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Chapter-3-1 Chemistry 481, Spring 2015, 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 9:30 - 11:30 a.m. April 7 , 2015: Test 1 (Chapters 1, 2, 3) April 30, 2015: Test 2 (Chapters 5, 6 & 7) May 19, 2015: Test 3 (Chapters. 19 & 20) May 19, Make Up: Comprehensive covering all Chapters Chemistry 481(01) Spring 2015

Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: [email protected] Office: CTH 311 Phone 257-4941 Office Hours:

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Page 1: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-1Chemistry 481, Spring 2015, 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 9:30 - 11:30 a.m.

April 7 , 2015: Test 1 (Chapters 1,  2, 3)

April 30, 2015: Test 2 (Chapters  5, 6 & 7)

May 19, 2015: Test 3 (Chapters. 19 & 20)

May 19, Make Up: Comprehensive covering all Chapters

Chemistry 481(01) Spring 2015

Page 2: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-2Chemistry 481, Spring 2015, 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.

Page 3: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-3Chemistry 481, Spring 2015, 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

Page 4: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-4Chemistry 481, Spring 2015, 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

Page 5: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-5Chemistry 481, Spring 2015, 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

Page 6: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-6Chemistry 481, Spring 2015, LA Tech

Loose packing

Simple cube SC

Body-centered cubic BCC

Packing and Geometry

Page 7: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-7Chemistry 481, Spring 2015, LA Tech

The Unit CellThe basic repeat unit that build up the whole solid

Page 8: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-8Chemistry 481, Spring 2015, 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

Page 9: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-9Chemistry 481, Spring 2015, 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.

Page 10: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-10Chemistry 481, Spring 2015, LA Tech

Fourteen Bravias Unit Cells

Page 11: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-11Chemistry 481, Spring 2015, LA Tech

Seven Crystal Systems

Page 12: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-12Chemistry 481, Spring 2015, 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

Page 13: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-13Chemistry 481, Spring 2015, LA Tech

Close Pack Unit Cells

CCP HCP

FCC = 4 ( 8 coners, 6 faces)

Page 14: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-14Chemistry 481, Spring 2015, LA Tech

Simple cube SC Body-centered cubic BCC

Unit Cells from Loose Packing

SC = 1 (8 coners) BCC = 2 (8 coners, 1 body)

Page 15: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-15Chemistry 481, Spring 2015, 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

Page 16: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-16Chemistry 481, Spring 2015, 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

Page 17: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-17Chemistry 481, Spring 2015, LA Tech

Holes in SC Unit Cells

Cubic Hole

Page 18: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-18Chemistry 481, Spring 2015, LA Tech

Octahedral Hole in FCC

Octahedral Hole

Page 19: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-19Chemistry 481, Spring 2015, LA Tech

Tetrahedral Hole in FCC

Tetrahedral Hole

Page 20: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-20Chemistry 481, Spring 2015, 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.

Page 21: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-21Chemistry 481, Spring 2015, 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.

Page 22: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-22Chemistry 481, Spring 2015, LA Tech

AlloysSubstitutional

Second metal replaces the metal atoms in the lattice

Interstitial

Second metal occupies interstitial space (holes) in the lattice

Page 23: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-23Chemistry 481, Spring 2015, 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.

Page 24: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-24Chemistry 481, Spring 2015, 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.

Page 25: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-25Chemistry 481, Spring 2015, LA Tech

Metallic solidsRepeating units are made up of metal atoms,

Valence electrons are free to jump from one atom to another

++ + +

++ + +

++ + +

++ + +

++

++

++ +

+

++ ++

++ + +

++ + +

Page 26: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-26Chemistry 481, Spring 2015, 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).

Page 27: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-27Chemistry 481, Spring 2015, 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.

Page 28: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-28Chemistry 481, Spring 2015, 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.

Page 29: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-29Chemistry 481, Spring 2015, 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).

Page 30: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-30Chemistry 481, Spring 2015, LA Tech

13. Describe metallic bonding and properties in terms of:

Electron-sea model of bonding:

 

 

 

 

 Band Theory:

 

Page 31: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-31Chemistry 481, Spring 2015, 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.

Page 32: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-32Chemistry 481, Spring 2015, LA Tech

Linear Combination of Atomic Orbitals

Page 33: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-33Chemistry 481, Spring 2015, LA Tech

Linear Combination of Atomic Orbitals

Page 34: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-34Chemistry 481, Spring 2015, LA Tech

14. Draw the s band (molecular orbitals) for ten Na on a line (one dimensional) and show bonding and anti-bonding molecular orbitals and fill electrons.

Page 35: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-35Chemistry 481, Spring 2015, LA Tech

15. Describe the metallic properties of sodium in terms of band theory

Page 36: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-36Chemistry 481, Spring 2015, LA Tech

Conduction Bands in Metals

Page 37: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-37Chemistry 481, Spring 2015, LA Tech

16. Using a band diagram, explain how magnesium can exhibit metallic behavior even though its 3s band is completely full.

Page 38: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-38Chemistry 481, Spring 2015, 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

Page 39: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-39Chemistry 481, Spring 2015, LA Tech

Band Gaps

Page 40: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-40Chemistry 481, Spring 2015, LA Tech

17. Draw a Band diagram for carbon/silicon/germanium/tin, and label valence band, conduction band and band gap?

Page 41: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-41Chemistry 481, Spring 2015, LA Tech

18. Draw a band diagrams to show the difference between(Band gaps: C =  5.47, Si  = 1.12, Ge =  0.66,   Sn =  0)

• Conductor (Sn):

•  •  

• Insulator (C):

•  •  

• Semiconductor (Ge):

Page 42: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-42Chemistry 481, Spring 2015, LA Tech

Band Theory of Metals

Page 43: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-43Chemistry 481, Spring 2015, 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

Page 44: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-44Chemistry 481, Spring 2015, 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

Page 45: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-45Chemistry 481, Spring 2015, LA Tech

Band Gaps

Page 46: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-46Chemistry 481, Spring 2015, LA Tech

Doping Semiconductors

Page 47: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-47Chemistry 481, Spring 2015, LA Tech

19. Draw a band diagram for thermal/photo (Intrinsic) and doped (Extrinsic) semiconductors and explain the origin of semicondictivity?

d)    Thermal/photo (Intrinsic) (Ge):

 

 

e)    Doped (Extrinsic) (Si/As):

Page 48: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-48Chemistry 481, Spring 2015, LA Tech

20. Draw a band diagram for a p-type (Si/Ga) and n-type (Si/As) semiconductors and show holes and electrons that is responsible for semiconductivity.

f)     p-type(Si/Ga):

 

 

g)    n-type(Si/As):

Page 49: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-49Chemistry 481, Spring 2015, LA Tech

21. What is a transistor with emitter (E), collector(C) and base (B), and how it works?

Page 50: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-50Chemistry 481, Spring 2015, LA Tech

21. What is a transistor with emitter (E), collector(C) and base (B), and how it works?

Page 51: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-51Chemistry 481, Spring 2015, LA Tech

Vacuum tubes and Transisters

Page 52: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-52Chemistry 481, Spring 2015, LA Tech

22. What the difference between a transistor (semiconductor device) and vacuum tube?

Page 53: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-53Chemistry 481, Spring 2015, LA Tech

• 23. Using the diagram explain how a diode works.

Page 54: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-54Chemistry 481, Spring 2015, LA Tech

24. What is an integrated circuit?

Page 55: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-55Chemistry 481, Spring 2015, 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

Page 56: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-56Chemistry 481, Spring 2015, LA Tech

Basic Ionic Crystal Unit Cells

Page 57: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-57Chemistry 481, Spring 2015, LA Tech

1) Give coordination number for both anion and cation

of the following ionic lattices.

a) CsCl Structure:

b) Rock Salt Structure:

c) Fluorite Structure:

d) Sphalrite Structure:

e) Wurtzite:

f) Rutile:

Page 58: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-58Chemistry 481, Spring 2015, LA Tech

1) Calculate the number of formula units in the unit cell of the following metallic and ionic compounds.

a) NaCl(fcc)

b) CsCl(bcc)

c) ZnS(fcc)

d) CaF2(bcc)

Page 59: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-59Chemistry 481, Spring 2015, 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

Page 60: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-60Chemistry 481, Spring 2015, LA Tech

Cesium Chloride Structure (CsCl)

Page 61: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-61Chemistry 481, Spring 2015, LA Tech

Rock Salt (NaCl)

© 1995 by the Division of Chemical Education, Inc., American Chemical Society.

Reproduced with permission from Soli-State Resources.

Page 62: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-62Chemistry 481, Spring 2015, LA Tech

Sodium Chloride Lattice (NaCl)

Page 63: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-63Chemistry 481, Spring 2015, LA Tech

NaCl Lattice Calculations

Page 64: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-64Chemistry 481, Spring 2015, LA Tech

CaF2

Page 65: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-65Chemistry 481, Spring 2015, LA Tech

Calcium Fluoride

© 1995 by the Division of Chemical Education, Inc., American Chemical Society.

Reproduced with permission from Solid-State Resources.

Page 66: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-66Chemistry 481, Spring 2015, LA Tech

Zinc Blende Structure (ZnS)

Page 67: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-67Chemistry 481, Spring 2015, LA Tech

Lead Sulfide

© 1995 by the Division of Chemical Education, Inc., American Chemical Society.

Reproduced with permission from Solid-State Resources.

Page 68: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-68Chemistry 481, Spring 2015, LA Tech

Wurtzite Structure (ZnS)

Page 69: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-69Chemistry 481, Spring 2015, 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

Page 70: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-70Chemistry 481, Spring 2015, 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

Page 71: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-71Chemistry 481, Spring 2015, LA Tech

Miller Indices

Miller indices are used to specify directions and planes

• These directions and planes could be in lattices or in

crystals

• The number of indices will match with the dimension of the

Lattice or the crystal

• (h, k, l) represents a point on a plane

• To obtain h, k, l of a plane Identify the intercepts on the a- , b- and c- axes of the

unit cell.

Page 72: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-72Chemistry 481, Spring 2015, LA Tech

Miller Indices

Eg. intercept on the x-axis is at a, b and c ( at the point (a,0,0) ), but the surface is parallel to the y- and z-axes - strictly

therefore there is no intercept on these two axes but we shall consider the intercept to be at infinity ( ∞ ) for the

special case where the plane is parallel to an axis.

The intercepts on the a- , b- and c-axes are thus

Intercepts :    1 , ∞ , ∞

Take the reciprocals of the fractional intercepts: 1/1 , 1/ ∞, 1/ ∞

• (h, k, l) for this plane becomes 1,0,0

Page 73: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-73Chemistry 481, Spring 2015, LA Tech

Rock Salt (NaCl)

© 1995 by the Division of Chemical Education, Inc., American Chemical Society.

Reproduced with permission from Soli-State Resources.

Page 74: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-74Chemistry 481, Spring 2015, LA Tech

Sodium Chloride Lattice (NaCl)

0,0,1 0,0,2

1,1,12,2,2

Page 75: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-75Chemistry 481, Spring 2015, LA Tech

CaF2

0,0,1 0,0,4 0,0,2 0,0,4

0,0,20,0,2 0,0,4

Page 76: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-76Chemistry 481, Spring 2015, LA Tech

Calcium Fluoride

© 1995 by the Division of Chemical Education, Inc., American Chemical Society.

Reproduced with permission from Solid-State Resources.

Page 77: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-77Chemistry 481, Spring 2015, LA Tech

Zinc Blende Structure (ZnS)

0,0,1 0,0,4 0,0,40,0,2

Page 78: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-78Chemistry 481, Spring 2015, LA Tech

Lead Sulfide

© 1995 by the Division of Chemical Education, Inc., American Chemical Society.

Reproduced with permission from Solid-State Resources.

Page 79: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-79Chemistry 481, Spring 2015, LA Tech

Wurtzite Structure (ZnS)

Page 80: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-80Chemistry 481, Spring 2015, LA Tech

Antifluorite Structure

Page 81: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-81Chemistry 481, Spring 2015, LA Tech

Radius ratio rule states

As

the size (ionic radius, r+

) of a cation increases,

more anions of a

particular size can pack around it.

Thus, knowing the size of the ions, we should be able to predict

a priori

which type of crystal packing

will be observed.

We can account for the relative size of both ions by using the RATIO of

the ionic radii:

ρ = r+

r−

Radius ratio rule

Page 82: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-82Chemistry 481, Spring 2015, 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

Page 83: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-83Chemistry 481, Spring 2015, LA Tech

Radius Ratio AppplicationsSuggest the probable crystal structure of (a) barium fluoride; (b) potassium bromide; (c) magnesium sulfide. You can use tables to obtain ionic radii.

a) barium fluoride; Ba2+= 142 pm F- = 131 pm

b) potassium bromide; K+= 138 pm Br- = 196 pm

c) magnesium sulfide; Mg2+= 103 pm S2- = 184 pm

a) Radius ratio(barium fluoride): 142/131 =1.08

b) Radius ratio(potassium bromide): 138/196=0.704

c) Radius ratio(magnesium sulfide): 103/184= 0.559

Page 84: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-84Chemistry 481, Spring 2015, LA Tech

Radius Ratio Appplicationsa) Radius ratio(barium fluoride): 142/131 =1.08

b) Radius ratio(potassium bromide): 138/196=0.704

c) Radius ratio(magnesium sulfide): 103/184= 0.559

• Barium fluoride: 142/131 =1.08 (0.732-1) CN 8 FCC fluorite• Potassium bromide: 138/196=0.704 (0.414-0.732) CN 6 FCC K+ in

octahedral holes• Magnesium sulfide: 103/184= 0.559 (0.414-0.732) CN 6 FCC

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

Page 85: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-85Chemistry 481, Spring 2015, LA Tech

Radius Ratio Applications• Barium fluoride: 142/131 =1.08 (0.732-1) CN 8 FCC

• Potassium bromide: 138/196=0.704 (0.414-0.732) CN 6 FCC K+ in octahedral holes

• Magnesium sulfide: 103/184= 0.559 (0.414-0.732) CN 6 FCC

Page 86: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-86Chemistry 481, Spring 2015, LA Tech

Unit Cells dimensions and radius

a = 2r or r = a/2

Page 87: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-87Chemistry 481, Spring 2015, 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

Page 88: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-88Chemistry 481, Spring 2015, 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

Page 89: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-89Chemistry 481, Spring 2015, LA Tech

3. What is Coulombs law how it applies to ionic bond?

Page 90: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-90Chemistry 481, Spring 2015, LA Tech

Coulomb’s Law

k = constant

q+ = cation charge

q- = anion charge

r = distance between two ions

Page 91: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-91Chemistry 481, Spring 2015, 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

Page 92: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-92Chemistry 481, Spring 2015, 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

Page 93: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-93Chemistry 481, Spring 2015, 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

Page 94: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-94Chemistry 481, Spring 2015, LA Tech

Lattice Energy

The Lattice energy, U, is the amount of energy required to separate a mole of the solid (s) into a gaseous atoms (g) of its ions.

Lattice Enthalpy:

Page 95: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-95Chemistry 481, Spring 2015, LA Tech

4. What is lattice energy? Take NaCl as an example.

Page 96: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-96Chemistry 481, Spring 2015, 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

Page 97: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-97Chemistry 481, Spring 2015, LA Tech

Lattice Energy

Page 98: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-98Chemistry 481, Spring 2015, LA Tech

5. Place the following compounds in order of increasing lattice energy: a) magnesium oxide b) lithium fluoride c) sodium chloride. Give the reasoning for this order.

Page 99: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-99Chemistry 481, Spring 2015, 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

Page 100: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-100Chemistry 481, Spring 2015, LA Tech

Trends in Melting Points

Compound Lattice Energy (Enthalpy)

(kcal/mol)

NaF -201

NaCl -182

NaBr -173

NaI -159

Page 101: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-101Chemistry 481, Spring 2015, LA Tech

Trends in Melting Points

Compound Lattice Energy

(kcal/mol)

NaF -201

NaCl -182

NaBr -173

NaI -159

Page 102: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-102Chemistry 481, Spring 2015, 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

Page 103: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-103Chemistry 481, Spring 2015, LA Tech

6. Explain the lattice energy and melting point trends:

CompoundCation radius

(Angstroms)

Anion radius

(Angstroms)

Melting Point

(Centigrade)

Lattice Energy (kcal/mol)

MgCl2 0.65 1.81 714 2326CaCl2 0.94 1.81 782 2223

MgO 0.65 1.45 2852 3938

CaO 0.94 1.45 2614 3414

Page 104: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-104Chemistry 481, Spring 2015, LA Tech

Madelung ConstantMadelung constant is geometric factor that

depends on the lattice structure.

Page 105: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-105Chemistry 481, Spring 2015, LA Tech

Madelung Constant Calculation

Page 106: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-106Chemistry 481, Spring 2015, LA Tech

7. Why is Madalung constant for NaCl is significantly different from CaF2 value and why is it different for different ionic lattice types?

Ionic Solid Madelung Constant

Coor. #A : C Lattice Type

NaCl 1.747558 6 : 6 Rock salt

CaF2 2.51939 8 : 4 Fluorite

Page 107: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-107Chemistry 481, Spring 2015, LA Tech

8. Calculate the first two terms of the series for the Madelung constant for the cesium chloride lattice. How does this compare with the limiting value?

Page 108: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-108Chemistry 481, Spring 2015, 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

Page 109: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-109Chemistry 481, Spring 2015, LA Tech

Trends in Melting Points Silver Halides

Compound M.P. oC

AgF 435

AgCl 455

AgBr 430

AgI 553

Page 110: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-110Chemistry 481, Spring 2015, LA Tech

9. In calculating lattice energy, why should Coulombs law equation is multiplied by the Avogadro’s number, N and Madelung constant, A?

 

N z2e2 N A z2e2

Lattice Energy = - ------ x N x A = - --------

4peor 4peor

Page 111: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-111Chemistry 481, Spring 2015, 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 exponent depend on the electron configuration

n = Born exponent, typically a number between 5 and 12, determined experimentally by measuring the compressibility of the solid

Page 112: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-112Chemistry 481, Spring 2015, LA Tech

10. In the correction to lattice energy what is factor n in Born-Lande equation accounted for and how it relate to electronic configuration?

Page 113: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-113Chemistry 481, Spring 2015, LA Tech

11. Using the Born-Lande equation, calculate the lattice energy of cesium chloride.

N A z2e2 1Lattice Energy = - -------- ( 1 - ---) 4peor n

Page 114: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-114Chemistry 481, Spring 2015, LA Tech

• 12. What are Born-Mayer and Kapustinskii equations? How are they different from the Born-Lande equation?

Page 115: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-115Chemistry 481, Spring 2015, LA Tech

Born_Haber CycleEnergy Considerations in Ionic Structures

Page 116: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-116Chemistry 481, Spring 2015, 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

Page 117: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-117Chemistry 481, Spring 2015, LA Tech

13. What is a Born-Haber cycle?

Page 118: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-118Chemistry 481, Spring 2015, LA Tech

Ionic bond formation

Page 119: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-119Chemistry 481, Spring 2015, 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

Page 120: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-120Chemistry 481, Spring 2015, 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)

Page 121: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-121Chemistry 481, Spring 2015, LA Tech

Calculation of DHf from lattice Energy

Page 122: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-122Chemistry 481, Spring 2015, LA Tech

14. Calculate the Lattice energy of NaCl from following thermodynamic data:

  Steps DHo, kJ

1. Vaporization of sodium: Na(s) Na(g) +92

2. Decomposition of Cl2: 1/2 Cl2 (g) Cl(g) +121

3. Ionization of sodium: Na(g) Na+(g) +496

4. Electron affinity to chlorine:Cl(g) + e- Cl-(g) -349

5. Formation of NaCl(s): Na(g)+1/2Cl2 (g) NaCl(s) -411

Page 123: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-123Chemistry 481, Spring 2015, LA Tech

15. Construct a Born-Haber cycle for the formation of aluminum fluoride. Do not perform any calculation.

Page 124: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-124Chemistry 481, Spring 2015, LA Tech

Hydration of Cations

Page 125: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-125Chemistry 481, Spring 2015, 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.

Page 126: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-126Chemistry 481, Spring 2015, 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.

Page 127: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-127Chemistry 481, Spring 2015, LA Tech

Thermodynamics of the Solution Process of Ionic Compounds

Heat of solution, DHsolution :

Enthalpy of hydration, DHhyd,

Lattice Energy, Ulatt

Page 128: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-128Chemistry 481, Spring 2015, LA Tech

Solution Process of Ionic Compounds

Page 129: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-129Chemistry 481, Spring 2015, LA Tech

16. Define following terms:Enthalpy of solution, DHsolution:

 

 Enthalpy of hydration, DHhydration:

 

 Solvent-solvent intermolecular attractions,

DH°solvent-solvent:

Page 130: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-130Chemistry 481, Spring 2015, LA Tech

17 . How is Enthalpy of solution, DHsolution, Enthalpy of hydration: DHhydration, and Lattice energy:Ulatt are related?

Page 131: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-131Chemistry 481, Spring 2015, 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.

Page 132: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-132Chemistry 481, Spring 2015, LA Tech

Hydration Process

Page 133: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-133Chemistry 481, Spring 2015, LA Tech

Different types of Interactions for Dissolution

Page 134: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-134Chemistry 481, Spring 2015, LA Tech

Hydration Energy of Ions

Page 135: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-135Chemistry 481, Spring 2015, LA Tech

Hydration Process

Page 136: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-136Chemistry 481, Spring 2015, LA Tech

Calculation of DHsolution

Page 137: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-137Chemistry 481, Spring 2015, LA Tech

Heat of Solution and Solubility

Page 138: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-138Chemistry 481, Spring 2015, LA Tech

18.Predict the solubility of following ionic compounds:

a) LiF:

 b) LiI:

 c) CsI:

 d) MgF2:

  Lattice Energy(U)

DHhyd, M+ DHhyd, M-

LiF 1030 -950 -60

LiI 720 -950 -80

CsI 585 -700 -80

MgF2 3100 -2800 -120

Page 139: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-139Chemistry 481, Spring 2015, LA Tech

19. Give rational explanation to the solubility rules in terms of ion sizes, lattice energy(U), DHhyd, and DHsolution.

 a) All compounds containing alkali metal cations and the ammonium ion are soluble.

 

 

  b) All compounds containing NO3

-, ClO4-, ClO3

-, and C2H3O2

- anions are soluble.

Page 140: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-140Chemistry 481, Spring 2015, LA Tech

20. Calculate the enthalpy of formation of calcium oxide using a Born-Haber cycle. Obtain all necessary information from the data tables in the Appendices. Compare the value that you obtain with the actual entropy measured value of DHf(CaO(s)).

Page 141: Chapter-3-1 Chemistry 481, Spring 2015, LA Tech Instructor: Dr. Upali Siriwardane e-mail: upali@latech.edu Office: CTH 311 Phone 257-4941 Office Hours:

Chapter-3-141Chemistry 481, Spring 2015, LA Tech

21. Although the hydration energy of the calcium ion, Ca2+, is much greater than that of the potassium ion, K+, the molar solubility of calcium chloride is much less than that of potassium chloride. Suggest an explanation.