Crystallographic Calculations

Similar documents
Axial Ratios, Parameters, Miller Indices

GEOL. 40 ELEMENTARY MINERALOGY

CRYSTAL MEASUREMENT AND AXIAL RATIO LABORATORY

The structure of liquids and glasses. The lattice and unit cell in 1D. The structure of crystalline materials. Describing condensed phase structures

Crystal Chem Crystallography

Earth Materials Lab 2 - Lattices and the Unit Cell

Biaxial Minerals This document last updated on 27-Oct-2014

Symmetry. 2-D Symmetry. 2-D Symmetry. Symmetry. EESC 2100: Mineralogy 1. Symmetry Elements 1. Rotation. Symmetry Elements 1. Rotation.

Introduction to Crystallography and Mineral Crystal Systems by Mike and Darcy Howard Part 6: The Hexagonal System

Symmetry Crystallography

5 Symmetries and point group in a nut shell

Straight Line. SPTA Mathematics Higher Notes

n-dimensional, infinite, periodic array of points, each of which has identical surroundings.

Basic Crystallography Part 1. Theory and Practice of X-ray Crystal Structure Determination

Mineralogy Problem Set Crystal Systems, Crystal Classes

Crystallographic Symmetry. Jeremy Karl Cockcroft


1/2, 1/2,1/2, is the center of a cube. Induces of lattice directions and crystal planes (a) Directions in a crystal Directions in a crystal are

Condensed Matter Physics Prof. G. Rangarajan Department of Physics Indian Institute of Technology, Madras

I.G.C.S.E. Matrices and Transformations. You can access the solutions from the end of each question

SANDERSON HIGH SCHOOL AP CALCULUS AB/BC SUMMER REVIEW PACKET

UNIT I SOLID STATE PHYSICS

Chemical Crystallography

9.7 Extension: Writing and Graphing the Equations

SOLID STATE 18. Reciprocal Space

Applications of X-ray and Neutron Scattering in Biological Sciences: Symmetry in direct and reciprocal space 2012

Sect The Slope-Intercept Form

Mineralogy ( ) Chapter 5: Crystallography

Math 1 packet for Coordinate Geometry part 1. Reviewing the basics. The coordinate plane

Cartesian Plane. Analytic Geometry. Unit Name

PX-CBMSO Course (2) of Symmetry

Graphing Review Part 1: Circles, Ellipses and Lines

Hello Future Calculus Level One Student,

Math 8 Honors Coordinate Geometry part 1 Unit Updated July 29, 2016

Analytical Methods for Materials

Table of contents. Jakayla Robbins & Beth Kelly (UK) Precalculus Notes Fall / 53

ACCESS TO SCIENCE, ENGINEERING AND AGRICULTURE: MATHEMATICS 1 MATH00030 SEMESTER / Lines and Their Equations

Resolution: maximum limit of diffraction (asymmetric)

Introduction to. Crystallography

The Reciprocal Lattice

Phys 460 Describing and Classifying Crystal Lattices

Class 27: Reciprocal Space 1: Introduction to Reciprocal Space

Calculus I Sample Exam #01

GY-343 Petrology Petrographic Microscope Laboratory

Algebra Review. 1. Evaluate the expression when a = -3 and b = A) 17 B) 1 C) Simplify: A) 17 B) 29 C) 16 D)

St. Xavier s College Mumbai

Summer 2017 Review For Students Entering AP Calculus AB/BC

- A general combined symmetry operation, can be symbolized by β t. (SEITZ operator)

DIFFERENTIATION RULES

GEOMETRY AND VECTORS

Trigonometry Exam II Review Problem Selected Answers and Solutions

Recognise the Equation of a Circle. Solve Problems about Circles Centred at O. Co-Ordinate Geometry of the Circle - Outcomes

MATH 1130 Exam 1 Review Sheet

MAPS AND CROSS SECTIONS (I)

0-2. 2) Plot the points and connect them. X

Equation. A mathematical sentence formed by setting two expressions equal to each other. Example 1: 3 6 = 18 Example 2: 7 + x = 12

Scattering and Diffraction

Math M111: Lecture Notes For Chapter 3

CHAPTER ONE FUNCTIONS AND GRAPHS. In everyday life, many quantities depend on one or more changing variables eg:

Math 121: Calculus 1 - Fall 2013/2014 Review of Precalculus Concepts

DIFFERENTIAL EQUATIONS REVIEW. Here are notes to special make-up discussion 35 on November 21, in case you couldn t make it.

Materials Science and Engineering 102 Structure and Bonding. Prof. Stephen L. Sass. Midterm Examination Duration: 1 hour 20 minutes

Section 6.1 Sinusoidal Graphs

Math 121: Calculus 1 - Fall 2012/2013 Review of Precalculus Concepts

X-ray analysis. 1. Basic crystallography 2. Basic diffraction physics 3. Experimental methods

Crystallographic structure Physical vs Chemical bonding in solids

Analytical Methods for Materials

Chapter 1: Precalculus Review

PHYSICS LAB: CONSTANT MOTION

Test Corrections for Unit 1 Test

Understanding Single-Crystal X-Ray Crystallography Exercises and Solutions

4 The Cartesian Coordinate System- Pictures of Equations

Crystallography basics

Basics of crystallography

Tables of crystallographic properties of double antisymmetry space groups

4 Ab C4 Integration 1 ln. 12 Bc C4 Parametric differentiation dy

Math 121: Calculus 1 - Winter 2012/2013 Review of Precalculus Concepts

Chapter 3: Inequalities, Lines and Circles, Introduction to Functions

CHAPTER 3 THE STRUCTURE OF CRYSTALLINE SOLIDS PROBLEM SOLUTIONS

Chapter 2 Introduction to Phenomenological Crystal Structure

Reteach 2-3. Graphing Linear Functions. 22 Holt Algebra 2. Name Date Class

Crystallography Reading: Warren, Chapters 2.1, 2.2, 2.6, 8 Surface symmetry: Can be a clue to underlying structure. Examples:

VCE. VCE Maths Methods 1 and 2 Pocket Study Guide

Geometry Summer Assignment 2018

MATH 32 FALL 2012 FINAL EXAM - PRACTICE EXAM SOLUTIONS

Math 147 Exam II Practice Problems

We need to be able to describe planes and directions.

Calculus I Practice Final Exam B

Higher Mathematics Course Notes

Chapter 3 Representations of a Linear Relation

1 Geometry of R Conic Sections Parametric Equations More Parametric Equations Polar Coordinates...

VECTORS AND THE GEOMETRY OF SPACE

Symmetry and Properties of Crystals (MSE638) Spherical Trigonometry

STUDY KNOWHOW PROGRAM STUDY AND LEARNING CENTRE. Functions & Graphs

MATH 1301, Solutions to practice problems

ALGEBRA 2 Summer Review Assignments Graphing

Midterm 1 Review. Distance = (x 1 x 0 ) 2 + (y 1 y 0 ) 2.

Vector equations of lines in the plane and 3-space (uses vector addition & scalar multiplication).

CHAPTER 4. APPLICATIONS AND REVIEW IN TRIGONOMETRY

2018 Canadian Senior Mathematics Contest

Transcription:

Page 1 of 7 EENS 2110 Tulane University Mineralogy Prof. Stephen A. Nelson This page last updated on 07-Sep-2010 Crystallographic calculations involve the following: 1. Miller Indices (hkl) 2. Axial ratios -. a: 1: c 3. ρ and φ angles corresponding to a Miller Index (hkl) 4. angles between crystallographic axes if in monoclinic, or triclinic systems. Most of what you will do in lab or on exams will involve crystallographic calculations in the orthorhombic, tetragonal, hexagonal, or isometric systems, where the axes angles are fixed. Note that you will always be given enough information to solve the problem. Some of the problems you might be expected to solve involve determination of Miller Indices from the ρ and φ angles, to determine the ρ and φ angles for faces of mineral with known axial ratios, or to determine axial ratios of minerals that have faces of known ρ and φ angles. First let's review some of the things we know about Miller indices and ρ and φ angles. In the orthorhombic, tetragonal, or isometric systems. If h is 0, i.e. (0kl) is the Miller Index, then the face is parallel to the a crystallographic axis. So, φ = 0 o or φ = 180 o If k is 0 i.e. (h0l) is the Miller Index, then the face is parallel to the b crystallographic axis. So, φ = 90 o or φ = 270 o If l is 0, i.e. (hk0) is the Miller Index, then the face is parallel to the c crystallographic axis. So, ρ = 90 o If h & k are 0, i.e. (00l) is the Miller Index, then the face is perpendicular to the c axis So, ρ = 0 o or ρ = 180 o, and φ is undefined.

Page 2 of 7 If h & l are 0, i.e. (0k0) is the Miller Index, then the face is perpendicular to the b axis. So, ρ = 90 o and φ = 0 o or φ = 180 o. If l and k are 0, i.e. (h00) is the Miller Index, then the face is perpendicular to the a axis. So, ρ = 90 o and φ = 90 o or φ = 270 o. Now let's do some examples 1. Given Miller indices and ρ and φ angles for crystal faces that, in combination, intersect all crystallographic axes, calculate the axial ratios of the mineral. a. Faces ρ φ (110) 90 o 45 o (011) 70 o 0 o For the (110) we note that it does not intersect the c axis, so we can look at it in the two dimensional plane containing the a and b axes, as shown in the drawing below. From this face we should be able to determine the a/b axial ratio. Since the φ angle is the angle between the normal to the face and the b axis, by similar triangles we know that the φ angle also occurs between the a axis and the face. Thus, we can write: tan 45 o = 1b/1a then 1a/1b = 1/tan 45 o = 1 So, a/b: b/b = 1: 1 We next note that the (011) intersects the b and c axes only, so we can examine this face in the plane containing only b and c, as shown below. From this drawing we can obtain the c/b axial ratio. Since the ρ angle is the angle between the pole to the face and the c axis, again by similar triangles we know that the ρ angle also occurs between the b axis and the (011) face.

Page 3 of 7 Thus, we can write: tan 70 o = 1c/1b then c/b = arctan 70 o So, c/b = 2.7475 so, a : b : c = 1 : 1 : 2.7475 and the mineral must be tetragonal, since a/b =1. b. Faces ρ φ (120) 90 o 70 o (011) 32 o 0 o The face (120) does not intersect the c axis, so we can look at this face in the plane containing only the a and b axes. We must also remember that Miller Indices represent the inverse of the intercepts, so the face (120) intersects the a axis at twice the number of unit lengths that it intersects the b axis. Since the φ angle is the angle between the normal to the face and the b axis, by similar triangles we know that the φ angle also occurs between the a axis and the (120) face. Then we can write: tan 70 o = 1b/2a a/b = 1/2tan70 o 1a/1b = 0.18199 We next note that the (011) intersects the b and c axes only, so we can examine this face in the plane containing only b and c, as shown below. From this drawing we can obtain the c/b axial ratio. Since the ρ angle is the angle between the face and the c axis, again by similar triangles we know that the ρ angle also occurs between the b axis and the (011) face.

Page 4 of 7 For this face we can determine that tan 32 o = 1c/1b 1c/1b = 0.6248 so, a : b : c = 0.18199 : 1 : 0.6248, and the mineral is orthorhombic c. Faces ρ φ (311) 24 o 33 o This face is more complicated because it intersects all three axes. We first attempt to draw a 3-dimensional view of this face. Notice that the φ angle is measured in the horizontal plane that includes the a and b axes. The ρ angle is measured in a vertical plane that includes the c axis and the line normal to the face in the a - b horizontal plane, and is measured between the c axis and a line normal to the face. Note also, that for the (311) face, the intercept on the a axis is 1/3 what it is on the b and c axes, because the Miller Index is the inverse of the intercepts.. We can determine the a/b part of the axial ratio by looking at the projection of this face in the a - b plane. 1b/(1/3)a = tan 33 o 1a/3b = 1/tan 33 1a/1b = 3/tan 33 1a/1b = 4.6196 In order to determine the length of the c axis, we need to know the length of the line labeled t, because this line forms the base of the triangle in which the ρ angle is measured. The length of the line t is:

Page 5 of 7 t/b = cos 33 o t/b = 0.8397 t = 0.8397 b We can now use this to determine the c/b axial ratio. 1c/t = tan 24 o 1c = 0.8387 b tan 24 o c/b = 0.3747 Thus, the axial ratio for this mineral is 4.6196 : 1 : 0.3747 Now we'll look at an example where we are given the axial ratio of the mineral and asked to calculate the ρ and φ angles for the faces. 1. Given the axial ratio for a mineral is 1 : 1 : 5.0, what are ρ and φ for the face (111). We first attempt to draw a 3-dimensional view of this face. Notice that again the φ angle is measured in the horizontal plane that includes the a and b axes. The ρ angle is measured in a vertical plane that includes the c axis and the line normal to the face in the a - b horizontal plane, and is measured between the c axis and a line normal to the face. In this case the intercept on the all three axes is 1.

Page 6 of 7 Since the φ angle for this face is measured in the horizontal a - b plane, we can draw the plane containing only the a and b axes to determine the angle. Since the axial ratio tells us that the relative lengths of the a and b axes are equal tan φ = 1b/1b = 1 φ = 45 o In order to determine the ρ angle, we need to know the length of the line labeled t, because this line forms the base of the triangle in which the ρ angle is measured. The length of the line t is: t/b = cos 45 o t = 0.7071 b Now we can determine the angle by drawing the plane that includes the c axis and the line t. In this plane we can let the length of the c = 5b, from the axial ratio. Then: tan ρ = 5b/t tan ρ = 5b/0.7071b tan ρ = 5/0.7071 tan ρ = 7.071 ρ = arctan (7.071) = 81.95 o So for the (111) face in this crystal ρ =81.95 o and φ = 45 o.

Page 7 of 7 2. Given the tetragonal crystal shown below and the following information: For the face (101) ρ = 70 o φ = 90 o a. What is the axial ratio for this crystal? b. What are the Miller Indices for the faces labeled (0kl) and (h0l), given that both of these faces have ρ = 53.9478 o? a. To find the axial ratio we note that we can use the face (101) and draw this in plane of the a and c axes (since the face doesn't intersect the b axis. Then, we can determine that tan ρ = 1c/1a so, tan 70 o = c/a = 2.7475 and the axial ratio is: 1 :1 : 2.7475 b. To find the Miller indices of the face (h0l) we proceed as follows: Since all we need is the relative lengths of intersection to calculate the parameters, we can assume one of the lengths = 1, i.e. 1a. This is the same as moving the face parallel to itself so that it intersects the a axis at a unit length of 1. The face intersects the c axis at 2.7475x, where the 2.7475 value is the length of the c axis relative to the unit length of the a axis. Then tan (53.9478) = 2.7475x/1, and thus, x = 0.5 The parameters for this face are then: 1,, 1/2, which can be inverted to give the Miller Index - (102). Since the mineral is tetragonal, the face labeled (0hl) would have the Miller Index (012). Problems such as these could be asked on any laboratory exam. Return to EENS 2110 Page