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• Group 1
  : Eponymously discovered by Faraday[1], Faraday Waves are standing waves on a fluid caused by vertical oscillator ...t \left(\nabla\vec{v} + \nabla\vec{v}^T \right)+ \frac{1}{Fr}F(cos(2\pi t)-1)\mathbf{j}</math>
  28 KB (4,305 words) - 09:57, 12 January 2012
• Group 1 2010
  #REDIRECT [[Group-1 (2010)]]
  28 bytes (2 words) - 22:31, 28 November 2011
• Group-1 (2010)
  29 bytes (3 words) - 22:31, 28 November 2011
• Group 1 2012
  ...determines a smooth vector field on <math>\mathbb{R}^{2}\times \mathbb{S}^{1}</math> (a 3 dimensional space) and hence truly chaotic behavior is possibl ...nd the trajectories are curves of constant energy <math>E(x,\dot{x})=\frac{1}{2}\dot{x}^{2}+V(x)</math>. In this case it is easy to see that we have a s
  25 KB (4,001 words) - 22:50, 28 October 2014
• Group 1 2014
  [[File:Shear.png | thumb | 300px | Figure 1: Force gradient viewed from above.]] Where <math>\chi = \{ 0,-1,1 \}</math> indicates the direction of the particle's chirality, <math>g</mat
  10 KB (1,538 words) - 16:25, 12 December 2014
• Group 1 2023
  <!--fig example [[File:NAME.png | thumb | 300px | Figure 1: FIG NAME.]]--> [1] ...
  574 bytes (64 words) - 12:06, 18 April 2023

Page text matches

• Group 1 2023
  <!--fig example [[File:NAME.png | thumb | 300px | Figure 1: FIG NAME.]]--> [1] ...
  574 bytes (64 words) - 12:06, 18 April 2023
• Group 2 2023
  <!--fig example [[File:NAME.png | thumb | 300px | Figure 1: FIG NAME.]]--> [1] ...
  570 bytes (64 words) - 12:07, 18 April 2023
• Team Rijke 2020
  * [[Media: Rijke Mitchell Passarelli.pdf | Final report 1]]
  391 bytes (60 words) - 11:19, 29 January 2021
• Team Fire 2020
  *[[Media: Fire Benjamin Musci.pdf | Final report 1]]
  437 bytes (67 words) - 11:17, 29 January 2021
• Team Faraday 2020
  * [[Media:Faraday Alejandro Escontrela.pdf | Final report 1]]
  452 bytes (67 words) - 11:18, 29 January 2021
• Team Vortex 2020
  * [[Media: Vortex Jaesung Jeon.pdf | Final report 1]]
  441 bytes (67 words) - 11:18, 29 January 2021
• Team Metronome 2020
  * [[Media: Metronome Aris Kanellopoulos.pdf | Final report 1]]
  474 bytes (68 words) - 11:20, 29 January 2021
• Chua's circuit
  -x & |x| < 1 \\ [-1 + \beta(|x| - 1)sgn(x) & 1 < |x| < 10 \\
  8 KB (1,234 words) - 14:27, 17 October 2011
• Assignments
  ===Assignment 1=== ...rom Strogatz, 2nd edition: 2.2.7, 2.3.3, 2.4.2, 2.5.6G, 2.6.2G, 2.8.8, 3.1.1, 3.4.11, 3.4.14, 3.5.6G, 3.6.6. Problems with a G at the end are problems a
  7 KB (1,124 words) - 11:36, 30 October 2014
• Hopping dynamics
  [[File:ScreenHunter_92_Sep._21_18.03.jpg | thumb | 300px | Simple 1-D freedom jumping robot]] ...or analyzed using various accepted techniques. The jumping robot exhibited 1-cycle, 2-cycle, 3-cycle and chaotic motion, which was mostly consistent wit
  6 KB (970 words) - 14:35, 24 September 2012
• Syllabus
  Jan 9: Lecture 1, intro to the subject Feb 1: Lecture 6, imperfect bifurcations (Chap 3)
  3 KB (386 words) - 11:31, 18 April 2023
• Planning
  {|cellpadding="5" cellspacing="0" border="1" width="60%" | Faraday waves ([[Group 1]] requested this) and Plinko dynamics
  4 KB (570 words) - 16:31, 17 October 2011
• Main Page
  {|cellpadding="5" cellspacing="0" border="1" width="60%" ...Fire.pdf |Presentation]]. [[Media: Fire Benjamin Musci.pdf | Final report 1]], [[Media: Match Lezheng Fang.pdf | Final report 2]], [[Media: Match Mateo
  10 KB (1,348 words) - 11:25, 18 April 2023
• Double pendulum
  ...sions. As such small differences in initial conditions grow exponentially [1]. Due to its simplicity and rich dynamical behavior, this system is widely ...d the second arm (vertical axis) from -180 to 180 degrees in approximately 1 degree steps. It is overlaid with experimental data points of time to flip,
  6 KB (954 words) - 18:11, 23 September 2012
• Group 3
  \frac{A\omega^2}{g} [\sin(\omega t) + c^2 \sin(c \omega t)] &\geq 1 x_b(t) = &x_p(t_0) - x_p(t) + \dot{x}_p(t_0)(t-t_0) - 1/2 g(t-t_0)^2 \notag\\
  15 KB (2,451 words) - 09:59, 12 January 2012
• Group 2 2012
  ...isplaystyle{d\theta_{i}\over{dt}} = \omega_t + {K\over{N}}\sum\limits_{j = 1}^{N} \sin(\theta_j - \theta_i)$$ (i) $\displaystyle{d\phi \over{dt}} = {1\over{T}}$ models the change of phase of the oscillator
  22 KB (3,469 words) - 22:50, 28 October 2014
• Final
  \documentclass[twocolumn,aip,cha]{revtex4-1} %\includegraphics[scale=1]{Fig.jpg}
  6 KB (870 words) - 10:20, 11 September 2012
• Group 1 2014
  [[File:Shear.png | thumb | 300px | Figure 1: Force gradient viewed from above.]] Where <math>\chi = \{ 0,-1,1 \}</math> indicates the direction of the particle's chirality, <math>g</mat
  10 KB (1,538 words) - 16:25, 12 December 2014
• Group 7
  === Single Inverted Pendulum, $N = 1$ === \epsilon = 0.450 + 1.799/\Omega^{2}
  27 KB (4,171 words) - 10:01, 12 January 2012
• Group 1 2012
  ...determines a smooth vector field on <math>\mathbb{R}^{2}\times \mathbb{S}^{1}</math> (a 3 dimensional space) and hence truly chaotic behavior is possibl ...nd the trajectories are curves of constant energy <math>E(x,\dot{x})=\frac{1}{2}\dot{x}^{2}+V(x)</math>. In this case it is easy to see that we have a s
  25 KB (4,001 words) - 22:50, 28 October 2014