Group meeting: November 10, 2005




PV Budgets

Vertical profiles
LHS vs. RHS contributions
LHS - RHS with and without vertical advection used


Potential vorticity and contributing components on select pressure levels.
500:450 hPa EPV 850:800 hPa EPV
500:450 hPa EPV change - (EPV changes from diabatic + (horizontally) advective components) 850:800 hPa EPV change - (EPV changes from diabatic + (horizontally) advective components)
500:450 hPa EPV change - (EPV changes from diabatic + (horizontally + vertically) advective components) 850:800 hPa EPV change - (EPV changes from diabatic + (horizontally + vertically) advective components)
500:450 hPa EPV diabatic changes 850:800 hPa EPV diabatic changes
500 hPa vertial motion (omega) 850 hPa vertical Motion (omega)
500:450 hPa EPV advective (horizontal) changes 850:800 hPa EPV advective (horizontal) changes
500:450 hPa EPV advective (vertical) changes 850:800 hPa EPV advective (vertical) changes
500:450 hPa EPV advective (total) changes 850:800 hPa EPV advective (total) changes



Terrain



Reanalysis analysis

Histogram of maximum potential temperature amplitude changes for cyclones and anticyclones
TPV intensity changes (growth and decay; 1 K bins)
Plots of TPV strong amplitude change locations. For each vortex, the location in which the maximum growth and decay occurred was saved. Those vortices in which the growth and decay was more than 30 K were retained in the following plot. The plots shows the locations where the number of vortices (normalized by cos(latitude)) within a 2.5 degree latitude by 7.5 degree longitude box had more than a 30 K tropopause potential temperature amplitude change.
TPV high amplitude change density plot
However from the histogram, it is suspicious that amplitude changes of these intensities were occurring. Since the mean and median are significantly different for the cyclones, it is apparent that at the very least there are some strong outliers. Upon eye examination of the datasets, two startling discoveries were made. (1) In some vortex tracks (data include latitude, longitude, date, theta, theta amplitude) that were physically adjacent to each other, there were sometimes exact repeats! Further investigation revealed that there were some tracks that had different lengths, different staring times, and/or different ending times, but that clearly the data in the middle were the same as the adjacent track. To take care of this problem, I made a filter that compares adjacent vortex tracks by looking at their correlations. If the correlation is unity, then they are repeats. But what about the ones with different track lengths that were not exact repeats? Here, I took half of the first track centered about the middle, then took the second track and phase compared it with the previous track. There had to be at least 4 (24 hours of data) phase matches (correlation of unity) before eliminating one. (2) There were sudden "spikes" in potential temperature amplitudes. It is reasonable to assume that a spike of more than 30K is not physically realistic and can be thrown out. So to eliminate these spikes, I found each time that the amplitude changed by more than 30 K. If this amplitude change was followed by an immediate amplitude change of the opposite sign at the next data point of more than 90% of the original amplitude change, it seems reasonable to replace the corresponding large amplitude with NaN.
Unfiltered cyclone growth
After filtering out the repeats only
After filtering out the spikes only
Filtering out both the repeats and the spikes
So what percentage vortices with growth over 50K get removed?
Vortex before and after correlations
TPV density plots: Comparisons of filtered vs. unfiltered
Cyclones and anticyclones



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