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Copyright©2000 by Houghton Mifflin Company. All rights reserved.

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1 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
Ideal gas …has no volume and no mutual attraction. Sometimes called a point mass. Therefore a balloon inflates not because of the volume but because of the motion of the particles. Copyright©2000 by Houghton Mifflin Company. All rights reserved.

2 Intermolecular Forces
Forces between (rather than within) molecules. dipole-dipole attraction: molecules with dipoles orient themselves so that “+” and “” ends of the dipoles are close to each other. Copyright©2000 by Houghton Mifflin Company. All rights reserved.

3 Copyright©2000 by Houghton Mifflin Company. All rights reserved.

4 Intermolecular Forces
Forces between (rather than within) molecules. dipole-dipole attraction: molecules with dipoles orient themselves so that “+” and “” ends of the dipoles are close to each other. hydrogen bonds: dipole-dipole attraction in which hydrogen is bound to a highly electronegative atom. (F, O, N) Copyright©2000 by Houghton Mifflin Company. All rights reserved.

5 Intermolecular Forces
Copyright©2000 by Houghton Mifflin Company. All rights reserved.

6 London Dispersion Forces
relatively weak forces that exist among noble gas atoms and nonpolar molecules. (Ar, C8H18) caused by instantaneous dipole, in which electron distribution becomes asymmetrical. Copyright©2000 by Houghton Mifflin Company. All rights reserved.

7 London Dispersion Forces
Copyright©2000 by Houghton Mifflin Company. All rights reserved.

8 London Dispersion Forces
relatively weak forces that exist among noble gas atoms and nonpolar molecules. (Ar, C8H18) caused by instantaneous dipole, in which electron distribution becomes asymmetrical. the ease with which electron “cloud” of an atom can be distorted is called polarizability. Copyright©2000 by Houghton Mifflin Company. All rights reserved.

9 Some Properties of a Liquid
Surface Tension: The resistance to an increase in its surface area (polar molecules). Copyright©2000 by Houghton Mifflin Company. All rights reserved.

10 Some Properties of a Liquid
Copyright©2000 by Houghton Mifflin Company. All rights reserved.

11 Some Properties of a Liquid
Surface Tension: The resistance to an increase in its surface area (polar molecules). Capillary Action: Spontaneous rising of a liquid in a narrow tube. Copyright©2000 by Houghton Mifflin Company. All rights reserved.

12 Some Properties of a Liquid
Copyright©2000 by Houghton Mifflin Company. All rights reserved.

13 Some Properties of a Liquid
Surface Tension: The resistance to an increase in its surface area (polar molecules). Capillary Action: Spontaneous rising of a liquid in a narrow tube. Viscosity: Resistance to flow (molecules with large intermolecular forces). Copyright©2000 by Houghton Mifflin Company. All rights reserved.

14 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
Types of Solids Crystalline Solids: highly regular arrangement of their components [table salt (NaCl), pyrite (FeS2)]. Amorphous solids: considerable disorder in their structures (glass). Copyright©2000 by Houghton Mifflin Company. All rights reserved.

15 Representation of Components in a Crystalline Solid
Lattice: A 3-dimensional system of points designating the centers of components (atoms, ions, or molecules) that make up the substance. Copyright©2000 by Houghton Mifflin Company. All rights reserved.

16 Representation of Components in a Crystalline Solid
Unit Cell: The smallest repeating unit of the lattice. simple cubic body-centered cubic face-centered cubic Copyright©2000 by Houghton Mifflin Company. All rights reserved.

17 Representation of Components in a Crystalline Solid
Copyright©2000 by Houghton Mifflin Company. All rights reserved.

18 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
Bragg Equation Used for analysis of crystal structures. n = 2d sin  d = distance between atoms n = an integer  = wavelength of the x-rays Copyright©2000 by Houghton Mifflin Company. All rights reserved.

19 Types of Crystalline Solids
Ionic Solid: contains ions at the points of the lattice that describe the structure of the solid (NaCl). Molecular Solid: discrete covalently bonded molecules at each of its lattice points (sucrose, ice). Copyright©2000 by Houghton Mifflin Company. All rights reserved.

20 Types of Crystalline Solids
Copyright©2000 by Houghton Mifflin Company. All rights reserved.

21 Types of Crystalline Solids
Copyright©2000 by Houghton Mifflin Company. All rights reserved.

22 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
Packing in Metals Model: Packing uniform, hard spheres to best use available space. This is called closest packing. Each atom has 12 nearest neighbors. hexagonal closest packed (“aba”) cubic closest packed (“abc”) Copyright©2000 by Houghton Mifflin Company. All rights reserved.

23 Bonding Models for Metals
Electron Sea Model: A regular array of metals in a “sea” of electrons. Band (Molecular Orbital) Model: Electrons assumed to travel around metal crystal in MOs formed from valence atomic orbitals of metal atoms. Copyright©2000 by Houghton Mifflin Company. All rights reserved.

24 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
Metal Alloys Substances that have a mixture of elements and metallic properties. 1. Substitutional Alloy: some metal atoms replaced by others of similar size. brass = Cu/Zn Copyright©2000 by Houghton Mifflin Company. All rights reserved.

25 Metal Alloys (continued)
2. Interstitial Alloy: Interstices (holes) in closest packed metal structure are occupied by small atoms. steel = iron + carbon Copyright©2000 by Houghton Mifflin Company. All rights reserved.

26 Metal Alloys (continued)
Copyright©2000 by Houghton Mifflin Company. All rights reserved.

27 Metal Alloys (continued)
2. Interstitial Alloy: Interstices (holes) in closest packed metal structure are occupied by small atoms. steel = iron + carbon 3. Both types: Alloy steels contain a mix of substitutional (carbon) and interstitial (Cr, Mo) alloys. Copyright©2000 by Houghton Mifflin Company. All rights reserved.

28 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
Network Solids Copyright©2000 by Houghton Mifflin Company. All rights reserved.

29 Network Solids Composed of strong directional covalent bonds that are best viewed as a “giant molecule”. brittle do not conduct heat or electricity carbon, silicon-based graphite, diamond, ceramics, glass Copyright©2000 by Houghton Mifflin Company. All rights reserved.

30 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
Network Solids Copyright©2000 by Houghton Mifflin Company. All rights reserved.

31 Copyright©2000 by Houghton Mifflin Company. All rights reserved.

32 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
Semiconductors A substance in which some electrons can cross the band gap. Conductivity is enhanced by doping with group 3a or group 5a elements. Copyright©2000 by Houghton Mifflin Company. All rights reserved.

33 Vapor Pressure . . . is the pressure of the vapor present at equilibrium. . . . is determined principally by the size of the intermolecular forces in the liquid. . . . increases significantly with temperature. Volatile liquids have high vapor pressures. Copyright©2000 by Houghton Mifflin Company. All rights reserved.

34 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
Vapor Pressure The more electrons a substance has the more polarizable it is, and the greater are the dispersion forces. Copyright©2000 by Houghton Mifflin Company. All rights reserved.

35 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
Vapor Pressure Copyright©2000 by Houghton Mifflin Company. All rights reserved.

36 Melting Point Molecules break loose from lattice points and solid changes to liquid. (Temperature is constant as melting occurs.) vapor pressure of solid = vapor pressure of liquid Copyright©2000 by Houghton Mifflin Company. All rights reserved.

37 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
Boiling Point Constant temperature when added energy is used to vaporize the liquid. vapor pressure of liquid = pressure of surrounding atmosphere Copyright©2000 by Houghton Mifflin Company. All rights reserved.

38 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
Phase Diagram Represents phases as a function of temperature and pressure. critical temperature: temperature above which the vapor can not be liquefied. critical pressure: pressure required to liquefy AT the critical temperature. critical point: critical temperature and pressure (for water, Tc = 374°C and 218 atm). Copyright©2000 by Houghton Mifflin Company. All rights reserved.

39 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
Phase Diagram Copyright©2000 by Houghton Mifflin Company. All rights reserved.

40 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
Phase Diagram Copyright©2000 by Houghton Mifflin Company. All rights reserved.


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