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Transcript of Chapter-3-1 Chemistry 481, Spring 2014, LA Tech Instructor: Dr. Upali Siriwardane e-mail:...
![Page 1: Chapter-3-1 Chemistry 481, Spring 2014, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:](https://reader036.fdocuments.us/reader036/viewer/2022062305/56649e575503460f94b4f288/html5/thumbnails/1.jpg)
Chapter-3-1Chemistry 481, Spring 2014, LA Tech
Instructor: Dr. Upali Siriwardane
e-mail: [email protected]
Office: CTH 311 Phone 257-4941
Office Hours:
M,W 8:00-9:00 & 11:00-12:00 am;
Tu,Th, F 10:00 - 12:00 a.m.
April 10 , 2014: Test 1 (Chapters 1, 2, 3,)
May 1, 2014: Test 2 (Chapters 5, 6 & 7)
May 20, 2014: Test 3 (Chapters. 19 & 20)
May 22, Make Up: Comprehensive covering all Chapters
Chemistry 481(01) Spring 2014
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Chapter-3-2Chemistry 481, Spring 2014, LA Tech
Chapter 3. Structures of simple solids
Crystalline solids: The atoms, molecules or ions pack together in an ordered arrangement
Amorphous solids: No ordered structure to the particles of the solid. No well defined faces, angles or shapes
Polymeric Solids: Mostly amorphous but some have local crystiallnity. Examples would include glass and rubber.
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Chapter-3-3Chemistry 481, Spring 2014, LA Tech
The Fundamental types of Crystals
Metallic: metal cations held together by a sea of electrons
Ionic: cations and anions held together by predominantly electrostatic attractions
Network: atoms bonded together covalently throughout the solid (also known as covalent crystal or covalent network).
Covalent or Molecular: collections of individual molecules; each lattice point in the crystal is a molecule
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Chapter-3-4Chemistry 481, Spring 2014, LA Tech
Metallic Structures
Metallic Bonding in the Solid State: Metals the atoms have low electronegativities; therefore the
electrons are delocalized over all the atoms.
We can think of the structure of a metal as an arrangement of positive atom cores in a sea of electrons. For a more detailed picture see "Conductivity of Solids".
Metallic: Metal cations held together by a sea of valanece electrons
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Chapter-3-5Chemistry 481, Spring 2014, LA Tech
Packing and GeometryClose packing
ABC.ABC... cubic close-packed CCP
gives face centered cubic or FCC(74.05% packed)
AB.AB... or AC.AC... (these are equivalent). This is called hexagonal close-packing HCP
CCPHCP
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Chapter-3-6Chemistry 481, Spring 2014, LA Tech
Loose packing
Simple cube SC
Body-centered cubic BCC
Packing and Geometry
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Chapter-3-7Chemistry 481, Spring 2014, LA Tech
The Unit CellThe basic repeat unit that build up the whole solid
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Chapter-3-8Chemistry 481, Spring 2014, LA Tech
Unit Cell Dimensions
The unit cell angles are defined as:
a, the angle formed by the b and c cell
edges
b, the angle formed by the a and c cell edges
g, the angle formed by the a and b cell
edges
a,b,c is x,y,z in right handed cartesian
coordinates
a g b a c b a
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Chapter-3-9Chemistry 481, Spring 2014, LA Tech
Bravais Lattices & Seven Crystals Systems
In the 1840’s Bravais showed that there are only fourteen different space lattices.
Taking into account the geometrical properties of the basis there are 230 different repetitive patterns in which atomic elements can be arranged to form crystal structures.
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Chapter-3-10Chemistry 481, Spring 2014, LA Tech
Fourteen Bravias Unit Cells
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Chapter-3-11Chemistry 481, Spring 2014, LA Tech
Seven Crystal Systems
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Chapter-3-12Chemistry 481, Spring 2014, LA Tech
Number of Atoms in the Cubic Unit Cell• Coner- 1/8• Edge- 1/4• Body- 1• Face-1/2• FCC = 4 ( 8 coners, 6 faces)• SC = 1 (8 coners)• BCC = 2 (8 coners, 1 body) Face-1/2
Coner- 1/8Edge - 1/4Body- 1
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Chapter-3-13Chemistry 481, Spring 2014, LA Tech
Close Pack Unit Cells
CCP HCP
FCC = 4 ( 8 coners, 6 faces)
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Chapter-3-14Chemistry 481, Spring 2014, LA Tech
Simple cube SC Body-centered cubic BCC
Unit Cells from Loose Packing
SC = 1 (8 coners) BCC = 2 (8 coners, 1 body)
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Chapter-3-15Chemistry 481, Spring 2014, LA Tech
Coordination NumberThe number of nearest particles surrounding a
particle in the crystal structure.
Simple Cube: a particle in the crystal has a coordination number of 6
Body Centerd Cube: a particle in the crystal has a coordination number of 8
Hexagonal Close Pack &Cubic Close Pack: a particle in the crystal has a coordination number of 12
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Chapter-3-16Chemistry 481, Spring 2014, LA Tech
Holes in FCC Unit Cells
Tetrahedral Hole (8 holes)
Eight holes are inside a face centered cube.
Octahedral Hole (4 holes)
One hole in the middle and 12 holes along the edges ( contributing 1/4) of the face centered cube
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Chapter-3-17Chemistry 481, Spring 2014, LA Tech
Holes in SC Unit Cells
Cubic Hole
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Chapter-3-18Chemistry 481, Spring 2014, LA Tech
Octahedral Hole in FCC
Octahedral Hole
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Chapter-3-19Chemistry 481, Spring 2014, LA Tech
Tetrahedral Hole in FCC
Tetrahedral Hole
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Chapter-3-20Chemistry 481, Spring 2014, LA Tech
Structure of MetalsCrystal Lattices
A crystal is a repeating array made out of metals. In describing this structure we must distinguish between the pattern of repetition (the lattice type) and what is repeated (the unit cell) described above.
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Chapter-3-21Chemistry 481, Spring 2014, LA Tech
PolymorphismMetals are capable of existing in more than one form at a time
Polymorphism is the property or ability of a metal to exist in two or more crystalline forms depending upon temperature and composition. Most metals and metal alloys exhibit this property.
Uranium is a good example of
a metal that exhibits
polymorphism.
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Chapter-3-22Chemistry 481, Spring 2014, LA Tech
AlloysSubstitutional
Second metal replaces the metal atoms in the lattice
Interstitial
Second metal occupies interstitial space (holes) in the lattice
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Chapter-3-23Chemistry 481, Spring 2014, LA Tech
Properties of AlloysAlloying substances are usually metals or metalloids. The
properties of an alloy differ from the properties of the pure metals or metalloids that make up the alloy and this difference is what creates the usefulness of alloys. By combining metals and metalloids, manufacturers can develop alloys that have the particular properties required for a given use.
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Chapter-3-24Chemistry 481, Spring 2014, LA Tech
Structure of Ionic SolidsCrystal Lattices
A crystal is a repeating array made out of ions. In describing this structure we must distinguish between the pattern of repetition (the lattice type) and what is repeated (the unit cell) described above.
Cations fit into the holes in the anionic lattice since anions are lager than cations.
In cases where cations are bigger than anions lattice is considered to be made up of cationic lattice with smaller anions filling the holes
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Chapter-3-25Chemistry 481, Spring 2014, LA Tech
Basic Ionic Crystal Unit Cells
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Chapter-3-26Chemistry 481, Spring 2014, LA Tech
Radius Ratio Rules
r+/r- Coordination Holes in Which
Ratio Number Positive Ions Pack
0.225 - 0.414 4 tetrahedral holes FCC
0.414 - 0.732 6 octahedral holes FCC
0.732 - 1 8 cubic holes BCC
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Chapter-3-27Chemistry 481, Spring 2014, LA Tech
Cesium Chloride Structure (CsCl)
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Chapter-3-28Chemistry 481, Spring 2014, LA Tech
Rock Salt (NaCl)
© 1995 by the Division of Chemical Education, Inc., American Chemical Society.
Reproduced with permission from Soli-State Resources.
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Chapter-3-29Chemistry 481, Spring 2014, LA Tech
Sodium Chloride Lattice (NaCl)
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Chapter-3-30Chemistry 481, Spring 2014, LA Tech
NaCl Lattice Calculations
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Chapter-3-31Chemistry 481, Spring 2014, LA Tech
CaF2
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Chapter-3-32Chemistry 481, Spring 2014, LA Tech
Calcium Fluoride
© 1995 by the Division of Chemical Education, Inc., American Chemical Society.
Reproduced with permission from Solid-State Resources.
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Chapter-3-33Chemistry 481, Spring 2014, LA Tech
Zinc Blende Structure (ZnS)
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Chapter-3-34Chemistry 481, Spring 2014, LA Tech
Lead Sulfide
© 1995 by the Division of Chemical Education, Inc., American Chemical Society.
Reproduced with permission from Solid-State Resources.
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Chapter-3-35Chemistry 481, Spring 2014, LA Tech
Wurtzite Structure (ZnS)
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Chapter-3-36Chemistry 481, Spring 2014, LA Tech
Summary of Unit Cells
Volume of a sphere = 4/3pr3
Volume of sphere in SC = 4/3p(½)
3 = 0.52
Volume of sphere in BCC = 4/3p((3)½
/4)3
= 0.34
Volume of sphere in FCC = 4/3p( 1/(2(2)½
))3
= 0.185
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Chapter-3-37Chemistry 481, Spring 2014, LA Tech
Density CalculationsAluminum has a ccp (fcc) arrangement of atoms. The radius
of Al = 1.423Å ( = 143.2pm). Calculate the lattice parameter of the unit cell and the density of solid Al (atomic weight = 26.98).
Solution:
4 atoms/cell [8 at corners (each 1/8), 6 in faces (each 1/2)]
Lattice parameter: a/r(Al) = 2(2)1/2
a = 2(2)1/2 (1.432Å) = 4.050Å= 4.050 x 10-8 cm
Density = 2.698 g/cm3
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Chapter-3-38Chemistry 481, Spring 2014, LA Tech
Lattice Energy
The Lattice energy, U, is the amount of energy required to separate a mole of the solid (s) into a
gas (g) of its ions.
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Chapter-3-39Chemistry 481, Spring 2014, LA Tech
Lattice energy
The higher the lattice energy, the stronger the attraction between ions.
Lattice energy
Compound kJ/mol
LiCl 834
NaCl 769
KCl 701
NaBr 732
Na2O 2481
Na2S 2192
MgCl2 2326
MgO 3795
Lattice energy
Compound kJ/mol
LiCl 834
NaCl 769
KCl 701
NaBr 732
Na2O 2481
Na2S 2192
MgCl2 2326
MgO 3795
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Chapter-3-40Chemistry 481, Spring 2014, LA Tech
Lattice Energy
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Chapter-3-41Chemistry 481, Spring 2014, LA Tech
Properties of Ionic Compounds
Crystals of Ionic Compounds are hard and brittle
Have high melting points
When heated to molten state they conduct electricity
When dissolved in water conducts electricity
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Chapter-3-42Chemistry 481, Spring 2014, LA Tech
Trends in Melting Points
Compound Lattice Energy
(kcal/mol)
NaF -201
NaCl -182
NaBr -173
NaI -159
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Chapter-3-43Chemistry 481, Spring 2014, LA Tech
Trends in Melting Points
Compound Lattice Energy
(kcal/mol)
NaF -201
NaCl -182
NaBr -173
NaI -159
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Chapter-3-44Chemistry 481, Spring 2014, LA Tech
Compound q+ radius q- radius M.P (oC) L.E. (kJ/mol)
LiCl 0.68 1.81 605 834
NaCl 0.98 1.81 801 769
KCl 1.33 1.81 770 701
LiF 0.68 1.33 845 1024
NaF 0.98 1.33 993 911
KF 1.33 1.33 858 815
MgCl2 0.65 1.81 714 2326
CaCl2 0.94 1.81 782 2223
MgO 0.65 1.45 2852 3938
CaO 0.94 1.45 2614 3414
Trends in Properties
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Chapter-3-45Chemistry 481, Spring 2014, LA Tech
Coulomb’s Law
k = constant
q+ = cation charge
q- = anion charge
r = distance between two ions
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Chapter-3-46Chemistry 481, Spring 2014, LA Tech
Coulomb’s Model
where e = charge on an electron = 1.602 x 10-19
C
e0
= permittivity of vacuum = 8.854 x 10-12
C2
J-1
m-1
ZA = charge on ion A
ZB = charge on ion B
d = separation of ion centers
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Chapter-3-47Chemistry 481, Spring 2014, LA Tech
An ionic bond is simply the electrostatic attraction between opposite charges.
Ions with charges Q1 and
Q2:
The potential energy is given by:
d
· ·
d
QQE
21µ
Ionic Bonds
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Chapter-3-48Chemistry 481, Spring 2014, LA Tech
Arrange with increasing lattice energy:
KCl
NaF
MgO
KBr
NaCl788 kJ
671 kJ
3795 kJ
910 kJ
701 kJ
d
· ·K
+Cl
· ·K
+Br
d
d
QQE
21µ
Estimating Lattice Energy
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Chapter-3-49Chemistry 481, Spring 2014, LA Tech
Madelung ConstantMadelung constant is geometric factor that
depends on the lattice structure.
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Chapter-3-50Chemistry 481, Spring 2014, LA Tech
Madelung Constant Calculation
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Chapter-3-51Chemistry 481, Spring 2014, LA Tech
Degree of Covalent Character
Fajan's Rules (Polarization)Polarization will be increased by:• 1. High charge and small size of the cation• 2. High charge and large size of the anion• 3. An incomplete valence shell electron configuration
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Chapter-3-52Chemistry 481, Spring 2014, LA Tech
Trends in Melting Points Silver Halides
Compound M.P. oC
AgF 435
AgCl 455
AgBr 430
AgI 553
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Chapter-3-53Chemistry 481, Spring 2014, LA Tech
Born-Lande Model:This modes include repulsions due to overlap of
electron electron clouds of ions.
eo = permitivity of free space
A = Madelung Constant
ro = sum of the ionic radii
n = average born exponet depend on the electron configuration
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Chapter-3-54Chemistry 481, Spring 2014, LA Tech
Born_Haber CycleEnergy Considerations in Ionic Structures
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Chapter-3-55Chemistry 481, Spring 2014, LA Tech
Born-Haber Cycle?
Relates lattice energy ( L.E) to:
Sublimation (vaporization) energy (S.E)
Ionization energy metal (I.E)
Bond Dissociation of nonmetal (B.E)
DHf formation of NaCl(s)
L.E. = E.A.+ 1/2 B.E. + I.E. + S.E. - DHf
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Chapter-3-56Chemistry 481, Spring 2014, LA Tech
Ionic bond formation
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Chapter-3-57Chemistry 481, Spring 2014, LA Tech
Energy and ionic bond formationExample - formation of sodium chloride.
Steps DHo, kJVaporization of Na(s) Na(g) +92sodium
Decomposition of 1/2 Cl2 (g) Cl(g) +121chlorine molecules
Ionization of sodium Na(g) Na+(g) +496
Addition of electron Cl(g) + e- Cl-(g) -349to chlorine
( electron affinity)Formation of NaCl Na+(g)+Cl-(g) NaCl -771
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Chapter-3-58Chemistry 481, Spring 2014, LA Tech
Energy and ionic bond formation
Na(s) + 1/2 Cl2(g)
Na(g) + 1/2 Cl2(g)
Na(g) + Cl(g)
Na+
(s) + Cl(g)
Na+
(s) + Cl-(g)
NaCl(s)
+496 kJ(I.E.)
+121 kJ(1/2 B.D.E.)
+92 kJ(S.E.)
-349 kJ (E.A.)
-771 kJ (L.E.)
-411 kJ(DHf)
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Chapter-3-59Chemistry 481, Spring 2014, LA Tech
Calculation of DHf from lattice Energy
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Chapter-3-60Chemistry 481, Spring 2014, LA Tech
Hydration of Cations
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Chapter-3-61Chemistry 481, Spring 2014, LA Tech
Solubility: Lattice Energy and Hydration Energy
Solubility depends on the difference between lattice energy and hydration energy holds ions and water.
For dissolution to occur the lattice energy must be overcome by hydration energy.
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Chapter-3-62Chemistry 481, Spring 2014, LA Tech
Solubility: Lattice Energy and Hydration Energy
For strong electrolytes lattice energy increases with increase in ionic charge and
decrease in ionic size
H hydration energies are greatest for small, highly charged ions
Difficult to predict solubility from size and charge of ions. we use solubility rules.
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Chapter-3-63Chemistry 481, Spring 2014, LA Tech
Thermodynamics of the Solution Process of Ionic Compounds
Heat of solution, DHsolution :
Enthalpy of hydration, DHhyd,
Lattice Energy, Ulatt
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Chapter-3-64Chemistry 481, Spring 2014, LA Tech
Solution Process of Ionic Compounds
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Chapter-3-65Chemistry 481, Spring 2014, LA Tech
Enthalpy from dipole – dipole Interactions
The last term, DH L-L, indicates the loss of enthalpy
from dipole - dipole interactions between solvent
molecules (L) when they become solvating
ligands (L') for the ions.
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Chapter-3-66Chemistry 481, Spring 2014, LA Tech
Hydration Process
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Chapter-3-67Chemistry 481, Spring 2014, LA Tech
Different types of Interactions for Dissolution
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Chapter-3-68Chemistry 481, Spring 2014, LA Tech
Hydration Energy of Ions
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Chapter-3-69Chemistry 481, Spring 2014, LA Tech
Hydration Process
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Chapter-3-70Chemistry 481, Spring 2014, LA Tech
Calculation of DHsolution
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Chapter-3-71Chemistry 481, Spring 2014, LA Tech
Heat of Solution and Solubility
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Chapter-3-72Chemistry 481, Spring 2014, LA Tech
Metallic Bonding ModelsThe difference in chemical properties
between metals and non-metals lie mainly in the fact those atoms of metals fewer valence electrons and they are shared among all the atoms in the substance: metallic bonding.
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Chapter-3-73Chemistry 481, Spring 2014, LA Tech
Metallic solidsRepeating units are made up of metal atoms,
Valence electrons are free to jump from one atom to another
++ + +
++ + +
++ + +
++ + +
++
++
++ +
+
++ ++
++ + +
++ + +
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Chapter-3-74Chemistry 481, Spring 2014, LA Tech
Electron-sea model of bonding
The metallic bond consists of a series of metals atoms that have all donated their valence electrons to an electron cloud, referred to as an electron sea which permeates the entire solid. It is like a box (solid) of marbles (positively charged metal cores: known as Kernels) that are surrounded by water (valence electrons).
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Chapter-3-75Chemistry 481, Spring 2014, LA Tech
Electron-sea model Explanation
Metallic bond together is the attraction between the positive kernels and the delocalized negative electron cloud.
Fluid electrons that can carry a charge and kinetic energy flow easily through the solid making metals good electrical and thermal conductor.
The kernels can be pushed anywhere within the solid and the electrons will follow them, giving metals flexibility: malleability and ductility.
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Chapter-3-76Chemistry 481, Spring 2014, LA Tech
Delocalized Metallic Bonding
Metals are held together by delocalized bonds formed from the atomic orbitals of all the atoms in the lattice.
The idea that the molecular orbitals of the band of energy levels are spread or delocalized over the atoms of the piece of metal accounts for bonding in metallic solids.
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Chapter-3-77Chemistry 481, Spring 2014, LA Tech
Molecular orbital theory
Molecular Orbital Theory applied to metallic bonding is known as Band Theory.
Band theory uses the LCAO of all valence atomic orbitals of metals in the solid to form bands of s, p, d, f bands (molecular orbitals) just like simple molecular orbital theory is applied to a diatomic molecule, hydrogen(H2).
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Chapter-3-78Chemistry 481, Spring 2014, LA Tech
Types of conducting materials
a) Conductor (which is usually a metal) is a solid with a partially full band.
b) Insulator is a solid with a full band and a large band gap.
c) Semiconductor is a solid with a full band and a small band gap.
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Chapter-3-79Chemistry 481, Spring 2014, LA Tech
Linear Combination of Atomic Orbitals
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Chapter-3-80Chemistry 481, Spring 2014, LA Tech
Linear Combination of Atomic Orbitals
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Chapter-3-81Chemistry 481, Spring 2014, LA Tech
Conduction Bands in Metals
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Chapter-3-82Chemistry 481, Spring 2014, LA Tech
Types of MaterialsA conductor (which is usually a metal) is a solid
with a partially full band
An insulator is a solid with a full band and a large band gap
A semiconductor is a solid with a full band and a small band gap
Element Band Gap C 5.47 eVSi 1.12 eVGe 0.66 eVSn 0 eV
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Chapter-3-83Chemistry 481, Spring 2014, LA Tech
Band Gaps
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Chapter-3-84Chemistry 481, Spring 2014, LA Tech
Band Theory of Metals
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Chapter-3-85Chemistry 481, Spring 2014, LA Tech
Band TheoryInsulators – valence electrons are tightly bound to (or
shared with) the individual atoms – strongest ionic (partially covalent) bonding.
Semiconductors - mostly covalent bonding somewhat weaker bonding.
Metals – valence electrons form an “electron gas” that are not bound to any particular ion
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Chapter-3-86Chemistry 481, Spring 2014, LA Tech
Bonding Models for MetalsBand Theory of Bonding in Solids
Bonding in solids such as metals, insulators and semiconductors may be understood most effectively by an expansion of simple MO theory to assemblages of scores of atoms
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Chapter-3-87Chemistry 481, Spring 2014, LA Tech
Band Gaps
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Chapter-3-88Chemistry 481, Spring 2014, LA Tech
Doping Semiconductors