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A (0001) plane for an HCP unit cell is show below.

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Presentation on theme: "A (0001) plane for an HCP unit cell is show below."— Presentation transcript:

1 A (0001) plane for an HCP unit cell is show below.
Each of the 6 perimeter atoms in this plane is shared with three other unit cells, whereas the center atom is shared with no other unit cells; this gives rise to three equivalent atoms belonging to this plane. In terms of the atomic radius R, the area of each of the 6 equilateral triangles that have been drawn is , or the total area of the plane shown is . . And the planar density for this (0001) plane is equal to or the total area of the plane shown is (b) the atomic radius for titanium is nm. Therefore, the planar density for the (0001) plane is

2 CHAPTER 4: IMPERFECTIONS IN SOLIDS
ISSUES TO ADDRESS... • What are the solidification mechanisms? • What types of defects arise in solids? • Can the number and type of defects be varied and controlled? • How do defects affect material properties? • Are defects undesirable?

3 • How do defects affect material properties?
sterling silver (7.5% copper) much harder and stronger than silver silicon transistors rely on controlled “doping” • Are defects undesirable? NO 1

4

5 Imperfections in Solids
Solidification- result of casting of molten material 2 steps Nuclei form Nuclei grow to form crystals – grain structure Start with a molten material – all liquid nuclei crystals growing grain structure liquid Adapted from Fig.4.14 (b), Callister 7e. Crystals grow until they meet each other

6 Polycrystalline Materials
Grain Boundaries regions between crystals transition from lattice of one region to that of the other slightly disordered low density in grain boundaries high mobility high diffusivity high chemical reactivity Adapted from Fig. 4.7, Callister 7e.

7 Solidification Grains can be - equiaxed (roughly same size in all directions) - columnar (elongated grains) ~ 8 cm heat flow Shell of equiaxed grains due to rapid cooling (greater T) near wall Columnar in area with less undercooling Adapted from Fig. 4.12, Callister 7e. Grain Refiner - added to make smaller, more uniform, equiaxed grains.

8 Imperfections in Solids
There is no such thing as a perfect crystal. What are these imperfections? Why are they important? Many of the important properties of materials are due to the presence of imperfections.

9 Types of Imperfections
• Vacancy atoms • Interstitial atoms • Substitutional atoms Point defects • Dislocations Line defects • Grain Boundaries Area defects

10 Point Defects Vacancy self- interstitial • Vacancies:
-vacant atomic sites in a structure. Vacancy distortion of planes • Self-Interstitials: -"extra" atoms positioned between atomic sites. self- interstitial distortion of planes

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12 Equilibrium Concentration: Point Defects
• Equilibrium concentration varies with temperature! No. of defects Activation energy æ - ö N Q v ç v ÷ = exp ç ÷ No. of potential è ø N k T defect sites. Temperature Boltzmann's constant -23 (1.38 x 10 J/atom-K) -5 (8.62 x 10 eV/atom-K) Each lattice site is a potential vacancy site

13 Measuring Activation Energy
ç ÷ N v = exp - Q k T æ è ö ø • We can get Qv from an experiment. • Measure this... N v T exponential dependence! defect concentration • Replot it... 1/ T N v ln - Q /k slope

14 Estimating Vacancy Concentration
• Find the equil. # of vacancies in 1 m3 of Cu at 1000C. • Given: 3 r = 8.4 g / cm A = 63.5 g/mol Cu Q = 0.9 eV/atom N = 6.02 x 1023 atoms/mol A v 8.62 x 10-5 eV/atom-K 0.9 eV/atom 1273K ç ÷ N v = exp - Q k T æ è ö ø = 2.7 x 10-4 For 1 m3 , N = N A Cu r x 1 m3 = 8.0 x 1028 sites • Answer: N v = (2.7 x 10-4)(8.0 x 1028) sites = 2.2 x 1025 vacancies

15 Observing Equilibrium Vacancy Conc.
• Low energy electron microscope view of a (110) surface of NiAl. • Increasing T causes surface island of atoms to grow. • Why? The equil. vacancy conc. increases via atom motion from the crystal to the surface, where they join the island. Reprinted with permission from Nature (K.F. McCarty, J.A. Nobel, and N.C. Bartelt, "Vacancies in Solids and the Stability of Surface Morphology", Nature, Vol. 412, pp (2001). Image is 5.75 mm by 5.75 mm.) Copyright (2001) Macmillan Publishers, Ltd. I sland grows/shrinks to maintain equil. vancancy conc. in the bulk.

16 Completely pure metal (or other substance) – Impossible!!
Pay – really pay – for % - NIST standards still 1022 to 1023 impurities per m3 Alloy – deliberately add “impurity” to engineer properties. Copper (7.5%) in silver

17 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.

18 Terminology - Alloys Solvent – component in highest concentration – also called – host Solute – component present in minor concentration

19 Remember metals- often crystallize in
close packed structures – high packing density. More interstitial or substitutional ?? Usually < 10%

20 Imperfections in Solids
Conditions for substitutional solid solution (S.S.) W. Hume – Rothery rule 1. r (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

21 Carbon in Iron Element C Fe Radii 0.017 nm 0.124 Unit cell Hex BCC
Electronegativity 2.5 1.6 Valence +4 +2 (+3) Solid solution ? Interstitial or substitional? C - 2s2 2p2 Fe – 3d6 4s2

22 Copper and Nickel Element Cu Ni Radii 0.128 nm 0.125 Unit cell FCC
Electronegativity 1.9 1.8 Oxidation (Valence) +1 (+2) +2 Expect to form solid solution? Ni – 3d8 4s2 (28) Cu - 3d10 4s1 (29)

23 Imperfections in Solids
Application of Hume–Rothery rules – Solid Solutions 1. Would you predict more Al or Ag to dissolve in Zn? 2. More Zn or Al in Cu? Element Atomic Crystal Electro- Valence Radius Structure nega- (nm) tivity Cu FCC C H O Ag FCC Al FCC Co HCP Cr BCC Fe BCC Ni FCC Pd FCC Zn HCP Table on p. 106, Callister 7e.

24 IMPURITIES • Impurities must also satisfy charge balance • Ex: NaCl
• Substitutional cation impurity • Substitutional anion impurity 11

25 Imperfections in Solids
Specification of composition weight percent m1 = mass of component 1 nm1 = number of moles of component 1 atom percent


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