WARM CONVEYOR BELT - METEOROLOGICAL PHYSICAL BACKGROUND
by ZAMG
A Warm Conveyor Belt is defined as a layer of air which:
- originates in a relative easterly to south-easterly flow within the lower levels of the troposphere in
the ridge area ahead of the front;
- generally ascends poleward (north to north-eastern direction) forming cloudiness due to the
condensation of moist air;
- after turning to south-eastward directions ascending motion changes to descending motion, where cloud
dissolution takes place.
As already mentioned Warm Conveyor Belts are directly involved in the frontal processes, but typical cloud configurations can also be observed separately from the frontal cloudiness. Different states of the atmosphere are responsible for these two types:
- The cloudiness of a front is developed within two relative streams: the Warm Conveyor Belt and a less
wet relative stream from the trough area behind; the Warm Conveyor Belt is connected at least with the
leading part of the cloudiness, therefore the relative stream lines approach or even overrun the surface
front (or the TFP).
- In the case of separated Warm Conveyor Belt cloudiness the relative stream lines are in front of
the frontal cloud band and the relative stream from behind crosses the frontal line in a forward direction,
consequently approaching the stream lines of the Warm Conveyor Belt.
- These different situations show up in the vertical cross section of equivalent potential temperature in
the case of a Warm Conveyor Belt being involved in the front. The upper troposphere in front of the Cold
Front surface shows either an indistinct or a trough configuration of isentropes. In the case of a Warm
Conveyor Belt being separated from the front, a second downward inclined crowding zone of isentropes can be
observed in high and middle levels. The air in the Warm Conveyor Belt moves on these isentropic surfaces.
15 April 1996/06.00 UTC - Vertical cross section; black: isentropes (ThetaE), orange thin: IR pixel values, orange thick: WV pixel values
The 308K isentrope belongs to the Cold Front, the 318K isentrope to the
Warm Conveyor Belt cloudiness.
15 April 1996/06.00 UTC - Meteosat IR image; magenta: relative streams 308K - system velocity: 258°
10 m/s, yellow: isobars 308K, position of vertical cross section indicated
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15 April 1996/06.00 UTC - Meteosat IR image; magenta: relative streams 318K - system velocity: 258°
10 m/s, yellow: isobars 318K, position of vertical cross section indicated
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At the 308K isentropic surface, which is relevant for the cloud band of the Cold Front, the whole frontal cloudiness is under the influence of the upper relative stream from behind. The limiting stream line between this stream and the Warm Conveyor Belt can be found at the eastern edge of the cloudless area between Cold Front and Warm Conveyor Belt. The cloudiness with the embedded cells in front of this zone is already under the influence of the Warm Conveyor Belt.
At the 318K surface the Warm Conveyor Belt, which has an ascending poleward direction, forms the cloudiness Warm Conveyor Belt. Above the Atlantic (at approximately 48N/11W) the conveyor belt splits into two branches. The southern branch turns from a north-eastward direction to a south-eastward one and forms the cloudiness which extends to the north coast of Spain. The northern branch turns from a north-eastward to a northward direction forming the cloudiness above the Atlantic towards the west coast of Ireland. The limiting stream line between the relative stream from behind the front and the Warm Conveyor Belt can be found above the convective cells. Therefore the cells are under the influence of the warm moist air mass of the Warm Conveyor Belt in lower layers, but in the colder drier air of the upper relative stream in higher layers. This is a typical situation for instability and convective development.
- At the rear boundary of the Warm Conveyor Belt close to the Cold Front cloud band, sometimes convective cells
develop. This is the area where in lower levels the moist air of the Warm Conveyor Belt streams northward, while
in higher levels the air in the drier relative stream from behind the front crosses over. This is a typical
unstable layer of the troposphere leading, in combination with upward motion, to convective developments (compare
the example before).