CFT, LFT, MOT It is all about d orbitals 3 d 2 2 x y 3 / 2 - - PowerPoint PPT Presentation

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CFT, LFT, MOT It is all about d orbitals 3 d 2 2 x y 3 / 2 - - PowerPoint PPT Presentation

CFT, LFT, MOT It is all about d orbitals 3 d 2 2 x y 3 / 2 2 1 Z Z 2 2 = r exp( Zr / 3 a ) sin cos 2 3 d a a 2 2 81 2 x y


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SLIDE 1

CFT, LFT, MOT

It is all about d orbitals

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SLIDE 2
  • Y. U. Sasidhar

r/a

φ θ π 2 cos sin ) 3 / exp( 2 81 1

2 2 2 2 / 3 3

2 2

a Zr r a Z a Z

y x

d

−             = Ψ

) 3 / exp( 1 30 81 4

2 2 2 / 7 2 / 3 3

a Zr r a Z a R d − = ×

2 2

3

y x

d

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SLIDE 3

Angular nodes: x = ± y x/a y/a

+

  • +
  • φ

θ π 2 cos sin ) 3 / exp( 2 81 1

2 2 2 2 / 3 3

2 2

a Zr r a Z a Z

y x

d

−             = Ψ

2 2 2

/ ) ( r y x −

2 2

3

y x

d

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SLIDE 4

x/a y/a angular nodes: x=0, y=0

+

  • +
  • φ

θ π 2 sin sin ) 3 / exp( 2 81 1

2 2 2 2 / 3 3

a Zr r a Z a Z

xy

d

−             = Ψ

2

/ r xy

xy

d 3

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SLIDE 5

2 angular nodes

+ +

  • z/a

x/a

( )

) 1 cos 3 ( ) 3 / exp( 1 6 81 1

2 2 2 2 / 7 2 / 3 3

2

− − = Ψ θ π a Zr a r Z a

dz

) 1 3 (

2 2

− r z

2

3

z

d

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SLIDE 6

( )

) 1 cos 3 ( ) 3 / exp( 1 6 81 1

2 2 2 2 / 7 2 / 3 3

2

− − = Ψ θ π a Zr a r Z a

dz

2

3

z

d

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SLIDE 7

( )

) 1 cos 3 ( ) 3 / exp( 1 6 81 1

2 2 2 2 / 7 2 / 3 3

2

− − = Ψ θ π a Zr a r Z a

dz

2

3

z

d

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SLIDE 8

is only a nickname

Full label:

2

3 z d

2 2 2

2

3

y x z

d

− −

( )

) 1 cos 3 ( ) 3 / exp( 1 6 81 1

2 2 2 2 / 7 2 / 3 3

2

− − = Ψ θ π a Zr a r Z a

dz

) 1 3 (

2 2

− r z ) (

2 2 2

z y x + +

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SLIDE 9

The eg and t2g groups

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SLIDE 10

The eg and t2g groups

Which group is destabilized to a greater extent in an octahedral field? What are high spin and low spin complexes? Which configurations yield HS complexes? Which yield LS complexes?

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SLIDE 11

Jahn Teller theorem

For any nonlinear molecular system in a degenerate electronic state, a distortion will occur so as to lower the symmetry and remove the degeneracy Nondegenerate systems: d3, d5 high spin, d6 low spin, d8, d10 Doubly degenerate: more pronounced Jahn-Teller distortions Triply degenerate: less pronounced Jahn-Teller distortions

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SLIDE 12

Tetragonal distortion (axial ligands moving

  • ut)

Oh to D4h b1g (dx2-y2) a1g (dz2) b2g (dxy) eg (dxz, dyz) What happens for a compression along z-axis? What happens in a square planar complex?

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SLIDE 13

Molecular Orbital Theory

  • Ligand

SALCs for an

  • ctahedral

complex

  • Metal AOs with matching symmetry
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SLIDE 14

Molecular Orbital Theory: ML6, σ-bond only

σ-SALCs: a1g + eg + t1u 3d orbitals: eg + t2g 4s orbital: a1g 4p orbitals: t1u a1g a1g* t1u t1u* eg eg* t2g

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SLIDE 15

Molecular Orbital Theory: ML6, σ-bonds

  • nly

σ-SALCs: a1g + eg + t1u 3d orbitals: eg + t2g 4s orbital: a1g 4p orbitals: t1u a1g a1g* t1u t1u* eg eg* t2g 10Dq Electrons from ligand Electrons from Metal ion

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SLIDE 16

Molecular Orbital Theory: ML6, σ-and π- bonds

σ-SALCs: a1g + eg + t1u 3d orbitals: eg + t2g 4s orbital: a1g 4p orbitals: t1u a1g a1g* t1u t1u* eg eg* t2g π-SALCs: t1g +t2g + t1u + t2u π(t2g) π∗(t2g) 10Dq t1u t1g + t2u

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SLIDE 17

Revision and Home Work

  • Tetrahedral ML4 complexes