CHEM 2060 Lecture 23: VB Theory HF L23-1 Valence bond picture for HF… A nice example H atom ground state electronic configuration: 1s1 F atom ground state electronic configuration: 1s2 2s2 2px2 2py2 2pz1 The simplest VB wavefunction for HF is: ψ = 1sF2 2sF2 2pxF2 2pyF2 [1sH(1) 2pzF(2) + 1sH(2) 2pzF(1)] We can rewrite a simplified version of this wavefunction by ignoring the nonbonding electrons of the F atom: ψ = 1sH(1) 2pzF(2) + 1sH(2) 2pzF(1) This first guess does not adequately describe the bond energy of HF. We can improve the stability of the wavefunction by allowing the 2s orbital of the F atom to participate in bonding. CHEM 2060 Lecture 23: VB Theory HF L23-2 Improvements made by including 2s on F atom: We do this by hybridizing the fluorine 2s and 2pz atomic orbitals to get a set of two sp hybrid atomic orbitals, one of which is oriented towards the H nucleus. i.e. 2pzF is replaced by φ F = N(2pzF + γ2sF) (new sp hao) (recall: should be sp3) • Ionic terms can also be introduced into the wavefunction. • Good Idea! …based upon electronegativity considerations. H+ F- will contribute more than H- F+ New wavefunction is now: ψ = 1sH(1) φF(2) + 1sH(2) φF(1) + λ(φF(1) φF(2)) Both electrons on F “Ionic Term” Ionic term contributes ~50% (compare only 6% in H2). CHEM 2060 Lecture 23: VB Theory HF L23-3 Advantages in Hybridization Electron Density concentrated between nucleii Decrease in e-e repulsion Since part of 2s was mixed with the 2p φF = N(2pzF + γ2sF) the LONE PAIR is not simply 2s2 ! φlp = N(γ2s - 2p) This decreases e-e repulsion for one of the F lone pairs and makes it more directional. Question: Which orbitals describe the other two lone pairs? CHEM 2060 Lecture 23: VB Theory HF L23-4 Hybrids for HF - formation of bonding hybrid (sp) - overlap with H 1s - formation of lone pair hybrid (sp) - electron density in of lone pair points away from bond ⇐ HF BOND ⇐ “LONE PAIR” CHEM 2060 Lecture 23: VB Theory HF L23-5 A Note on Normalization: φF = N(2pzF + γ2sF) 2 2 φ ∂ τ = N ∫ F 2 2 2 2 2 2 p ∂ τ + N γ 2s ∂ τ + 2N γ ∫ (2 pzF 2s)∂τ = 1 ( ) ( ) ∫zF ∫F =1 =1 2 2 2 1 = N +N γ ⇒ N = =0 1 1+ γ 2 Normalization means that when an orbital is "scanned” over all space (i.e., take the integral over all space…area under the curve) the probability of finding the electron is 1 (i.e., 100%). € [Def] For a normalized wavefunction Nψ, the probability of finding the electron in all space (i.e., anywhere in the universe) is exactly 1. N is the normalization constant. CHEM 2060 Lecture 23: VB Theory HF L23-6 Water: VB Model (hybrid orbitals) Goal: To describe the bonding in H2O and account for the structure, (i.e., appropriate bond angle and 2 lone pairs). O H H Ground state electronic configuration of atomic O is: 1s2 2s2 2px2 2py1 2pz1 What would the water molecule look like if we simply used the 2py and 2pz orbitals of oxygen as our bonding orbitals? ⇒ We would end up with 2 bonds BUT an H-Ô-H bond angle of 90° …obviously not a good model for the bonding! VB approach: Since the 2s orbital is spherical, mixing some 2s character in can adjust the bond angle! CHEM 2060 Lecture 23: VB Theory HF L23-7 Question: What is the hybridization of the O atom in water? We learn in 1st year that the hybridization of the oxygen atom is sp3. Bonding hybrids Lone pair hybrids 4 orbital lobes in (“tails”) 4 orbital lobes out (“bodies”) MIX 4 (s, px, py, pz) ⇒ GET 4 (4 x sp3) CHEM 2060 Lecture 23: VB Theory HF L23-8 How do we get a better bond angle? • Water is almost 4 x sp3 but not perfectly! • The 4 lobes are not quite a perfect tetrahedron. • The H-O-H bond angle is SMALLER than 109.5° (It is closer to 104.5°.) We can rationalize this by thinking about the s and p characters of the hybrids... In a perfectly sp3 hybridized set of hao’s, each sp3 orbital should have: 25% s character and 75% p character. For our water molecule, our hao’s can’t have exactly ¼ s and ¾ p… …in other words there is uneven distribution of s and p character between the 4 hybrid orbitals. First we will write down the wavefunction and see what this means and then we will rationalize it. CHEM 2060 Lecture 23: VB Theory HF L23-9 In this course we will write sp hybrids in the general form: φ = N ( p + γs) N is the normalization coefficient γ tells us how much s is added to the p. It must € be related to the s character of the hybrid. In order to get at this we need to normalize the wavefunction. All this means is that the new orbital contains 1 electron. So the integral of the function squared over all space =1 ∫ φ 2 dτ = 1 2 2 ∫ N ( p + γ s ) dτ = 1 = N 2 ∫ p 2 dτ + N 2γ 2 ∫ s 2 dτ + N 2 2γ ∫ spdτ =1 =1 =0 (orthogonal!) CHEM 2060 Lecture 23: VB Theory HF L23-10 So… Therefore… 2 2 2 N + N γ =1 € hybrid wavefunction is then: N= ( φ = 1+ γ € 1 2 − 2 ) 1 1+ γ 2 ( p + γs) The s and p characters are now easy to get… square of that part of φ € # 2 & 1 1 ( % = Amount p character: % 2 2( 1+ γ 1+ γ $ ' 2 # 1 &2 γ (( γ 2 = %% € Amount s character: 2 2 1+ γ 1+ γ $ ' …as γ →0, p-character →100% …as γ →1, s-character →50% CHEM 2060 Lecture 23: VB Theory HF L23-11 How do we choose the correct value of γ ? The mixing coefficient γ is clearly related to the bond angle θ. Using some simple trigonometric relationships, it can be proven that: 2 cos θ = - γ (If you really want to know how this was derived, see DeKock & Grey “Chemical Structure and Bonding”, pp.146-147) For example a 50:50 mix (sp hybrid orbital) The bond angle is 180°. φ sp = 1 s+ ( 2 p) cos180° = -1 O=C=O carbon atom in CO2 so γ = 1 REMEMBER: Mix 2 (s & p) → Get 2 (2 x sp) CHEM 2060 Lecture 23: VB Theory HF L23-12 Applying the bond angle equation to H2O Water: The bond angle is 104.5°. cos104.5° = -0.25 so γ = 0.25 = 0.5 1 1 Amount p character: i.e. 80% p-character = = 0.80 2 2 1+ γ 1+ 0.5 € This should leave us with 20% s-character…let’s double check that: γ2 0.5 2 = = 0.20 Amount s character: 2 2 1+ γ 1+ 0.5 € i.e. 20% s-character The two hybridized atomic orbitals of oxygen involved in bonding are each 80% p and 20% s € What are the remaining atomic orbitals of oxygen that contain the 2 lone pairs? CHEM 2060 Lecture 23: VB Theory HF L23-13 Water: p-character of lone pair atomic orbitals of O atom Without a bond angle to start from, we cannot derive γ. But we do know that the O atom has 3 p orbitals. So the TOTAL p-character count must be 3. Let x be the p-character in the lone pairs: 0.8 + 0.8 + x + x = 3 (Note: we are assuming the lone pairs are identical.) Solving for this, x = 0.7 (i.e. 70% p and 30% s) (Double check for yourself that we’ve used only one s orbital in total.) Angle between lone pairs p-character = 1/(1 + γ2) = 0.7 so: -γ2 = 1/0.7 – 1 = -0.42 therefore θ = 115o CHEM 2060 Lecture 23: VB Theory HF L23-14 Water: conclusions The angle between the lone pairs is greater (115°) than the bond angle (104.5°). The sp3 hybrid atomic orbitals of the lone pairs have > 25% s-character. - less directional - held more tightly to the O atom The sp3 hybrid atomic orbitals of the bonding pairs have < 25% s-character. - more directional (more p-character) - electron density found in the bonding region between O and H HOMEWORK: Can you now write down the full wavefunctions for the O atom hybrid orbitals of water? (bonding & lone pair)