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Winds
Meteorology · Chapter 10

Winds

Describing the wind

6 min read
Written from Joshi 6, Winds, terms and measurement Oxford Vol 9, 10, Introduction to Measurement of Winds

Wind is air in horizontal motion. A wind velocity has two parts, a direction and a speed, and there are a handful of terms for how it varies that the exam expects you to have straight.

Direction and speed

  • Wind direction is the direction the wind blows from, given in degrees true, except that ATC gives it in degrees magnetic.
  • Speed is usually in knots. Some countries use metres per second, and the Met Office often works in km/h.
  • Veering is a change of direction clockwise. Backing is a change anticlockwise. Both terms mean the same thing in both hemispheres.

Sudden changes

TermWhat it is
GustA brief increase, under a minute, local. Reported only if 10 kt or more above the mean
LullA brief decrease
SquallAn increase lasting a minute or more, over a wide area, often with cumulonimbus and cold fronts
GaleSustained wind over 33 kt, or gusts over 42 kt, and Joshi ties it to a depression
Hurricane forceSustained wind over 63 kt

Measurement

Surface wind is read from a wind vane for direction and a cup anemometer for speed. The ICAO standard position is 10 m, about 33 ft, above aerodrome level, clear of buildings. Upper winds come from tracking a radiosonde and from aircraft reports. Lines of equal wind speed on a chart are isotachs.

The geostrophic wind, pressure gradient and Coriolis

7 min read
Written from Joshi 6, Coriolis and Geostrophic Wind Oxford Vol 9, 10, PGF, Coriolis Force, Geostrophic Wind

Above the friction layer the wind is close to a simple balance of just two forces. Get that balance and you can read both the direction and the speed of the wind straight off a pressure chart.

Pressure gradient force

The pressure gradient force acts from high pressure straight to low pressure, at right angles to the isobars. Its size is shown by the isobar spacing: close isobars, strong force, strong wind. Wind speed is directly proportional to the PGF.

Coriolis force

The Coriolis force is the apparent deflection caused by the earth's rotation. It acts at 90° to the wind, turning it to the right in the Northern Hemisphere and to the left in the Southern.

Exam wording Coriolis force is proportional to wind speed and to the sine of the latitude. It is greatest at the poles and near zero at the equator.

The geostrophic wind

The geostrophic wind is the balance of PGF against Coriolis only. It blows parallel to straight isobars, above the friction layer, at latitudes greater than about 15°, when the pressure pattern is not changing fast. Buys Ballot still holds: back to the wind in the Northern Hemisphere, low pressure on your left.

The latitude effect that is examined For the same isobar spacing, a higher latitude has a larger sine, so the Coriolis force balances the PGF at a lower wind speed. So the same spacing gives a faster geostrophic wind at low latitude. Near the equator the balance fails entirely.
Interactive The geostrophic balance
Pressure gradientModerate
Latitude45°
Geostrophic windabout 30 kt
Same spacing, higher latitudeSlower wind
The pressure gradient force points from the high isobar to the low one. Coriolis turns the flow until it runs along the isobars with the two forces opposed. Squeeze the isobars for a stronger wind. Raise the latitude and the same spacing gives a lighter wind.

The gradient wind and the surface wind

7 min read
Written from Joshi 6, Gradient Wind and friction effects Oxford Vol 9, 10, The Gradient Wind to Diurnal Variation

Real isobars curve, and near the ground friction gets in the way. Both change the wind from the plain geostrophic value.

The gradient wind

When isobars are curved, a third force, the centrifugal force, joins the PGF and Coriolis. The gradient wind is the balance of all three, blowing parallel to the curved isobars.

SystemCentrifugal forceGradient wind vs geostrophic
Depression, cyclonicOpposes the PGFSlower than geostrophic. The geostrophic wind scale over reads
AnticycloneAdds to the PGFFaster than geostrophic. The geostrophic wind scale under reads

The surface wind

Below about 2000 to 3000 ft, surface friction slows the wind. A slower wind means a weaker Coriolis force, so the PGF wins and the wind is pulled across the isobars, towards the low.

The rough rules, Northern Hemisphere Over land: surface wind is backed about 30° from the 2000 ft wind and its speed is about 50 per cent. Over sea: backed about 10°, speed about 70 per cent. In the Southern Hemisphere the surface wind is veered instead, same numbers.

Diurnal variation

By day, thermal mixing couples the surface to the stronger air above, so the surface wind veers and increases, peaking about 1500. By night the mixing stops, the surface wind backs and decreases, and the 1500 ft wind does the opposite, so a windshear develops between 1500 ft and the surface at night, which matters on an approach. Over the sea the daily change is small.

Local winds

7 min read
Written from Joshi 6, land and sea breeze, katabatic, anabatic, Fohn Oxford Vol 9, 10, Land and Sea Breezes to Fohn Winds

Small scale winds set up by local heating and terrain. They are too small for the Coriolis force to matter, so they do not obey Buys Ballot's law.

Land and sea breezes

Sea breezeLand breeze
WhenDay, land warmer than seaNight, land cooler than sea
DirectionFrom sea to landFrom land to sea
Strength, reachAbout 10 kt, 8 to 14 NM inland, more in the tropicsAbout 5 kt, about 5 NM offshore

The sea breeze veers with time under the Coriolis force. Practical effects at a coastal aerodrome: the landing direction can reverse between the two breezes, sea fog can be carried inland by day, and small clouds mark the sea breeze front over the coast.

Slope winds

  • Katabatic. Cold, dense air draining down a slope, mainly at night. About 10 kt, strongest with snow cover, a clear sky and a slack pressure gradient. It feeds valley frost and fog and leaves an inversion. Example: the Bora of the northern Adriatic.
  • Anabatic. Air warmed on a sunlit slope rising up the hill by day. A light wind, about 5 kt, weaker than the katabatic.

The Fohn wind

A warm, dry wind on the lee side of a mountain range. Moist air is forced up the windward side, cooling at the DALR then the SALR once saturated, and rains out, so its dew point falls. On the lee side it descends and warms at the DALR over a greater height than it cooled at the SALR going up. The result is a lee side base temperature much higher than the windward side, gains over 10°C are common.

The two sides Windward: cloud and precipitation. Lee: clear, warm, turbulent, and a Fohn can be a sign of mountain waves. The Chinook, lee of the Rockies, and the Zonda, lee of the Andes, are the same wind.
Interactive The Fohn effect across a ridge
Cloud base, windward2 000 ft
Temperature at the ridge1 °C
Temperature, lee ground25 °C
Net gain across the range+9 °C
Windward ground air starts at 16°C, dew point 10°C. It cools at 3°C per 1000 ft to the condensation level, then at 1.5°C per 1000 ft to the ridge, raining out its moisture. On the lee side it descends dry, warming at 3°C per 1000 ft the whole way, and arrives warmer than it left.