Introduction to Molecular Orbital Theory

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Presentation transcript:

Introduction to Molecular Orbital Theory With Applications to Modern Materials

Valence Bond Theory First quantum mechanical model proposed The main idea behind V-B theory is the hybridization of atomic orbitals Actually explains the shapes from VSEPR theory more accurately Ex: CH4 Electron configuration of C:___________________ Promotion 2s 2p 2s 2px 2py 2pz

Linear Combination of Atomic Orbitals Consider 4 atomic orbitals, which are waves centered on a nucleus, as being ripples spreading from a single point on a lake The result are areas of constructive and destructive interference: Standing waves on a drum surface Analysis is performed via Linear Combination of Atomic Orbitals (LCAO) In the case of C: h1 = s + px + py + pz h2 = s - px - py + pz h3 = s - px + py – pz h4 = s + px - py - pz

Hybrid Orbitals and Orbital Overlap The number of atomic orbitals used in hybridization is equal to the number of hybrid orbitals produced: ______ _______ ________ ________ produces 4 x _________ Two types of overlap are possible with the newly created hybrid orbitals  (head to head) bonding:  (side to side) bonding:

Molecular Orbital Theory MO Theory ultimately depends on solutions to the Schrodinger equation: In order to make it at all useful there are several approximations which are made for ease of calculation

MO Theory Approximations Orbital approximation The wave function, , of the N electrons in a molecule can be written as a product of N one-electron wave functions:  = (1) + (2) + (3)………. (N) The one electron wave functions are the molecular orbitals We also assume that the wave function of each electron closely resembles the shape of the atomic orbital that it originated from Molecular orbitals are then approximated by a LCAO N AO’s  N MO’s

Hydrogen Example Consider the hydrogen molecule as a simple example: H—H  = cAøA + cBøB where ø = atomic orbitals of H; c = coefficient The coefficient, c, can be (+) or (-) and the greater its value, the greater the contribution it has to the new molecular orbital For H2 the coefficients are equal In these terms 100% covalent simply means equal contribution from the individual atomic orbitals that are involved in bonding The sign of c indicates whether the electron waves are constructively or destructively interfering For H2: + = cAøA + cBøB - = cAøA - cBøB e-A e-B Bonding Orbital Antibonding Orbital

Bonding and Antibonding Orbitals + = Bonding - = Antibonding For bonding orbitals there is greater orbital overlap due to constructive interference Greater overlap means electrons can move between and interact with both nuclei Bonding Antibonding * Always higher in energy ** If electrons occupy this orbital they are forbidden from crossing the nodal plane

Molecular Orbital Energy Level Diagrams H2: **Absorption @ 109 nm - Energy Ø1s (A) Ø1s (B) +

Calculating Bond Order from MO Diagram MO diagrams allow us to predict/confirm bond orders according to the following relationship: Bond Order = # of Bonding e- - # of Antibonding For H2: (2 – 0)/2 = 1 Confirming a bond order of 1 for molecular hydrogen 2

Diatomic Helium (He2) - Energy Ø1s (A) Ø1s (B) +

MO Diagrams for B—N With the introduction of p atomic orbitals, a new type of orbital overlap is possible

MO Diagram for O-Ne Ordering of 2p and 2p is reversed for these elements