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gtspring2009:gibson:w03 [2009/04/13 09:08]
gibson
gtspring2009:gibson:w03 [2009/04/27 08:01]
predrag suggested a desymmetrized plot of Poincare sections
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 with Poincare sections placed at θ = 0, pi/4, pi/2, 3pi/4, etc. The θ = 0 section is marked with small with Poincare sections placed at θ = 0, pi/4, pi/2, 3pi/4, etc. The θ = 0 section is marked with small
 circles and the θ = pi/4 with dots.  circles and the θ = pi/4 with dots. 
- 
 ===== 2009-04-13 Poincare sections 4 ===== ===== 2009-04-13 Poincare sections 4 =====
  
-{{gtspring2009:​gibson:​eq2poincare_ubef2_3.png?​300}}{{gtspring2009:​gibson:​eq2poincare_ubef2_section_zero.png?​300}} +{{gtspring2009:​gibson:​eq2poincare_ubef2_3.png?​400}}{{gtspring2009:​gibson:​eq2poincare_ubef2_section_zero.png?​400}} 
  
 Here we have the poincare sections at θ=0 (black, and θ=π in green). The left plot Here we have the poincare sections at θ=0 (black, and θ=π in green). The left plot
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 \end{align} $ </​latex>​ \end{align} $ </​latex>​
  
-{{gtspring2009:​gibson:​eq2poincare_ubef2_2.png?​300}}{{gtspring2009:​gibson:​eq2poincare_ubef2_section_pi2.png?​300}}+{{gtspring2009:​gibson:​eq2poincare_ubef2_2.png?​400}}{{gtspring2009:​gibson:​eq2poincare_ubef2_section_pi2.png?​400}}
  
 Same as above but with the Poincare section at θ=π/2 (black) and θ=3π/2 (green). ​ Same as above but with the Poincare section at θ=π/2 (black) and θ=3π/2 (green). ​
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-{{gtspring2009:​gibson:​eq2poincare_ubef2_section_zeroB.png?​300}}{{gtspring2009:​gibson:​eq2poincare_ubef2_section_zeroC.png?​300}}+{{gtspring2009:​gibson:​eq2poincare_ubef2_section_zeroB.png?​400}}{{gtspring2009:​gibson:​eq2poincare_ubef2_section_zeroC.png?​400}}
  
 Ok, some Poincare sections at θ=0 orientation,​ with vertical axis (u, e3) on left and Ok, some Poincare sections at θ=0 orientation,​ with vertical axis (u, e3) on left and
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 unstable manifold and plot a return map. This involves some more arbitrary decisions, namely, when to continue increasing arclength and when to project back onto previous portions of the unstable manifold. ​ // 2009-04-13 12:07 EST// unstable manifold and plot a return map. This involves some more arbitrary decisions, namely, when to continue increasing arclength and when to project back onto previous portions of the unstable manifold. ​ // 2009-04-13 12:07 EST//
  
 +
 +{{gtspring2009:​gibson:​eq2poincare_ubef2_section_zeroD.png?​400}}
 +
 +The plot above shows a number of points on the unstable manifold and their iterates under the return map. 
 +A triangle symbol maps into the next triangle out along the unstable manifold, etc. The symbols are, in sequence,
 +triangle, square, diamond, star, circle. The first iterates of the symbols are all clustered just to the right of
 +EQ2 (at the origin). One return later they are spread from the triangle at (0.03, 0.03) to the circle at (-0.01, 0.08).
 +The next return, they are all over the map, and it no longer makes sense to draw lines connecting them (though I have
 +done so to show you that I am insane). ​
 +
 +This is bad news, I believe. In order for the approximate return map s^(n+1) = f(s^n) (where s is pseudo-arclength ​
 +along the unstable manifold) to produce good guesses for periodic orbits, it needs to intersect the identity. ​
 +has to intersect the identity. In this plot, that would correspond to some portion of the lower part of the fold
 +to be mapped into the upper part. But the symbols show us this doesn'​t happen. ​
 +
 +Corrections?​ Suggestions? ​
 +
 +//John Gibson 2009-04-13 14:52 EST//
 +
 +===== Desymmetrized Poincare sections =====
 +
 +Can you plot these sections in desymmetrized space of Gibson //et al?//
 +
 +{{:​gtspring2009:​howto:​gtspring2009:​2008-spring-p7.png?​800}}
 +
 +It should be easier to visualize them without discontinuities... ​ --- //​[[predrag.cvitanovic@physics.gatech.edu|Predrag Cvitanovic]] 2009-04-27 07:53//
  
  
  
gtspring2009/gibson/w03.txt · Last modified: 2010/02/02 07:55 (external edit)