the latter surrounded by six oxygen atoms arranged at the vertices of a distorted octahedron. One of the six 0 atoms is an atom from the bromite anion (see Figure l ) , and the remainder are water molecules. The stoichiometry requires that some of the water molecules be associated with more than one octahedron, and zigzag chains of edge-linked octahedra are present in the solid. The compound is isomorphous with the corresponding chlorine compound,22 and Br-0 distances of 1.731 (2) and 1.702 (2) A may be compared with CI-0 distances of 1.564 (1) and 1.557 (1) A.The anion, as expected, is a bent species with a bond angle (0-Br-0 = 105.3 (1)O) comparable with the 0-(21-0 angle (108.23 (6)') in NaC102.3H20.22 The Br-0 distances in the oxoanions decrease with increasing bromine oxidation state, and the present values can be compared with the Br-0 distances in NaBr0323(1.648 (4) A) and KBr0424 (1.59 (1)-1.62 (1) A).Bromine K-edge EXAFS data were obtained for solid NaBr-O2.3H20 diluted with boron nitride and for saturated aqueous solutions. The k3 weighted data obtained after background subtraction were used for curve fitting without smoothing or Fourier filtering, and the background-subtracted data and the corresponding Fourier transform for solid NaBr02.3H20 are shown in Figure 2. The fitting employed the single scattering curved wave theory as contained in the EXCURVE program and utilized ab initio phase shifts calculated in the usual manner.'* Analysis of the data from solid-state samples gave an average Br-O distance of 1.75 A,25 and no further shells arising from other neighboring atoms are statistically significant. In solution, a Br-O bond length of 1.72 A25 was obtained. Both values compare well with the bond lengths obtained from the X-ray study and suggest that EXAFS results for related compounds of uncertain structure may be viewed with confidence.
Acknowledgment.(25) Systematic errors in data collection and analysis give rise to errors of ca. f0.02-0.03 A in the first shell distances. NaBr02+3H20: 2u2 = 0.013 A, FI = 0.04, R = 11.9. NaBr02 aqueous solution ' 2u2 = 0.009 A, FI = x 100. 0.20, R = 11.4. FI = xi (x: -xi k )k?. R = [Ilx4'-xElk' dk/.fIXEl dk]Abstract: We present the application of molecular mechanics/dynamics and free energy perturbation computational techniques to simulation of iron(I1) porphyrin systems. Force field parameters were developed by modeling the geometry of four systems whose crystal structure is known. This force field was then used in molecular dynamics/free energy perturbation calculations, at 300 K in vacuo, on a separate set of four iron(I1) porphyrin systems including models of 5,Spyridine cyclophane heme( 1,5-DCI) (I), picket fence heme(2-MeIm) (11), monochelated heme (111), and 7,7-durene cyclophane heme( 1,5-DCI) (IV). The perturbation calculations reproduced reasonably well the trend in the partition coefficient, M value, of this set. Our simplified model indicates that the electrostatic component of both I and I1 favors the binding of O2 over CO, whereas the electrostatic...