Transcript osu06f.ppt
Experimental Rotational Spectra for MnRe(CO)10 and o-C6H4† Required Accurate theoretical Calculations for Successful Analysis STEPHEN KUKOLICH, Chemistry Dept., University of Arizona, MICHAEL PALMER School of Chemistry, University of Edinburgh, PETER GRONER, Chemistry, University of Missouri-Kansas City, and CHAKREE TANJAROON, Chemistry, University of Alberta, C1 C2 H1 b C3 Mn a C6 Re C4 C5 H2 † Measured at Harvard with Pat Thaddeus and Mike McCarthy OSU – June - 2006 1 Observing and Measuring the Rotational Transition Frequencies was Difficult B = 200.3687 MHz (187Re ) eQq(187Re) = 370.42(38) MHz eQq(55Mn) = -16.52(5) MHz Mn Re C1 C2 H1 b C3 a C4 H2 C5 C6 Normal Isotopomer transitions were readily observed 13C Isotopomer lines often obscured by other products of Discharge (Shotgun effect) OSU – June - 2006 2 MnRe(CO)10 + >Symmetric top with C4v symmetry - >Combination of small B-values with two quadrupoles resulted in congested and difficult-to-assign spectra (J=11→ 12 and 12→ 13) + > Michael Palmer and Martyn Guest (Edinburgh) calculated the eQq values sufficiently accurately to allow unambiguous assignments of the spectra OSU – June - 2006 3 Example Spectra for 8, and 10 MHz “pieces” of the spectrum OSU – June - 2006 4 Pair of measured transitions 2000 Shots OSU – June - 2006 5 C4v symmetry Only K=4n transitions observed Staggered or Eclipsed? † (S) † F. A. Cotton, Austin 2004 (E) (E) Mn Re (S) Mn Re xx OSU – June - 2006 6 Experimental and theoretical molecular parameters for Mn 187Re(CO)10 . Calculated Values (B3LYP) from M. H. Palmer, et al. (J. Chem. Phys. 121, 7187 (2004)). B and eQq values in MHz. 187 Parameter Mn Re(CO)10 MICROWAVE Mn187Re(CO)10 Mn187Re(CO)10 Calculated Calculated (STAGGERED) (ECLIPSED) MnRe(CO)10 X-ray1 eQq(55Mn) -16.52(5) 5.87 0.68 - eQq(187Re) 370.42(38) 310.11 327.6 - B 200.36871(8) 188.77 178.40 204.2304 rMnRe (Å) 2.99 3.086 Å 3.224 2.909(1) 212(1) 199(1) De(kJ/mol) Calculated from the geometry 1 A. L. Rheingold, W. K. Meckstroth, and D.P. Ridge, Inorg. Chem. 25, 3706-3707 (1986) OSU – June - 2006 7 The structure of o – benzyne and vibrational averaging effects. • • • • • • • • • 1. Spectra Measured on HARVARD FTMWS1 Discharge 0.5% BENZENE in NEON Normal Isotopomer - 27 b-dipole transitions 13C - 12 b-dipole transitions 6 D1 - 26 b-dipole transitions D2 - 23 b-dipole transitions 13C (1) - 10 b-dipole transitions 1 DIFFICULT 13C (3) - 9 b-dipole transitions 1 To MEASURE 13C (5) - 10 b-dipole transitions 1 S. G. Kukolich, M. C. McCarthy and P. Thaddeus, J. Phys. Chem. 108, 2645-2651, (2004) OSU – June - 2006 8 Search for 13C lines… in a sea of lines from other radicals and molecules produced in the DISCHARGE. WRONG MOLECULE GOOD ONE JUNK C1 C2 H1 b C3 a C4 C6 C5 H2 kHz OSU – June - 2006 9 Least-squares structure fit The inertial defect for the normal isotopomer of o-benzyne is = ICC – IAA – IBB = 0.06935(1) amu Å2, consistent with a PLANAR STRUCTURE. This value is sufficiently large that when trying to fit the measured A, B, and C rotational constants with a planar structure, some of the deviations will be as large as 1 MHz. EXPT STANDARD DEVIATION CALC. DEV. NORMAL A 6989.729 6989.915 -0.186 FOR FIT = 1.05 MHz B 5706.806 5706.891 -0.085 Experimental errors are < 2 kHz! C 3140.371 3141.789 -1.418 13C1 A 6859.730 6859.886 -0.155 B 5679.516 5679.369 0.147 C 3105.740 3107.029 -1.289 OSU – June - 2006 10 Least-squares fit to determine the structure Most of the same vibrational averaging effects which contribute to the differences between the r0 and re coordinates, will also contribute to this inertial defect. Problem 1. We are trying to fit a PLANAR, (re ) structure to EXPERIMENTAL A, B, and C which have non-zero inertial defect, (characteristic of the r0 coordinates ) Problem 2. The r0 coordinates are different for each of the measured isotopomers SOLUTION: Find the ak, vibration-rotation constants, so we fit the re structure, same for all isotopomers OSU – June - 2006 11 VIBRATIONAL AVERAGING EFFECTS – RELATED TO VIBRATION-ROTATION INTERACTION CONSTANTS k a A rotational constant for the GROUND VIBRATIONAL STATE, Bo, is related to the EQUILIBRIUM rotational constant, Be by: (summed over k vibrational states) αα o B B αα e 1 2 αk k The corresponding relation for MOMENTS OF INERTIA is: I αα o I αα e 1 2 C1 C2 kαα H1 b C3 a C4 C6 C5 H2 k and the INERTIAL DEFECT is: Δo I occ I oaa I obb Values for these ak were calculated by Peter Groner1, University of Missouri OSU – June - 2006 12 Final Structure of o-benzyne 1.255 1.383 127 H1 C2 o 127 C3 Now the fit is MUCH improved ( s < 30 kHz) C1 o o b 1.080 a 111 r(C1-C2) for HCCH =1.203 Å r(C1-C2) for H2CCH2 =1.332 Å C6 o 122 1.403 o 119 H2 C4 C5 1.405 1.082 r(C2-C3) for benzene =1.3914 Å r(C2-C3), NMR value → 1.24(2) Å Grant, Michl, et al. P. Groner and S. G. Kukolich, J. Mol. Struct. 780-781, 178 (2006) OSU – June - 2006 13 The re structure of o-benzyne Structural parameter re MP2/ 6-31G(d) (Distances r in Å) rs / Kraitchman B3LYP/ 631G(d,p) BPW9 1/ ccpVDZ Ref. This work This work [a] [b] [c] r(C1-C2) 1.255(3) 1.268 1.255(8) 1.251 1.266 r(C2-C3) 1.383(2) 1.389 1.40(2) 1.385 1.391 r(C3-C4) 1.403(2) 1.405 1.39(2) 1.412 1.423 r(C4-C5) 1.405(3) 1.410 1.404(14) 1.407 1.412 r(C3-H1) 1.080(1) 1.086 1.08(2) 1.085 1.098 r(C4-H2) 1.082(1) 1.088 1.084(9) 1.087 1.100 r(C-C) b 1.3914(1) 1.395 r(C-H) b 1.0825(3) 1.087 Benzene [a] S. G. Kukolich, M. C. McCarthy, P. Thaddeus, J. Phys. Chem A 108 (2004) 2645-2651. [b] S. G. Kukolich, C. Tanjaroon, M. C. McCarthy, P. Thaddeus, J. Chem. Phys. 119 (2003) 4353-4359. [c] C. J. Cramer, Nash, J. J. and R. R. Squires, Chem. Phys. Lett. 277 (1997) 311-320. OSU – June - 2006 14 Acknowledgements • Willis Flygare and Terry Balle •Harvard: Pat Thaddeus, Mike McCarthy •Arizona: Kristen Keck •Edingburgh: Martyn Guest, Phillip Camp •Department of Chemistry, University of Arizona. • N$F - This material is based upon work supported by the National Science Foundation under Grant No. CHE-0304969. This support from the National Science Foundation is gratefully acknowledged OSU – June - 2006 15 OSU – June - 2006 16 Other isomers of benzyne The structural isomers of didehydrobenzene – ortho-benzyne, meta-benzyne and para-benzyne. Calculations show Hf(o-benzyne) >Hf(mbenzyne)>Hf(p-benzyne) OSU – June - 2006 17 O - BENZYNE Brown, Godfrey, Rodler, Robertson (1st microwave, no structure) Pyrolyzed: pthalic anhydride, or ninhydrin, or benzocyclobutene-R (1986, 2003) Lineberger, Squires, et al. (1998)- electron afinities, singlet triplet splittings & vibrational frequencies • PRESENT WORK (2002…) Discharge 0.5% BENZENE in NEON HARVARD SPECTROMETER (Sabbatical) OSU – June - 2006 18