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Chapter 19 d-Metal complexes: electronic structure and spectra

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<strong>Chapter</strong> <strong>19</strong> d-<strong>Metal</strong> <strong>complexes</strong>: <strong>electronic</strong><br />

<strong>structure</strong> <strong>and</strong> <strong>spectra</strong><br />

Electronic <strong>structure</strong><br />

<strong>19</strong>.1 Crystal-field theory<br />

<strong>19</strong>.2 Lig<strong>and</strong>-field theory<br />

Electronic-<strong>spectra</strong><br />

<strong>19</strong>.3 <strong>electronic</strong> <strong>spectra</strong> of atoms<br />

<strong>19</strong>.4 <strong>electronic</strong> <strong>spectra</strong> of <strong>complexes</strong><br />

<strong>19</strong>.5 Charge-transfer b<strong>and</strong>s<br />

<strong>19</strong>.6 Selection rules <strong>and</strong> intensities<br />

<strong>19</strong>.7 Luminescence


<strong>Chapter</strong> 10 Coordination Chemistry II:<br />

Bonding<br />

10-1 Experimental Evidence for Electronic Structures<br />

10-2 Theories of Electronic Structure<br />

10-3 Lig<strong>and</strong> Field Theory<br />

10-4 Angular Overlap<br />

10-5 The Jahn-Teller Effect<br />

10-6 Four- <strong>and</strong> Six-Coordinate Preferences<br />

10-7 Other Shapes<br />

“Inorganic Chemistry” Third Ed. Gary L. Miessler, Donald A. Tarr, 2004, Pearson<br />

Prentice Hall<br />

http://en.wikipedia.org/wiki/Expedia


Experimental Evidence for Electronic Structures<br />

Thermodynamic Data<br />

Magnetic Susceptibility<br />

Electronic Spectra<br />

Coordination Numbers <strong>and</strong> Molecular<br />

Shapes


Experimental Evidence for Electronic Structures;<br />

Thermodynamic Data<br />

One of the primary goal of a bonding theory is to<br />

explain the energy of compound.<br />

The energy is openly not determined directly by<br />

experiment.<br />

Thermodynamic measurements of enthalpies <strong>and</strong><br />

free energies of reaction are used to compare.<br />

Bonding strength Stability constants(formation constants)


Experimental Evidence for Electronic Structures;<br />

Thermodynamic Data<br />

What is the stability constants<br />

The equilibrium constants for formation of<br />

coordination complex.


Experimental Evidence for Electronic Structures;<br />

Thermodynamic Data<br />

Stability constants<br />

HSAB concepts<br />

Thermodynamic values <br />

Prediction of properties, <strong>structure</strong>s


Experimental Evidence for Electronic Structures;<br />

Thermodynamic Data<br />

HSAB concepts<br />

The gist of this theory is that soft acids react faster <strong>and</strong> form<br />

stronger bonds with soft bases, whereas hard acids react<br />

faster <strong>and</strong> form stronger bonds with hard bases, all other factors<br />

being equal.<br />

The classification in the original work was mostly based on<br />

equilibrium constants for reaction of two Lewis bases competing<br />

for a Lewis acid.<br />

Hard acids <strong>and</strong> hard bases tend to have:<br />

small size<br />

high oxidation state<br />

low polarizability<br />

high electronegativity<br />

energy low-lying HOMO (bases) or energy high-lying LUMO<br />

(acids).


Experimental Evidence for Electronic Structures;<br />

Thermodynamic Data<br />

HSAB concepts


Experimental Evidence for Electronic Structures;<br />

Thermodynamic Data<br />

Chelating Lig<strong>and</strong>s<br />

Entropy Effect<br />

Chelate Effect<br />

Five or six membered ring<br />

en vs methyl amine<br />

Figure in head….<br />

Stability….


Experimental Evidence for Electronic Structures;<br />

Magnetic Susceptibility<br />

The magnetic properties of a coordination<br />

compound can provide indirect evidence of the<br />

orbital energy level.<br />

Hund’s rule the max. # of unpaired e - .<br />

Diamagnetic: all e - paried repelled by a magnetic field<br />

Paramagnetic: all e - paried attracted into a magnetic field<br />

Magnetic Susceptibility: Measuring Magnetism


Experimental Evidence for Electronic Structures;<br />

Magnetic Susceptibility<br />

Magnetic Susceptibility<br />

Gouy method<br />

A sample that is to be tested is suspended<br />

from a balance between the poles of a<br />

magnet. The balance measures the<br />

apparent change in the mass of the<br />

sample as it is repelled or attracted by the<br />

magnetic field.


Experimental Evidence for Electronic Structures;<br />

Magnetic Susceptibility<br />

In physics <strong>and</strong> applied disciplines such as electrical<br />

engineering, the magnetic susceptibility is the degree of<br />

magnetization of a material in response to an applied<br />

magnetic field.<br />

Electron spin Spin magnetic moment (m s )<br />

Total spin magnetic moment Spin quantum # S (sum of m s )<br />

Isolated oxygen atom 1s 2 2s 2 p 4<br />

S = +1/2 +1/2 +1/2 -1/2 = 1<br />

Electron spin Orbital magnetic moment (m l )<br />

Total orbital magnetic moment Orbital quantum # L (sum of m l )<br />

Max. L for the p 4<br />

L = +1 +0 -1 +1 = 1


Experimental Evidence for Electronic Structures;<br />

Magnetic Susceptibility<br />

Two sources of magnetic moment – spin (S) <strong>and</strong> Angular (L) motions of electrons<br />

Spin quantum number<br />

Angular momentum quantum number<br />

The equation for the magnetic moment<br />

Contribution from L is small in first transition series<br />

2.00023 ≈ 2


Experimental Evidence for Electronic Structures;<br />

Electronic Spectra<br />

Give a direct evidence of orbital energy level<br />

Give an information for geometry of <strong>complexes</strong>


Theories of Electronic Structure<br />

Valence bond theory<br />

Crystal field theory<br />

Lig<strong>and</strong> field theory<br />

Angular overlap method


Theories of Electronic Structure;<br />

Valence bond theory<br />

Hybridization ideas<br />

Octahedral: d 2 sp 3<br />

d orbitals could be 3d or 4d for the first-row<br />

transition metals. (hyperligated, hypoligated)


Theories of Electronic Structure;<br />

Valence bond theory<br />

Fe(III)<br />

Isolated ion; 5 unpaired e -<br />

In O h compound; 1 or 5 unpaired e -<br />

Co(II)<br />

Low spin<br />

Low spin<br />

High spin<br />

High spin


Theories of Electronic Structure;<br />

Crystal field theory<br />

Crystal field theory (CFT) is a model that describes the<br />

<strong>electronic</strong> <strong>structure</strong> of transition metal compounds, all of<br />

which can be considered coordination <strong>complexes</strong>.<br />

CFT successfully accounts for some magnetic properties,<br />

colours, hydration enthalpies, <strong>and</strong> spinel <strong>structure</strong>s of<br />

transition metal <strong>complexes</strong>, but it does not attempt to<br />

describe bonding.<br />

CFT was developed by physicists Hans Bethe <strong>and</strong> John<br />

Hasbrouck van Vleck in the <strong>19</strong>30s.<br />

CFT was subsequently combined with molecular orbital<br />

theory to form the more realistic <strong>and</strong> complex lig<strong>and</strong> field<br />

theory (LFT), which delivers insight into the process of<br />

chemical bonding in transition metal <strong>complexes</strong>.


Theories of Electronic Structure;<br />

Crystal field theory<br />

Repulsion between d-orbital electrons <strong>and</strong> lig<strong>and</strong> electrons<br />

Splitting of energy levels of d-orbitals


Theories of Electronic Structure;<br />

Crystal field theory


Theories of Electronic Structure;<br />

Crystal field theory


Theories of Electronic Structure;<br />

Crystal field theory<br />

Electrostatic approach<br />

In an Octahedral field of lig<strong>and</strong> e - pairs; any e -<br />

in them are repelled by the field.<br />

Crystal field stabilization energy (CFSE);<br />

the actual distribution vs the uniform field.<br />

Good for the concept of the repulsion of<br />

orbitals by the lig<strong>and</strong>s but no explanation<br />

for bonding in coordination <strong>complexes</strong>.


Theories of Electronic Structure;<br />

Crystal field theory


Theories of Electronic Structure;<br />

Crystal field theory


Theories of Electronic Structure;<br />

Crystal field theory


Theories of Electronic Structure;<br />

Crystal field theory


Theories of Electronic Structure;<br />

Crystal field theory


Theories of Electronic Structure;<br />

Crystal field theory


Theories of Electronic Structure;<br />

Crystal field theory<br />

Why are <strong>complexes</strong> formed in crystal field theory<br />

Crystal Field Stabilization Energy (CFSE)<br />

Or Lig<strong>and</strong> Field Stabilization Energy (LFSE)<br />

the stabilization of the d orbitals because of<br />

metal-lig<strong>and</strong> environments


Theories of Electronic Structure;<br />

Crystal field theory<br />

∆E = strong field – weak field<br />

∆E > 0 weak field<br />

∆E < 0 strong field


Theories of Electronic Structure;<br />

Crystal field theory<br />

What determine <br />

Depends on the relative energies<br />

of the metal ions <strong>and</strong> lig<strong>and</strong><br />

orbitals <strong>and</strong> on the degree of<br />

overlap.


Theories of Electronic Structure;<br />

Crystal field theory<br />

Spectrochemical Series for <strong>Metal</strong> Ions<br />

Oxidation # ∆<br />

Small size & higher charge<br />

Pt 4+ > Ir 3+ > Pd 4+ > Ru 3+ > Rh 3+ >Mo 3+ ><br />

Mn 4+ > Co 3+ > Fe 3+ > V 2+ > Fe 2+<br />

Co 2+ > Ni 2+ > Mn 2+<br />

Only low spin aqua complex


Lig<strong>and</strong> field theory;<br />

Molecular orbitals for Octahedral <strong>complexes</strong><br />

CFT & MO were combined<br />

The d x2-y2 <strong>and</strong> d z2 orbitals can form bonding orbitals<br />

with the lig<strong>and</strong> orbitals, but d xy , d xz , <strong>and</strong> d yz orbitals<br />

cannot form bonding orbitals


Lig<strong>and</strong> field theory;<br />

Molecular orbitals for Octahedral <strong>complexes</strong><br />

The combination of<br />

the lig<strong>and</strong> <strong>and</strong> metal<br />

orbitals (4s, 4p x , 4p y ,<br />

4p z , 3d z2 , <strong>and</strong> 3d x2-y2 )<br />

form six bonding <strong>and</strong><br />

six antibonding with<br />

a 1g , e g , t 1u symmetries.<br />

The metal T 2g orbitals<br />

do Electron not have in bonding<br />

appropriate orbitals provide symmetry the<br />

- nonbonding<br />

potential energy that holds<br />

molecules together


Lig<strong>and</strong> field theory;<br />

Orbital Splitting <strong>and</strong> Electron Spin<br />

Strong-field lig<strong>and</strong> – Lig<strong>and</strong>s whose orbitals<br />

interact strongly with the metal orbitals <br />

large ∆ o<br />

Weak-field lig<strong>and</strong>.<br />

d 0 ~d 3 <strong>and</strong> d 8 ~d 10 – only one electron<br />

configuration possible no difference in the<br />

net spin<br />

Strong fields lead to low-spin <strong>complexes</strong><br />

Weak fields lead to high-spin <strong>complexes</strong>


Lig<strong>and</strong> field theory;<br />

Orbital Splitting <strong>and</strong> Electron Spin<br />

What determine <br />

Depends on the relative<br />

energies of the metal ions<br />

<strong>and</strong> lig<strong>and</strong> orbitals <strong>and</strong> on<br />

the degree of overlap.


Lig<strong>and</strong> field theory;<br />

Orbital Splitting <strong>and</strong> Electron Spin<br />

Spectrochemical Series for <strong>Metal</strong> Ions<br />

Oxidation # ∆<br />

Small size & higher charge<br />

Pt 4+ > Ir 3+ > Pd 4+ > Ru 3+ > Rh 3+ >Mo 3+ ><br />

Mn 4+ > Co 3+ > Fe 3+ > V 2+ > Fe 2+<br />

Co 2+ > Ni 2+ > Mn 2+


Lig<strong>and</strong> field theory;<br />

Lig<strong>and</strong> field Stabilization Energy


Lig<strong>and</strong> field theory;<br />

Orbital Splitting <strong>and</strong> Electron Spin<br />

Orbital configuration of the complex is<br />

determined by ∆ o , c , <strong>and</strong> e<br />

In general ∆ o for 3 + ions is larger than ∆ o for 2 + ions<br />

with the same # of e - .<br />

∆ o > low-spin<br />

∆ o < high-spin<br />

For low-spin<br />

configuration<br />

Require a strong<br />

field lig<strong>and</strong>


Lig<strong>and</strong> field theory;<br />

Lig<strong>and</strong> field Stabilization Energy


Lig<strong>and</strong> field theory;<br />

Orbital Splitting <strong>and</strong> Electron Spin<br />

The position of the metal in the periodic<br />

table<br />

Second <strong>and</strong> third transition series form lowspin<br />

more easily than metals form the first<br />

transition series<br />

-The greater overlap between the larger 4d<br />

<strong>and</strong> 5d orbitals <strong>and</strong> the lig<strong>and</strong> orbitals<br />

-A decreased pairing energy due to the<br />

larger volume available for electrons


Lig<strong>and</strong> field theory;<br />

Pi-Bonding<br />

The reducible representation is


Lig<strong>and</strong> field theory;<br />

Pi-Bonding<br />

LUMO orbitals:can be used<br />

for bonding with metal<br />

HOMO


Lig<strong>and</strong> field theory;<br />

Pi-Bonding<br />

metal-to-lig<strong>and</strong> bonding<br />

or back-bonding<br />

-Increase stability<br />

-Low-spin configuration<br />

-Result of transfer of<br />

negative charge away from<br />

the metal ion<br />

Lig<strong>and</strong>-to metal bonding<br />

-decrease stability<br />

-high-spin configuration


Lig<strong>and</strong> field theory;<br />

Square planar Complexes; Sigma bonding


Lig<strong>and</strong> field theory;<br />

Square planar Complexes; Sigma bonding<br />

ll<br />

⊥<br />

16 e - e - from metal<br />

8 e -


Lig<strong>and</strong> field theory;<br />

Tetrahedral Complexes; Sigma bonding<br />

The reducible representation is<br />

A 1 <strong>and</strong> T 2


Lig<strong>and</strong> field theory;<br />

Tetrahedral Complexes; Pi bonding<br />

The reducible representation is<br />

E, T 1 <strong>and</strong> T 2


Angular Overlap<br />

LFT <br />

No explicit use of the energy change that results<br />

Difficult to use other than octahedral, square<br />

planar, tetrahedral.<br />

Deal with a variety of possible geometries <strong>and</strong><br />

with a mixture of lig<strong>and</strong>. Angular Overlap<br />

Model<br />

The strength of interaction between individual lig<strong>and</strong><br />

orbitals <strong>and</strong> metal d orbitals based on the overlap<br />

between them.


Angular Overlap:<br />

Sigma-Donor Interactions<br />

The strongest interaction<br />

There are no examples of <strong>complexes</strong> with e - in<br />

the antibonding orbitals from s <strong>and</strong> p orbitals,<br />

<strong>and</strong> these high-energy antibonding orbitals are<br />

not significant in describing the <strong>spectra</strong> of<br />

<strong>complexes</strong>. we will not consider them further.


Angular Overlap:<br />

Sigma-Donor Interactions


Angular Overlap:<br />

Sigma-Donor Interactions<br />

Stabilization is 12e


Angular Overlap:<br />

Pi-Acceptor Interactions<br />

The strongest interaction is considered to<br />

be between a metal d xy orbitals <strong>and</strong> a lig<strong>and</strong> *<br />

orbital.<br />

Because of the overlap for these orbitals is<br />

smaller than the overlap, e < e .


Angular Overlap:<br />

Pi-Acceptor Interactions


Angular Overlap:<br />

Pi-Acceptor Interactions


Angular Overlap:<br />

Pi-Donor Interactions<br />

In general, in situations involving lig<strong>and</strong>s that can<br />

behave as both acceptors <strong>and</strong> donors (such<br />

as CO, CN - ), the acceptor nature predominates.


Angular Overlap:<br />

Pi-Donor Interactions


Angular Overlap:<br />

Pi-Acceptor Interactions


Angular Overlap:<br />

Types of the lig<strong>and</strong>s <strong>and</strong> the spectrochemical series<br />

Spectrochemical Series for Lig<strong>and</strong>s<br />

CO > CN - > PPh 3 > NO 2- > phen > bipy > en<br />

NH 3 > py > CH 3 CN > NCS - > H 2 O > C 2 O 4<br />

2-<br />

OH - > RCO 2- > F - > N 3- > NO 3- > Cl - > SCN -<br />

S 2- > Br - > I -<br />

donor only<br />

acceptor (strong field lig<strong>and</strong>)<br />

donor(weak field lig<strong>and</strong>)


Angular Overlap:<br />

Magnitudes of e e<strong>and</strong> ∆<br />

<strong>Metal</strong> <strong>and</strong> lig<strong>and</strong>


Angular Overlap:<br />

Magnitudes of e e<strong>and</strong> ∆<br />

Angular overlap<br />

parameters derived<br />

from <strong>electronic</strong><br />

<strong>spectra</strong><br />

e is always larger<br />

than e . overlap<br />

iso<strong>electronic</strong><br />

The magnitudes of<br />

both the <strong>and</strong> <br />

parameters with<br />

size <strong>and</strong> <br />

electronegativity of<br />

the halide ions.<br />

overlap


Angular Overlap:<br />

Magnitudes of e e<strong>and</strong> ∆<br />

Can describe the<br />

<strong>electronic</strong> energy<br />

of <strong>complexes</strong> with<br />

different shapes or<br />

with combinations<br />

of different liagnds.<br />

The magnitude of<br />

∆ o Magnetic<br />

properties <strong>and</strong><br />

visible spectrum.


Angular Overlap:<br />

The Jahn-Teller Effect<br />

There cannot be unequal occupation of orbitals with identical orbitals.<br />

To avoid such unequal occupation, the molecule distorts so that<br />

these orbitals no longer degenerate.<br />

In other words, if the ground electron configuration of a nonlinear<br />

complex is orbitally degenerate, the complex will distort to remove<br />

the degeneracy <strong>and</strong> achieve a lower energy.


Angular Overlap:<br />

The Jahn-Teller Effect


Angular Overlap:<br />

Four- <strong>and</strong> Six-Coordinate Preference<br />

Only bonding is considered.<br />

Angular overlap calculations<br />

Low-spin square planar<br />

Large # of bonds formed in<br />

the octahedral <strong>complexes</strong>.


Angular Overlap:<br />

Four- <strong>and</strong> Six-Coordinate Preference


Angular Overlap:<br />

Four- <strong>and</strong> Six-Coordinate Preference<br />

How accurate are these predictions<br />

Their success is variable, because of there are other differences<br />

between metals <strong>and</strong> between lig<strong>and</strong>s.<br />

In addition, bond lengths for the same lig<strong>and</strong>-metal pair depend on<br />

the geometry of the complex.<br />

The interactions of the s <strong>and</strong> p orbitals.<br />

The formation enthalpy for <strong>complexes</strong> also becomes more negative<br />

with increasing atomic number <strong>and</strong> increasing ionization energy.<br />

By careful selection of lig<strong>and</strong>s, many of the transition metal ions can<br />

form compounds with geometries other than octahedral.


Angular Overlap:<br />

Other shapes<br />

1<br />

1<br />

1<br />

Strength of –interaction<br />

1<br />

1<br />

2+3/4 9/8 9/8 0 0


Angular Overlap:<br />

Other shapes<br />

Trigonal-bipyramidal ML 5 (D 3h ) -donor only


Homework<br />

Exercise 10-1~10-11<br />

Problem 2, 6a, 6c,11, 13, 16.

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