and to what degree they may be forbidden depends on selection rules:

Slides:



Advertisements
Similar presentations
Mysteries of polarized light Enantiomers have identical properties except in one respect: the rotation of the plane of polarization of light Enantiomers.
Advertisements

Schedule Lecture 1: Electronic absorption spectroscopy Jahn-Teller effect and the spectra of d1, d4, d6 and d9 ions Lecture 2: Interpreting electronic.
Lecture 30 Electronic Spectra of Coordination Compounds 1) Jahn-Teller effect Octahedral complexes can be a subject to tetragonal or trigonal distortions.
Coordination Chemistry Bonding in transition-metal complexes.
Coordination Chemistry III: Electronic Spectra
Coordination Chemistry Electronic Spectra of Metal Complexes
Placing electrons in d orbitals (strong vs weak field)
The Electronic Spectra of Coordination Compounds.
6  ligands x 2e each 12  bonding e “ligand character” “d 0 -d 10 electrons” non bonding anti bonding “metal character” ML 6  -only bonding The bonding.
1 Electronic (UV-visible) Spectroscopy | Electronic | XPS UPS UV-visible.
Coordination Chemistry Bonding in transition-metal complexes.
End result is that solution phase absorptions at room temperature are almost always broad because of the various number of photons (with different energies)
Transition Metals, Compounds and Complexes
Before we did: p2p2 M L & M S Microstate Table States (S, P, D) Spin multiplicity Terms 3 P, 1 D, 1 S Ground state term 3 P.
CHAPTER 5: CRYSTAL FIELD THEORY
UV-Vis spectroscopy Electronic absorption spectroscopy.
Bonding in coordination compounds
Vibrational and Rotational Spectroscopy
Spectral properties Colour of Transition metal complexes A substance exhibit colour because it has property of absorbing certain radiation from visible.
Electronic Spectroscopy
Lecture 18. d-d spectra and MO theory:
The Electronic Spectra of Coordination Compounds.
FT NMR WORKSHOP/===/ S.A.I.F./===/ NEHU/==/ Shillong INTRODUCTORY LECTURE S.ARAVAMUDHAN Distinct Spectroscopic context.
NATURE OF THE LIGAND- SMALL LIGANDS APPROACH THE LIGANDS EASILY, SO THEY CAN CAUSE GREAT CRYSTAL FIELD SPLITTING. LIGANDS CONTAINING EASILY POLARISABLE.
The Electronic Spectra of Coordination Compounds
Slide 2/12 Schedule Lecture 4: Re-cap Lecture 5:  -Acceptor Ligands and Biology N 2, CO, N 2 and O 2 complexes Lecture 6: M-M bonding Multiple bonds.
Ligand field theory considers the effect of different ligand environments (ligand fields) on the energies of the d- orbitals. The energies of the d orbitals.
The Electronic Spectra of Coordination Compounds
Sub-Topics Introduction to Transition Metals
Spectroscopy 2: Electronic Transitions CHAPTER 14.
Electronic Spectra of Coordination Compounds
Magnetic Properties from Molecules to Solids
Coordination complexes
Coordination Chemistry Bonding in transition-metal complexes
metal ion in a spherical
Isomerism & Crystal Field Theory Chapter 24 – Lecture 3
Octahedral Crystal Field Splitting
Applications of UV-Vis Spectroscopy
Applications of Crystal Field Theory: Ionic Radii
Free Ion Spectroscopic Terms for dn Configurations
Electronic spectra of transition metal complexes
Electronic spectra of transition metal complexes
Chem. 1B – 11/17 Lecture.
Metal-Ligand bonding in transition metal complexes
Electromagnetic Radiation, Cont….
RDCH 702 Lecture 4: Orbitals and energetics
Dear Students of Inorganic Chemistry 2,
Electronic Structure of Atoms
Metal-Ligand bonding in transition metal complexes
Character Tables for Point Groups
Diatomic molecules
Chemistry 481(01) Spring 2016 Instructor: Dr. Upali Siriwardane
Crystal Field Theory The relationship between colors and complex metal ions.
FT NMR WORKSHOP/===/ S.A.I.F./===/ NEHU/==/ Shillong
Quantum Numbers: specify the properties of atomic orbitals and their electrons.
Inorganic Spectra By Dr. Ahmed Hussein
Total Angular Momentum
10.3 NMR Fundamentals nuclear spin calculations and examples
Schedule Lecture 1: Electronic absorption spectroscopy Jahn-Teller effect and the spectra of d1, d4, d6 and d9 ions Lecture 2: Interpreting electronic.
A/Prof Adam Bridgeman CHEM2402/2912/2916 [Part 2]
Physical Chemistry Chapter V Polyatomic Molecular Structure 2019/4/10
semester 2 Lecture note 1 Crystal Field Theory
Invisible Ink 2[Co(H2O)6]Cl2(s) Co[CoCl4](s) + 12 H2O
Magnetic Properties of Complexes
Schedule Lecture 1: Electronic absorption spectroscopy Jahn-Teller effect and the spectra of d1, d4, d6 and d9 ions Lecture 2: Interpreting electronic.
Transition Metals and Color
Understanding the Absorption Electronic Spectra of Coordination Compounds at greater depth Ligand Field Theory Chapter 20.
CHEM 251 INORGANIC CHEMISTRY Chapter 4.
Dr. Pandit Khakre Asst. Prof Mrs. K.S.K. College, Beed.
Lecture 5: p-Acceptor Ligands and Biology N2, CO, N2 and O2 complexes
Presentation transcript:

and to what degree they may be forbidden depends on selection rules: Some transitions are not allowed does not mean that such a transition will never occur, but that it is less likely and that the intensity (molar absorption coefficient) of such an absorption band is very low. Whether transitions are allowed or forbidden, and to what degree they may be forbidden depends on selection rules: Laporte Selection Rule: In a molecule having center of symmetry, transitions between states of the same parity (symmetry with respect to a center of inversion) are forbidden. For example, transitions between states that arise from d orbitals are forbidden (g→g transitions; d orbitals are symmetric to inversion), but transitions between states arising from d and p orbitals are allowed (g→u transitions; p orbitals are anti-symmetric to inversion). Therefore, all d-d transitions in octahedral complexes are Laporte-forbidden. Laporte-allowed transitions involve Δl = ±1. ‘s ↔ p’, ‘p ↔ d’, ‘d ↔ f’ etc allowed (Δl = ±1) ‘s ↔ d’, ‘p ↔ f’ etc forbidden (Δl = ±2) ‘s ↔ s’, ‘p ↔ p’ , ‘d ↔ d’, ‘f ↔ f’ etc forbidden (Δl = 0) 1

Relaxation of Laporte Selection Rule ▪ Like all chemical bonds, octahedral complexes vibrate in ways (unsymmetrical vibrations) in which the center of symmetry is temporarily lost. This phenomenon, called vibronic (vibrational-electronic) coupling, can relax Laporte selection rule. They are often responsible for the bright colors of these complexes. ▪ In tetrahedral complexes, there is no center of symmetry and thus orbitals have no g or u designation. Therefore, the Laporte rule does not apply and the complexes exhibit strong colors. Intensities of Spectroscopic Bands in 3d Complexes Band Type εmax (L mol-1 cm-1) Spin forbidden, Laporte forbidden 10-3-1 Spin allowed, Laporte forbidden 1-100 Spin allowed, Laporte allowed 100-1000 Symmetry allowed (charge-transfer bands) 1,000-106

Selection Rules Spin Selection Rule: The overall spin S of a complex must not change during an electronic transition, hence, ΔS = 0. To be allowed, a transition must involve no change in spin state. This is because electromagnetic radiation usually cannot change the relative orientation of an electron spin. ▪ [Mn(H2O)6]2+ has a d5 configuration and it is a high-spin complex. Electronic transitions are not only Laporte-forbidden, but also spin-forbidden. The dilute solutions of Mn2+ complexes are therefore colorless. ▪ Certain complexes like MnO4- and CrO42- are intensely colored even though they have metal ions without electrons in d orbitals. The color of these complexes are not from d-d transitions, but from charge-transfer from ligand to metal orbitals.

Theoretical Paramagnetic Moment Paramagnetic moment originates from spin and orbital motion of unpaired electrons. ▪ When there is significant spin and orbital angular momentum contributions, theoretical μ is given by: The observed value of μ in complexes is always less than the theoretical value calculated from above equation. This occurs because the ligand field quenches orbital contribution to some extent. In the extreme case when L = 0, the orbital contribution to the magnetic moment is said to be quenched. When orbital angular momentum is absent, theoretical μ is given by: S = n/2 gives spin-only formula: μS+L μs.o. μs.o.

Orbital contribution to Magnetic Moment All values are for high-spin octahedral complexes.

When does orbital angular momentum contribute to paramagnetic moment? For orbital angular momentum to contribute, there must be an equivalent and degenerate orbital (similar in energy to that of the orbital occupied by the unpaired electrons). If this is so, the electrons can make use of the available orbitals to circulate or move around the center of the complexes and hence generate L and μL (it is the rotation of the electrons which induces the orbital contribution). Essential Conditions: 1) The orbitals should be degenerate (t2g or eg). 2) The orbitals should be similar in shape and size, so that they are transferable into one another by rotation about the same axis. 3) Orbitals must not contain electrons of identical spin.

When does orbital angular momentum contribute to paramagnetic moment? For an octahedral complex: Condition t2g set eg set 1 Obeyed 2 Not obeyed 3 Since condition 1 and 2 are satisfied, condition 3 will dictate whether it will generate μl or not. Does not matter since condition 2 is already not obeyed. These conditions are fulfilled whenever one or two of the three t2g orbitals contain an odd number of electrons. For an octahedral complex, orbital contributions are possible only when the t2g orbitals are asymmetrically occupied and for a tetrahedral complex, the t2 orbitals have to be asymmetrically occupied.

When does orbital angular momentum contribute to paramagnetic moment? 90o rotation about z-axis 45o rotation about z-axis dxy orbital can be converted into dx2-y2 orbital by a 45° rotation about z-axis. But, in an octahedral crystal field, the degeneracy between the dxy and dx2-y2 orbitals is lifted. Hence, orbital contribution about z-axis from dxy, dx2-y2 pair of orbitals disappears. dx2-y2 and dz2 orbitals can not be interconverted by rotation due to their different shapes. Thus, e(g) electrons have no orbital contribution to magnetic moment.

When does orbital angular momentum contribute to paramagnetic moment? dxz orbital can be converted into dyz orbital by a 90° rotation about z-axis. Thus, all t2(g) orbitals may be interconverted by rotation about suitable axes and we may expect orbital contributions from t2(g) electrons. If all the t2g orbitals are singly occupied (t2g3), an electron in, say, dxz orbital cannot be transferred into dyz orbital because it already contains an electron having the same spin quantum number as the incoming electron; if all the t2g orbitals are doubly occupied (t2g6), the transfer is not possible. Thus, only configurations other than t2g3 and t2g6 make orbital contributions to magnetic moments. For high-spin octahedral complexes, orbital contribution is expected for: t2g1, t2g2, t2g4eg2 and t2g5eg2. For tetrahedral complexes, orbital contribution is expected for: e2t21, e2t22, e4t24 and e4t25.