Some time ago I wrote a post on the Norwegian Cyclone Model
and how great it is. Well, it actually has some major flaws. A large portion of
these flaws stem from the limited number of available observations the Bergen
School had to work with when developing their model in the early 1900s. Essentially,
their data only represented the weather found over the northeast Atlantic and Western
Europe. Therefore, it completely lacks data on storms such as those that
rapidly develop near the east coast of North America (i.e. Nor’easters) or
those that form in the lee of the Rockies and move across central U.S. Another
source of the problems associated with the Norwegian Model is that aside from
some aspects of fronts and air masses, it is mostly described in 2-D. A likely
cause for this oversight was the fact that little research had been done on
upper level dynamics. At that time, meteorologists did not have access to
technologies we now take for granted such as radar and satellite imagery. Even
phenomena as critical as jet streams were unknown, in fact the jets were not
identified until high altitude bombing missions over the Pacific during the latter
part of WWII. Clearly, the Model needed some adjustment.
As a result of its shortcomings, many weather features that are
now observed every day are simply impossible to explain using the Norwegian
Model. As an example, check out the MODIS image below of an intense Mid-Latitude
Cyclone (MLC) in the Gulf of Alaska from October of 2005. At this time the
system featured warm, cold, and occluded fronts and packed Hurricane Force
winds. I will be using this impressive system as a great example throughout this post.
Notice the two highlighted regions; these are both examples
of features not found in the Norwegian Model. However, it should be noted that
these are just two examples, not the only examples of features absent in the
Model.
This image highlights a region of the storm where the air
flow has wrapped around the low center several times. Much of the outer parts
of the spiral happen to contain the end of the Occluded Front. This complex
spiral is not described in the Norwegian Model, which depicts a developed low
such as this as having a very strong cold front that continues as a short
occluded front and makes only a small portion of a spiral into the low’s
center.
In this image, a portion of the scattered convection on the
cold side (west) of the MLC is clearly enhanced relative to the surrounding
cloud field. This region is likely the beginnings of a Comma Cloud. A comma
cloud is small system that often looks a bit like a MLC, but much smaller and
without fronts. These formations are important to follow because they can have
a large effect on the main MLC and its cold front if it interacts with them.
All of these features are depicted above. This image consists of a simple version of the MODIS image above, overlaid with the surface map from about the same time.
So, what have scientists done about these issues? Answer: they devised a new model that adjusts and builds upon the Norwegian Model named The Conveyor Belt Model. In the next 101 post I’ll describe this model in more detail, but for now, consider the diagram of a MLC as a teaser.
So, what have scientists done about these issues? Answer: they devised a new model that adjusts and builds upon the Norwegian Model named The Conveyor Belt Model. In the next 101 post I’ll describe this model in more detail, but for now, consider the diagram of a MLC as a teaser.
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