Coordination Polyhedra

Slides:



Advertisements
Similar presentations
Objectives By the end of this section you should:
Advertisements

Objectives By the end of this section you should: understand the concept of close packing know the difference between hexagonal and cubic close packing.
Packing of more than one type of sphere into unit cells:
Figure 16.9: Three cubic unit cells and the corresponding lattices.
Lecture 4 (Chapter 13 in Perkins) Crystal Chemistry Part 3: Coordination of Ions Pauling’s Rules Crystal Structures The packing animations below are due.
Nuclear reactions determine element abundance… Is the earth homogeneous though? Is the solar system?? Is the universe???
Unless otherwise stated, all images in this file have been reproduced from: Blackman, Bottle, Schmid, Mocerino and Wille, Chemistry, 2007 (John Wiley)
Unit Cell of Crystal Structure
Crystal Structures zTypes of crystal structures yFace centered cubic (FCC) yBody centered cubic (BCC) yHexagonal close packed (HCP) zClose Packed Structures.
Solids Ch.13. Solids Fixed, immobile (so to speak) Fixed, immobile (so to speak) Symmetry Symmetry Crystals Crystals So what’s the inner order? So what’s.
PH0101,UNIT 4,LECTURE 51 PH0101 UNIT 4 LECTURE 5 FACE CENTERED CUBIC STRUCTURE HEXAGONAL CLOSED PACKED STRUCTURE PROBLEMS.
How do atoms ARRANGE themselves to form solids? Unit cells
Unit Cells Let’s look at two different ways to visualize the structure of a solid.
Previously in Chem 104: types of solids Unit Cell 3 types of cubic cells contents of unit cell Lecture 1 posted! TODAY Z quantify relationship between.
Chapter 3 -1 ISSUES TO ADDRESS... How do atoms assemble into solid structures? How does the density of a material depend on its structure? When do material.
L Consider coordination of anions about a central cation Coordination Polyhedra Halite Cl Cl Cl Cl Na.
Solid State Physics (1) Phys3710
Ionic Coordination and Silicate Structures Lecture 4.
Nuclear reactions determine element abundance… Is the earth homogeneous though? Is the solar system?? Is the universe???
Chapter 3 The Structure of Crystalline Solids Session I
Packing of more than one type of sphere into unit cells: -Packing of ions in salts -Which is usually larger, negative (anions) or positive (cations) ions?
2D Packing Examples hole Answer the following questions for both packing diagrams. 1.Find the smallest unit that, if repeated, would give you the entire.
Hole Answer the following questions for both packing diagrams. 1.Draw the unit cell for each packing example. How many atoms I are there in each unit cell?
Crystalline Structures Edward A. Mottel Department of Chemistry Rose-Hulman Institute of Technology.
Previously in Chem 104: types of solids Unit Cell TODAY 3 types of cubic cells contents of unit cell, Z quantify relationship between cell and density.
Crystalline Structures Edward A. Mottel Department of Chemistry Rose-Hulman Institute of Technology.
Crystalline Structures Edward A. Mottel Department of Chemistry Rose-Hulman Institute of Technology.
Chapter 3: Structures of Metals & Ceramics
I. Structural Aspects Sphere PackingsWells, pp Densest Packing of Spheres Two-Dimensions: Unit Cell Hand-Outs: 7.
Ionic – Bonding and Crystal Structure. Valence and Lewis Bond Theory metals and non-metals exchange electrons eg. Na 2 O O [He]    2s 2 2p 4 Na [Ne]
Unit cell/ packing efficiency. Given 8 spheres to stack, how would you do it? Simple cubic structure.
Introduction to Mineralogy Dr. Tark Hamilton Chapter 4: Lecture 11 The Chemical Basis of Minerals (Closest Packing & Valency) Camosun College GEOS 250.
Closest Packing of Spheres How do spheres (atoms) pack to best fill space?? The concept of closest packing is important for understanding many solid structures.
Announcement Date Change 10/13/10 Nick Heinz 11/05/10 8:30am start
Anandh Subramaniam & Kantesh Balani
Chemistry. Solid State-II Session Objectives  Voids  Packing fraction.
Close-packed Spheres Units cells: point and space symmetry
Chapter 3: The Structure of Crystalline Solids
Objectives By the end of this section you should: know how atom positions are denoted by fractional coordinates be able to calculate bond lengths for octahedral.
§2.4 Crystal Structure and Complex Lattice
1 Pauling’s Rules GLY 4200 Fall, Planar Packing Hexagonal array of spheres.
Inorganic Material Chemistry
Paulings model.
Crystal lattice structure
Crystal Defects Steel spheres:
Presented By: Dr. Vatsala Soni
How do atoms arrange themselves to form solids?
Next time: Diffraction
Metals - Bonding and Crystal Structure
Metals - Bonding and Crystal Structure
Pauling’s Rules GLY 4200 Fall, 2017
Topics Significant figures Structural motifs Ionic conduction
Lab 1 Pauling’s rules.
CRYSTAL LATTICE & UNIT CELL
Crystallography and Structure
Solid State Lattices.
Solids Amorphous Solids: Disorder in the structures Glass
Coordination Principle
Coordination Principle
Coordination Principle
Crystal and Amorphous Structure in Materials
Pauling’s Rules GLY 4200 Fall, 2018
Crystal and Amorphous Structure
UNIT CELLS UNIT CELL – The smallest repeating unit of a crystalline solid EXP11-1 (of 11)
Atomic Structure.
Earth = anion balls with cations in the spaces…
There are not more than 4 ways of arranging spheres in any shape of unit cell These are Primitive, Body Centered, Face Centered & End Centered.
10.4 Structure and Bonding In Metals
Meeting 1, Tuesday, Jan. 8, 2019 Goals for this Meeting:
Presentation transcript:

Coordination Polyhedra Consider coordination of anions about a central cation Halite Na Cl Cl Cl Cl

Coordination Polyhedra Could do the opposite, but conventionally choose the cation Can predict the coordination by considering the radius ratio: RC/RA Cations are generally smaller than anions so begin with maximum ratio = 1.0 Na Na Cl Na

Coordination Polyhedra Radius Ratio: RC/RA = 1.0 (commonly native elements) Equal sized spheres “Closest Packed” Hexagonal array: 6 nearest neighbors in the plane Note dimples in which next layer atoms will settle Two dimple types: Type 1 point NE Type 2 point SW They are equivalent since you could rotate the whole structure 60o and exchange them 2 1

Closest Packing Add next layer (red) Red atoms can only settle in one dimple type Both types are identical and red atoms could settle in either Once first red atom settles in, can only fill other dimples of that type In this case filled all type 2 dimples 1

Closest Packing Third layer ?? Third layer dimples are now different! Call layer 1 A sites Layer 2 = B sites (no matter which choice of dimples is occupied) Layer 3 can now occupy A-type site (directly above yellow atoms) or C-type site (above voids in both A and B layers)

Closest Packing Third layer: If occupy A-type site the layer ordering becomes A-B-A-B and creates a hexagonal closest packed structure (HCP) Coordination number (nearest or touching neighbors) = 12 6 coplanar 3 above the plane 3 below the plane

Closest Packing Third layer: If occupy A-type site the layer ordering becomes A-B-A-B and creates a hexagonal closest packed structure (HCP)

Closest Packing Third layer: If occupy A-type site the layer ordering becomes A-B-A-B and creates a hexagonal closest packed structure (HCP)

Closest Packing Third layer: If occupy A-type site the layer ordering becomes A-B-A-B and creates a hexagonal closest packed structure (HCP)

Closest Packing Third layer: If occupy A-type site the layer ordering becomes A-B-A-B and creates a hexagonal closest packed structure (HCP) Note top layer atoms are directly above bottom layer atoms

Closest Packing Third layer: Unit cell

Closest Packing Third layer: Unit cell

Closest Packing Third layer: Unit cell

Closest Packing Third layer: View from top shows hexagonal unit cell

Closest Packing Third layer: View from top shows hexagonal unit cell

Hexagonal Closest Packing Click to run animation Case Klein animation for Mineral Science, © John Wiley & Sons

Closest Packing Alternatively we could place the third layer in the C-type site (above voids in both A and B layers)

Closest Packing Third layer: If occupy C-type site the layer ordering is A-B-C-A-B-C and creates a cubic closest packed structure (CCP) Blue layer atoms are now in a unique position above voids between atoms in layers A and B

Closest Packing Third layer: If occupy C-type site the layer ordering is A-B-C-A-B-C and creates a cubic closest packed structure (CCP) Blue layer atoms are now in a unique position above voids between atoms in layers A and B

Closest Packing Third layer: If occupy C-type site the layer ordering is A-B-C-A-B-C and creates a cubic closest packed structure (CCP) Blue layer atoms are now in a unique position above voids between atoms in layers A and B

Closest Packing Third layer: If occupy C-type site the layer ordering is A-B-C-A-B-C and creates a cubic closest packed structure (CCP) Blue layer atoms are now in a unique position above voids between atoms in layers A and B

Closest Packing Third layer: If occupy C-type site the layer ordering is A-B-C-A-B-C and creates a cubic closest packed structure (CCP) Blue layer atoms are now in a unique position above voids between atoms in layers A and B

Closest Packing A-layer C-layer B-layer A-layer View from the same side shows the face-centered cubic unit cell that results. The atoms are slightly shrunken to aid in visualizing the structure A-layer C-layer B-layer A-layer

Closest Packing Rotating toward a top view

Closest Packing Rotating toward a top view

Closest Packing You are looking at a top yellow layer A with a blue layer C below, then a red layer B and a yellow layer A again at the bottom

Cubic Closest Packing Click to run animation Case Klein animation for Mineral Science, © John Wiley & Sons

What happens when RC/RA decreases? The center cation becomes too small for the XII site (as if a hard-sphere atom model began to rattle in the XII site) and it drops to the next lower coordination number (next smaller site). It will do this even if it is slightly too large for the next lower site. It is as though it is better to fit a slightly large cation into a smaller site than to have one rattle about in a site that is too large.

Coordination Polyhedra Click to run animation Case Klein animation for Mineral Science, © John Wiley & Sons

The next smaller crystal site is: Body-Centered Cubic (BCC) with cation (red) in the center of a cube Coordination number is now 8 (corners of cube)

A central cation will remain in VIII coordination with decreasing RC/RA until it again reaches the limiting situation in which all atoms mutually touch. Then a hard-sphere cation would “rattle” in the position, and it would shift to the next lower coordination (next smaller site). What is the RC/RA of that limiting condition?? Set = 1 arbitrary since will deal with ratios Diagonal length then = 2

A central cation will remain in VIII coordination with decreasing RC/RA until it again reaches the limiting situation in which all atoms mutually touch. Then a hard-sphere cation would “rattle” in the position, and it would shift to the next lower coordination (next smaller site). What is the RC/RA of that limiting condition?? Rotate

A central cation will remain in VIII coordination with decreasing RC/RA until it again reaches the limiting situation in which all atoms mutually touch. Then a hard-sphere cation would “rattle” in the position, and it would shift to the next lower coordination (next smaller site). What is the RC/RA of that limiting condition?? Rotate

A central cation will remain in VIII coordination with decreasing RC/RA until it again reaches the limiting situation in which all atoms mutually touch. Then a hard-sphere cation would “rattle” in the position, and it would shift to the next lower coordination (next smaller site). What is the RC/RA of that limiting condition?? Rotate

A central cation will remain in VIII coordination with decreasing RC/RA until it again reaches the limiting situation in which all atoms mutually touch. Then a hard-sphere cation would “rattle” in the position, and it would shift to the next lower coordination (next smaller site). What is the RC/RA of that limiting condition?? Rotate

A central cation will remain in VIII coordination with decreasing RC/RA until it again reaches the limiting situation in which all atoms mutually touch. Then a hard-sphere cation would “rattle” in the position, and it would shift to the next lower coordination (next smaller site). What is the RC/RA of that limiting condition?? Rotate

A central cation will remain in VIII coordination with decreasing RC/RA until it again reaches the limiting situation in which all atoms mutually touch. Then a hard-sphere cation would “rattle” in the position, and it would shift to the next lower coordination (next smaller site). What is the RC/RA of that limiting condition?? Rotate

A central cation will remain in VIII coordination with decreasing RC/RA until it again reaches the limiting situation in which all atoms mutually touch. Then a hard-sphere cation would “rattle” in the position, and it would shift to the next lower coordination (next smaller site). What is the RC/RA of that limiting condition?? Rotate

A central cation will remain in VIII coordination with decreasing RC/RA until it again reaches the limiting situation in which all atoms mutually touch. Central Plane What is the RC/RA of that limiting condition?? 1.732 = dC + dA If dA = 1 then dC = 0.732 dC/dA = RC/RA = 0.732/1 = 0.732

The limits for VIII coordination are thus between 1 The limits for VIII coordination are thus between 1.0 (when it would by CCP or HCP) and 0.732 Note: BCC is not a cosest-packed oxygen arrangement, so it may not occur in all ionic crystal lattices

As RC/RA continues to decrease below the 0 As RC/RA continues to decrease below the 0.732 the cation will move to the next lower coordination: VI, or octahedral. The cation is in the center of an octahedron of closest-packed oxygen atoms

As RC/RA continues to decrease below the 0 As RC/RA continues to decrease below the 0.732 the cation will move to the next lower coordination: VI, or octahedral. The cation is in the center of an octahedron of closest-packed oxygen atoms

As RC/RA continues to decrease below the 0 As RC/RA continues to decrease below the 0.732 the cation will move to the next lower coordination: VI, or octahedral. The cation is in the center of an octahedron of closest-packed oxygen atoms

As RC/RA continues to decrease below the 0 As RC/RA continues to decrease below the 0.732 the cation will move to the next lower coordination: VI, or octahedral. The cation is in the center of an octahedron of closest-packed oxygen atoms

As RC/RA continues to decrease below the 0 As RC/RA continues to decrease below the 0.732 the cation will move to the next lower coordination: VI, or octahedral. The cation is in the center of an octahedron of closest-packed oxygen atoms

As RC/RA continues to decrease below the 0 As RC/RA continues to decrease below the 0.732 the cation will move to the next lower coordination: VI, or octahedral. The cation is in the center of an octahedron of closest-packed oxygen atoms What is the RC/RA of that limiting condition?? 1.414 = dC + dA If dA = 1 then dC = 0.414 dC/dA = RC/RA = 0.414/1 = 0.414

As RC/RA continues to decrease below the 0 As RC/RA continues to decrease below the 0.414 the cation will move to the next lower coordination: IV, or tetrahedral. The cation is in the center of an tetrahedron of closest-packed oxygen atoms

As RC/RA continues to decrease below the 0 As RC/RA continues to decrease below the 0.414 the cation will move to the next lower coordination: IV, or tetrahedral. The cation is in the center of an tetrahedron of closest-packed oxygen atoms

As RC/RA continues to decrease below the 0 As RC/RA continues to decrease below the 0.414 the cation will move to the next lower coordination: IV, or tetrahedral. The cation is in the center of an tetrahedron of closest-packed oxygen atoms

As RC/RA continues to decrease below the 0 As RC/RA continues to decrease below the 0.414 the cation will move to the next lower coordination: IV, or tetrahedral. The cation is in the center of an tetrahedron of closest-packed oxygen atoms

As RC/RA continues to decrease below the 0 As RC/RA continues to decrease below the 0.414 the cation will move to the next lower coordination: IV, or tetrahedral. The cation is in the center of an tetrahedron of closest-packed oxygen atoms

As RC/RA continues to decrease below the 0 As RC/RA continues to decrease below the 0.414 the cation will move to the next lower coordination: IV, or tetrahedral. The cation is in the center of an tetrahedron of closest-packed oxygen atoms

As RC/RA continues to decrease below the 0 As RC/RA continues to decrease below the 0.414 the cation will move to the next lower coordination: IV, or tetrahedral. The cation is in the center of an tetrahedron of closest-packed oxygen atoms

As RC/RA continues to decrease below the 0 As RC/RA continues to decrease below the 0.414 the cation will move to the next lower coordination: IV, or tetrahedral. The cation is in the center of an tetrahedron of closest-packed oxygen atoms What is the RC/RA of the limiting condition?? Center-to-corner distance of a tetrahedron with edges of 1.0 = 0.6124 RC = 0.612 - 0.5 = 0.1124 RC/RA = 0.1124/0.5 = 0.225

As RC/RA continues to decrease below the 0 As RC/RA continues to decrease below the 0.22 the cation will move to the next lower coordination: III. The cation moves from the center of the tetrahedron to the center of an coplanar tetrahedral face of 3 oxygen atoms What is the RC/RA of the limiting condition?? cos 60 = 0.5/y y = 0.577 RC = 0.577 - 0.5 = 0.077 RC/RA = 0.077/0.5 = 0.155

If RC/RA decreases below the 0 If RC/RA decreases below the 0.15 (a are situation) the cation will move to the next lower coordination: II. The cation moves directly between 2 neighboring oxygen atoms

Homework Exercise Si+4 Mg2+ Al3+ Ti4+ K+ Ca2+ Fe2+ Na+ Use RC/ROxygen and the limits above to determine the probable coordination of the following elements in silicate and oxide minerals: Si+4 Mg2+ Al3+ Ti4+ K+ Ca2+ Fe2+ Na+ Correct RC for cases in which the coordination is not VI (the standard) and recalculate the ratio