Point coordinates. Point coordinates for unit cell center are. Point coordinates for unit cell corner are 111


 Mavis Cain
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1 Point coordinates c z 111 Point coordinates for unit cell center are a/2, b/2, c/2 ½ ½ ½ Point coordinates for unit cell corner are 111 x a z 000 b 2c y Translation: integer multiple of lattice constants identical position in another unit cell b y 1
2 Directions z Algorithm y 1. Vector repositioned (if necessary) to pass through origin. 2. Read off projections in terms of unit cell dimensions a, b, and c 3. Adjust to smallest integer values 4. Enclose in square brackets, no commas [xyz] x ex: 1, 0, ½ => 2, 0, 1 => [ 201 ] 1, 1, 1 => [ 111 ] where overbar represents a negative index families of directions <xyz> 2
3 Crystallographic planes Miller Indices: Reciprocals of the (three) axial intercepts for a plane, cleared of fractions & common multiples. All parallel planes have same Miller indices. Algorithm 1. Read off intercepts of plane with axes in terms of a, b, c 2. Take reciprocals of intercepts 3. Reduce to smallest integer values 4. Enclose in parentheses, no commas i.e., (hkl) z example a b c 1. Intercepts 1 1 c 2. Reciprocals 1/1 1/1 1/ 3. Reduction Miller Indices (110) a b y x 3
4 Crystallographic planes example a b c z 1. Intercepts 1/2 c 2. Reciprocals 1/½ 1/ 1/ Reduction Miller Indices (200) a b y x z example a b c 1. Intercepts 1/2 1 3/4 2. Reciprocals 1/½ 1/1 1/¾ c 3. Reduction 4. Miller Indices (634) 2 1 4/ x a b y 4
5 Crystallographic planes Family of Planes {hkl} Ex: {100} = (100), (010), (001),(100), (010), (001) Adapted from Fig. 3.9, Callister 7e. 5
6 Linear density: BCC Number of atoms Linear Density of Atoms LD = Unit length of direction vector [100]: LD = 1 = a 3 4R [111]: LD = 2 = 4R 1 2R 6
7 Linear density (FCC) and planar densitry [110] ex: linear density of Al in [110] direction a = nm # atoms LD = 2 = nm a length 2 a Planar Density of Atoms PD = Number of atoms Area of plane 7
8 Planar density We want to examine the atomic packing of crystallographic planes Iron foil can be used as a catalyst. The atomic packing of the exposed planes is important. a) Draw (100) and (111) crystallographic planes for Fe. b) Calculate the planar density for each of these planes. R = nm and Fe has a BCC structure at room temperature 2D repeat unit a = atoms R 2D repeat unit Planar Density = area 2D repeat unit 1 a 2 = R 2 Adapted from Fig. 3.2(c), Callister 7e. = 1.2 x atoms m 2 8
9 Planar density 2D repeat unit atoms area = 2 ah = 3 a = 3 R = R 2 2D repeat unit Planar Density = area 2D repeat unit R 2 = 7.0 atoms = nm x atoms m 2 9
10 Single crystal vs. Polycrystalline structures Single crystals: Atoms all have the same arrangement throughout. Polycrystalline: Many crystals put together. Anisotropic Adapted from Fig. K, color inset pages of Callister 5e. (Fig. K is courtesy of Paul E. Danielson, Teledyne Wah Chang Albany) 1 mm Isotropic NbHfW plate with an electron beam weld. Each "grain" is a single crystal. If grains are randomly oriented, overall component properties are not directional. Grain sizes typ. range from 1 nm to 2 cm (i.e., from a few to millions of atomic layers). 10
11 Polycrystalline structures Grain Boundaries regions between crystals transition from lattice of one region to that of the other slightly disordered low density in grain boundaries o o o high mobility high diffusivity high chemical reactivity Adapted from Fig. 4.7, Callister 7e. 11
12 Single crystal vs. Polycrystalline structures Single Crystals Properties vary with direction: anisotropic. Example: the modulus of elasticity (E) in BCC iron: E (diagonal) = 273 GPa E (edge) = 125 GPa Data from Table 3.3, Callister 7e. (Source of data is R.W. Hertzberg, Deformation and Fracture Mechanics of Engineering Materials, 3rd ed., John Wiley and Sons, 1989.) Polycrystals Properties may/may not vary with direction. If grains are randomly oriented: isotropic. (E poly iron = 210 GPa) If grains are textured, anisotropic. 200 µm Adapted from Fig. 4.14(b), Callister 7e. (Fig. 4.14(b) is courtesy of L.C. Smith and C. Brady, the National Bureau of Standards, Washington, DC [now the National Institute of Standards and Technology, Gaithersburg, MD].) 12
13 Point defects Vacancies: vacant atomic sites in a structure. Vacancy distortion of planes SelfInterstitials: "extra" atoms positioned between atomic sites. distortion of planes selfinterstitial 13
14 Equilibrium concentration of defects Equilibrium concentration varies with temperature Each lattice site is a potential vacancy No. of defects Activation energy No. of potential defect sites. N Q v = exp v N k T Boltzmann's constant Temperature 14
15 Point defects in alloys Two outcomes if impurity (B) added to host (A): Solid solution of B in A (i.e., random dist. of point defects) OR Substitutional solid soln. (e.g., Cu in Ni) Interstitial solid soln. (e.g., C in Fe) Solid solution of B in A plus particles of a new phase (usually for a larger amount of B) Second phase particle different composition often different structure. 15
16 Imperfections of solids Conditions for substitutional solid solution (S.S.) W. Hume Rothery rule 1. Δr (atomic radius) < 15% 2. Proximity in periodic table i.e., similar electronegativities 3. Same crystal structure for pure metals 4. Valency All else being equal, a metal will have a greater tendency to dissolve a metal of higher valency than one of lower valency 1. Would you predict more Al or Ag to dissolve in Zn? 2. More Zn or Al in Cu? Table on p. 106, Callister 7e. Element Atomic Crystal Electro Valence Radius Structure nega (nm) tivity Cu FCC C H O Ag FCC Al FCC Ni FCC Zn HCP
17 Line defects Linear Defects (Dislocations) Are onedimensional defects around which atoms are misaligned Edge dislocation: extra halfplane of atoms inserted in a crystal structure b to dislocation line Screw dislocation: spiral planar ramp resulting from shear deformation b to dislocation line Fig. 4.3, Callister 7e. 17
18 Screw defects Adapted from Fig. 4.4, Callister 7e. 18
19 Mixed defects Mixed Edge Adapted from Fig. 4.5, Callister 7e. Screw 19
20 Planar defects External defects On the surface Unsatisfied bonds Internal defects Grain boundaries 20
21 Planar defects Twin boundary (plane) Essentially a reflection of atom positions across the twin plane. Adapted from Fig. 4.9, Callister 7e. Stacking faults For FCC metals an error in ABCABC packing sequence Ex: ABCABABC 21