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Unformatted text preview: Chem 3502/5502 Physical Chemistry II (Quantum Mechanics) 3 Credits Fall Semester 2010 Laura Gagliardi Lecture 25, November 15 and 17, 2010 (Some material in this lecture has been adapted from Cramer, C. J. Essentials of Computational Chemistry , Wiley, Chichester: 2002; pp. 96109.) Recapitulation of the Variational Principle and the Secular Equation Recall that for any system where we cannot determine exact wave functions by analytical solution of the Schrödinger equation (because the differential equation is simply too difficult to solve), we can make a guess at the wave function, which we will designate Φ , and the variational principle tells us that the expectation value of the Hamiltonian for Φ is governed by the equation Φ ∫ * H Φ d r Φ ∫ * Φ d r ≥ E (251) where E is the correct groundstate energy. Not only does this lowerlimit condition provide us with a convenient way of evaluating the quality of different guesses (lower is better), but it also permits us to use the tools of variational calculus to identify minimizing values for any parameters that appear in the definition of Φ . In the LCAO (linear combination of atomic orbitals) approach, the parameters are coefficients that describe how molecular orbitals (remember, orbital is another word for a oneelectron wave function contributing to a manyelectron wave function) are built up as linear combinations of atomic orbitals. In particular, manyelectron wave functions Φ can be written as antisymmetrized Hartree products—i.e., Slater determinants—of such one electron orbitals φ , where the oneelectron orbitals are defined as φ = a i ϕ i i = 1 N ∑ (252) where the set of N atomicorbital basis functions ϕ i is called the “basis set” and each has associated with it some coefficient a i , where we will use the variational principle to find the optimal coefficients. To be specific, for a given oneelectron orbital we evaluate 252 E = a i * ϕ i * i ∑ ∫ H a j ϕ j j ∑ d r a i * ϕ i * i ∑ ∫ a j ϕ j j ∑ d r = a i * a j ij ∑ ϕ i * ∫ H ϕ j d r a i * a j ij ∑ ϕ i * ∫ ϕ j d r = a i * a j ij ∑ ij H a i * a j ij ∑ ij S . (253) where the shorthand notation H ij and S ij is used for the resonance and overlap integrals in the numerator and denominator, respectively. If we impose the minimization condition ∂ E ∂ a k = ∀ k (254) we get N equations which must be satisfied in order for equation 254 to hold true, namely a i i = 1 N ∑ H ki – ES ki ( ) = ∀ k . (255) these equations can be solved for the variables a i if and only if H 11 – ES 11 H 12 – ES 12 H 1 N – ES 1 N H 21 – ES 21 H 22 – ES 22 H 2 N – ES 2 N H N 1 – ES N 1 H N 2 – ES N 2 H NN – ES NN = (256) where equation 256 is called the secular equation. There are N roots (i.e., N different values of...
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 Fall '08
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 Physical chemistry, pH, Quantum Chemistry, Atomic orbital, Chemical bond, secular equation

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