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Lecture 9: Coordination and Pauling's Rules

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<strong>Lecture</strong> 9:<br />

<strong>Coordination</strong> <strong>and</strong> Pauling’s <strong>Rules</strong><br />

To underst<strong>and</strong> the atomic structure of minerals, , we typically think in<br />

terms of spherical cations <strong>and</strong> anions held together predominantly<br />

by ionic bonds<br />

One of the properties of these ions that we would like to know is their<br />

RADIUS, , I.e., their size<br />

This sounds easy, but remember, ions are really formed from nuclei<br />

with probability density clouds of electrons moving around them.<br />

Thus, we refer to:<br />

Effective Electrostatic Radii: “imaginary” fixed radii of an ion<br />

Why imaginary? Because electrons are in probability density<br />

clouds <strong>and</strong> because radii actually change somewhat depending on<br />

bonding environment


Given that the effective electrostatic radii is imaginary, how<br />

do we “measure” it???<br />

! Look at anion-cation bond lengths in structures with predominantly<br />

ionic bonding<br />

! Once you know the total bond distance <strong>and</strong> one ion radius, , you can<br />

calculate the other<br />

!Shannon <strong>and</strong> Prewitt (1969); Shannon (1976) used many oxide<br />

structures to regress average effective electrostatic radii of cations<br />

Example:<br />

Periclase (MgO)<br />

Mg-O length 2.11Å according to XRD<br />

O -2 eff = 1.32Å (by definition)<br />

So, Mg +2 eff = 2.11Å - 1.32Å = 0.79Å


Effective Electrostatic Radii<br />

Cation Radii ?? Elemental Radii (> or


Some General <strong>Rules</strong> Regarding Effective Electrostatic Radii:<br />

! Larger with Z within groups (going down columns)<br />

! Larger with increasing number<br />

Note: An exception is the so-called “Lanthanide Contraction”; trivalent<br />

lanthanides (La +3 to Lu +3 ) decrease in radius with increasing Z<br />

Why? Inner electron orbitals build before outer orbitals are added;<br />

higher nuclear charge combined with relatively weak shielding draws<br />

electrons into the nucleus<br />

! For cations with same electronic structure, radii decrease with<br />

increasing charge<br />

i.e. R eff P +5 < R eff Na + due to larger nuclear charge in P +5<br />

Effective Electrostatic Radii of Ions typically change somewhat with:<br />

COORDINATION NUMBER


COORDINATION NUMBER (C.N.): in packed ionic structures, the<br />

number of nearest neighbors (1st coordination shell); i.e. the<br />

number of anions surrounding a cation (or number of cations<br />

surrounding an anion)<br />

Example: K +<br />

6-fold coordination -> 1.38Å<br />

8-fold coordination -> 1.51Å<br />

10-fold coordination -> 1.59Å<br />

This increase in radius with coordination number reflects expansion of the<br />

cation into more available space between larger number of anions<br />

Regular <strong>Coordination</strong> Polyhedra: : all cation-anion distances assumed to<br />

be equal


Is it possible to predict coordination environments?


Pauling’s Rule #1 (‘Radius(<br />

Ratio Principal’):<br />

! The distance between cations <strong>and</strong> anions can be calculated<br />

from their effective electrostatic radii; coordination number<br />

depends on the relative radii of cations <strong>and</strong> surrounding<br />

anions<br />

! Greater radius = greater coordination number<br />

Note: ONLY strictly true for ionic bonding with undistorted polyhedra,<br />

pretending that ions are spheres (which they aren’t t ) <strong>and</strong> they are<br />

unpolarized<br />

Polarization: : distortion of ion shape; large, monovalent ions are<br />

most easily polarized


Pauling’s Rule #1 (‘Radius(<br />

Ratio Principal’):<br />

Radius Ratio (R.R.) = R c /R a<br />

R c = cation radius<br />

R a = anion radius<br />

2-fold: R.R. < 0.155<br />

3-fold: R.R. 0.155 - 0.225<br />

4-fold: R.R. 0.225 5 - 0.414<br />

6-fold: R.R. 0.414 - 0.732<br />

8-fold: R.R. 0.732 - 1.000


Pauling’s Rule #1 (‘Radius(<br />

Ratio Principal’):<br />

Example:<br />

R eff Na + = 1.10Å<br />

Cl - = 1.72Å<br />

R eff Cl<br />

C.N. of Na in NaCl?<br />

R.R. = 1.10/1.72 = 0.64<br />

6-Fold<br />

In 1929 Linus Pauling came up with some other useful rules…


Pauling’s Rule #2 (‘Electrostatic(<br />

Valency Principal’):<br />

! The strength of a bond (electrostatic valence) equals the ionic<br />

valence (charge) divided by the coordination number<br />

! Sum of bond valences = ionic valence<br />

E.V. = Z./C.N.<br />

Example: SiO 4<br />

Si +4 Each: Si-O<br />

O -2<br />

Si-O bond<br />

E.V. = +4/4 = 1<br />

O -2<br />

Si +4 O -2 O -2<br />

Each: O-Si bond<br />

E.V. = -2/2 = -1


Pauling’s Rule #2 (‘Electrostatic(<br />

Valency Principal’):<br />

Example: NaCl<br />

Cl -<br />

Each: Na-Cl bond<br />

E.V. = +1/6 = +1/6<br />

Cl - Cl -<br />

Na +<br />

Cl -<br />

Cl -<br />

Cl -<br />

Each: Cl-Na bond<br />

E.V. = -1/6 = -1/6<br />

Note: some problems with this approach -- irregular coordination<br />

polyhedra, , mixed bonding types


Pauling’s Rule #2 (‘Electrostatic(<br />

Valency Principal’):<br />

Isodemic: compounds with all bonds of equal strength<br />

Ex. Spinel<br />

AB 2 O 4 A = +2; B = +3<br />

By XRD, we know that AIV, BVI<br />

So, A = +2/4 = +1/2<br />

B = +3/6 = +1/2<br />

Anisodesmic: bonds of unequal strength; common in compounds with<br />

anionic complexes; electrostatic valence within the anionic<br />

complex is greater than half the anion charge<br />

Ex. Carbonate<br />

CO -2 3 C +4 is 3-fold with respect to O -2<br />

E.V. = +4/3 = 1 1/3<br />

(most strength within complex)<br />

Mesodesmic: bond strength is exactly half the anion charge<br />

Ex. Si-O<br />

O in silicates<br />

Si is 4-fold with respect to O E.V. = +4/4 = +1


Pauling’s Rule #3<br />

! Vertex-sharing (2 cations share 1 anion) between tetrahedra<br />

or octahedra is energetically stable<br />

! Edge-sharing (2 cations share 2 anions) between polyhedra is<br />

less stable; ; rare for tetrahedra, , more common for octahedra<br />

! Face-sharing (2 cations share 3 anions) between polyhedra is<br />

unstable; ; never occurs for tetrahedra; ; rare for octahedra<br />

Why? Electrostatic Repulsion<br />

Less of a problem for octahedra because cation-cation distances are<br />

longer <strong>and</strong> cations are typically of lower charge


Pauling’s Rule #4<br />

! Cations of high charge <strong>and</strong> small coordination number tend not to<br />

share anions with other cations<br />

! Why? Repulsion between cations<br />

Pauling’s Rule #5 (‘Principal(<br />

of Parsimony’)<br />

! The number of different components in a crystal tends to be small;<br />

if lots of ions are present, they tend to occupy the same structural<br />

position (‘sites(<br />

sites’)


<strong>Coordination</strong> of Common Cations <strong>and</strong> Anions:<br />

Most common element in crust by weight? O<br />

Therefore, many minerals contain O<br />

O -2 effective electrostatic radius: 1.27-1.34Å<br />

Si +4 : 4-fold<br />

Al +3 : 4-fold or 6-fold<br />

Fe +3 : 6-fold (4-fold)<br />

Mg +2 : 6-fold or 8-fold<br />

Fe +2 : 6-fold<br />

Mn +2 : 6-fold or 8-fold<br />

Na + : 8-fold<br />

Ca +2 : 8-fold<br />

K + : 12-fold

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