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Chapter 10. Chemical Bonding II. Molecular Geometry and Hybridization of Atomic Orbitals 10.1 Molecular Geometry (what, how, why) General Summary -- Structure and Bonding Concepts Octet Rule Electronic Configuration of Atoms Lewis Electron Dot Formula of Molecule VSEPR Theory 3-D Shape of Molecule Electronegativity and Bond Polarity Polarity of Molecule Intermolecular Forces and Bulk Properties Valence Bond Theory Bonding Description of Molecule Chemical Reactivity Valence Shell Electron Pair Repulsion Theory Hypothesis -- The structure of a molecule is that which minimizes the repulsions between pairs of electrons on the central atom. "Effective Number" (EN) = (number of atoms attached to central atom) + (number of lone pairs on central atom) (Using the number of atoms is simpler than the number of bonding pairs, because this accounts for double and triple bonds which essentially occupy the same space as a single bond.) EN Arrangement of Electron Pairs linear 180° 2 3 trigonal planar 120° tetrahedral 109.5° 4 e e e trigonal bipyramidal 120° & 90° a 6 Examples linear BeCl2, CO2 trigonal planar BCl3, CH3+ bent SnCl2, NO2- tetrahedral pyramidal CH4, PO43NH3, ClO3- bent H2O, SeF2 trigonal bipyramid a 5 Molecular Shape (Geometry) "see saw" T-shaped linear ClF3, XeO32XeF2, ICl2- square pyramid SF6, PCl6BrF5, SF5- square planar XeF4, IF4- octahedral octahedral 90° PF5, SeCl5+ SF4, BrF4+ Important corollaries: • In trigonal bipyramid structures, lone e- pairs adopt equatorial positions (e) • Order of repulsions: Lp - Lp > Lp - Bp > Bp - Bp (Predicts distortions from ideal geometries) Molecules with more than one central atom, e.g., CH3OH, methanol H H C H • • • O H C and H are "central" HCH and OCH ∠ 109 ° O is like water with two lone pairs and two bonding pairs: ∠HOC = 105 10.2 Dipole Moments (Polarity of Molecules) predict from molecular shape A. Bond Polarity e.g., HF molecule • F is more electronegative than H, so there is partial charge separation in the H-F bond: δ+ δ− H F • or H F the H-F bond is described as "polar covalent bond" and is said to have a "dipole moment" B. Molecule Polarity (Polar or Non-Polar?) • Polar bonds do not always mean the molecule is polar • In very symmetrical structures (e.g., CO2 or CF4), the individual bond dipoles effectively cancel each other and the molecule is non-polar. F O C O F C F F • In less symmetrical structures (e.g., SO2 and SF4), the bond dipoles do not cancel and there is a net dipole moment which makes the molecule polar. F .. O S F S O F F .. Other examples for practice: Polar: H2O Non-Polar: SnCl2 BeCl2 NH3 CH4 SeF2 PF5 PF3 XeF2 BrF5 XeF4 10.3 Valence Bond Theory A. Why is additional theory needed? • VSEPR predicts H2 and F2 are the same type of bond • • • H2 bond dissociation energy = 436.4 kJ/mole F2 bond dissociation energy = 150.6 kJ/mole Need better theory to explain these types of differences. XeO3 SO3 B. Basic Concept Covalent Bonds result from overlap of atomic orbitals consider the H2 molecule 1s . H 1s + σ bond . . . H H2 Figure 10.5 shows the change in potential energy with distance between atoms • atoms distant - no interaction • atoms approach - electron from one atom is attracted to nucleus of other • atoms get very close - nuclei repel each other F2 molecule 2p σ bond 2p . . + F . . F F2 HF molecule . 2p + H σ bond . . . F H F Two types of covalent bonds: σ (sigma) bond: "head-to-head" overlap along the bond axis (as in previous pictures) π (pi) bond: "side-to-side" overlap of p orbitals: π bond . 2p + . . . 2p • single bond -- always a σ bond • double bond -- combination of one σ bond and one π bond • triple bond -- combination of one σ bond and two π bonds 10.4 Hybridization of Atomic Orbitals Problem: • • • Describe the bonding in CH4 molecule. experimental fact -- CH4 is tetrahedral (H-C-H angle = 109.5°) VSEPR theory "explains" this with 4 e- pairs, ∴ tetrahedral however, if only s and p orbitals are used, the angles ought to be 90° since the p orbitals are mutually perpendicular! Solution: Modify the theory of atomic orbitals and use: Hybridization: combination of 2 or more atomic orbitals on the same atom to form a new set of "Hybrid Atomic Orbitals" used in bonding. CH4 (methane) Energy Level Diagram C ↑↓ 2s ↑ 2p ↑ 2p 2p ground state - valence shell orbital diagram • H electrons can only share with C p orbitals • So try promoting C ↑ 2s ↑ 2p ↑ 2p ↑ 2p bond angles can only be 90° angles required by p orbitals -- wrong, must be 109° Now have four orbitals, but still have three that are 90° apart So try mixing the four into new orbitals C ↑ ↑ ↑ ↑ hybridized state (mixing of s and p orbitals) 3 3 3 3 sp sp sp sp (gives 4 identical bonds that are 109.5° angles -- right!) So what do these new orbitals look like? see Figures 10.7 and 10.8 and 10.9 Types of Hybrid Orbitals (see Table 10.4) Atomic Orbitals Hybrid Orbitals Geometry linear (180°) trigonal planar (120°) tetrahedral (109.5°) one s + one p two sp one s + two p three sp2 one s + three p four sp3 one s + three p + one d five dsp3 trigonal bipyramid 90° & 120° one s + three p + two d six d2sp3 octahedral 90° Unhybridized p Orbitals (left over) 2 1 0 { Note: combination of n AO's yields n Hybrid Orbitals) Practice: Use valence bond theory to describe the bonding in H2O, NH3, CH4, PF3. Draw clear 3-D pictures (method shown in class) showing orbital overlap, etc. [Note: All use only simple σ bonds and lone pairs.] 10.5 Hybridization in Molecules Containing Double & Triple Bonds ethylene: sigma + pi bond H H C H C H (see Figure 10.16) acetylene sigma + two pi bonds (see Figure 10.19) PRACTICE on • H2CNH • HCN (use double bond like H2CO and H2CCH2) (use triple bond like HCCH) 10.6 Molecular Orbital Theory A. Comparison of VB and MO Theory Valence Bond Theory ("simple" but somewhat limited) • e- pair bonds between two atoms using overlap of atomic orbitals on two atoms • sometimes fails to explain facts, e.g., O2 is paramagnetic indicating unpaired electrons, but VB theory would indicate that electrons in the σ and π orbitals are paired. Molecular Orbital Theory (more general but "complex") • all e-'s in molecule fill up a set of molecular orbitals that are made up of linear combinations of atomic orbitals on two or more atoms MO's can be: • • "localized" -- combination of AO's on two atoms, as in the diatomic molecules "delocalized" -- combination of AO's on three or more atoms, as in benzene (C6H6) -- page 424 B. Bonding and Antibonding Molecular Orbitals Molecular Orbitals for simple diatomic molecules (H2 and He2) in H2 the 1s atomic orbitals on the two H atoms are combined into: • • a bonding MO -- σ1s • lower energy than the atomic orbitals from which it was formed, .i.e., greater stability • more electron density between nuclei from constructive interference (wave properties of the electron) an antibonding MO -- σ*1s • higher energy and lower stability than the atomic orbitals from which it was formed • no electron density between nuclei from destructive interference MO energy level diagram for H2 (only the bonding MO is filled): σ*1s 1s 1s σ1s H H2 H Figure 10.23 In contrast, the MO diagram for the nonexistent molecule, He2 shows that both bonding and antibonding MO's are filled: σ*1s 1s 1s σ1s He He2 He Figure 10.25 Bond Order = ½ [(# bonding e-'s) - (# antibonding e-'s)] for H2 = ½ [2 - 0] = 1 (a single bond) for He2 = ½ [2 - 2] = 0 (no net bonding interaction) C. Bonding and Antibonding Molecular Orbitals from p Atomic Orbitals Figure 10.24 - shows interaction to form • σ bonds when atomic orbitals approach end to end • π bonds when atomic orbitals approach side to side 10.7 Molecular Orbital Configurations/Rules A. Rules 1. The number of MO's equal the number of AO's used to make the MO's 2. The more stable the bonding MO, the less stable the antibonding MO 3. MO's fill from low to high energies 4. In stable molecules, the number of electrons in bonding MO's > electrons in antibonding MO's 5. Maximum of 2 electrons per MO (with opposite spins) 6. Follow Hund's rule - electrons do not pair until all MO's of the same energy are half filled 7. The number of electrons in MOs equals sum of all of the electrons in the atoms B. MO's for 2nd Row Diatomic Molecules (e.g., N2, O2, F2, etc.) MO energy level diagram -- Figures10.26 plus 10.27 σ*2p x π*2p y π*2p z 2p 2p σ2p x π2p π2pz y σ*2s 2s 2s σ2s σ*1s 1s 1s σ1s Examples -- Table 10.5 (Note the change at O2 and F2) Fill in MO diagram for C2, N2, O2, F2, and Ne2 and determine bond order for each: molecule C2 N2 O2 F2 Ne2 bond order 2 3 2 1 0 B. Electron Configurations valence electrons in blue Example: N2 (σ1s)2(σ*1s)2(σ2s)2(σ*2s)2(π2p )2(π2p )2(σ2p )2 y z x Example: O2 (σ1s)2(σ*1s)2(σ2s)2(σ*2s)2 (σ2p )2 (π2p )2(π2p )2 (π*2p )1(π*2p )1 x y z y z 10.7 Delocalized Molecular Orbitals By combining AO's from three or more atoms, it is possible to generate MO's that are "delocalized" over three or more atoms Examples: Resonance in species like HCO32-, CO3-2 and benzene (C6H6) can be "explained" with a single MO description containing delocalized π bonds. • see Figure 10.28 sigma framework in benzene H H H C C C C C C H H H • • see Figure 10.29 for pi framework see Figure 10.30 for the carbonate ion pi framework Computer model:: HIV enzyme with buckeyball occupying the active site preventing enzyme from working as it usually does. Carbonate Ion Bonding in Solids -- Band Theory An energy "band" is composed of a very large number of closely spaced energy levels that are formed by combining similar atomic orbitals of atoms throughout the substance Metals and metalloids have a • "conduction band" -- set of highly delocalized, partially filled, MO's that extend over the entire solid lattice structure • "band gap" -- energy difference between filled "valence band" and the conduction band (Figure 20.10)