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Schedule • Last Week: Electronic spectroscopy Interelectron repulsion, covalency and spin-orbit coupling • Lecture 4: Re-cap • Lecture 5: π-Acceptor Ligands and Biology CO, N2 and O2 complexes • Lecture 6: M-M bonding Multiple bonds and metal clusters Summary of Course – week 5 Complexes of π-acceptor ligands • be able to explain synergic (σ-donation, π-back donation) model for bonding in M-CO and M-N2 complexes • be able to explain reduction in CO stretching frequency in complex • be able to explain changes in CO stretching frequency with metal charge and with ligands • electron counting in CO CO, N2 and NO complexes: 18 e- rule Resources • Slides for lectures 5-6 • Winter, Chapter 6.5-6.7 and 6.10-6.11(basic) • Shriver and Atkins “Inorganic Chemistry” Chapter 21.1-5, 21.18 (4th Edition) • Housecroft and Sharpe “Inorganic Chemistry” Chapter 23.2 (2nd Edition) 1 Summary of the Last Lecture Electronic spectroscopy • Be able to explain number of bands • Be able to obtain Δoct from spectrum for d1, d3, d4, d6, d7, d8 and d9 Selection rules • Be able to predict relative intensity of spin-allowed vs spin forbidden, octahedral vs tetrahedral and ligand-field vs charge-transfer transitions Today • Bonding and vibrational spectroscopy in complexes containing π-acceptor ligands Slide 4/25 Molecular Orbitals for O2 and CO 2pσ 2pσ 2pπ 2pπ 2p 2p 2pσ 2p 2pπ 2pπ 2p 2pσ 2s O O2 2s 2s O O 2s CO C JKB Lecture 5 slides 8-9 Slide 5/25 Molecular Orbitals for O2 and CO • O2: ¾ bond order = 2 (O=O double bond) ¾ Two singly occupied 2pπg antibonding orbitals O O M • CO: CO ¾ bond order = 3 (C≡O triple bond) ¾ HOMO is dominated by C 2pz (~ C “lone pair”) O ¾ LUMOs are dominated by C 2px and 2py: C M Slide 6/25 2 Metal Carbonyl Complexes • CO: ¾ bond order = 3 (C≡O triple bond) ¾ donation from HOMO into empty metal d-orbital: increases e- density on metal self-enhancing: ¾ back donation from filled metal orbitals into LUMOs synergic decreases e- density on metal JKB Lecture 5 slide 10 Slide 7/25 Metal Carbonyl Complexes • M-CO: ¾ synergic: σ and π bonding are both weak in the absence of each other ¾ therefore requires d electrons on metal and non-contracted d-orbitals to overlap with CO orbitals carbonyls are found for low-oxidation state metals only (+2 or less) carbonyls almost always obey the 18e rule ¾ σ-donation strengthens M-C bond ¾ π-back donation strengthens M-C bond and weakens C≡O M C M O C O JKB Lecture 5 slide 10 Slide 8/25 Metal Carbonyl Complexes – Vibrations • M-CO – effect of bonding mode: ¾ σ-donation strengthens M-C bond ¾ π-back donation strengthens M-C bond and weakens C≡O ¾ C≡O stretching frequency is reduced from value in free CO ¾ more metals = more back donation: free CO: vco = 2143 cm-1 O O C C M M O C M 1850–2120 cm-1 1750–1850 cm-1 M MM 1620–1730 cm-1 Slide 9/25 3 Metal Carbonyl Complexes – Vibrations • M-CO – effect of charge: ¾ σ-donation strengthens M-C bond ¾ π-back donation strengthens M-C bond and weakens C≡O ¾ C≡O stretching frequency is reduced from value in free CO ¾ positive charge on complex contracts d-orbitals = less back bonding ¾ negative charge on complex expands d-orbitals = more back bonding free CO: vco = 2143 cm-1 Mn(CO)6+: 2090 cm-1 Ni(CO)4: 2060 cm-1 Co(CO)4−: 1890 cm-1 Cr(CO)6: 2000 cm-1 V(CO)6−: 1860 cm-1 Fe(CO)42−: 1790 cm-1 Slide 10/25 Metal Carbonyl Complexes – Vibrations • M-CO – effect of other ligands: ¾ σ-donation strengthens M-C bond ¾ π-back donation strengthens M-C bond and weakens C≡O ¾ C≡O stretching frequency is reduced from value in free CO ¾ in LnM(CO)m complexes, weak π-acceptor ligands increase M Æ CO back-donation free CO: vco = 2143 cm-1 L: good π-acceptor Mo(CO)6: 2005 cm-1 (PF3)3Mo(CO)3: 2055, 2090 cm-1 (PCl3)3Mo(CO)3: 1991, 2040 cm-1 (P(OMe)3)3Mo(CO)3: 1888, 1977 cm-1 L: poor π-acceptor (CH3CN)3Mo(CO)3: 1783, 1915 cm-1 Slide 11/25 Metal Carbonyl Complexes – Vibrations • M-CO – symmetry of the molecule: ¾ octahedral M(CO)6 dipole moment change? no yes no Slide 12/25 4 Metal Carbonyl Complexes – Vibrations • M-CO – symmetry of the molecule: ¾ octahedral M(CO)6 vCO 1 IR 2 Raman rule of mutual exclusion: for molecules with a centre of inversion, no vibrations are both IR and Raman active Slide 13/25 Metal Carbonyl Complexes – Vibrations • M-CO – symmetry of the molecule: ¾ cis-[M(CO)4Cl2] vco: 4 IR (1 very weak) 4 Raman (1 very weak) some common bands ¾ trans-[M(CO)4Cl2] vco: 1 IR 2 Raman no common bands – rule of mutual exclusion Metal Carbonyl Complexes – Vibrations • M-CO – symmetry of the molecule: ¾ fac-[M(CO)4Cl2] vco: 2 IR (which overlap) 2 Raman (which overlap) some common bands ¾ mer-[M(CO)4Cl2] vco: 3 IR (1 week) 3 Raman (1 week) some common bands 5 Molecular Orbitals for O2 2pσ 2pσ 2pπ 2pπ 2p 2p 2pσ 2p 2pπ 2p 2pπ 2pσ 2s O O2 2s 2s O O 2s CO C JKB Lecture 5 slides 8-9 Spin-Triplet O2 • O2 in the atmosphere is the result of continuous photosynthesis ¾ it is a potentially highly toxic in the presence of fuels (carbohydrates etc) ¾ however, it is metastable because of the 2 unpaired electrons (“triplet”) 2H2(g) + O2(g) Æ 2H2O(l) ΔcombH = -484 kJ mol-1 spin H-H H-H O=O inhibited H O H H O H ¾spin-selection rules prevents “spin-flip” transition in O2 being important so reaction is not initiated by sunlight ¾initiation happens via a spark or a catalyst O2 Transport Complexes • Almost all reactions between O2 and metal complexes are irreversible: 4Fe2+ + O2 + 2H2O + 8OH- Æ 4Fe(OH)3 Æ 2Fe2O3 + 6H2O • Transport system for O2 in animals must: ¾ carry O2 in its ground state form (with two unpaired electrons) ¾ capture gas phase O2 ¾ transport it via the circulatory system ¾ release it completely to intermediate storage site • Transport system for O2 in animals must: ¾ not react irreversibly with O2 ¾ be highly efficient and cope with changes in supply and demand ¾ have a lower affinity for O2 than the storage system Slide 18/25 6 O2 Transport Complexes • In humans, transport system (haemoglobin) and storage system (myoglobin) are both Fe(II) complexes: myoglobin haemoglobin affinity of myoglobin > affinity of haemoglobin affinity of haemoglobin increases as O2 pressure grows – cooperative effect muscle lungs Slide 19/25 Haemoglobin and Myoglobin - Structures • Haemoglobin consists of 4 haem groups, myoglobin consists of 1 haem group: N HN N N Fe2+ N distal histidine residue Fe2+ N N HN proximal histidine residue Slide 20/25 Haemoglobin and Myoglobin - Function • Unoxygenated protein contains high spin Fe(II) d6: N HN O O • Oxygenated protein contains low spin Fe(III) d5 and O2−: distal histidine residue Fe2+ N • Unpaired electron on Fe(III) is weakly coupled to unpaired electron on O2−: ¾ complex is diamagnetic HN proximal histidine residue Slide 21/25 7 Haemoglobin and Myoglobin - Function N N weak Hbond? HN distal histidine residue O O enforced bending HN distal histidine residue O C Fe33+ Fe2+ N N HN HN proximal histidine residue proximal histidine residue partial prevention of (irreversible) CO attachment Slide 22/25 Haemoglobin – Cooperative Effect • Unoxygenated protein contain high spin Fe(II) d6: • High spin ion has is too large to fit in haem ring and actually sits slightly below it O N • Fe2+ O N Oxygenated protein contains smaller O low spin Fe(III) d5 which fits into ring N Fe 3+ N N Fe3+ N N •The motion of the proximal group is transferred through protein structure to the next deoxygenated haem group decreasing its activation energy for O2 attachment HN proximal histidine residue Slide 23/25 Summary By now you should be able to.... • Explain that metal-carbonyl bonding is due to synergic OC Æ M σ-donation and M Æ CO π-back donation • Explain that the reduction in vco stretching frequency is related to the extent of back-bonding • Appreciate that the number of vCO in IR and Raman can be used to work out structure • Explain that haemoglobin and myoglobin bind weakly to O2 allowing transport and storage of highly reactive molecule Next lecture • N2 complexes and Metal-Metal bonding Slide 24/25 8 Practice Slide 25/25 9