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Nonlinearity: From Nature to Plasma Waleed Moslem Port Said University The British University 1 / 74 Aim of the lecture History + Science + Fun Lecture How the scientific research was developed Learn how to think.....not what


  1. Nonlinearity: From Nature to Plasma Waleed Moslem Port Said University The British University 1 / 74

  2. Aim of the lecture ● History + Science + Fun → Lecture ● How the scientific research was developed ● Learn how to think.....not what to think 2 / 74

  3. Outline ● Why Nature? ● Soliton ● Cnoidal ● Tsunami ● Envelope Soliotn ● Rogon ● Mach Cones ● Wakefield 3 / 74

  4. Outline ● Why Nature? ● Soliton ● Cnoidal ● Tsunami ● Envelope Soliotn ● Rogon ● Mach Cones ● Wakefield 4 / 74

  5. Why Nature? ● Nature → (Matter & Motion & Energy & Force….) → Physics → How the Universe Behaves ● Movie ● Conclusion: Development of new products → Improvement/development our modern-day society 5 / 74

  6. Outline ● Why Nature? ● Soliton ● Cnoidal ● Tsunami ● Envelope Soliotn ● Rogon ● Mach Cones ● Wakefield 6 / 74

  7. Soliton ● In 1834, while conducting experiments to determine the most efficient design for canal boats, he discovered a phenomenon that he described as the wave of translation . ● Stable – Large distances – Speed(size) – Width(depth) – Never merge – Splits into two John Scott Russell waves (1808-1882) 7 / 74

  8. Soliton, cont. 8 / 74

  9. Soliton, cont. ● 89.3 m long ● 4.13 m wide ● 1.52 m deep J. S. Russell Aqueduct 9 / 74

  10. Soliton, cont. e v a w y r a t i l o S 10 / 74

  11. Soliton, cont. Gustav de Vries Diederik Johannes Korteweg (1866 – 1934) (1848 – 1941) 11 / 74

  12. Soliton, cont. 3 u u u    0 u       3 x x t   Nonlinearity Dispersion Korteweg-de Vries Equation (1895) 12 / 74

  13. Soliton, cont. Linear & Nondispersive Linear & Dispersive Nonlinear & Nondispersive 13 / 74

  14. Soliton, cont. ● Zabusky & Kruskal (1965) → numerically → solutions seemed to decompose at large times into a collection of "solitons" ● Shallow-water waves ● Long internal waves in ocean (Tsunami) ● Ion acoustic waves in a plasma ● Acoustic waves on a crystal lattice ● Also, soliton exists in biology 14 / 74

  15. Soliton, cont. ● Solitary Waves → Movie 1 ● Soliton → Movie 2 & Movie 3 15 / 74

  16. Soliton, cont. 16 / 74

  17. Outline ● Why Nature? ● Soliton ● Cnoidal ● Tsunami ● Envelope Soliotn ● Rogon ● Mach Cones ● Wakefield 17 / 74

  18. Cnoidal ● Korteweg and de Vries → 1895 → KdV Eq. ● Jacobi elliptic function cn , which is why they are coined cnoidal waves ● In the limit of infinite wavelength → the cnoidal wave becomes a solitary wave. ● Surface water waves & Ion-acoustic waves in plasma physics & Optical fiber & Graphene-based superlattice & Solids & Traffic flow…….etc 18 / 74

  19. Cnoidal, cont. 19 / 74

  20. Cnoidal, cont. ● Soliton vs. Cnoidal ● Soliton → vanishing boundary condition at infinity ● Cnoidal → soliton formation in a periodic wave train 20 / 74

  21. Cnoidal, cont. 21 / 74

  22. Outline ● Why Nature? ● Soliton ● Cnoidal ● Tsunami ● Envelope Soliotn ● Rogon ● Mach Cones ● Wakefield 22 / 74

  23. Tsunami ● Soliton ~ Cnoidal ● What do you do if you’re at the seaside, and notice the sea gradually withdrawing and the water getting further and further away, further than for ordinary tides? ● Catastrophic water accident → Tsunami ● Movies 1, 2 23 / 74

  24. Tsunami, cont. ● Challenge: search for a credible role that mathematicians can play in predicting their danger or in alleviating their impact ● Where is it feasible for Mathematics to contribute to the problem of tsunamis? ✔ Modeling of tsunami wave generation and propagation across oceans ✔ Design of early warning systems (or some of its components) ✔ Clarification of the character of tsunami waves 24 / 74

  25. Tsunami, cont. 25 / 74

  26. Tsunami, cont. 26 / 74

  27. Tsunami, cont. 27 / 74

  28. Tsunami, cont. 28 / 74

  29. Tsunami, cont. 29 / 74

  30. Soliton & Cnoidal & Tsunami 30 / 74

  31. Outline ● Why Nature? ● Soliton ● Cnoidal ● Tsunami ● Envelope Soliotn ● Rogon ● Mach Cones ● Wakefield 31 / 74

  32. Envelope Soliotn 32 / 74

  33. Envelope Soliotn, cont. ● The amplitude of the harmonic wave may vary in space and time ● Understanding the time scales 33 / 74

  34. Envelope Soliotn, cont. ● This modulation due to nonlinearity may be strong enogh to lead to the formation of envelope soliton ● Three forms of envelope: bright, dark, and Gray ● Evloution equation → Nonlinear Schrödinger Eq. 34 / 74

  35. Envelope Soliotn, cont. 35 / 74

  36. Envelope Soliotn, cont. 36 / 74

  37. Envelope Soliotn, cont. 37 / 74

  38. Envelope Soliotn, cont. 38 / 74

  39. Envelope Soliotn, cont. ● 1973: Akira Hasegawa of AT&T Bell Labs was the first to suggest that envelope solitons could exist in optical fibers. ● 1973: Robin Bullough made the first mathematical report of the existence of optical solitons → suggest its application in optical telecommunications. ● 1987: Emplit et al. made the first experimental observation of the propagation of a dark soliton, in an optical fiber. ● 1970‘s: Starting the Nonlinear Plasma Physics Era 39 / 74

  40. Envelope Soliotn, cont. 40 / 74

  41. Outline ● Why Nature? ● Soliton ● Cnoidal ● Tsunami ● Envelope Soliotn ● Rogon ● Mach Cones ● Wakefield 41 / 74

  42. Rogon (Rogue wave) Freak Freak Freak Freak waves waves waves waves Giant Giant Giant Giant Rogue Rogue Rogue Rogue waves waves waves waves waves waves waves waves Extreme Extreme Extreme Extreme waves waves waves waves 42 / 74

  43. Rogue waves ● H H max =25.6 m & 1 in 200,000 waves max =25.6 m & 1 in 200,000 waves ● Extreme waves → appear from nowhere → high-energy Extreme waves → appear from nowhere → high-energy → high amplitude → carry dramatic impact → high amplitude → carry dramatic impact ● How this wave exist? → Use & Avoid How this wave exist? → Use & Avoid ● Movie 43 / 74 Movie 1 1

  44. Rogue waves, cont. 44 / 74

  45. Rogue waves, cont. 45 / 74

  46. Rogue waves, cont. 46 / 74

  47. Rogue waves, cont. 47 / 74

  48. Rogue waves, cont. ● How to create/control rogue waves? ● Why? ● Movie 1 48 / 74

  49. Rogue waves, cont. 49 / 74

  50. Rogue waves, cont. 50 / 74

  51. Rogue waves, cont. 51 / 74

  52. Rogue waves, cont. 52 / 74

  53. Rogue waves, cont. 53 / 74

  54. Rogue waves, cont. 54 / 74

  55. Some Physical Applications of Soliton Equations ● Electrical transmission ● Protein dynamics and lines DNA ● General relativity ● Quantum field theory ● Josephson junctions and ● Rossby waves superconductors ● Statistical mechanics ● Liquid crystals ● Stratified fluids ● Optical fibres and ● Water waves in channels, telecommunications shallow water and the ● Plasma physics ocean ● B-E condensate ● Waves in lattices, rods and 55 / 74 strings

  56. Outline ● Why Nature? ● Soliton ● Cnoidal ● Tsunami ● Envelope Soliotn ● Rogon ● Mach Cones ● Wakefield 56 / 74

  57. Mach Cones ● When an object moves through the air it pushes the air in front of it away, creating a pressure wave. ● This pressure wave travels away from the object at the speed of sound. ● If the object itself is travelling at the speed of sound then these pressure waves build up on top of each other to create a shock wave 57 / 74

  58. Mach Cones, cont. 58 / 74

  59. Mach Cones, cont. ● Movie Overlapping Shock Cone Wavefronts Subsonic Mach Supersonic speed One speed 59 / 74

  60. Mach Cones, cont. ● Astronomical scales (e.g. the Earth’s magnetotail formed by interaction with the solar wind) ● microscopic scales (e.g. Cherenkov radiation created by rapidly moving elementary charge) ● Havnes et al (1995, 1996b) theoretically predicted the existence of super DA Mach cones in dusty plasmas that are relevant to planetary rings and interstellar space. 60 / 74

  61. Mach Cones, cont. 61 / 74

  62. Mach Cones, cont. 62 / 74

  63. Outline ● Why Nature? ● Soliton ● Cnoidal ● Tsunami ● Envelope Soliotn ● Rogon ● Mach Cones ● Wakefield 63 / 74

  64. Wakefield, cont. ● In 1979 John Dawson, in a paper with T. Tajima, proposed that Landau damping effect could be used to accelerate particles ● In plasma, there are electrons both faster and slower than the wave. 64 / 74

  65. Wakefield, cont. 65 / 74

  66. Wakefield, cont. ● There were two early ideas on plasma accelerators: beatwave and wakefield . 66 / 74

  67. Wakefield, cont. a) No Plasma → Only electron beam with 1 GeV energy. b) 10 cm long lithium plasma → the core of the electron bunch has lost energy driving the plasma wake while particles in the back of the bunch have been accelerated to 2.7 GeV 67 / 74

  68. Wakefield, cont. Duck effect 68 / 74

  69. Wakefield, cont. 69 / 74

  70. Wakefield, cont. The charged particles having the same polarity can attract each other...!! 70 / 74

  71. Wakefield, cont. 71 / 74

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