c-h plane analysis of plasma turbulence in ssx and lapd

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C-H plane analysis of plasma turbulence in SSX and LAPD Last updated 6/20/14 by Peter Weck

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C-H plane analysis of plasma turbulence in SSX and LAPD. Last updated 6/20/14 by Peter Weck. Contents. Complexity -entropy planes for full datasets Helicity dependence of SSX complexity-entropy plane SSX complexity -entropy planes for varied embedding delay - PowerPoint PPT Presentation

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Page 1: C-H plane analysis of plasma turbulence in SSX and LAPD

C-H plane analysis of plasma turbulence in SSX and LAPD

Last updated 6/20/14by Peter Weck

Page 2: C-H plane analysis of plasma turbulence in SSX and LAPD

I. Complexity-entropy planes for full datasets

II. Helicity dependence of SSX complexity-entropy plane

III. SSX complexity-entropy planes for varied embedding delay

IV. Dependence of SSX complexity-entropy plane on time window

Contents

Page 3: C-H plane analysis of plasma turbulence in SSX and LAPD

Section I

Complexity-entropy planes for full datasets

Page 4: C-H plane analysis of plasma turbulence in SSX and LAPD

Figure 1: SSX points are averages over 12 channels, all 3 directions, and ~40 shots for two helicity settings. LAPD points are averages over 25 runs at two positions. Error bars represent standard deviations in C and PE, below and above averages.

The CH Plane

Page 5: C-H plane analysis of plasma turbulence in SSX and LAPD

The full CH Plane for SSX

Figure 2: As for all diagrams here presented, n=5 was used. 15456 SSX points are plotted, corresponding to time series from 3 directions, 16 channels, 8 helicity settings, and ~40 runs per helicity.

Page 6: C-H plane analysis of plasma turbulence in SSX and LAPD

The SSX CH Plane, first 12 channels only

Figure 3: 11592 SSX points are plotted, corresponding to time series from 3 directions, 12 channels, 8 helicity settings, and ~40 runs per helicity.

Page 7: C-H plane analysis of plasma turbulence in SSX and LAPD

The Full CH Plane for LAPD

Figure 4: 775 LAPD points are plotted, corresponding to time series from 25 runs and 31 positions.

Page 8: C-H plane analysis of plasma turbulence in SSX and LAPD

Section II

Helicity dependence of SSX complexity-entropy plane

Page 9: C-H plane analysis of plasma turbulence in SSX and LAPD

All SSX data for each helicity setting:

0.25 mWb

0.1 mWbunstuffed

0.5 mWb

Page 10: C-H plane analysis of plasma turbulence in SSX and LAPD

All SSX data for each helicity cont.

1.25 mWb 1.5 mWb

0.75mWb 1.0 mWb

Page 11: C-H plane analysis of plasma turbulence in SSX and LAPD

Figure 5: Note that points represent the radial direction, plus signs theta, and x-marks z. The color scale represents helicity.

SSX CH Plane, averaged over shots (channel 1 of 16)

Page 12: C-H plane analysis of plasma turbulence in SSX and LAPD

Figure 6: The color scale again represents helicity. Note the loop executed in the right side of the plane as helicity is varied. The least entropic helicity setting (pale blue) appears to be 0.5mWb.

SSX CH Plane, averaged over shots and directions (channel 1 of 16)

Page 13: C-H plane analysis of plasma turbulence in SSX and LAPD

Figure 7: The same looping behavior as in Figure 6 seems to occur for channel 6 data, although the loop is angled a little higher in the plane

SSX CH Plane, averaged over shots and directions (channel 6 of 16)

Page 14: C-H plane analysis of plasma turbulence in SSX and LAPD

SSX CH Plane, averaged over shots and directions (channel 12 of 16)

Figure 8: Channel 12 data seems to loop through an even higher complexity region of the CH plane. Once again, 0.5mWb has the lowest entropy point.

Page 15: C-H plane analysis of plasma turbulence in SSX and LAPD

Section III

Complexity-entropy planes for varied embedding delay

Page 16: C-H plane analysis of plasma turbulence in SSX and LAPD

• The following two slides show SSX data up to channel 12 for various embedding delays.

• While τ denotes use of the embedding delay as described in most of the literature, which effectively reduces the length of the analyzed series by a factor of τ, τ ’ indicates that a delay analysis like that used for the increments method was applied.

• So τ ’ analyzed series are kept significantly longer, only losing (n-1) τ ’ or so values.

• Figure 3 (τ ’ = τ = 1) has been reproduced above to provide comparison with the diagrams to follow.

• I was surprised to see that keeping more of the series actually lowered the overall complexity of SSX data, according to these diagrams.

Page 17: C-H plane analysis of plasma turbulence in SSX and LAPD

τ = 2

τ = 6 τ = 8

τ = 4

Page 18: C-H plane analysis of plasma turbulence in SSX and LAPD

τ ’ = 2

τ ’ = 6 τ ’ = 8

τ ’ = 4

Page 19: C-H plane analysis of plasma turbulence in SSX and LAPD

Section IV

Dependence of SSX complexity-entropy plane on time window

Page 20: C-H plane analysis of plasma turbulence in SSX and LAPD

• The following six slides show the full range of SSX data on the CH plane for six different 20 μs windows.

• The data seems to drop further towards the rightmost corner of the plane the farther out in the time series you go, with 30-50 μs and 40-60 μs data occupying the upper/middle region of the plane and the 80-100 μs data closest to the PE=1, C=0 corner.

• The same six plots were generated for embedding delays τ = 2, 4, 6, and 8 and τ ’ = 2, 4, 6, and 8, but I did not include them since introducing a delay seemed to have the same qualitative effect on all time windows as was seen for the 40-60 μs window data in the previous section (i.e. delays of τ’ = τ = 2 pulled the data closer to noise, and delays of 4, 6, and 8 pulled it up into higher regions of the plane).

Page 21: C-H plane analysis of plasma turbulence in SSX and LAPD

t = 30-50 μs

Page 22: C-H plane analysis of plasma turbulence in SSX and LAPD

t = 50-70 μs

Page 23: C-H plane analysis of plasma turbulence in SSX and LAPD

t = 70-90 μs

Page 24: C-H plane analysis of plasma turbulence in SSX and LAPD

t = 40-60 μs

Page 25: C-H plane analysis of plasma turbulence in SSX and LAPD

t = 60-80 μs

Page 26: C-H plane analysis of plasma turbulence in SSX and LAPD

t = 80-100 μs

Page 27: C-H plane analysis of plasma turbulence in SSX and LAPD

• The next six slides show CH planes with unstuffed and 0.5 mWb SSX data for six different 20 μs windows.

• On each slide, the full range of the 0.5 mWb data up to channel 12 is shown top-left, the range of the unstuffed data up to channel 12 top-right, and the average position and standard deviations for both data sets bottom-center.

• The 30-50 μs, 50-70 μs, and 40-60 μs window diagrams all seem fairly similar, with comparable positions and deviations for both unstuffed and 0.5 mWb settings.

• The three windows after these ranges, however, drop the data dramatically towards the PE=1, C=0 corner of the plane. Latter portions of the time series also break the pattern of lower entropies for the 0.5 mWb setting which has consistently held for earlier portions of the time series.

Page 28: C-H plane analysis of plasma turbulence in SSX and LAPD

t = 30-50 μs

Page 29: C-H plane analysis of plasma turbulence in SSX and LAPD

t = 50-70 μs

Page 30: C-H plane analysis of plasma turbulence in SSX and LAPD

t = 70-90 μs

Page 31: C-H plane analysis of plasma turbulence in SSX and LAPD

t = 40-60 μs

Page 32: C-H plane analysis of plasma turbulence in SSX and LAPD

t = 60-80 μs

Page 33: C-H plane analysis of plasma turbulence in SSX and LAPD

t = 80-100 μs