Metallic and Ionic Solids Section 13.4 Copyright © 1999 by Harcourt Brace & Company All rights reserved. Requests for permission to make copies of any part of the work should be mailed to: Permissions Department, Harcourt Brace & Company, 6277 Sea Harbor Drive, Orlando, Florida Types of Solids Table 13.6 TYPE EXAMPLE FORCE Ionic NaCl, CaF2, ZnS Ion-ion Metallic Na, Fe Metallic Molecular Ice, I2 Dipole Ind. dipole Network Extended covalent Diamond Graphite Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Types of Solids Type Built from Examples Amorphous Covalently bonded network with limited ordering Glass, plastics, polymers Ionic + and – ions NaCl, CsCl, (NH4)2SO4 Metallic Atoms or metallic ions in sea of e- Molecular Molecules with internal covalent bonds, and intramolcular attractions: dipole-dipole, Hbond, London dispersion H 2 , ice, I2, CH30H Network Atoms held in network covalent bonds Graphite, diamond, quartz Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Properties of Solids 1. Molecules, atoms or ions locked into a CRYSTAL LATTICE 2. Particles are CLOSE together 3. STRONG IM forces 4. Highly ordered, rigid, incompressible Copyright (c) 1999 by Harcourt Brace & Company All rights reserved ZnS, zinc sulfide Crystal Lattices Regular 3-D arrangements of equivalent LATTICE POINTS in space. The lattice points define UNIT CELLS, the smallest repeating internal unit that has the symmetry characteristic of the solid. There are 7 basic crystal systems, but we are only concerned with CUBIC. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Cubic Unit Cells All sides equal length All angles are 90 degrees Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Cubic Unit Cells Figure 13.28 Metals have unit cells that are • simple cubic (SC) • body centered cubic (BCC) • face centered cubic (FCC) Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Simple Cubic Unit Cell Figure 13.28 • Simple cubic unit cell. • Note that each atom is at a corner of a unit cell and is shared among 8 unit cells. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Body-Centered Cubic Unit Cell Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Body Centered Cubic Unit Cell • Has 8 identical atoms or ions at the corners and additional particle at the center of the cube • Total of two particles in the unit cell • Ex: alkali metals, iron, K, Na, Ba, Ce, Li, V Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Face Centered Cubic Unit Cell Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Face Centered Cubic Unit Cell • There is a particle in each of the six faces of the cube in addition to the those at the corners • Each particle in the face of the cube is shared equally between two unit cells (1/2 of particle is within unit cell) • 4 atoms/ions within the unit cell Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Crystal Lattices—Packing of Atoms or Ions Assume atoms are hard spheres and that crystals are built by PACKING of these spheres as efficiently as possible. FCC is more efficient than either BC or SC. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved See Closer Look, pp. 622-623 Crystal Lattices—Packing of Atoms or Ions Packing of C60 molecules. They are arranged at the lattice points of a FCC lattice. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Crystal Lattices and Unit Cells Unit Cell is the smallest repeating unit that retains the symmetry properties of the Lattice Cubic Cells Copyright (c) 1999 by Harcourt Brace & Company All rights reserved An Atom in this corner is shared by eight unit cells sc Copyright (c) 1999 by Harcourt Brace & Company All rights reserved fcc bcc The cubic crystal lattices are of three types 1. simple cubic (sc) 8 x 1/8 atom per corner = one atom per cell 2. body-centered cubic (bcc) 8 x 1/8 atoms per corner + one atom in center = 2 atoms / cell 3. face-centered cubic (fcc) 8 x 1/8 atom / corner + ½ atom per side x 6 sides = 4 atoms per cell Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Density can be used to find atomic radius if type of crystal is known. For fcc 2 x cell edge e2 + e2 = l 2 l 2 = 2e2 l = 2 e l = four atom radii Volume of cell = e3 Copyright (c) 1999 by Harcourt Brace & Company All rights reserved d = m /V • density of metal = mass of cell/ Volume • Mass of cell is mass of four atoms of metal • Mass of cell = atom mass / mol x 1mol/ 6.022 x1023 atoms x 4 atom/cell Example: the density of Al is 2.699 g/cm3 the Volume of a unit cell is 6.640 x 10-23 cm3 and the atomic radius is then 143 pm l = 2 e l = four atom radii Volume of cell = e3 Copyright (c) 1999 by Harcourt Brace & Company All rights reserved For Iron which has a bcc unit cell the calculation is a little different The Density of Iron is 7.8470 g/cm3 2 e Copyright (c) 1999 by Harcourt Brace & Company All rights reserved D2 = (2 e)2+ e2 = 3e2 D = 3 e D e D2 = (2 e)2+ e2 = 3e2 D = 3 e 2 e There are two atoms per unit cell Volume of cell = e3 e = D/3 V = e3= m/density D=4xr m = 2 x 55.85 g/6.022 x 1023 atoms atom mass of Fe = 55.85 g/mol e3 = 1.85 x 10-22/ 7.8470 g/cm3 -8 cm e = 2.87 x 10 Copyright (c) 1999 by Harcourt Brace & Company All rights reserved This gives cell edge of 287 pm and r = 124 pm Finding the Lattice Type To find out if a metal is SC, BCC or FCC, use the known radius and density of an atom to calc. no. of atoms per unit cell. PROBLEM Al has density = 2.699 g/cm3 and Al radius = 143 pm. Verify that Al is FCC. SOLUTION 1. Calc. unit cell volume Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Finding the Lattice Type PROBLEM Al has density = 2.699 g/cm3 and Al radius = 143 pm. Verify that Al is FCC. SOLUTION 1. Calc. unit cell volume V = (cell edge)3 Edge distance comes from face diagonal. Diagonal distance = 2 • edge Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Finding the Lattice Type PROBLEM Al has density = 2.699 g/cm3 and Al radius = 143 pm. Verify that Al is FCC. SOLUTION V = (cell edge)3 and face diagonal = 2 • edge (Diagonal)2 = 2 (edge)2 Therefore, Diag = 2 • (edge) Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Finding the Lattice Type PROBLEM Al has density = 2.699 g/cm3 and Al radius = 143 pm. Verify that Al is FCC. SOLUTION Here diagonal = 4 • radius of Al = 572 pm Therefore, edge = 572 pm / 2 = 404 pm In centimeters, edge = 4.04 x 10-8 cm So, V of unit cell = (4.04 x 10-8 cm)3 V = 6.62 x 10-23 cm3 Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Finding the Lattice Type PROBLEM Al has density = 2.699 g/cm3 and Al radius = 143 pm. Verify that Al is FCC. SOLUTION 2. Use V and density to calc. mass of unit cell from DENS = MASS / VOL Mass = density • volume = (6.62 x 10-23 cm3)(2.699 g/cm3) = 1.79 x 10-22 g/unit cell Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Finding the Lattice Type PROBLEM Al has density = 2.699 g/cm3 and Al radius = 143 pm. Verify that Al is FCC. SOLUTION 3. Calculate number of Al per unit cell from mass of unit cell. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Finding the Lattice Type PROBLEM Al has density = 2.699 g/cm3 and Al radius = 143 pm. Verify that Al is FCC. SOLUTION 3. Calculate number of Al per unit cell from mass of unit cell. 26.98 g 1 mol Mass 1 Al atom = • mol 6.022 x 1023 atoms 1 atom = 4.480 x 10-23 g, so Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Finding the Lattice Type PROBLEM Al has density = 2.699 g/cm3 and Al radius = 143 pm. Verify that Al is FCC. SOLUTION 3. Calculate number of Al per unit cell from mass of unit cell. 26.98 g 1 mol Mass 1 Al atom = • mol 6.022 x 1023 atoms 1 atom = 4.480 x 10-23 g, so 1.79 x 10-22 g 1 atom • = 3.99 Al atoms/unit cell -23 unit cell 4.480 x 10 g Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Number of Atoms per Unit Cell How can there be 4 atoms in a unit cell? 1. Each corner Al is 1/8 inside the unit cell. 8 corners (1/8 Al per corner) = 1 net Al 2. Each face Al is 1/2 inside the cell 6 faces (1/2 per face) = 3 net Al’s Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Number of Atoms per Unit Cell Unit Cell Type Net Number Atoms FCC 4 SC 1 BCC 2 Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Simple Ionic Compounds Lattices of many simple ionic solids are built by taking a SC or FCC lattice of ions of one type and placing ions of opposite charge in the holes in the lattice. EXAMPLE: CsCl has a SC lattice of Cs+ ions with Cl- in the center. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Simple Ionic Compounds CsCl has a SC lattice of Cs+ ions with Cl- in the center. 1 unit cell has 1 Cl- ion plus (8 corners)(1/8 Cs+ per corner) = 1 net Cs+ ion. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Simple Ionic Compounds Salts with formula MX can have SC structure — but not salts with formula MX2 or M2X Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Simple Ionic Compounds Many common salts have FCC arrangements of anions with cations in OCTAHEDRAL HOLES — e.g., salts such as CA = NaCl • FCC lattice of anions ----> 4 A-/unit cell • C+ in octahedral holes ---> 1 C+ at center + [12 edges • 1/4 C+ per edge] = 4 C+ per unit cell Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Construction of NaCl We begin with a cube of Cl- ions. Add more Cl- ions in the cube faces, and then add Na+ ion in the octahedral holes. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved The Sodium Chloride Lattice Na+ ions are in OCTAHEDRAL holes in a face-centered cubic lattice of Clions. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Comparing NaCl and CsCl • Even though their formulas have one cation and one anion, the lattices of CsCl and NaCl are different. • The different lattices arise from the fact that a Cs+ ion is much larger than a Na+ ion. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Common Ionic Solids Titanium dioxide, TiO2 There are 2 net Ti4+ ions and 4 net O2- ions per unit cell. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Common Ionic Solids • Zinc sulfide, ZnS • The S2- ions are in TETRAHEDRAL holes in the Zn2+ FCC lattice. • This gives 4 net Zn2+ ions and 4 net S2- ions. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Common Ionic Solids • Fluorite or CaF2 • FCC lattice of Ca2+ ions • This gives 4 net Ca2+ ions. • F- ions in all 8 tetrahedral holes. • This gives 8 net Fions. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Summary Ionic Solids • Compounds with formula MX are commonly either sc or fcc • Many salts have NaCl structure (fcc) especially alkali metals • Exceptions are CsCl, CsBr, CsI, alkaline oxides and sulfides, and oxides of 4th row transition metals (MO) • Formulas can always be found from unit cell structure Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Types of Solids Table 13.6 TYPE EXAMPLE FORCE Ionic NaCl, CaF2, ZnS Ion-ion Metallic Na, Fe Metallic Molecular Ice, I2 Dipole Ind. dipole Network Extended covalent Diamond Graphite Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Molecular Solids • Covalently bonded molecules • Arrangement depends on shape of molecules and types of IM forces • Ex: Ice molecules pack densely and maximize their attraction Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Network Solids • Covalently bonded atoms • High mp’s and bp’s, hard, rigid, and high energy required to break bonds • Ex: graphite, diamond, elemental silicon, silica • Silicon exists in diamond structure • Silicates – made of silicon and oxygen (ex: sand, talc, quartz) Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Network Solids Diamond Graphite Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Network Solids A comparison of diamond (pure carbon) with silicon. Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Amorphous Solids • Properties –Solid lacks regular structures –Has a melting range –Restrictive movement of molecules –Unable to identify unit cell in solid phase –Breaks in random pieces • Examples: glass, polymers, nylon Copyright (c) 1999 by Harcourt Brace & Company All rights reserved Properties of Solids • Melting point – the crystal lattice of a solid breaks converting to a liquid • Enthalpy of fusion – energy needed to convert one mole from sl – increase in with increasing MW due to strength of IM forces – Increase in ionic compounds due to increase in lattice energy (depends on size and charge) • Sublimation – conversion of a solid to a gas Copyright (c) 1999 by Harcourt Brace & Company All rights reserved