THICKNESS RIDGE CLOUDINESS - TYPICAL APPEARANCE IN VERTICAL CROSS SECTIONS
by ZAMG
- Isentropes:
A vertical cross section taken across the Cold Front - Thickness Ridge Cloudiness - Warm Front shows the typical frontal gradient of isentropes
connected to the Cold Front and Warm Front. In between a maximum of isentropes is observed in the area of the Thickness Ridge Cloudiness. This
maximum is an indication of a tongue of warm air. It consists of a maximum of closed isolines in the lower layers indicating unstable conditions.
The height of the maximum differs according to the seasons and can be very extreme in summer. The upper part over the maximum has some
similarities with an "isentropic trough" usually associated with an Occlusion, but corresponding to a rising warm conveyor belt which
is superimposed upon the unstable zone. Depending on the season the layer of the warm conveyor belt can be rather deep.
- Temperature advection:
As the Thickness Ridge Cloudiness appears in front of a Cold Front, it generally exists within positive temperature advection (WA) at all levels
This is, in effect, the dominating warm conveyor belt stream.
- Relative humidity:
Although there is a maximum of humidity at the low levels, the rising air of the warm conveyor belt stream leads to a secondary relative
humidity maximum associated with Thickness Ridge Cloudiness in middle and upper levels.
- Divergence:
Although there is a distinct convergence maximum in lower levels, there is a broad zone of convergence representing the warm conveyor belt stream
at middle and higher levels.
- Vertical motion (Omega):
Convergence in lower levels leads to a distinct maximum of upward motion in middle and even higher levels.
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20 June 2000/06.00 UTC - Meteosat IR image; blue: thermal front parameter (TFP) 500/850 hPa, green: equivalent
thickness 500/850 hPa, position of vertical cross section indicated
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Isentropes, equivalent potential temperature
The above left diagram shows a typical appearance of isentropes associated with a Thickness Ridge Cloudiness in summer time. The tongue of warm air represented by a maximum, or at least a bulge of isentropes within the centre of a vertical cross section, is a most evident feature with Thickness Ridge Cloudiness. The above right diagram shows the common distribution of isentropes for the winter season, where the warm air tongue is not so strong. The cross section below shows a typical distribution of isentropes in the summer season.
20 June 2000/06.00 UTC - Vertical cross section; black: isentropes (ThetaE), orange thin: IR pixel values, orange thick: WV pixel
values
Temperature advection
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20 June 2000/06.00 UTC - Vertical cross section; black: isentropes (ThetaE), red thin: temperature advection - CA, red thick:
temperature advection - WA, orange thin: IR pixel values, orange thick: WV pixel values
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In the above riht hand cross section, distinct WA, representing the rising warm conveyor belt, can clearly be seen in the central and right side parts. The maximum located at the right side at lower levels can be assigned to the Warm Front (indicated by ascending tight gradient of isentropes) whereas the secondary maximum near the centre at middle levels and the maximum at upper levels can clearly be linked to the Thickness Ridge Cloudiness.
Relative humidity
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20 June 2000/06.00 UTC - Vertical cross section; black: isentropes (ThetaE), blue: relative humidity, orange thin: IR pixel
values, orange thick: WV pixel values
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A broad zone of increased relative humidity advected within the warm conveyor belt stream can be seen in the above right cross section.
Divergence
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20 June 2000/06.00 UTC - Vertical cross section; black: isentropes (ThetaE), magenta thick: convergence, magenta thin:
divergence, orange thin: IR pixel values, orange thick: WV pixel values
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Vertical motion (Omega)
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20 June 2000/06.00 UTC - Vertical cross section; black: isentropes (ThetaE), cyan thick: vertical motion (omega) - upward
motion, cyan thin: vertical motion (omega) - downward motion, orange thin: IR pixel values, orange thick: WV pixel
values
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