From chemistry-request /at\www.ccl.net Fri Feb 12 19:47:48 1999 Received: from bioorganic.mechanisms.ucsb.edu. ([128.111.114.116]) by www.ccl.net (8.8.3/8.8.6/OSC/CCL 1.0) with ESMTP id TAA11488 Fri, 12 Feb 1999 19:47:47 -0500 (EST) Received: (from kalju #at# localhost) by bioorganic.mechanisms.ucsb.edu. (8.9.1a/8.9.1) id QAA17983 for chemistry _-at-_)www.ccl.net; Fri, 12 Feb 1999 16:44:26 -0800 (PST) From: "Kalju Kahn" Message-Id: <9902121644.ZM17981 # - at - # bioorganic> Date: Fri, 12 Feb 1999 16:44:26 -0800 X-Mailer: Z-Mail (3.2.3 08feb96 MediaMail) To: chemistry \\at// www.ccl.net Subject: BSSE in calc. of activation energies? Mime-Version: 1.0 Content-Type: text/plain; charset=us-ascii Dear CCLers, I realize there has been some controversy about basis set superposition error (BSSE), and that the current consensus favors the view that full counterpoise procedure (CP) of Boys and Bernardini is a good way to correct for BSSE. (e.g. van Duijneveldt et. al. in Chem. Rev, 1994, 94, 1873-1885) My question concerns application of BSSE correction via CP to bimolecular reactions. Let's take gas phase SN2 displacement as an example. Here we have a two reactants, A and B, forming first a bimolecular "reactants complex" (RC), followed by transition state (TS): A + B -> (A...B)[RC] -> A-B[TS] The activation barrier can be defined as an energy difference between TS and RC. What is the correct way to calculate this energy difference? (Assuming Born-Oppenheimer approximation, and dealing with size-consistent methods, e.g. HF level of theory) My own answer would be: If one accepts a view that energies of both RC and TS (relative to isolated reactants) are affected by BSSE, one should correct both according to the CP scheme, and now: E_act = E(TS,TS_basis_in_TS_geometry)-E(RC,RC_basis_in_RC_geometry)- E(A,TS_basis_in_TS_geometry) -E(B,TS_basis_in_TS_geometry)+ E(A,RC_basis_in_RC_geometry) +E(B,RC_basis_in_RC_geometry) Obviously, the number of basis functions in TS_basis and RC_basis is the same, but the geometrical position of ghost orbitals relative to partner molecule are different in TS_geometry and RC_geometry. So, the last four terms do not cancel out. This seems a right way to account for BSSE, but the above method was quoted as "misinterpretation of the BSSE concept" by Dr. J. A. Sordo in "Comment on "Ab initio investigation of internal rotation in the ethylene-sulfur dioxide dimer"" (J. Chem. Phys., 106(14), 6204). Could somebody kindly explain me how do I misinterpret the BSSE concept here? Or do we need to be concerned about BSSE when calculating ab initio activation barriers? Thanks a lot, Kalju P.S. I will summarize your responses. P.S.2. Happy Valentine's Day! ****************************************************************** Kalju Kahn kalju- at -bioorganic.ucsb.edu Chemistry Department tel: (805)-893-7158 University of California Santa Barbara Santa Barbara, CA 93106 ##################################################################