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  1. Descriptive Inorganic Chemistry, DIC, Fifth edition, 5 edition
  2. Chapter 1 even answers:
  3. 1
  4. Chapter 1
  5. THE ELECTRONIC STRUCTURE OF THE ATOM: A REVIEW
  6. Exercises
  7. 1.2 (a) Region in space around a nucleus where the probability of finding an
  8. electron is high.
  9. (b) Orbital energy levels of the same energy.
  10. (c) When occupying orbitals of equal energy, it is energetically preferable
  11. for the electrons to adopt a parallel spin arrangement.
  12. 1.4 5.
  13. 1.6 6s.
  14. 1.8 The quantum number l relates to the orbital shape.
  15. 1.10 The pairing energy for the double occupancy of the 2s orbital is less than
  16. the energy separation of the 2s and 2p orbitals.
  17. 1.12 (a) [Ar]4s2; (b) [Ar]4s13d5; (c) [Xe]6s24f145d106p2.
  18. 1.14 (a) [Ar]; (b) [Ar]3d7; (c) [Ar]3d3.
  19. 1.16 2+ and 4+. Tin has a noble gas core ground-state electron configuration of
  20. [Kr]5s24d105p2. The two 5p electrons are lost first, giving an ion of 2+
  21. charge; the two 5s electrons are lost next, giving an ion of 4+ charge.
  22. 1.18 4+. Zirconium has a noble gas core ground-state electron configuration of
  23. [Ar]4s23d2. Thus loss of both the two 4s electrons and the two 3d
  24. electrons will give a 4+ ion.
  25. 2 Chapter 1
  26. 1.20 (a) 3; (b) 2; (c) 4.
  27. 1.22 (a) and (d).
  28. Beyond the Basics
  29. 1.24 The Dirac wave equation was developed by the English physicist P. A. M.
  30. Dirac. He applied the ideas of Einstein’s special theory of relativity to
  31. quantum mechanics. Dirac’s model requires four quantum numbers, not
  32. the three of the Schrödinger model (where the spin quantum number is not
  33. part of the solution to the equation). A fourth quantum number results
  34. from the special theory of relativity where events are defined by the three
  35. spatial coordinates plus a time coordinate.
  36. In the Dirac model, like the Schrödinger model, the principal
  37. quantum number, n, determines the size of an orbital. The other quantum
  38. numbers have different meanings—the third and the fourth (instead of the
  39. second) determine the shape of the orbitals. The shapes of the orbitals
  40. themselves differ from those using the Schrödinger equation, and there are
  41. no nodes. This removes the conceptual problem of how an electron moves
  42. from one lobe of a p orbital to the other if there is a zero probability in
  43. between. The answer is that the ―simplistic‖ Schrödinger equation is in
  44. error. For high-atomic-number atoms, relativistic effects become of
  45. increasing importance and the Schrödinger equation becomes inadequate;
  46. the Dirac equation must be used.
  47. For a good introduction to the Dirac equation, see R. E. Powell,
  48. Relativistic Quantum Chemistry, J. Chem. Educ. 45 (1968): 558–563.
  49. 1.26 Curium. [Rn]7s
  50. 2
  51. 5f
  52. 7
  53. 6d
  54. 1
  55. .
  56. 1.28 Of course, one can argue that orbitals are human constructs only! This
  57. question is a good topic for debate, but these authors veers toward the
  58. view that an orbital actually exists only when it is populated. Empty
  59. orbitals only potentially exist.

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