At long last, a most belated 'lesson'. Given that it's been so long since my last lesson post, I suggest you take the time to re-read what I wrote last time on the Norwegian Cyclone Model before plunging into this one.
Following the Norwegian Model, which was developed as a result of increased atmospheric measurements during the First World War, it wasn't until the age of computerised data analysis and vastly increased data-gathering from sources such as balloon soundings, weather buoys and early meteorological satellites that it was realised that the observed data from western Atlantic maritime extratropical cyclones (i.e. those which are located outside the tropics and therefore are not going to develop into hurricanes, typhoons or tropical cyclones) often don't follow the classical pattern of the Norwegian Model. Rather than a long, trailing cold front catching-up to a shorter warm front and occluding it, these storms, most of which show rapid deepening (so-called Explosive Cyclogenesis or 'bombogenesis') like Storm Doris did a couple of months ago, are characterised by initial occlusion near the triple point, where the fronts meet at the centre of the depression, after which the cold front, instead of swinging anti-clockwise around the low centre, instead heads south, perpendicular to the axis of the cold front. As it does so, it 'fractures' away from the triple point, allowing the head of the occlusion to bend around the western flank of the low centre, in turn allowing cold air to rush around the western side of the centre, cutting-off warm air from the warm sector in the centre of the low. This cutting-off of warm air is termed a Seclusion. To quote the Weather FAQs site (
http://weatherfaqs.org.uk/node/98):
As with the Norwegian cyclone model, an incipient cyclone develops cold and warm fronts, but in this case, the cold front moves roughly perpendicular to the warm front such that the fronts never meet, the so-called 'T-bone'. Also, a weakness appears along the poleward portion of the cold front near the low center, the so-called 'frontal fracture' and a back-bent front forms behind the low center. (In the final stage), colder air encircles warmer air near the low center, forming a warm seclusion. Typically, the Shapiro-Keyser cyclone is oblong, elongated east-west along the strong warm front
Here is a schematic comparing the Norwegian Model and Shapiro-Keyser Model - note the differing behaviour of the cold front between the two, and try to visualise cold air from the northern side of the polar front 'wrapping around' the low centre and rushing in to surround warmer air at the core as the occlusion bends back:
Characteristic of this stage of the formation of a Shapiro-Keyser cyclone is that the region of strongest thermal gradient in (b)III in the above diagram is not at the former triple point near the low centre, but is instead to the south-east. As the system matures beyond stage IV, the cold front may form a new triple point with the warm front further south along the warm front, away from the low centre, thereby shifting the strongest thermal gradient further south still.
Next time, how rapidly-developing depressions following the Shapiro-Keyser Model sometimes include Sting Jets.