At 22:43 10/10/2005, Graeme wrote:
Robert Hart wrote:
In response to several questions, I have written an article that shows how to obtain and interpret (in a gliding friendly way) the forecast atmospheric soundings available from the US National Oceanic and Atmospheric Administration (NOAA).

The article is at http://www.hart.wattle.id.au/alice/gliding/SkewT-logPexplain.html

I hope this is useful to other people.
Robert,
Thanks for your article. I assume that to find the origin of the dry adiabatic line to slide up, it is necessary trace down the red lines from the red numbers on the righthand edge to their intersection with the 1050 mBar line and extrapolate the position of the required DALR black line. If so, what are the black numbers across the top and down the left side, ie 440, 430, .....260, 250. on the ends of the DALR lines? Am I missing something?
Thanks,
Graeme

Yes you are, Graeme.

For some odd reason, the SALR lines are labelled with their CELSIUS temperatures whilst the corresponding DALR lines are labelled with their KELVIN temperatures. (At least you know from the label what kind of line it is - little numbers for SALR and big numbers for DALR.)

Because they are based on the International Standard Atmosphere, the label temperatures are for the 1013.2 hPa (millibar) level. Following up the lines from bottom to top shows how a parcel of air will cool if it is caused to rise and no heat is gained or added from outside the airmass itself (this is what 'adiabatic' means).

To predict the cooling of any given mass of air, you start from the conditions you have at your starting point (temperature and pressure). From the temperature trace line (red 'squiggly') you follow parallel to the nearest dry adiabatic line (up and left) until you meet the short black mixing ratio line (up and right from the dewpoint line at your starting level). Where these two lines meet gives the condensation level (temperature and pressure, hence height). Further upwards movement causes the air to cool along the SALR line through the intersection point. Water vapour condenses from the air as it rises, and so cloud forms.

However, if the only cause of the air rising in the first place is that it has been heated, it will only rise as far as the point where it stays above the red squiggly line (plus a little bit further that its momentum will carry it). Once it reaches the red line it is no longer buoyant, so it stops rising.

I'll stop here and let somebody else explain cloud tops, spread-out, rain formation and the several other things that can be deduced from the graphs.

However, just a reminder that the sounding only gives a valid prediction in the same airmass - so if there is a new airmass moving in, don't expect an early morning temp trace to predict the conditions in the airmass that was different to when you measured its temperature and humidity!

Wombat

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