3502_25_nove1517 - Chem 3502/5502 Physical Chemistry II...

Info iconThis preview shows pages 1–3. Sign up to view the full content.

View Full Document Right Arrow Icon

Info iconThis preview has intentionally blurred sections. Sign up to view the full version.

View Full DocumentRight Arrow Icon
This is the end of the preview. Sign up to access the rest of the document.

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. 96-109.) 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 Schrdinger equation (because the differential equation is simply too difficult to solve), we can make a guess at the wave function, which we will designate , and the variational principle tells us that the expectation value of the Hamiltonian for is governed by the equation * H d r * d r E (25-1) where E is the correct ground-state energy. Not only does this lower-limit 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 . 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 one-electron wave function contributing to a many-electron wave function) are built up as linear combinations of atomic orbitals. In particular, many-electron wave functions can be written as antisymmetrized Hartree productsi.e., Slater determinantsof such one- electron orbitals , where the one-electron orbitals are defined as = a i i i = 1 N (25-2) where the set of N atomic-orbital basis functions 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 one-electron orbital we evaluate 25-2 E = a i * i * i H a j j j d r a i * i * i a j j j d r = a i * a j ij i * H j d r a i * a j ij i * j d r = a i * a j ij ij H a i * a j ij ij S . (25-3) 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 (25-4) we get N equations which must be satisfied in order for equation 25-4 to hold true, namely a i i = 1 N H ki ES ki ( ) = k . (25-5) 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 = (25-6) where equation 25-6 is called the secular equation. There are N roots (i.e., N different values of...
View Full Document

This note was uploaded on 12/18/2010 for the course CHEM 3502 taught by Professor Staff during the Fall '08 term at Minnesota.

Page1 / 7

3502_25_nove1517 - Chem 3502/5502 Physical Chemistry II...

This preview shows document pages 1 - 3. Sign up to view the full document.

View Full Document Right Arrow Icon
Ask a homework question - tutors are online