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Structure-Property Relationships in Crystal Structures of Polar Molecules

Structure-Property Relationships in Crystal Structures of Polar Molecules. Graham Tizzard Supervisor: Mike Hursthouse. Background. No. of different attractive forces determine packing in molecular crystals London forces, multipolar forces, H- bonding, CT forces

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Structure-Property Relationships in Crystal Structures of Polar Molecules

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  1. Structure-Property Relationships in Crystal Structures of Polar Molecules Graham Tizzard Supervisor: Mike Hursthouse

  2. Background • No. of different attractive forces determine packing in molecular crystals • London forces, multipolar forces, H- bonding, CT forces • Complex interplay of these + repulsion E → many local minima in crystal lattice E • → Polymorphism - the existence of more than one crystalline form in a substance

  3. Polymorphism & H-bonding • H-bonds: • Highest E interactions in molecular crystals  most important attractive force • Multiple H-bonding sites → different H-bonding topologies → polymorphism • However: • Polymorphism also in systems w.out strong H-bonds (D – H ∙∙∙ A; D = N, O, S; A = N, O, S, Hal) • Weak H-bonds may exist (C – H ∙∙∙ A, C – H ∙∙∙ π) • Importance of H-bonding in defining polymorphism greatly reduced

  4. Aims • Detailed study of weak or non H-bonding systems • Especially those w. non-centrosymmetric polymorphs • V. important for development of materials w. NLO properties • Electrostatic interactions expected to exert greater influence on xtal structure

  5. Dataset • Constructed from Cambridge Structural Database1 (CSD) v5.25 (November 2003) • CSD mined for polymorphic clusters with ≥ one non-centrosymmetric member • 835 ‘hits’ made up of 258 polymorphic clusters each comprising of 2-3 different polymorphs [1] F. H. Allen, Acta Crystallogr., B58, 380-388, 2002..

  6. Analyses • XPac2: • Many polymorphic families of a compound show no similarity when analysed • For those that do ‘structure-forming’ motif may be able to be elucidated from results • Short contact analysis (Mercury v1.2.13) + modelling of electrostatic charges (Spartan’04 for windows4) • Correlation between short contact distances & matching of potentials would suggest these are important in a crystal structure [2] XPac; T. Gelbrich; 2002; University of Southampton, UK. [3] Mercury v1.2.1; CCDC, Cambridge, UK. [4] Spartan’04; Wavefunction, Inc.; Irvine, CA, USA.

  7. 4’-Bromo-trans-1,4-dihydro-4-tritylbiphenyl (BAWSAT) CSD code BAWSAT BAWSAT01 Crystal System orthorhombic monoclinic Space Group (No.) Pnam (62) Pc (7) a / Å 13.012 9.011 b / Å 17.264 16.187 c / Å 10.431 8.463 α / º 90 90 β / º 90 108.98 γ / º 90 90 Cell Volume / Å3 2343.211 1167.309 Z 4 2 Z’ 0.5 1.0 • 2 polymorphs identified from CSD: BAWSAT & BAWSAT01 • BAWSAT01 is non-centrosymmetric Reference [5] [5] [5] A. K. Cheetham, M. C. Grossel, J. M. Newsam; J. Am. Chem. Soc.; 103; 5363; 1981.

  8. XPac Analysis of BAWSAT • Views of BAWSAT along the c-axis (top) & BAWSAT01 between the a and c axes (bottom) • XPac reveals 1d chain along these respective axes common to both crystal structures (green) • In both structures the same chain motif is interspaced (in different ways) between the original (dark green) • Is this a ‘structure-forming’ motif?...

  9. Short Contact & Electrostatic Charge Analyses of BAWSAT BAWSAT01 • Each molecule in BAWSAT01 (top) & BAWSAT (bottom) has short contacts w. 8 neighbours • None of these is particularly strong • ESC & SC data correlation: 4/10 wrt. BAWSAT01; 0 wrt. BAWSAT • Suggests electrostatic interactions unimportant in crystal formation • Other interactions e.g. simple space-filling may dictate these structures. Atom1 Electrostatic charge 1 Atom2 Electrostatic charge 2 Length / Å Length-VdW / Å H8 0.130679 H24 :1 0.136779 2.314 -0.086 H24 0.136779 H8 :2 0.130679 2.314 -0.086 H3 0.097207 Br1 :3 -0.117756 2.97 -0.08 Br1 -0.117756 H3 :4 0.097207 2.97 -0.08 H13 0.104592 H19 :5 0.120092 2.342 -0.058 H19 0.120092 H13 :6 0.104592 2.342 -0.058 H4 0.155091 C28 :7 -0.191035 2.844 -0.056 C28 -0.191035 H4 :8 0.155091 2.844 -0.056 H22 0.136788 H4 :8 0.155091 2.359 -0.041 H4 0.155091 H22 :7 0.136788 2.359 -0.041 BAWSAT Atom1 Electrostatic charge 1 Atom2 Electrostatic charge 2 Length / Å Length-VdW / Å H13 0.104592 H4 :1 0.155091 2.28 -0.12 H4 0.155091 H18 :2 0.104591 2.28 -0.12 H4 0.155091 H13 :3 0.104592 2.28 -0.12 H18 0.104591 H4 :4 0.155091 2.28 -0.12 H3 0.097207 H5 :5 0.097216 2.298 -0.102 H5 0.097216 H3 :6 0.097207 2.298 -0.102 H13 0.104592 H18 :7 0.104591 2.37 -0.03 H18 0.104591 H13 :8 0.104592 2.37 -0.03 H5 0.097216 C3 :5 0.078511 2.898 -0.002 C5 0.078478 H3 :5 0.097207 2.898 -0.002 C3 0.078511 H5 :4 0.097216 2.898 -0.002 H3 0.097207 C5 :4 0.078478 2.898 -0.002

  10. 2-(α-p-Bromophenyl-β-nitroethyl)-cyclohexanone (BPNECH) CSD code BPNECH BPNECH01 Crystal System monoclinic orthorhombic Space Group (No.) P21/c (14) P212121 (19) a / Å 5.630 5.539 b / Å 8.560 8.495 c / Å 30.570 30.777 α / º 90 90 β / º 90.30 90 γ / º 90 90 Cell Volume / Å3 1473.234 1448.175 Z 4 4 Z’ 1.0 1.0 • 2 polymorphs identified from CSD: BPNECH & BPNECH01 • BPNECH01 is non-centrosymmetric Reference [6] [7] [6] M. Calligaris, F. Giordano, L. Randaccio; Ric. Sci., Parte 1; 36; 1333; 1966. [7] D. Seebach, I. M. Lyapkalo, R. Dahinden; Helv Chim Acta; 82; 1829; 1999.

  11. XPac Analysis of BPNECH • Views of BPNECH (top) and BPNECH01 (bottom) along the b-axis • XPac reveals 2d sheet along these respective axes common to both crystal structures (green) • In BPNECH both highlighted sheets (green & dark green) are identical • In BPNECH01 second sheet highlighted (red) is same sheet structure after a 21 screw operation

  12. Short Contact & Electrostatic Charge Analyses of BPNECH BPNECH01 Atom1 Electrostatic charge 1 Atom2 Electrostatic charge 2 Length Length-VdW • Each molecule in BPNECH01 (top) and BPNECH (bottom) has short contacts w. 8 / 9 neighbours respectively • Short contacts are stronger on the whole than in BAWSAT & BAWSAT01 • ESC & SC data correlate in both polymorphs • Suggests that electrostatic interactions may be significant in formation of both crystal systems O2 -0.434661 H13 :1 0.166816 2.498 -0.222 H13 0.166816 O2 :2 -0.434661 2.498 -0.222 H12 0.203696 O2 :2 -0.434661 2.508 -0.212 O2 -0.434661 H12 :1 0.203696 2.508 -0.212 O2 -0.434661 H1 :3 0.130828 2.596 -0.124 H1 0.130828 O2 :4 -0.434661 2.596 -0.124 O1 -0.447545 H7 :5 0.106818 2.636 -0.084 H7 0.106818 O1 :6 -0.447545 2.636 -0.084 H5 0.093177 Br1 :7 -0.05641 2.987 -0.063 Br1 -0.05641 H5 :8 0.093177 2.987 -0.063 O3 -0.451598 H2 :1 0.12995 2.661 -0.059 H2 0.12995 O3 :2 -0.451598 2.661 -0.059 BPNECH Atom1 Electrostatic charge 1 Atom2 Electrostatic charge 2 Length Length-VdW H1 0.130828 O2 :1 -0.434661 2.394 -0.326 O2 -0.434661 H1 :2 0.130828 2.394 -0.326 O2 -0.434661 H13 :3 0.1308283 2.45 -0.27 H13 0.1308283 O2 :4 -0.434661 2.45 -0.27 H12 0.1308282 O2 :4 -0.434661 2.496 -0.224 O2 -0.434661 H12 :3 0.1308282 2.496 -0.224 H2 0.12995 O3 :4 -0.451598 2.575 -0.145 O3 -0.451598 H2 :3 0.12995 2.575 -0.145 H7 0.106818 O1 :5 -0.447545 2.624 -0.096 O1 -0.447545 H7 :6 0.106818 2.624 -0.096 O1 -0.447545 Br1 :7 -0.05641 3.313 -0.057 Br1 -0.05641 O1 :7 -0.447545 3.313 -0.057 H9 0.06238 O2 :4 -0.434661 2.672 -0.048 O2 -0.434661 H9 :3 0.06238 2.672 -0.048 O3 -0.451598 H3 :8 0.062736 2.691 -0.029 H3 0.062736 O3 :9 -0.451598 2.691 -0.029

  13. Comments I • Several points worth noting: • Overall analysis involves several techniques - hard to draw conclusions using them in isolation • XPac analysis uses ’top-down’ approach - data derived from polymorph crystal structures • Modelling of electrostatic charges is ‘bottom-up’ approach - data derived from molecule • One goal of Comb-e-Chem project - combine data from different analyses to derive novel data & develop it into meaningful knowledge

  14. Comments II • Major ‘bottlenecks’ throughout project have been workflow related: • Data transfer from one application to another • ‘Driving’ applications to obtain the data • Methods of automation investigated: • perl to write data-transfer scripts • Spreadsheets to automate calculations • Ultimate aim of providing complete analysis of electrostatic interactions of a molecule in context of its crystal packing as a single ‘callable’ process

  15. Acknowledgements • Prof. Mike Hursthouse • The Group – Dr. Simon Coles, Dr. Mark Light, Dr. Peter Horton, Dr. Ann Bingham, Dr. Thomas Gelbrich, Dr. Stefan Christensen, Dr. Yang Li, Dr. David Hughes, Suzanna Ward • EPSRC E-Science project (GR/R67729, Comb-e-Chem)

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