Outline Molecular Orbitals in Inorganic Chemistry L2 build a MO diagram to show you the process quick revision stage 1: basic MO diagram for H2O stage 2: include MO mixing Dr. P. Hunt [email protected] Rm 167 (Chemistry) http://www.ch.ic.ac.uk/hunt/ Socrative: WHZ9KBWC3 real MOs (how good are qualitative diagrams) Walsh or correlation diagrams L3 come back and look closely at the details @quantumchemist #MO_lectures 1 2 Revision Setting Up MO are combinations of AOs determine the shape of the molecule Fig. 1 details: Lecture 1 find the point group of the molecule: C2v Maths lectures with Kim Jelfs ↓ ψ 1s atomic orbitals define the axial system find all of the symmetry elements ↓ R1sY1s ✦ radial and angular components ✦ radial: as quantum shell increases x ↓ ‣ inner nodes ‣ radius max density increases ✦ cartoons represent outer portion ✦ shaded part represents negative part of function ✦ angular nature represented by the lobes θ θ positive the “Orbitron” C2v Y1s z y=ax2+bx+c x negative sign change with θ ✦ link from my website Fig. 2 3 C2(z) σv(yz) y ⎡⎣ 2Z 3 2 e− ρ 2 ⎤⎦ ⎡⎣(1 4π )1 2 ⎤⎦ !#"#$ !#"#$ R1s z E A1 1 A2 B1 B2 σv(xz) σv'(yz) C2 h=4 z 1 1 1 1 1 -1 -1 1 -1 1 -1 x 1 -1 -1 1 y O H1 H2 σv(xz) Fig. 4 Fig. 3 4 Fragments Fragments map onto each other under the symmetry operations ✦ H atoms map onto each other ✦ O atom maps onto its self ✦ H2 and O atom are the fragments z x O H place holder y H use place holders! place holder O H H H2 fragment map onto each other under the symmetry operations H O ✦ H atoms map onto each other ✦ O atom maps onto its self ✦ H2 and O atom are the fragments H whole molecule z place holder x O H O fragment place holder y O H H use place holders! H H2 fragment H O H whole molecule O fragment Fig. 5 Fig. 5 5-1 5-2 Fragments map onto each other under the symmetry operations ✦ H atoms map onto each other ✦ O atom maps onto its self ✦ H2 and O atom are the fragments z O H y place holder x H use place holders! place holder O H H H2 fragment H O H whole molecule O fragment reproduce the whole of the molecular structure in the MO fragment orbitals ✦ H2 orbitals ✦ O atom orbitals Set Up MO Diagram vertical axis: Energy tant! Impor H 1s AO position AOs ✦ O more electronegative than H so valence orbitals lie below H 1s reference orbital ✦ H atoms are further apart than in H2 so stablilsation and destabilsation are less ie splitting energy is less py H x y s H O H H O H H2O O (s and p) orbitals Fig. 6 6 pz z O H H2 orbitals px ??? Fig. 6 7 Fragment Orbital Symmetry Short Cuts! How does each orbital transform under the symmetry operations of the group? σv Lecture 1 C2v No change under σv 1 1 χ =1 t! u Short-C rtant! Impo a1 1 C2v ✦ sometimes also written as just x, y, z ✦ gives you the axis symmetry label C2 σv(xz) σv'(yz) E 1 Γ look in the last columns of the character table ut! Short-C ✦ find Tx, Ty, Tz σv(yz) ✦ orbital is unchanged => character = 1 ✦ a sign change => character = -1 ✦ check against the character table E C2 σv(xz) σv'(yz) h=4 A1 1 1 1 1 A2 1 1 -1 -1 B1 1 -1 1 -1 Tx B2 1 -1 -1 1 Ty Tz Fig. 7 Fig. 7 totally bonding orbitals are always totally symmetric ✦ which is the first symmetry label listed for all point groups ✦ for C2v this is the a1 irreducible representation 8 9 Fragment Orbitals Fragment Orbitals look for similarities in the phase of orbitals and the cartesian axes C2 v E ut! Short-C look for similarities in the phase of orbitals and the cartesian axes C2 σv(xz) σv'(yz) E C2 σv(xz) σv'(yz) Γ 1 -1 -1 1 py b2 Γ 1 -1 1 -1 px b1 Γ 1 1 1 1 pz C2v x Γ O a1 1 Γ 1 Γ 1 -1 -1 1 -1 1 1 1 Ty b2 -1 Tx b1 1 Tz a1 O H H O H H O a1 Fig. 7 H2 Fig. 8 σv(xz) σv'(yz) E C2 Γ 1 1 1 1 a1 Γ 1 -1 1 -1 b1 C2v Fig. 7 10 11 ut! Short-C Form the MOs work out MOs first then the splitting tant! Impor Only fragment orbitals (FOs) of the same symmetry can combine bels to try la ymme Add s O diagram M + ✦ for water: a1 and b1 + FO can only combine ONCE a1 ✦ more than one FO of same symmetry? ✦ then combine the lowest energy two ✦ leave the last one non-bonding (for now!) Form MOs by ✦ “adding” FOs together “as is” ✦ “adding” FOs with ONE FO phase inverted b1 Fig 10 Fig. 9 12 13 Stage One MO Diagram Stage One MO Diagram Evaluate splitting ✦ FOs far apart interact only weakly ✦ in-phase interactions are bonding ✦ destabilisation is always larger ✦ number within symmetry label ✦ count the core orbitals t! tan 2b1 4a1 b1 a1 Annotate your diagrams! MO labeling or Imp antibonding MO is always destabilised more than the bonding MO is stabilised b2 1b 2 a1 FO left nonbonding in the first stage diagram a1 3a1 FOs are closer in energy and so the interaction between the orbitals is larger for the b1 MO 1b 1 Annotate your diagrams! b1 Figure 11 a1 2a1 add the electrons! Figure 12 ✦ fill sequentially 1a 1 is the O 1sAO which is not shown because this is a valence MO diagram z O H y x H O H H 2 valence e 14 15 H O H 6 valence e Fig 11/12 Stage 2: MO Mixing a1 MO Mixing mixing orbitals ONLY MOs of the same symmetry can mix ✦ “add” MOs together “as is” 0 ✦ “add” MOs with ONE MO phase inverted ✦ inspect to determine which is the bonding mixed MO to occur mixing MUST stabilise the total energy mixing tends to be large when: ✦ MOs are close in energy ✦ one MO is non-bonding ✦ one MO is unoccupied ✦ orbitals are in HOMO-LUMO region tant! occupied Impor antibonding due to increased out-ofphase interaction unoccupied + ψ (3a1 ) ψ (4a1 ) ψ 1 = ψ (3a1 ) + ψ (4a1 ) antibonding MO Fig 13 16 17 In-Class Activity 4a1 Mixing mixing orbitals ✦ “add” MOs together “as is” ✦ “add” MOs with ONE MO phase inverted 0 ✦ inspect to determine which is the bonding mixed MO 2b1 b1 strong mixing: a1 ✦ 4a1 MO unoccupied ✦ 3a1 MO non-bonding ✦ in HOMO/LUMO region ✦ close in energy ✦ occupied MO is stabilised form (4a 1) )+ψ 3a 1 -ψ( b2 1b 2 a1 b1 significant mixing drives 3a1 MO down in energy and chanes the shape of the MO 3a1 1b 1 a1 extra lines drawn to show the main mixing interaction 2a1 Fig 14 z O H y x H O H H 2 valence e 18 19 H O H H2O 6 valence e Fig 15 4a1 Final MO Diagram of H2O Annotate your diagrams! antibonding MO is always destabilised more than the bonding MO is stabilised 4a1 Final MO Diagram of H2O 2b1 the 4a1 lies above the 2b1 MO because there is strong directional antibonding overlap in the 4a1 MO and weaker less directional overlap in the 2b1 MO b1 a1 b2 1b 2 b2 FO left nonbonding as there is no other FO of this symmetry for it to interact with 3a1 FOs are closer in energy and so the interaction between the orbitals is larger for the 1b 1 than the 2a1 MO O H y H 2 valence e H do not repeat information tant! Impor O O y a1 b1 significant mixing drives 3a1 MO down in energy and chanes the shape of the MO a1 2a1 1a 1 is the O 1sAO which is not shown because this is a valence MO diagram z H 6 valence e 3a1 FOs are closer in energy and so the interaction between the orbitals is larger for the 1b 1 than the 2a1 MO H H2O b2 1b 2 1b 1 2a1 O H b1 a1 a1 x H the 4a1 lies above the 2b1 MO because there is strong directional antibonding overlap in the 4a1 MO and weaker less directional overlap in the 2b1 MO b2 FO left nonbonding as there is no other FO of this symmetry for it to interact with Annotate your diagrams! 1a 1 is the O 1sAO which is not shown because this is a valence MO diagram z 2b1 a1 b1 significant mixing drives 3a1 MO down in energy and chanes the shape of the MO 1b 1 antibonding MO is always destabilised more than the bonding MO is stabilised x H O H H 2 valence e Fig 15 H O H H2O 6 valence e 20 21 “Real” MOs Experimental Evidence Fig 15 Photoelectron spectrum ✦ energy required to eject an electron from its orbital computed molecular orbitals 2a1 “traditional” theory: 1b1 ✦ expect 2 equivalent bonds and 2 equivalent lone pairs for water = 2 lines in photo-electron spectrum we have “solved” the Schrödinger equation!!! 3a1 BUT O b2 H H Fig 17 Fig 16 22 ✦ have 3 lines in photo-electron spectrum which relate to delocalised 1b1, 3a1 and 1b2 MOs Fig 5.13 from “Structure and Bonding" by J. Barrett Fig 18 23 Delocalisation Analysis 4a1 MO diagrams are transferable MOs are delocalised ✦ not 2 center 2 electron ✦ most of MOs extend over ALL atoms in molecule ✦ there are no “bonds” 2b1 ✦ one diagram is good for many molecules or fragments! ✦ molecules BeH2 (homework), H2S ✦ fragments CH2 (lecture 4), NH2 ✦ we can even treat metal fragments: MH2 Bonds represent a build up of the TOTAL electron density b1 a1 1b1 ✦ A=main group element, M=metal ✦ slight modifications: ✦ different numbers of electrons ✦ slightly different position of the fragment orbitals a1 2a1 z O H y x H O H H 2 valence e 24 b1 3a1 general formula AH2 We keep ideas of hybridisation and 2c-2e bonds because they are USEFULL b2 1b2 H O H H2O 6 valence e 25 Correlation Diagram Walsh Diagram Walsh diagram: change one geometric parameter and examine changes in MOs and energies typically start from the highest symmetry ✦ I’ve constructed the MO diagram for linear H2O for you (Self-study for you to reproduce) ✦ normally a bond distance or angle ✦ link the MOs for two extreme geometries example: Why is H2O bent? start with high symmetry Fig 20 ≈105º C2v 180º O H end with lower symmetry O H H H H O H D∞h Prof. A.D Walsh University of Dundee from: http:// www.dundee.ac.uk/museum/ scientists.htm H-O-H angle Fig 21 26 27 a1 Walsh Diagram Energy of MOs then examine how MOs change under geometric distortion examine how MOs change under geometric distortion 2σ g+ (2a1) stabilised ✦ ↑ H...H through space bonding overlap ✦ ↓ O-H bonding overlap ✦ net result small stabilisation Fig 21 Fig 21 28 29 Energy of MOs Energy of MOs then examine how MOs change under geometric distortion then examine how MOs change under geometric distortion 1π 1σ u+ (1b1) destabilised u (1b2) no change ✦ non-bonding orbital ✦ ↑ H...H through space antibonding ✦ ↓ O-H bonding overlap ✦ net result large destabilisation Fig 21 30 Fig 21 31 Energy of MOs Energy of MOs then examine how MOs change under geometric distortion then examine how MOs change under geometric distortion 1π u / 3σ g+ or 3a1/4a1 special ✦ as planar molecule 1πu and 3σg+ cannot mix (not same symmetry) ✦ when molecule distorts they become the same symmetry: mixing occurs ✦ 1πu goes to 3a1 ✦ 3σg+ goes to 4a1 ✦ on mixing the 1πu ( 3a1) is stabilised 2σ u+(2b1) stabilised socrative quiz! 3 KBWC 9 Z H W nt! Importa Fig 21 Fig Fig 21 18 32 33 Change of Axes When the symmetry point group changes the axial definition changes! z z y Walsh Diagram x ✦ z-axis reorientated ✦ orbital remains the same ✦ only labels change ✦ then follow with mixing x x O H H O H y z y 2σ g+ 4a1 H H y H H 3a1 z ✦ AOs move with the atoms ✦ form or shape of AOs remains constant ✦ !! except for MOs which undergo mixing Molecular stability H ✦ examine how occupied MOs change under geometric distortion ✦ look for occupied MOs which show a large change in energy ✦ these orbitals drive the change in shape 1π u mixing + 4a1 Orbital changes x 3a1 Fig 22 Fig 21 34 35 Symmetry Breaking Symmetry Breaking But how does the drop in symmetry start? But how does the drop in symmetry start? nuclear vibrations provide infinitesimal distortion required for MO mixing nuclear vibrations provide infinitesimal distortion required for MO mixing vibronic coupling = coupling of electronic and nuclear motions vibronic coupling = coupling of electronic and nuclear motions breakdown of the Born-Oppenheimer approximation! breakdown of the Born-Oppenheimer approximation! ✦ collapse of a VERY fundamental approximation ✦ more common than you think! ✦ of which Jahn-Teller theorem is a special case ✦ collapse of a VERY fundamental approximation ✦ more common than you think! ✦ of which Jahn-Teller theorem is a special case 36-1 36-2 Symmetry Breaking MO checklist Steps to construct a MO diagram symmetry & symmetry breaking underlies many theories in physics and chemistry Noether’s Theorem Shows that a conservation law can be derived from any continuous symmetry. VERY nt! Importa • invariance with respect to translation gives the law of conservation of linear momentum • invariance with respect to time translation gives the law of conservation of energy Emmy Noether ity magnetism nductiv superco Heisen Serious b ity Uncerta erg l relativ a r e n e in g Stuff! Princip ty le ce of standard model of existen ticle ar particle physics eory Higgs p field th 37 source: http://en.wikipedia.org/wiki/ Image:Noether.jpg accessed 17/08/07 ✦ determine the molecular shape and identify the point group ✦ define the axial system and all of the symmetry operations ✦ identify the chemical fragments, put them on the bottom of the diagram ✦ determine the energy levels and symmetry labels of the fragment orbitals (use H1s as a reference) ✦ combine fragment orbitals of the same symmetry, determine the MOs and then estimate the splitting energy; draw in the MO energy levels and MOs (in pencil!) ✦ determine the number of electrons in each fragment and hence the central MO region, add them to the diagram ✦ identify if any MO mixing occurs, determine the mixed orbitals and redraw the MO diagram with shifted energy levels and the mixed MOs ✦ annotate your diagram ✦ use the MO diagram to understand the structure, bonding and chemistry of the molecule 38 Finally Key Points be able to form MO diagrams for molecules with the general formula AH2 and AH3 (tutorial) where A= main group element or a metal be able to explain and illustrate MO mixing be able to critically evaluate VSEPR theory, localised 2c-2e bonding and the delocalised MO picture of bonding be able to describe how a PES is formed and be able to relate a spectrum to the MOs, and MO diagram of a molecule be able to form correlation diagrams and explain why a particular geometry is more stable than another with reference to the stability of the MOs be able to discuss symmetry breaking and vibronic coupling http://www.huntresearchgroup.org.uk/ See my web-site ✦ notes AND slides ✦ link to panopto when it becomes available ✦ optional background support for beginners ✦ optional material to take you a little further ✦ links to interesting people and web-sites ✦ links to relevant research papers on MOs ✦ model answers!! Tweet! @quantumchemist #MO_lectures ◆ share questions ◆ let me know what is easy or hard ◆ I can adjust the problems classes & workshops (even lectures) based on your feedback! be able to describe the process of forming a MO diagram (the MO checklist) 39 40
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