21 people
died in US due to severe frostbite. States within the midwest region of the United States had windchills just above -50°F (-45°C), which is colder than the frozen tundra and Antarctica.
The Polar vortex has also thought to have had effects in Europe. For example, the 2013–14 United Kingdom winter floods were blamed on the Polar vortex bringing severe cold in the United States and Canada. Similarly, the severe, brutal cold in the United Kingdom in the winters of 2009/10 and 2010/11 were also blamed on the Polar vortex.
Identification
Polar
cyclones are low-pressure zones embedded within the polar air masses,
and exist year-round. The stratospheric polar vortex develops at
latitudes above the subtropical jet stream. Horizontally, most polar vortices have a radius of less than 1,000 kilometres (620 mi). Since polar vortices exist from the stratosphere downward into the mid-troposphere,
a variety of heights/pressure levels are used to mark its position. The
50 mb pressure surface is most often used to identify its stratospheric
location. At the level of the tropopause, the extent of closed contours of potential temperature
can be used to determine its strength. Others have used levels down to
the 500 hPa pressure level (about 5,460 metres (17,910 ft) above sea
level during the winter) to identify the polar vortex.
Duration and power
Polar vortices are weakest during summer and strongest during winter. Extratropical cyclones that migrate into higher latitudes when the polar vortex is weak can disrupt the single vortex creating smaller vortices (cold-core lows) within the polar air mass. Those individual vortices can persist for more than a month.
Volcanic eruptions in the tropics can lead to a stronger polar vortex during winter for as long as two years afterwards. The strength and position of the polar vortex shapes the flow pattern in a broad area about it. An index which is used in the northern hemisphere to gauge its magnitude is the Arctic oscillation.
When the Arctic vortex is at its strongest, there is a single
vortex, but normally, the Arctic vortex is elongated in shape, with two
cyclone centers, one over Baffin Island in Canada and the other over northeast Siberia.
When the Arctic pattern is at its weakest, subtropic air masses can
intrude poleward causing the Arctic air masses to move equatorward, as
during the Winter 1985 Arctic outbreak. The Antarctic polar vortex is more pronounced and persistent than the Arctic one. In the Arctic the distribution of land masses at high latitudes in the Northern Hemisphere gives rise to Rossby waves
which contribute to the breakdown of the polar vortex, whereas in the
Southern Hemisphere the vortex is less disturbed. The breakdown of the
polar vortex is an extreme event known as a sudden stratospheric warming, here the vortex completely breaks down and an associated warming of 30–50 °C (54–90 °F) over a few days can occur.
The waxing and waning of the polar vortex is driven by the
movement of mass and the transfer of heat in the polar region. In the
autumn, the circumpolar winds increase in speed and the polar vortex rises into the stratosphere.
The result is that the polar air forms a coherent rotating air mass:
the polar vortex. As winter approaches, the vortex core cools, the winds
decrease, and the vortex energy declines. Once late winter and early
spring approach the vortex is at its weakest. As a result, during late
winter, large fragments of the vortex air can be diverted into lower
latitudes by stronger weather systems intruding from those latitudes. In
the lowest level of the stratosphere, strong potential vorticity
gradients remain, and the majority of that air remains confined within
the polar air mass into December in the Southern Hemisphere and April in
the Northern Hemisphere, well after the breakup of the vortex in the
mid-stratosphere.
The breakup of the northern polar vortex occurs between mid March
to mid May. This event signifies the transition from winter to spring,
and has impacts on the hydrological cycle,
growing seasons of vegetation, and overall ecosystem productivity. The
timing of the transition also influences changes in sea ice, ozone, air
temperature, and cloudiness. Early and late polar breakup episodes have
occurred, due to variations in the stratospheric flow structure and
upward spreading of planetary waves from the troposphere.
As a result of increased waves into the vortex, the vortex experiences
more rapid warming than normal, resulting in an earlier breakup and
spring. When the breakup comes early, it is characterized by
with persistent of remnants of the vortex. When the breakup is late,
the remnants dissipate rapidly. When the breakup is early, there is one
warming period from late February to middle March. When the breakup is
late, there are two warming periods, one January, and one in March.
Zonal mean temperature, wind, and geopotential
height exert varying deviations from their normal values before and
after early breakups, while the deviations remain constant before and
after late breakups. Scientists are connecting a delay in the Arctic
vortex breakup with a reduction of planetary wave activities, few
stratospheric sudden warming events, and depletion of ozone.
Sudden stratospheric warming
events are associated with weaker polar vortices. This warming of
stratospheric air can reverse the circulation in the Arctic Polar Vortex
from counter-clockwise to clockwise. These changes aloft force changes in the troposphere below.
An example of an effect on the troposphere is the change in speed of
the Atlantic Ocean circulation pattern. A soft spot just south of
Greenland is where the initial step of downwelling
occurs, nicknamed the "Achilles Heel of the North Atlantic". Small
amounts of heating or cooling traveling from the polar vortex can
trigger or delay downwelling, altering the Gulf Stream Current
of the Atlantic, and the speed of other ocean currents. Since all other
oceans depend on the Atlantic Ocean's movement of heat energy, climates
across the planet can be dramatically affected. The weakening or
strengthening of the polar vortex can alter the sea circulation more
than a mile beneath the waves. Strengthening storm systems within the troposphere that cool the poles, intensify the polar vortex. La Niña–related climate anomalies significantly strengthen the polar vortex.
Intensification of the polar vortex produces changes in relative
humidity as downward intrusions of dry, stratospheric air enter the
vortex core. With a strengthening of the vortex comes a longwave
cooling due to a decrease in water vapor concentration near the vortex.
The decreased water content is a result of a lower tropopause within the vortex, which places dry stratospheric air above moist tropospheric air. Instability is caused when the vortex tube, the line of concentrated vorticity,
is displaced. When this occurs, the vortex rings become more unstable
and prone to shifting by planetary waves. The planetary wave activity in
both hemispheres varies year-to-year, producing a corresponding
response in the strength and temperature of the polar vortex.
The number of waves around the perimeter of the vortex are related to
the core size; as the vortex core decreases, the number of waves
increase.
The degree of the mixing of polar and mid-latitude air depends on the evolution and position of the polar night jet.
In general, the mixing is less inside the vortex than outside. Mixing
occurs with unstable planetary waves that are characteristic of the
middle and upper stratosphere in winter. Prior to vortex breakdown,
there is little transport of air out of the Arctic Polar Vortex due to
strong barriers above 420 km (261 miles). The polar night jet which
exists below this, is weak in the early winter. As a result, it does not
deviate any descending polar air, which then mixes with air in the
mid-latitudes. In the late winter, air parcels do not descend as much,
reducing mixing. After the vortex is broken up, the ex-vortex air is dispersed into the middle latitudes within a month.
Sometimes, a mass of the polar vortex breaks off before the end
of the final warming period. If large enough, the piece can move into
Canada and the Midwestern, Central, Southern, and Northeastern United
States. This diversion of the polar vortex can occur due to the
displacement of the polar jet stream; for example, the significant
northwestward direction of the polar jet stream in the western part of
the United States during the winters of 2013–2014, and 2014–2015. This
caused warm, dry conditions in the west, and cold, snowy conditions in
the north-central and northeast.
Occasionally, the high-pressure air mass, called the Greenland Block,
can cause the polar vortex to divert to the south, rather than follow
its normal path over the North Atlantic.