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050 02 00 00 WIND
050 02 01 00 Definition and measurement of wind
050 02 01 01 Definition and measurement
(01) Define ‘wind’ and ‘surface wind’.(02) State the units of wind directions (degrees true in reports; degrees magnetic from tower) and speed (kt, m/s).
(03) Describe that the reported wind is an average wind derived from measurements with an anemometer at a height of 10 m over 2 min for local routine and special reports and ATS units, and over 10 min for aerodrome routine meteorological reports (METARs) and aerodrome special meteorological reports (SPECIs).
050 02 02 00 Primary cause of wind
050 02 02 01 Primary cause of wind, pressure gradient, Coriolis force, gradient wind
When there is a pressure differential, a force is exists from high to low pressure. It acts at right angles to the isobars.
The formula is:
Coriolis Force = 2 Ω ρ V sin θ
Ω = Angular rotation of the Earth
ρ = Density
V = Wind speed
θ = Latitude
It is proportional to both wind speed and latitude. At the equator sin 0° = 0 and therefore no Coriolis force there. Equally, there is no Coriolis force when the wind velocity is zero. Anything multiplied by zero is of course….
(04) Explain the development of the geostrophic wind.
The geostrophic wind blows parallel to the isobars when the pressure gradient force and Coriolis for are in balance.
(05) Indicate how the geostrophic wind flows in relation to the isobars/isohypses in the northern and in the southern hemisphere.
(06) Analyse the effect of changing latitude on the geostrophic wind speed.
With little or no Coriolis force at the equator (only really with high winds) it is all PGF. Between 10° latitude, the geostrophic scale does not work. This is the same when the isobars are very close, PFG is much more than Coriolis.
(07) Explain the gradient wind effect and indicate how the gradient wind differs from the geostrophic wind in cyclonic
and anticyclonic circulation.
There is additional centrifugal force when flowing around curved isobars. The gradient wind is the geostrophic wind modified by the centrifugal force. This opposes the PGF around a low reducing wind speed which in turn reduces the Coriolis effect thereby reducing total wind speed. Around a high the centrifugal force now compliments the PGF which increases Coriolis and therefore total wind speed.
050 02 02 02 Variation of wind in the friction layer
(01) Describe why and how the wind changes direction and speed with height in the friction layer in the northern and in the southern hemisphere (rule of thumb).Slack and back – northern hemisphere
Slack and veer – Southern hemisphere
Due to surface friction the wind at the surface slows down and therefore reduces the Coriolis effect.
(02) State the surface and air-mass conditions that influence the wind in the friction layer (diurnal variation).
The diurnal temperature change affects the surface wind.
Rising thermal currents during the day mix with the faster upper layers thereby increasing surface wind.
During the cooler night the upwards currents are less, no mixing, slower wind.
(03) Name terrain, wind speed and stability as the main factors that influence the vertical extent of the friction layer.
Ok
(04) Explain the relationship between isobars and wind (direction and speed).
Geostrophic wind scale.
Remark: Approximate value for variation of wind in the friction layer (values to be used in examinations) Type of landscape Wind speed in friction layer in % of the geostrophic wind The wind in the friction layer blows across the isobars towards the low pressure. Angle between wind direction and isobars.
over water ca 70 % ca 10°
over land ca 50 % ca 30°
WMO No 266
050 02 02 03 Effects of convergence and divergence
(01) Describe atmospheric convergence and divergence.
Convergence – mostly caused by rising or sinking air drawing in air from either side, i.e bottom of a low and the top of a high.
(02) Explain the relationship between convergence and divergence on the following: pressure systems at the surface and aloft; wind speed; vertical motion and cloud formation (relationship between upper-air conditions and surface pressure systems).
Convergence at the surface and divergence aloft create low pressure areas and cause air to rise, possibly creating clouds and rain and all the things convection brings us. It can be quite strong, increasing PGF and therefore wind.
Divergence at the surface and convergence aloft creates high pressure, dispersing clouds and rain, and conversely can calm the wind down.
050 02 03 00 General global circulation
050 02 03 01 General circulation around the globe
Drives global weather patterns. Heating at the equator causes rising air and spreads out when it his the isothermal bit at the tropopause. Coriolis makes it head north in the north and south in the south before it cools and sinks – these are the Hadley cells. At the surface, some air returns round the Hadley and some goes the other way into the Ferrel cell. This happens again and forms the polar cell.
(02) Name and sketch or indicate on a map the global distribution of the surface pressure and the resulting wind pattern for all latitudes at low level in January and July.
It goes low high low high, between the cells. The low pressure area created at the equator is a strong area of convergence, the ITCZ, then there is the sub-tropical highs at the next convergence zone, then the traveling lows (the polar front depressions).
The surface wind blowing into the ITCZ are the trade winds. NE in the northern and SE in the southern Hemisphere.
As the equator moves with the seasons, so do the cells and their pressure patterns.
(03) Sketch or indicate on a map the westerly and easterly tropospheric winds at high level in January and July.
I think this is referring to jet streams, the strongest jet stream is the polar jet because of the largest temperature differential.
Starting from the equator or rather, at the equator there is the Tropical easterly jet (seasonal).
Next, north and south is the sub tropical westerly jets (permanent). Move with the heat equator. (Stronger in winter)
Then the westerly polar front jets, then; arctic front jet (seasonal)
050 02 04 00 Local winds
050 02 04 01 Anabatic and katabatic winds, mountain and valley winds, Venturi effects, land and sea breezes
(01) Describe and explain anabatic and katabatic winds.
Anabatic flows up terrain, caused by heating. Good for thermals and connective fluffy clouds.
Katabatic flows down. Caused by cooling, can cause fog and a temperature inversion above
(02) Describe mountain and valley winds.
Very local, some given names because the always exist.
(03) Describe the Venturi effect, convergence in valleys and mountain areas.
When the wind is constricted by a valley is speeds the air flow and wind up…
(04) Describe land and sea breezes, and sea-breeze front.
Temperature differential between land and sea which reverses during the night.
Sea breezes during the day – from sea to land.
Land breeze during the night – from land to sea, generally weaker.
(05) Describe that local, low-level jet streams can develop in the evening.
The same principle as high jet streams. A low level inversion at night acts like a low tropopause where the high level jets sit.
050 02 05 00 Mountain waves (standing waves, lee waves)
050 02 05 01 Origin and characteristics
(01) Explain the origin and formation of mountain waves.
(02) State the conditions necessary for the formation of mountain waves.
Wind speed at mountain height >15-20 its increasing with height.
Wind direction within 30° of the perpendicular to the mountain range.
Marked stability, an inversion or isothermal layer so the wind doesn’t keep ascending.
(03) Describe the structure and properties of mountain waves.
(04) Explain how mountain waves may be identified by their associated meteorological phenomena.
Cap clouds over the mountain, lenticular clouds and rotor clouds.
(05) Describe that mountain wave effects can exceed the performance or structural capability of aircraft.
(06) Describe that mountain wave effects can propagate from low to high level, e.g. over Greenland and elsewhere.
050 02 06 00 Turbulence
050 02 06 01 Description and types of turbulence
(01) Describe turbulence and gustiness.
Turbulence: Disturbed air which causes a sudden change of speed and direction, generally affects altitude not altitude, of course if a different attitude remains altitude will change.
Gust: Increase in windspeed, can change in direction. Short lived and over a small area.
(02) List the common types of turbulence (convective, mechanical, orographic, frontal, clear-air turbulence).
050 02 06 02 Formation and location of turbulence
(01) Explain the formation of convective turbulence, mechanical and orographic turbulence, and frontal turbulence.Convective: An area of convection restricts the horizontal flow of the wind creating turbulence on the other side – similar to a physical object in the way.
Mechanical: mountains, buildings, any large enough solid object.
Orographic: Same I think.
(02) State where turbulence will normally be found (rough- ground surfaces, relief, inversion layers, cumulonimbus (CB), thunderstorm (TS) zones, unstable layers).
050 02 06 03 Clear-air turbulence (CAT) — description, cause and location
(01) Describe CAT.
(02) Describe the formation of CAT.
(03) State where CAT is found in association with jet streams, in high-level troughs and in other disturbed high-level air flows.
(04) State that remote sensing of CAT from satellites is not possible and that forecasting is limited.
(05) State that pilot reports of turbulence are a very valuable source of information as remote measurements are not available.
050 02 07 00 Jet streams
050 02 07 01 Description
(01) Describe jet streams.
(02) State the defined minimum speed of a jet stream (60 kt).
(03) State the typical figures for the dimensions of jet streams.
050 02 07 02 Formation and properties of jet streams
(01) Explain the formation and state the heights, the speeds, the seasonal variations of speeds, the geographical positions, the seasonal occurrence and the seasonal movements of the arctic (front) jet stream, the polar (front) jet stream, the subtropical jet stream, and the tropical (easterly/equatorial) jet stream.
Arctic front jet:
- Height: 300 – 400 hPA (20-30 000′)
- Speed:
- Seasonal speed:
- Geographical Location: Only in northern hemisphere 60°N.
- Seasonal Occurrence: Not very common, winter.
- Seasonal Movement:
Polar front jet:
- Height: 300 hPa 30 000′
- Speed:
- Seasonal speed: Faster in winter.
- Geographical Location: Both hemispheres between ferrel and polar cell. 40-65°N 50°S.
- Seasonal Occurrence: Permanent.
- Seasonal Movement: North in summer, south in winter.
Sub tropical jet:
- Height: 200hPa 40 000′
- Speed:
- Seasonal speed: Faster in winter due larger temperature difference.
- Geographical Location: Both hemispheres between Hadley and ferrel. 25-40° in winter. 40-45° in summer.
- Seasonal Occurrence: Permanent.
- Seasonal Movement: Lower in winter due lower tropopause.
Tropical Easterly jet:
- Height: 150 hPa 45 000′
- Speed:
- Seasonal speed:
- Geographical Location: 10-20°N
- Seasonal Occurrence: Only in northern hemisphere in summer.
- Seasonal Movement:
050 02 07 03 Location of jet streams and associated CAT areas
(01) Sketch or describe where polar front and arctic jet streams are found in the troposphere in relation to the tropopause and to fronts.
Top corner of the warmer air mass just below the tropopause..
(02) Describe and indicate the areas of worst wind shear and CAT.
Cold air side.
Also Strong jets, curved jets, above and to the lee of high mountains and developing and rapidly moving jets.
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