So lets start with the GFS and its crazy amplified solutions. In order to understand how each model run is evolving, lets look at the main players involved that make the solution happen:
THE PLAYERS
1. The Multiple Jet Interactions:
First up is the subtropical jet and the associated jet streak that is currently occurring over the central and eastern part of the United States. The jet streak in particular is an important feature, because it provides the necessary wind flow to evacuate air in the upper levels away from the developing surface cyclone center which allows for strong vertical motion that produces convection and precipitation. You can have a potent shortwave that little to no convection and precpitation because the orientation of the jet streak doesn't favor suface cyclogenesis. On the flip side, you can have a weak shortwave that has an explosion of deep convection and precipitation just because the jet dynamics were favorable to allow a large area of rising motion which favored condensation of air parcels and eventual rain/snow/thunderstorms.
So with that said, lets see what we have in store? Instead of looking at the 18z GFS solution, lets first focus on where we have been, showing the last suite of forecast solutions ending at 12z today. This is a d(prog)/dt map which highlights how the model has evolved for a given forecast interval over the past 7 days.
d(prog)/dt of 250 hPa Isotachs / 1000-500 hPa Thickness / MSLP
Here is a quick .gif animation (click the loop above to get better resolution) of the last 72 hours of model changes ending at the analysis time

Figure 1. 250 hPa isotachs / 1000-500 hPa Thickness / MSLP of GFS for the 12z 2/15 Forecast.
Starting from about 132 hours up to the model analysis, you notice a pretty distinct trend in the isotachs (shaded region of winds at 250 hPa) that represent the jet streak. We started out at around 50-60 m/s max (~120 knots) for a jet streak maximum centered over the gulf coastline. Note that over time as we get closer to the analysis, the jet streak intensifies quite a bit while also shifting further north and developing anticyclonic curvature. These two items are very key concepts in understanding how mid-latitude baroclinc lows are able to develop and intensify. Many of you on here understand that you want to have a surface cyclone in the left exit region or right entrance region of a jet in order to have favorable divergence aloft to support cyclogenesis. However, the curvature of a jet streak also plays a major role in modifying these regions. The right entrance region of a anticyclonic jet streak becomes the quadrant that experiences maximum divergence. This is where we will end up seeing our surface cyclone develop on the GFS. However, I just wanted to point out that the trend over the past 10+ model cycles has been to intensify the jet streak to 80-90 m/s max (~180 knots!) while making the flow more anticyclonic.
But WAIT, there is far more than one jet interaction going on. In fact, this system has the benefit of having three jet streak interactions, all in a seemly favorable interaction.

Figure 2. Same as figure one, except for 12 hour forecast at 6z on Feb 16th.
Thanks in large part to the current active MJO, we actually see the East Pacific is rather active convectively. This is pretty unusual for a La Nina regime this time of the year, but its actually going to play in this storms favor. Thanks to the active convection ongoing in the EPac we are experiencing a diabatic response with enhanced westerlies north of the convection. Part of this is also related to a dangling trough which has also helped to generate 100 knot westerlies aloft which is supporting the southernmost jet streak. This tropical connection is joined by two polar jet steam jet streaks bookending each side of the shortwave disturbance. Fast forward to 72 hours and we see how the jet streaks have combined together to aid in the rapid cyclogenesis that occurs over the southeast. This surface bombing rivals anything we have seen over the past year since the Boxing Day blizzard.

Figure 3. Same as figure 1 except for 72 hour forecast at 18z Feb 18th.
Of course the big question is how does this compare to the ECMWF? Generally they do look similar, but the GFS is notably stronger with almost all of the pieces of energy at 200 hPa by a factor of 5-10 m/s.
2-3. The Shortwaves and Anticyclonic Wave Breaking (AWB):
Another key factor we see with pretty much every major east coast snowstorm is the phasing between two shortwaves in a larger longwave trough. The interaction between two shortwaves that ride along two different jet streams is especially exciting. On rare occasions, we see a tripple jet interaction (March 1993 is one of the more extreme examples) that produces a historic storm. Now I could show you 500 hPa vorticity maps and heights, but that has already been done plenty of times before. This time, lets look at the dynamic tropopause (a measure of where in pressure the tropopause in the atmosphere is located) with winds plotted at that level. The animation below will go from 12-108 hours at 24 hour intervals.

Figure 4. Dynamic Tropopause and Wind. Relative vorticity contoured in fine black lines.
In the animation above, there are three key features which I attempted to show yesterday in some of the regional threads. The first shortwave is located in the southwestern United States and this is the main feature. Even without phasing this upper level feature is probably strong enough to generate a surface cyclone that will track across the Gulf Coast States. However, its the two more northern shortwaves that will be the real keys to properly forecast. The GFS shows that by 36 hours, the second shortwave (which is just entering the US near the MT/ND border) will be pinched off by an anticyclonic wave breaking event (a fancy term that signifies when a ridge aloft breaks off from the mean flow). This ridge will force both shortwaves further south between the 36-84 hour period. This is also where the greatest differences lie between the ECMWF and the GFS. The ECMWF is not nearly as strong with this ridge breaking off and thus the northern two shortwaves don't dig as much. The result is a southern stream storm with some snow on the northern end, but no significant storm that rides up the coast or inland. On the GFS, however, we see the first two shortwaves phase starting at 60 hours, and then by 84 hours the final shortwave phases. I want to note here that the AWB episode will allow for the shortwaves to drop southward as the jet level winds on the downstream side of the high will force southerly motion. This is one way we can get shortwaves to drop southward without a powerful west coast ridge, which is noticeably absent.
A three phasing solution should be sufficient, combined with favorable jet dynamics, to produce a meteorological "bomb" although this would likely mean a lot of the I-95 coordoor will have rain for this system. However, if we get shortwaves 1 and 2 to phase but not 3, we could still see a snowstorm for the I-95 crowd. If there is no phasing or weak phasing (which is closest to what the ECMWF shows) then we see mainly rain with a bit of snow on the northern end for folks in WNC and parts of VA.
THE OPTIONS
The Three Solutions:
This leads nicely into three possible solutions which I'll outline here. The jet configuration is such that we should see plenty of heavy precipitation break out. The biggest question though is where and how much, and will it be cold enough. Based on the maps and explanations above, here are three diagrams that outline what I think are three possible solutions.

Figure 5. Three potential surface low solutions based on the current synoptic pattern.
Solution one will most likely occur if we see a limited amount of phasing between shortwave 1 and 2 outlined in the animation above, and no interaction with shortwave three. While jet dynamics will still support widespread precipitation, the low track will remain suppressed and most of the big I-95 cities in the Northeast will remain dry.
Solution two will most likely occur if we see full phasing between shortwave 1 and 2, with limited to no phasing with shortwave 3. In this senerio we will see the low track move significantly inland with a large swath of heavy snow from DC to the extreme SNE. Note there will be lighter snows from the third shortwave across parts of new england and Upstate New York, but most of the heavy snow associated with the deepening surface cyclone will be missed.
Solution three will most likely occur if we see full phasing between shortwaves 1, 2, and 3. This will result in explosive cyclogenesis with surface pressure likely getting lower than 980 hPa at the peak of the systems lifespan. Unfortunately for snow-lovers, this will pull the 850 hPa 0 degree C isotherm further north and west and most of the I-95 cities (DC/PHL/NYC/BOS) may be spared the brunt of the snow. Right now its exceptionally difficult to tell which solution is more likely than the other. Considering the relative rarity of seeing a tripple phasing solution, intuition would say the extreme inland solution is the least likely of the three. However, the GFS's solution is certainly plausible given the 500 hPa and upper level setup for this system. If there was a system that had potential to bomb this winter, this is it.
THE UNCERTAINTY
Too many moving parts:

Figure 6. GEFS model spread of 250 hPa winds at initialization
Part of the reason why this forecast is so uncertain has a lot to do with the tiny pieces that have to come into play for a major phasing event to occur. Focusing first on aloft, we actually see the largest uncertainty in the GFS ensembles is actually the westerly flow coming from the tropics. A 10-14 m/s error could have some major ramifications down the road, especially in regards to the jet dynamics.
At 500 hPa, we see the largest uncertainty lies with the heights over the great lakes, not surprising considering this is where we are expecting to see several of the s/w to merge.

Figure 7. GEFS Model Spread of 500 hPa heights at 48 hours
The hardest part to forecast is the fact that These features are being stretched across the large ridge (the same one that will be breaking off from the mean flow) which makes it more difficult for models to handle the shortwave amplitude. Its harder to resolve waves when they are small and only have tiny changes horizontally.
So this leads us to now... the models are completely divergent because the small changes in the shortwave features are going to have huge repercussions downstream beyond the ridge. The anticyclonic ridge breaking allows for the shortwave features to dig down like the GFS suggests, and you don't necessarily have to have a ridge over the West Coast for this to occur. Still, the unusual nature of this pattern suggets that such deep amplification is rare. What happens from here on out is anyones guess, but I just wanted out outline the players and the options, and why its just so difficult to get a forecast solution 4-5 days out right now. It will be fun to watch, and I hope you will enjoy the roller coaster ride to come. After the boring weather across the East US the last month, its about time we have something exciting to talk about!
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