Quantum Stars by Professor G Srinivasan

Quantum Stars by Professor G Srinivasan

International Centre for Theoretical Sciences via YouTube Direct link

Sir Arthur Eddington, at the meeting of the Royal Astronomical Society in London in 1935.

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58 of 61

Sir Arthur Eddington, at the meeting of the Royal Astronomical Society in London in 1935.

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Quantum Stars by Professor G Srinivasan

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  1. 1 Summer course 2018 - A Random walk in astro-physics
  2. 2 Quantum Stars Lecture - 10
  3. 3 The strange companion of Sirius!
  4. 4 Are such super-dense stars doomed?
  5. 5 What will happen to the star when the nuclear reactor at its center fails?
  6. 6 Sir Ralph Howard Fowler 1889-1944
  7. 7 Quantum Physics
  8. 8 Energy levels of a particle in a one-dimensional box
  9. 9 Heisenberg's Uncertainty Principle
  10. 10 White Dwarfs are Quantum Stars
  11. 11 White Dwarfs are for ever!
  12. 12 Enter Chandra: 1928
  13. 13 Radiation Pressure
  14. 14 Hydrostatic Equilibrium
  15. 15 Gaseous Star & Quantum Star
  16. 16 Classical Physics: All momentum values are allowed.
  17. 17 Quantum Physics
  18. 18 Pauli's exclusion principle allows us to put two fermions in a cell in phase space.
  19. 19 Fermi Momentum
  20. 20 Fermi Energy
  21. 21 Pressure of an ideal classical gas
  22. 22 Pressure of a Fermi gas at T=0 K
  23. 23 Chandrasekhar's Theory of White Dwarfs
  24. 24 Chandrasekhar's Theory of White Dwarfs 1930
  25. 25 Mass - Radius Relation for White Dwarfs S. Chandrasekhar, 1930
  26. 26 Stars of all mass will find their ultimate peace as Quantum Stars supported by the pressure of electrons.
  27. 27 Diamonds in the sky!
  28. 28 History is made
  29. 29 Gravitational Collapse of massive white dwarfs
  30. 30 Relativistic Fermi Gas
  31. 31 Relativistic White Dwarfs
  32. 32 A fully relativistic WD has no radius! But it has a unique mass!
  33. 33 Mass - Radius Relation for White Dwarfs S. Chandrasekhar, 1934
  34. 34 Chandrasekhar Limit
  35. 35 Supernovae and Neutron Stars
  36. 36 Guest Stars
  37. 37 Supernovae and Cosmic Rays by W. Baade and F. Zwicky
  38. 38 Supernova Explosion
  39. 39 Between 1932 and 1937:
  40. 40 Lev Landau
  41. 41 Landau invents neutron stars in 1938
  42. 42 Neutronization of matter at high density
  43. 43 Dynamical instability
  44. 44 The maximum mass of neutron stars
  45. 45 Tolman, Oppenheimer, Volkoff equation
  46. 46 OV: Oppenheimer - Volkoff Equation of State
  47. 47 Oppenheimer and Volkoff, 1938
  48. 48 Limiting Mass for Neutron Stars
  49. 49 The fate of massive stars
  50. 50 If radiation pressure exceeds 9.2 percent of the total pressure then matter will never become degenerate no matter what the density is.
  51. 51 Condition for degeneracy
  52. 52 Radiation pressure and Degeneracy
  53. 53 Ideal gas versus relativistic degeneracy
  54. 54 Why are there only two classes of 'cold stars'?
  55. 55 Stability of Matter
  56. 56 HW: Harrison - Wheeler Equation of State OV: Oppenheimer - Volkoff Equation of State
  57. 57 There are only two types of cold stars in nature!
  58. 58 Sir Arthur Eddington, at the meeting of the Royal Astronomical Society in London in 1935.
  59. 59 Chandrasekhar Limit
  60. 60 Next Lecture: A Journey to the center of a Neutron Star
  61. 61 Q&A

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