For information contact H. C. Koons 25 May 2004 1 Preliminary Analysis of ABFM Data WSR “11 x 11 Volume Integral” Harry Koons 25.

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Presentation transcript:

For information contact H. C. Koons 25 May Preliminary Analysis of ABFM Data WSR “11 x 11 Volume Integral” Harry Koons 25 May 2004

For information contact H. C. Koons 25 May Scatter Plot of dBZ-km vs Emag WSR “11 x 11 Volume Integral”

For information contact H. C. Koons 25 May Approach Objective is to determine the probability of an extreme electric field intensity for a given radar return Use the statistics of extreme values to estimate the extreme electric field intensities –Reference: Statistical Analysis of Extreme Values, Second Edition, R. -D. Reiss and M. Thomas, Birkhäuser Verlag, Boston, 2001 As an example analyze WSR “11x11 Volume Integral” –Determine extreme value distribution functions for 10- (dBZ-km)-wide bins For example the  5-(dBZ-km) bin is defined to be the range:  10 < dBZ-km  0 –Use Frac11x11  0.1 selected from Frac11x11  0.05 database

For information contact H. C. Koons 25 May Scatter Plot of dBZ-km vs Emag WSR “11 x 11 Volume Integral”  5 dBZ-km bin

For information contact H. C. Koons 25 May Sample Statistics -10 < dBZ-m  0 Sample Size, N = 230 Minimum = 0.02 kV/m Maximum = 1.72 kV/m Median = 0.54 kV/m Mean = 0.59 kV/m Choose Peaks Over Threshold (POT) Method for Extreme Value Analysis u = kV/m (high threshold) k = 75 (right end of the stability zone)

For information contact H. C. Koons 25 May Gamma Diagram Point of stability is on the plateau near 75 at  ~  0.37

For information contact H. C. Koons 25 May Kernel Density Function and Model Density Function Peaks Over Threshold Method (POT) –N = 230 samples between –10 and 0 dBZ-km –u = 0.67 kV/m (high threshold) MLE (GP) – k = 75 (mean zone of stability) –  =  –  = (~left end point) –  = –RE = bw=0.2

For information contact H. C. Koons 25 May Sample and Model Distribution Functions

For information contact H. C. Koons 25 May Sample and Model Quantile Functions

For information contact H. C. Koons 25 May Q – Q Plot Sample Model

For information contact H. C. Koons 25 May T-Sample Electric Field Intensity -10 < dBZ-km  0 T, SampleLevel, kV/m , , , ,000, ,000,

For information contact H. C. Koons 25 May Extend Analysis to Other Bins Use bins centered at –5, +5, and +15 dBZ-km Kernel Density Plot Sample Statistics Model Parameters T-Sample Electric Field Intensity

For information contact H. C. Koons 25 May Sample Kernel Densities WSR, -10 dBZ Threshold, “11 x 11 Volume Integral” Blk:  5 dBZ-km Red: +5 dBZ-km Grn: +15 dBZ-km Electric Field, kV/m

For information contact H. C. Koons 25 May Sample Statistics and Model Parameters WSR, -10 dBZ Threshold, “11 x 11 Volume Integral”  5 dBZ-m +5 dBZ-km +15 dBZ-km N k u(k), kV/m      Right Endpoint, kV/m none E max, kV/m

For information contact H. C. Koons 25 May T-Sample Electric Field Intensity, kV/m WSR, -10 dBZ Threshold, “11 x 11 Volume Integral” T-Sample  5 dBZ-km +5 dBZ-km+15 dBZ-km , , , ,000, ,000,

For information contact H. C. Koons 25 May Sample Statistics and Model Parameters WSR, +15 dBZ-km, “11 x 11 Volume Integral” +15 dBZ-km -10 dBZ Thresh. +15 dBZ-km 0 dBZ Thresh. N E max, kV/m 2.94 k 9378 u(k), kV/m    Right Endpoint, kV/m none

For information contact H. C. Koons 25 May T-Sample Electric Field Intensity, kV/m WSR, +15 dBZ-km, “11 x 11 Volume Integral” T-Sample +15 dBZ-km -10 dBZ Thresh. +15 dBZ-km 0 dBZ Thresh , , , ,000, ,000, E max observed 2.94

For information contact H. C. Koons 25 May Gamma Diagrams (  vs. k) WSR “11 x 11 Volume Integral,” +15 dBZ-km -10 dBZ Threshold0 dBZ Threshold k=93 k=78

For information contact H. C. Koons 25 May Q-Q Plot WSR “11 x 11 Volume Integral,” +15 dBZ-km Threshold: Red: -10 dBZ Blk: 0 dBZ

For information contact H. C. Koons 25 May Revised Values for WSR “11x11 Average” I found an error in my previous analysis using the peaks-over- threshold method for the WSR “11 x 11 average” and the WSR “3 x 3 x3 cube – Average” –The parametric fits were properly done to the exceedances –The T-sample levels were improperly calculated because I interpreted T to be 1/p where p is the probability. In fact T = k/(N*p), so I had effectively offset the results in the T-sample columns. –The next two charts, 21 and 22, have the corrections. The only two rows on chart 21 that are different are u and . The results are about 200 V/m higher that the previous ones at each T-sample I have not had time to correct the results for the 3 x3 x 3 cube. –I expect the correction will be about the same.

For information contact H. C. Koons 25 May Sample Statistics and Model Parameters WSR “11 x 11 Average” -2 dBZ0 dBZ+2 dBZ+4 dBZ u, kV/m N k  0.0   revised 5/21/2004

For information contact H. C. Koons 25 May T-Sample Electric Field Intensity, kV/m WSR “11 x11 Average” T-Sample-2 dBZ0 dBZ+2 dBZ+4 dBZ , , , ,000, ,000, revised 5/21/2004