SECOND MIDTERM EXAM Chemistry April 2011 Professor Buhro

Similar documents
FIRST MIDTERM EXAM Chemistry March 2011 Professor Buhro

FINAL EXAM Chemistry May 2011 Professor Buhro. ID Number:

KEY FIRST MIDTERM EXAM Chemistry February 2009 Professor Buhro

FINAL EXAM KEY. Professor Buhro. ID Number:

KEY. FINAL EXAM Chemistry May 2012 Professor Buhro. ID Number:

These metal centres interact through metallic bonding


Problems. 104 CHAPTER 3 Atomic and Ionic Arrangements

Chem 253, UC, Berkeley. Chem 253, UC, Berkeley

CRYSTAL STRUCTURE TERMS

Metallic crystal structures The atomic bonding is metallic and thus non-directional in nature

CHAPTER. The Structure of Crystalline Solids

1.10 Close packed structures cubic and hexagonal close packing

بسم هللا الرحمن الرحیم. Materials Science. Chapter 3 Structures of Metals & Ceramics

Solids. The difference between crystalline and non-crystalline materials is in the extent of ordering

METALLIC CRYSTALS. tend to be densely packed. have several reasons for dense packing: have the simplest crystal structures.

Introduction to Solid State Physics

SOLID-STATE STRUCTURE.. FUNDAMENTALS

CHAPTER 3: SYMMETRY AND GROUPS, AND CRYSTAL STRUCTURES. Sarah Lambart

Chapter1: Crystal Structure 1

Structure of silica glasses (Chapter 12)

Chapter Outline. How do atoms arrange themselves to form solids?

Engineering 45 The Structure and Properties of Materials Midterm Examination October 26, 1987

Fundamental concepts and language Unit cells Crystal structures! Face-centered cubic! Body-centered cubic! Hexagonal close-packed Close packed

LAB II CRYSTAL STRUCTURE AND CRYSTAL GROWTH PART 1: CRYSTAL GROWTH. I. Introduction

Order in materials. Making Solid Stuff. Primary Bonds Summary. How do they arrange themselves? Results from atomic bonding. What are they?

Chapter Outline How do atoms arrange themselves to form solids?

Inorganic Chemistry with Doc M. Day 10. Ionic Thrills, Part 1.

Close Packings of Spheres I.

Inorganic Chemistry with Doc M. Fall Semester, 2012 Day 13. Ionic Thrills Part 3.

ENGINEERING MATERIALS LECTURE #4

PROPERTIES OF MATERIALS IN ELECTRICAL ENGINEERING MIME262 MID-TERM EXAM

CHAPTER 2: ATOMIC ARRANGEMENTS AND MINERALOGICAL STRUCTURES. Sarah Lambart

Stacking Oranges. Packing atoms together Long Range Order. What controls the nearest number of atoms? Hard Sphere Model. Hard Sphere Model.

Intermolecular Forces. Part 2 The Solid State: Crystals

CHAPTER 5 IMPERFECTIONS IN SOLIDS PROBLEM SOLUTIONS

9/29/2014 8:52 PM. Chapter 3. The structure of crystalline solids. Dr. Mohammad Abuhaiba, PE

Basic Solid State Chemistry, 2 nd ed. West, A. R.

9/28/2013 9:26 PM. Chapter 3. The structure of crystalline solids. Dr. Mohammad Abuhaiba, PE

Materials Science ME 274. Dr Yehia M. Youssef. Materials Science. Copyright YM Youssef, 4-Oct-10

Chapter 3: Atomic and Ionic Arrangements. Chapter 3: Atomic and Ionic Arrangements Cengage Learning Engineering. All Rights Reserved.

www-materials.eng.cam.ac.uk/typd

E45 Midterm 01 Fall 2007! By the 0.2% offset method (shown on plot), YS = 500 MPa

Point Defects in Metals

CHAPTER9. Phase Diagrams Equilibrium Microstructural Development

Energy and Packing. typical neighbor bond energy. typical neighbor bond energy. Dense, regular-packed structures tend to have lower energy.

Chapter 12 The Solid State The Structure of Metals and Alloys

INSTITUTE OF AERONAUTICAL ENGINEERING (Autonomous) Dundigal, Hyderabad

Solid State Physics 460- Lecture 2a Structure of Crystals (Kittel Ch. 1)

Chapter 10. Liquids and Solids

CH445/545 Winter 2008

Ceramic Science 4RO3. Lecture 2. Tannaz Javadi. September 16, 2013

9/16/ :30 PM. Chapter 3. The structure of crystalline solids. Mohammad Suliman Abuhaiba, Ph.D., PE

CHEM J-2 June 2014

Chapter 1. Crystal Structure

CHAPTER 5 IMPERFECTIONS IN SOLIDS PROBLEM SOLUTIONS ev /atom = exp. kt ( =

Solid State Device Fundamentals

Chem 241. Lecture 19. UMass Amherst Biochemistry... Teaching Initiative

Lecture 3: Description crystal structures / Defects

Crystal structure of the material :- the manner in which atoms, ions, or molecules are spatially.

UNIT V -CRYSTAL STRUCTURE

ECE440 Nanoelectronics. Lecture 08 Review of Solid State Physics

Physics 6180: Graduate Physics Laboratory. Experiment CM5: X-ray diffraction and crystal structures

Development of Microstructure in Eutectic Alloys

Physical Ceramics. Principles for Ceramic Science and Engineering. Yet-Ming Chiang Massachusetts Institute of Technology Cambridge, Massachusetts

but T m (Sn0.62Pb0.38) = 183 C, so this is a common soldering alloy.

Chapter 16. Liquids and Solids. Chapter 16 Slide 1 of 87

Chapter-3 MSE-201-R. Prof. Dr. Altan Türkeli

Chemistry/Materials Science and Engineering C150 Introduction to Materials Chemistry

Chapter 11. States of Matter Liquids and Solids. Enthalpy of Phase Change

Energy and Packing. Materials and Packing

Unit-1 THE SOLID STATE QUESTIONS VSA QUESTIONS (1 - MARK QUESTIONS)

The Science and Engineering of Materials, 4 th ed Donald R. Askeland Pradeep P. Phulé. Chapter 3 Atomic and Ionic Arrangements

SECTION A. NATURAL SCIENCES TRIPOS Part IA. Friday 4 June to 4.30 MATERIALS AND MINERAL SCIENCES

Introduction to phase diagrams

General Objective. To develop the knowledge of crystal structure and their properties.

Thermal Analysis phase diagrams

Packing of atoms in solids

Lecture C4b Microscopic to Macroscopic, Part 4: X-Ray Diffraction and Crystal Packing

Materials Science. Why?

MME 2001 MATERIALS SCIENCE

Solids SECTION Critical Thinking

MSE 513 Homework #1 Due Jan. 21, 2013

Chapter One: The Structure of Metals

USE OF IN-SITU XRD TO DEVELOP CONDUCTING CERAMICS WITH THE AURIVILLIUS CRYSTAL STRUCTURE

Two marks questions and answers. 1. what is a Crystal? (or) What are crystalline materials? Give examples

Density Computations

Cu/Ag Eutectic System

Phase diagrams are diagrammatic representations of the phases present in a

Two Components System

Now, let s examine how atoms are affected as liquids transform into solids.

Introduction to Engineering Materials ENGR2000 Chapter 3: The Structure of Crystalline Solids. Dr. Coates

CRYSTAL LATTICE. Defining lattice: Mathematical construct; ideally infinite arrangement of points in space.

(iii) Describe how you would use a powder diffraction pattern of this material to measure

A - Transformation of anatase into rutile

Lecture C4a Microscopic to Macroscopic, Part 4: X-Ray Diffraction and Crystal Packing

CHAPTER THE SOLID STATE

Phase Diagrams of Pure Substances Predicts the stable phase as a function of P total and T. Example: water can exist in solid, liquid and vapor

Transcription:

SECOND MIDTERM EXAM Chemistry 465 1 April 011 Professor Buhro Signature Print Name Clearly ID Number: Information. This is a closed-book exam; no books, notes, other students, other student exams, or any other resource materials may be consulted or examined during the exam period. Calculators are permitted. Partial credit will be given for partially correct reasoning in support of incorrect or correct final answers. Additional space for answers is provided at the end of this exam; please clearly label any answers you place there. Please find Potentially Useful Information attached as the last pages of this exam. 1. (15 pts). (0 pts) 3. (5 pts) 4. (0 pts) 5. (10 pts) 6. (10 pts) Total (100 pts) 1

1. 15 total pts. The compound having the nominal composition CeO has the fluorite crystal structure and exhibits good oxide-ion (O ) conductivity. This compound easily becomes oxygen deficient, and its formula is best described as CeO -x where x may have the values 0 < x < 0.5. Ionic conductivity data for CeO -x specimens having different compositions are plotted below. Please answer the questions below. For your reference the ionic radii are r(ce 3+ ) = 1.8 Å, r(ce 4+ ) = 1.11 Å, and r(o ) = 1.4 Å. The Pauling electronegativities are (Ce) = 1.1 and (O) = 3.44. ln CeO 1.75 CeO 1.9 1/T (a) 05 pts. The ln vs. T 1 data for both compounds give linear plots. What conclusion may be drawn from the linearity in these plots? Please explain briefly. (b) 05 pts. Please identify the conductivity mechanism or mechanisms active in CeO -x and provide a brief justification for your answer. (c) 05 pts. The plots above differ greatly (quantitatively) from one another. Please explain the physical or chemical origin of this difference.

. 0 total pts. The following description of the alumina-silica (Al O 3 -SiO ) phase diagram dates back to the 1960s (it has since been revised). Al O 3 and SiO melt at 060 and 170 C, respectively. Only one compound forms from alumina and silica, having the composition 3Al O 3 SiO or Al 6 Si O 13. This compound is known as mullite and it melts congruently at 1850 C. Eutectic points occur at 5 mol % Al O 3 and 1595 C, and at 67 mol % Al O 3 and 1840 C. Please sketch this 1960s-era phase diagram in the space below, and label all regions. (The corrected alumina-silica phase diagram is found in F. J. Klug et al. J. Am. Ceram. Soc. 1987, 70, 750-759.) T (C) Al O 3 mol % SiO SiO 3

3. 5 total pts. Please consider the Ti Ni phase diagram shown below and provide the requested information: (a) 01 pt. Please identify each line compound on the diagram by writing its formula below. (b) 04 pts. Please identify each congruent melting point on the diagram by writing its temperature and the corresponding component composition below. (c) 05 pts. Please identify each phase that forms solid solutions by writing its (nominal) formula below. 4

(d) 03 pts. Please identify each eutectic point on the diagram by writing its temperature and the corresponding component composition below. (e) 03 pts. Please identify the peritectic point on the diagram by writing its temperature and the corresponding component composition below. Please indicate if this peritectic point is also an incongruent melting point. (f) 04 pts. Assume that a liquid having a component composition of Ti:Ni = 30:70 is cooled infinitely slowly from 1600 o C to 1000 o C. Please give the component composition, the phase composition, and the composition(s) of the phase(s) present in the specimen at 1000 o C. (g) 05 pts. Now assume that the same liquid (as in part f) having a component composition of Ti:Ni = 30:70 is cooled at a normal cooling rate from 1600 o C to 1000 o C. Please sketch the microstructure of the specimen at 1000 o C. Please be sure to clearly label all phases and microconstituents that are present. 5

4. 0 total pts. The Madelung constant A for the NaCl structure is 1.75. Here you will calculate the Madelung constants for three small fragments of (clusters from) the NaCl structure in (a)- (c) below. Assume that the nearest cation-anion separations in these clusters are the same as in a NaCl crystal. Please show your work, and then answer the following questions. (a) 05 pts. Determine A for a cluster consisting of one anion and one cation: + A = (b) 05 pts. Determine A for a cluster consisting of two anions and two cations positioned at the vertices of a square: + + A = (c) 05 pts. Determine A for a cluster consisting of four anions and four cations positioned at the vertices of a cube: + + + + A = (d) 05 pts. Why is NaCl normally found as an extended, nonmolecular crystal lattice rather than as small molecular clusters like those shown above? Please explain briefly. 6

5. 10 total pts. The compound formed when graphite is fully intercalated with elemental K has the formula KC 8. The XRD pattern in the region of the 004 reflection ( = 16.56º) of KC 8 is shown below. KC 8 can be de-intercalated by heating, which expels and vaporizes the K. The XRD pattern undergoes changes as this process occurs, as described below. The experiment considered here was discontinued before all of the K was removed. Intensity (a.u.) 4 5 6 7 8 9 10 11 1 13 14 15 16 17 18 Degrees -Theta (a) 03 pts. As the de-intercalation proceeded, the XRD peak at 16.46º gradually disappeared as another peak grew in to a maximum intensity at one of the positions indicated by the vertical lines. This second peak then gradually disappeared as another peak grew in to a maximum intensity at one of the other positions indicated. Eventually peaks had appeared at all the positions marked by the verticals. What process was responsible for this behavior? Please give your answer in a single sentence. (b) 03 pts. Which new peak was the first to appear and which the last to appear as deintercalation proceeded? Please identify these peaks by their values. (c) 04 pts. Please provide an appropriate stage label for each vertical in the space above it. 7

6. 10 total pts. A and B are metallic elements having fcc crystal structures and the lattice parameters a = 3.5 and 4.95 Å, respectively. A partial A-B phase diagram, for the temperature range below the solidus, is given below. Please determine the lattice parameter(s) of the phase or phases present at state point p. Be sure to show your work. T (C) p 0 10 0 30 40 50 60 70 80 90 100 A mol % B B 8

Extra Work Space Please clearly label any work placed here for grading. 9

Potentially Useful Information Engel-Brewer rules: s, p electrons structure 1.0 1.5 bcc 1.7.1 hcp.5 3.0 fcc 4 diamond (cubic) 1 Å = 10 8 cm = 10 10 m Cu K radiation ( = 1.54 Å) n = dsin d hkl = a(h + k + l ) -1/ for cubic systems (a = b = c, = = = 90 o ) 1/ 4 l d hkl ( ) h k hk for hexagonal systems (a = b c, = = 90 o, = 10 o ) 3a c d hkl = (h /a + k /b + l /c ) -1/ for orthonormal (including tetragonal and orthorhombic) crystal systems ( = = = 90 o ); for tetragonal systems, a = b c for orthorhombic systems, a b c sin ( 1 )/sin ( ) = m 1 /m, where m = (h + k + l ) In an ideal hcp metal, in which all 1 nearest neighbors are equidistant, c/a = 1.63. The area of a parallelogram is: b = base h = height area = b h h parallelepiped b The volume of a parallelepiped is: h base area = parallelogram area h = height parallelepiped volume = (base area) h 10

The volume of a sphere is: V sphere = 1.3333r 3 Definitions of sine and cosine functions: sin = opposite side/hypotenuse (of a right triangle) cos = adjacent side/hypotenuse (of a right triangle) Lowest-angle reflections in XRD powder patterns: Primitive-cubic lattice 100 Primitive but non-cubic lattice 100, or 010, or 001 bcc lattice 110 fcc lattice 111 simple hcp-based structure 100 or 00 Reflections present (allowed by symmetry): primitive (P) all hkl may be present* body-centered (I) h + k + l = n (even)* face-centered (F) hkl are all odd or all even* A-centered (A) k + l = n* B-centered (B) h + l = n* C-centered (C) h + k = n* Systematic absences (extinctions): primitive (P) no absences required by lattice type* body-centered (I) h + k + l = odd* face-centered (F) 100, 110, 10, 11, (300, 1), 310, 30, 31, etc.* diamond (F) 100, 110, 00, 10, 11, (300, 1), 310,, 30, 31, etc. *Note well: additional absences may be present, depending on the space-group symmetry (rather than lattice symmetry) of specific, individual cases. radius ratio rules: r M /r X = 0. 0.41 CN of M = 4 0.41 0.73 CN of M = 6 0.73 1.00 CN of M = 8 Z 1Ze VCoul 4 0d U ( d) U 0 ANZ1Ze 4 d 0 ANZ 1Ze d 4 0 0 NB n d 1 1 n Structure Madelung constant A NaCl 1.75 CsCl 1.76 Zinc blende 1.6381 Wurtzite 1.6413 CaF.5 Rutile (TiO ).41 CdI.36 Ion configuration Born exponent, n He 5 Ne 7 Ar, Cu + 9 Kr, Ag + 10 Xe, Au + 1 11

e = 1.60 10-19 C 4 0 = = 1.11 10-10 C J -1 m -1 1 Å = 10 8 cm = 10 10 m n e i ii 1 i E Aexp a RT Coordination-number ratio: For a compound M n X m, CN M /CN X = m/n d-spacings in intercalated crystals: d 00l = d 1 + (n 1)d 0 where: d 00l is the characteristic spacing, the translational period length, in the z direction (such as d 001 ) d 1 is the interlayer spacing in the stage-1 compound d 0 is the interlayer spacing in the empty (non-intercalated) host crystal n is the stage number 1