1 / 126

Chapter 16

Chapter 16. Liquids and Solids. 16.1 Intermolecular Forces 16.2 The Liquid State 16.3 An Introduction to Structures and Types of Solids 16.4 Structure and Bonding in Metals 16.5 Carbon and Silicon: Network Atomic Solids 16.6 Molecular Solids 16.7 Ionic Solids

rhys
Télécharger la présentation

Chapter 16

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Chapter 16 Liquids and Solids

  2. 16.1 Intermolecular Forces 16.2 The Liquid State 16.3 An Introduction to Structures and Types of Solids 16.4 Structure and Bonding in Metals 16.5 Carbon and Silicon: Network Atomic Solids 16.6 Molecular Solids 16.7 Ionic Solids 16.8 Structures of Actual Ionic Solids 16.9 Lattice Defects 16.10 Vapor Pressure and Changes of State 16.11 Phase Diagrams Chapter 16: Liquids and Solids

  3. Red Beryl, Be3Al2Si6O18-

  4. Figure 16.1: Schematic representation of the three states of matter

  5. Figure 16.2: (a) The electrostatic interaction of two polar molecules. (b) The interaction of many dipoles in a condensed state.

  6. Figure 16.3: The polar water molecule.

  7. Figure 16.4: The boiling points of the covalent hydrides of elements in Groups 4A, 5A, 6A, and 7A.

  8. Figure 16.5: An instantaneous polarization can occur on atom a, creating instantaneous dipole.

  9. Relative Strength of Intermolecular Forces Ion - Ion Forces Strongest Attractive Forces Ion - Dipole Forces Dipole - Dipole Forces Ion - Induced Dipole Forces Dipole - Induced Dipole Forces London - Dispersive Forces Weakest Attractive Forces

  10. Figure 16.6: A molecule in the interior of a liquid is attracted to the molecules surrounding it, whereas a molecule at the surface of liquid is attracted only by molecules below it and on each side of it.

  11. Figure 16.7: Nonpolar liquid mercury forms a convex meniscus in a glass tube.

  12. Figure 16.8: Several crystalline solids Fluorite Rhodochrosite Pyrite Amethyst

  13. Figure 16.9: Three cubic unit cells and the corresponding lattices. Simple Cubic Body-centered Cubic Face-centered Cubic

  14. Figure 16.10: X-rays scattered from two different atoms may reinforce (constructive interference) or cancel (destructive interference) one another.

  15. Figure 16.11: Reflection of X rays of wavelength Bragg equation : nl = 2d sinJ

  16. A conch shell on a beach. Source: Corbis

  17. Figure 16.12: Examples of three types of crystalline solids. Elemental Ionic Molecular Solid Solid Solid

  18. The Hexagonal Structure of Ice Ice Structure with open holes giving Ice a density less than water it’s self. The delicate 6 point snow flake reflects the hexagonal structure.

  19. Figure 16.13: The closet packing arrangement of uniform spheres.

  20. Figure 16.14: When spheres are closest packed so that the spheres in the third layer are directly over those in the first layer (aba), the unit cell is the hexagonal prism illustrated here in red.

  21. Figure 16.15: When spheres are packed in the abc arrangement, the unit cell is face-centered cubic.

  22. A toy slide puzzle

  23. A section of a surface containing copper atoms (red) and an indium atom (yellow).

  24. Figure 16.17: The net number of spheres in a face-centered cubic unit cell.

  25. Figure 16.16: The indicated sphere has 12 equivalent nearest neighbors.

  26. Example 16.1 (P 780) Silver crystallizes in a cubic close packed structure. The radius of a sliver atom is 1.44A (14 pm). Calculate the density of Ag. Density = mass per unit volume. Use the Pythagorean theorem to calculate the edge of the cube “d” and then the cubic volume. d2 + d2 = (4r)2 d = 8r2 = r 8 since r = 1.44 A d = 1.44 A ( 8 ) = 4.07 A Volume of the unit cell = d3 = (4.07 A) = 67.4 A3 67.4 A3 x ( )3 = 6.74 x 10-23 cm3 In the face-centered cubic there are 4 atoms per cell: Density = Density = _________ g/cm3 1.00 x 10-8 cm A (4 atoms)(1.07.9 g/mol)(6.022 x 1023 atoms/mol) 6.74 x 10-23 cm3

  27. Volume of a unit cell (2r, 4r, r)

  28. Figure 16.18: In the body-centered cubic unit cell the spheres touch along the body diagonal.

  29. Figure 16.19: The body-centered cubic unit cell with the center sphere deleted.

  30. Figure 16.20: On the face of the body-centered cubic unit cell.

  31. Figure 16.21: The relationship of the body diagonal (b) to the face diagonal (f) and the edge (e) for the body-centered cubic unit cell.

  32. Figure 16.22: The electron sea model for metals postulates a regular array of cations in a "sea" of valence electrons.

  33. Figure 16.23: The molecular orbital energy levels produced when various numbers of atomic orbitals interact.

  34. Figure 16.24: A representation of the energy levels (bands) in a magnesium crystal

  35. Grains of nanophase palladium magnified 200,000 times by an electron microscope. Source: Nanophase Technologies Corporation

  36. Metal Alloys Alloy: a substance that contains mixture of elements and has metallic properties Substitutional alloy: some host metal atoms are replaced by other atoms of similar size Brass: ~66% copper, ~33% zinc (fig 16.25a) Sterling silver: 93% silver, 7% copper Pewter: 85% tin, 7% copper, 6% bismuth, and 2% antimony Plumbers solder: 67% lead, 33% tin Interstitial alloy: some of the interstices (holes) are filled by smaller atoms Mild steels: >0.2% carbon; Medium steels: 0.2-0.6% carbon, High carbon steels: 0.6-1.5% carbon (fig 16.25b)

  37. Figure 16.25: Two types of alloys

More Related