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Physical Methods in Organometallic Chemistry

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Textbook: The Organometallic Chemistry of the Transition Metals, Ch.10, 4th Ed. ... Two phosphorus atoms are cis a simple doublet for the Me group. ... CH, doublet ... – PowerPoint PPT presentation

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Title: Physical Methods in Organometallic Chemistry


1
Physical Methods in Organometallic Chemistry
  • ??? Hon Man Lee
  • 94.2.?????? (?)
  • Organometallic Chemistry (II)

Textbook The Organometallic Chemistry of the
Transition Metals, Ch.10, 4th Ed. by Robert H.
Crabtree
2
Synthesize and Characterization
  • For a new organometallic complex,
  • Needs isolation first
  • Air sensitive, especially d-block and f-block
    elements
  • Schlenk glassware, glove-box
  • Assign its stereochemistry
  • Knows something about its properties
  • Spectroscopic and crystallographic analysis
  • Mainly NMR

3
1H NMR spectroscopy
  • Metal hydrides in empty region of spectrum (d 0
    to -40 ), shielded by d electrons.
  • d -10.44 (d, 2J(P,H) 15.0 Hz, 1H, Ha)
  • Trans coupling (90-160 Hz)/cis coupling (10-30
    Hz)
  • Stereochemistry assignment

integration
splitting
J constant
assignment
4
Figure 10.1
5
Virtual coupling
  • Phosphorus, I 1/2
  • PMe3, PMe2Ph
  • Two phosphorus atoms are cis ? a simple doublet
    for the Me group.
  • When they are trans to each other ? a distorted
    triplet or virtual triplet.
  • Large P-P coupling ? methyl group couples to its
    own P and the trans P equally.

6
Figure 10.2
7
Diastereotopy
  • Diastereotopic groups
  • No symmetry element of the molecule relates the
    groups.
  • Resonate at different chemical shifts.
  • Regardless of MP or CC bonds are freely
    rotating

8
Chemical shifts
  • Chemical shift in organometallic compounds are
    much variable.
  • For example
  • Free alkene (d 5 -7)
  • Co-ordinated (d 2 5)
  • Ir(III) hydride complex
  • Trans to high field ligand e.g. H ? -10 ppm
  • Trans to low field ligand e.g. H2O ? -40 ppm
  • Neighboring group effect
  • InIrHL2 vs CpIrHL2
  • -0.27 ppm shift of the aromatic proton

9
Paramagnetic complexes
  • Large shifts in the NMR resonaces
  • (h6-C6H6)2V at 290 ppm
  • Broadened signals ? may be effectively
    unobserved.

10
13C NMR spectroscopy
  • 13C (I 1/2) only 1 of natural carbon
  • Needs longer acquistion time
  • 13C1H, proton-decoupled spectrum
  • Off-resonace-decoupled spectrum
  • Only 1-bond C,H couplings
  • Reveals number of H attached to the C
  • CH3, quartet
  • CH2, triplet
  • CH, doublet
  • Coupling is transmitted through s bond, the
    higher the s character of a bond, the higher is
    the coupling. For example in CH
  • sp3 125 Hz,
  • sp2 160 Hz
  • sp 250 Hz

10.5 and 10.6 inseparable
2 q, 2 t, 2 d, 2 s for each isomer
11
13C NMR Spectrum
  • Characteristic resonance positions
  • Alkyls 40 to 20 ppm
  • Alkenes, Cp, arenes 40 to 120 ppm
  • Terminal C?O 150 to 220 ppm
  • Bridging C?O 230 to 290 ppm
  • Carbenes 200 to 400 ppm

12
13C NMR Spectrum
  • Relaxation problem e.g. C?O, relaxation reagent,
    Cr(acac)3
  • Signals farther apart than in 1H NMR ?
    complicated molecules easier to assign.
  • trans coupling 2J(C,P) 100 Hz gtgt cis coupling
    2J(C,P) 10 Hz
  • Wide range of relaxation time, saturation problem
    ? Integration not reliable
  • Coordination shift for polyene and polyenyl
    ligands (25 ppm to high field)
  • Coupling to metal is also seen if th metal has I
    1/2

13
31P NMR spectroscopy
  • Very useful for phosphine complexes
  • Usually 31P1H spectrum
  • Phosphine vs. phosphites
  • Coordination shift free and bound phosphines
  • Chelation shift
  • For example if the P atom is part of 4-, 5-, or
    6-membered ring, it will shift by -50, 35, -15
    ppm relative to a coordinated but noncoordinating
    ligand.
  • Orgin of shift not well-understodd.

14
Mechanistic Study of Wilkinson Hydrogenation
at 30 C
  • 31P1H NMR
  • Rh (I ½, 100 abundance)
  • Fluxional process
  • Non-rigid vs static structures

at -25 C
15
Dynamic NMR
  • Many organometallic species are nonrigid
    molecules giving fewer signals than their static
    structures.
  • Rate of exchange (fluxional) process gtgt NMR
    timescale (10-1 to 10-6 s)
  • For Fe(CO)5
  • 13C NMR one signal at 25 C.
  • IR spectrum two types of CO
  • IR time scale 10-12 s

Berry pseudorotation Axial and equatorial COs
are exchanged.
16
Rate of Fluxionality
  • When rate of exchange is comparable to NMR time
    scale ? slow it down by cooling to get the static
    spectrum (low-temperature limit)
  • Accelerate the exchange process by heating ?
    fully averaged spectrum (high- temperature limit)

decoalescence
17
Rate of Fluxionality
  • Rate at which A and B leave the site during the
    exchange process
  • The exchange rate during coalescence
  • ?v separation of the two resonance in static
    structure
  • A single peak
  • The rate is field dependent.

18
Mechanism of Fluxionality
  • Fluxionality relates to coordination number.
  • very common in 5-coordinate TBP complexes
  • also in 7-, 8,-, 9- coordinate complexes
  • 4-, 6- coordinate complexes are usually rigid.
  • CN unrelated fluxionality

19
Mechanistic study
  • Different degree of initial broadening ?
    1,2-shift vs. 1,3-shift
  • 1,2-shift
  • one of Hc still in Hc site
  • all Hb sites are different.
  • Exchange rate of Hb 2 x that of Hc
  • Hc less initial broadening
  • 1,3-shift Hb less initial broadening

20
Mechanism of Fluxionality
  • Bridge-terminal exchange in CO complexes
  • one signal for Cp in 1H NMR at R.T.
  • Separate signals for cis and trans isomer at -50
    C
  • Adams-Cotton mechanism
  • via open form
  • The trans isomer gives faster exchange between
    terminal and bridging COs. (greater initial
    broadening of signal in 13C NMR)


21
Spin Saturation Transfer
  • A low temperature limiting spectrum at all
    accessible temperatures, exchange is slow on NMR
    timescales.
  • Too slow to affect the NMR line shapes.
  • Spin saturation transfer
  • To know which proton is exchanging to which.
  • Irradiate MeA (saturating the signal), MeB signal
    diminished.
  • Exchange rate k

Need to know T1(B)
22
Spin-lattice relaxation time, T1
  • T1 spin lattice relaxation
  • Inversion recovery method
  • 180 pulse
  • Sample spins after 0.1s, 0.2 s by applying 90
    pulse to bring the net magnetization back to xy
    plane
  • A first order process
  • Rate constant 1/T1

23
T1 and Dihydrogen Metal Complexes
  • Application of T1 measurement
  • Distinguish between M(H2) and MH2 complexes
  • When 2 protons are close to each other, they can
    relax via dipole-dipole mechanism.
  • Relate to tumbling of molecules in solution ? no
    dipole-dipole splitting seen.
  • Rate is very sensitive to r

MH2 gt 1.6 Å ? 0.5 s M(H2) 0.85 Å ? 10 ms
24
Nuclear Overhauser Effect
  • A valuable technique for conformational study in
    solution
  • Ha and Hb relax via dipole-dipole mechanism
  • The two nuclei need to be lt3 Å apart.
  • 50 increase in intensity
  • Usually 5 10

NOE effect observed
No NOE effect observed
Origin Irradiate Ha ? equalize Has a and b
states Dipole-dipole relaxation transfer some of
the increased upper b state of Ha to the lower a
state of Hb ? increase in intensity NOE factor
25
Isotopic Perturbation of Resonance
  • IPR technique
  • For fluxional system in the fast exchange limit
    at all accessible temperatures
  • 10.15 and 10.16 exchange rapidly even at -100 ?C

26
IR Spectroscopy
  • Vibrational modes of molecule
  • u depends on strength of the bond
  • Carbonyl complexes at 1700-2100 cm-1
  • Intensity is large ? dipole moment change, dm/dr,
    is large.
  • COs vibrate in concert ? depends on the symmetry
    of the M(CO)n fragment.

characteristic for a trans CO complex
facial (fac) or meridional (mer)
27
IR Spectroscopy
  • Shift in frequency
  • Other ligands
  • M-H ? bond low polarity ? weak intensity, 2000
    cm-1
  • Complexes of CO2, SO2, NO ? intense bands
  • Oxo ligand ? 500-1000 cm-1
  • Agostic C-H ? 2800 cm-1
  • M-X ? 200-400 cm-1 (not practical)
  • Isotopic subsitution
  • A band at 2000 cm-1 may due to M-H or M-CO
  • M-D shift to lower frequency according to
  • At about 2000/v2 1414 cm-1

28
Raman Spectroscopy
  • Useful for detecting nonpolar bonds (absorbs
    weakly in IR)
  • Rarely applied to organometallic species

29
Crystallography
  • Extremely important
  • X-ray and neutron diffraction
  • Unit cell
  • Braggs law
  • Diffractions give a pattern of spots.
  • The intensity of spots carry information about
    the locations of the atoms in the unit cell
  • The relative positions of the spots carry
    information about the arrangement of the unit
    cells in space (space group)
  • Limitations
  • X-rays diffracted by electron-clouds around each
    atom
  • Hydrogen atoms difficult to locate (MH2, M(H2),
    bond angle at metal-ethylene complex)
  • Neutron diffraction ? large crystal needed. ? few
    labs in the world has this facilities.
  • Single crystal ? bulk material
  • Solution structure ? solid state structure
  • May be the least soluble tautomer
  • IR technique (solid state solution )
  • Solid-state NMR

30
Other Methods
  • Microanalysis, Elemental analysis
  • C, H, N. acceptable if 0.03
  • Solvent may be present
  • Conductivity measurements
  • UV-Vis
  • Electron diffraction
  • Much less information
  • In vacuum, solvation and crystal packing are
    absent

31
Paramagnetic Organometallic Complexes
  • Magnetic moment ? Evans method
  • Measure the solvent resonance and a solution of
    paramagnetic complex
  • NMR shifted broadening
  • EPR
  • LNiII oxidation
  • ? Ni(II)(L?) g 2 or Ni(III)L g ? 2
  • Electrochemical methods
  • Cyclic voltammetry

32
Volatile Species
  • Mass spectrometry
  • Hard and soft ionization
  • Photoelectron spectroscopy (PES)
  • Molecular energy level
  • X-ray can ionize core electrons

33
  • Photoelectron Spectroscopy Where Orbital
    Energies Come From
  • Radiation can dislodge an electron from a
    molecule
  • UV radiation removes outer e-
  • X-Ray radiation can remove inner e-
  • The KE of the expelled e- tells us the energy of
    the orbital it came from
  • Ionization energy is equivalent to the orbital
    energy
  • IE hn KE
  • N2 spectrum
  • Lower E at top (outer orbital)
  • Fine structure is due to vibrational
  • Energy levels within electronic levels
  • i. Many levels bonding orbital
  • ii. Few levels less bonding

34
  • O2 Spectrum

35
Computational Methods
  • Molecular orbital (MO theory) based on quantum
    mechanical methods
  • Hückel method by Roald Hoffmann (Cornell)
  • Fenske-Hall methods
  • Ab initio (fewer assumptions, based on physics of
    the system)
  • Density Functional Theory (DFT) (the present
    standard method)
  • Molecular mechanics (MM) (useful for organic
    chemistry)
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