data_global #============================================================================= _audit_creation_method SHELXL-97 _audit_creation_date '13 February 2006' #========================================================================== # PROCESSING SUMMARY (IUCr Office Use Only) _journal_date_recd_electronic ? _journal_date_to_coeditor ? _journal_date_from_coeditor ? _journal_date_accepted ? _journal_date_printers_first ? _journal_date_printers_final ? _journal_date_proofs_out ? _journal_date_proofs_in ? _journal_coeditor_name ? _journal_coeditor_code ? _journal_paper_category ? _journal_coeditor_notes ; ? ; _journal_techeditor_code ? _iucr_compatibility_tag ACTA95 _journal_techeditor_notes ; ? ; _journal_coden_ASTM ? _journal_name_full ? _journal_year ? _journal_volume ? _journal_issue ? _journal_page_first ? _journal_page_last ? _journal_suppl_publ_number ? _journal_suppl_publ_pages ? #========================================================================== # SUBMISSION DETAILS _publ_contact_letter ; Date of submission: 2000-10-23 Please consider this CIF submission for publication in Acta Cryst., Section E. All authors have seen and approved this submission. The CIF has passed the Chester CHECKCIF routines and gives a satisfactory PRINTCIF file. Best wishes, Lee Daniels ; _publ_contact_author_name 'Lee Daniels' _publ_contact_author_address ; Rigaku Americas Corp. 9009 New Trails Dr. The Woodlands, TX 77381 U.S.A. ; _publ_contact_author_phone 1-281-362-2300 _publ_contact_author_fax 1-281-364-3628 _publ_contact_author_email ldaniels@Rigaku.com _publ_requested_journal 'Acta Crystallographica E' _publ_requested_category EI #============================================================================= # 3. TITLE AND AUTHOR LIST _publ_section_title ; Redetermination of bis(l-phenyl-2-amino-l,3-dihydroxypropano)ethylenediamino cobalt(III) iodide water solvate ; loop_ _publ_author_name _publ_author_address 'Benson, Ronald E.' ; Rigaku Americas Corporation, 9009 New Trails Dr., The Woodlands, TX 77381 U.S.A. ; 'Clearfield, Abraham' ; Department of Chemistry, PO Box 30012, Texas A&M University, College Station, TX 77842-3012 U.S.A. ; 'Daniels, Lee M.' ; Rigaku Americas Corporation, 9009 New Trails Dr., The Woodlands, TX 77381 U.S.A. ; 'Wardeska, Jeff G.' ; Department of Chemistry, P.O. Box 70695, East Tennessee State University, Johnson City, TN 37614-0695 U.S.A. ; #============================================================================= # 4. TEXT _publ_section_abstract ; New data for the title complex, C~20~H~32~CoN~4~O~4~, I, H~2~O, allows the modelling of previously unresolved disorder in the ethylenediamine ligand coordinated to the octahedral cation. ; #============================================================================= _publ_section_comment ; The title complex (I) was synthesized and crystallized in about 1978, and published the following year as part of a synthetic and spectroscopic project (Wardeska et al., 1979). Crystals of this obviously robust material were recently rediscovered in perfect condition after 28 years in a glass vial and its structure has been redetermined in order to resolve some disorder in the earlier determination. While the structure in the original report gave very good residuals, the disorder in the ethylenediamine ligand was not resolved and the determination of the absolute structure was based only on a comparison of the R values given by the correct versus the inverted structure. We also take this opportunity to present the first published structure from data collected on a new type of single-crystal diffraction instrument, the Rigaku SCXmini benchtop crystallography system. This structure was used as a test of the efficacy of this new paradigm for crystallographic instrumentation. As shown in Fig. 1, there are two distinct conformations of the NH~2~-CH~2~-CH~2~-NH~2~ ligand. The occupancy of the major orientation (specified by the letter A) refined to 0.66(1). The molecular structure of the cation, Table 1, and H bonding scheme, Table 2, involving all components of the unit cell contents, are, of course, similar to that originally described, although in the present structure the positions of the O-bound H atoms were fully refined. ; _publ_section_exptl_prep ; The compound was synthesized from a methanol/water solution of (1S,2S)-(+)-1-phenyl-2-amino-1,3-dihydroxypropane to which was added sodium hexanitrocobaltate(III). The resulting solids were dissolved in a 2:1 methanol/water solution and treated with ethylenediamine, warmed and filtered, then converted to the iodide salt by recrystallizing twice from potassium iodide solution. The complete experimental preparation is described in Wardeska et al. (1979). ; _publ_section_exptl_refinement ; The positions of H atoms bonded to O were fully refined; all other H atoms were used in idealized positions with C-H = 0.98 \%A (methine), 0.93 \%A (phenyl), 0.97 \%A (methylene), and N-H = 0.90 \%A. U(H) was set to 1.2 times that of the attached atom for C and N, and 1.5 times for O. For the disordered group, only the positions of the two C atoms were split; the N positions were not distinct enough to allow modelling over two positions. The isotropic displacement parameters for disordered atoms C7A and C7B were constrained to be equal, as were those for C8A and C8B. The error in the C-C distance introduced by the disorder is greatly reduced in this resolved model as compared to that in the earlier report. When these disordered C atoms are not resolved and they are allowed to refine anisotropically, the resulting apparent C-C distance is 1.395(10) (Wardeska et al., 1979). The present refinement allows for two separate positions for this C-C group, and the distances refine to 1.506(6) for the A group and 1.497(10) for the lower-occupancy B group (i.e. statistically indistinguishable at the 2\s level). ; _publ_section_references ; Altomare, A., Cascarano, G., Giacovazzo, C., Guagliardi, A., Burla, M., Polidori, G. & Camalli, M. (1994). J. Appl. Cryst. 27, 435-436. Flack, H. D. (1983). Acta Cryst. A39, 876--881. Higashi, T. (1995). ABSCOR: Empirical Absorption Correction based on Fourier Series Approximation. Rigaku Corporation, 3-9-12 Matsubara, Akishima, Tokyo 196-8666, JAPAN. Rigaku (1998). Process-Auto: Automatic Data Acquisition and Processing Package for Imaging Plate and CCD Diffractometers. Rigaku Corporation, 3-9-12 Matsubara, Akishima, Tokyo 196-8666, JAPAN. Rigaku (2005). CrystalStructure: Structure Solution and Refinement program, Version 3.7. Rigaku Americas Corp., 9009 New Trails Drive, The Woodlands, TX 77381-5209, USA. Rigaku (2006). SCXmini Benchtop Crystallography System software, Version 1.0. Rigaku Americas Corp., 9009 New Trails Drive, The Woodlands, TX 77381-5209, USA. Sheldrick, G. M. (1997) SHELXL97. University of G\"ottingen, Germany. Wardeska, J. G., Clearfield, A. & Troup, J. M. (1979). Inorg. Chem. 18, 1641--1648. ; _publ_section_figure_captions ; Figure 1 View of the cation in (I). The atoms and bonds in the minor orientation of the disordered ethylenediamine ligand are shown with dashed lines. ; _publ_section_table_legends ; ; _publ_section_acknowledgements ; ; data_enpaco10 _audit_creation_method SHELXL-97 _chemical_name_systematic ; ? ; _chemical_formula_moiety 'C20 H32 Co N4 O4, I, H2 O' _chemical_formula_sum 'C20 H34 Co I N4 O5' _chemical_formula_weight 596.34 _chemical_absolute_configuration ad loop_ _atom_type_symbol _atom_type_description _atom_type_scat_dispersion_real _atom_type_scat_dispersion_imag _atom_type_scat_source 'C' 'C' 0.0033 0.0016 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' 'H' 'H' 0.0000 0.0000 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' 'Co' 'Co' 0.3494 0.9721 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' 'N' 'N' 0.0061 0.0033 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' 'O' 'O' 0.0106 0.0060 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' 'I' 'I' -0.4742 1.8119 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' _symmetry_cell_setting orthorhombic _symmetry_space_group_name_H-M 'P 21 21 21' _symmetry_space_group_name_Hall 'P 21 21 21' loop_ _symmetry_equiv_pos_as_xyz 'x, y, z' 'x+1/2, -y+1/2, -z' '-x, y+1/2, -z+1/2' '-x+1/2, -y, z+1/2' _cell_length_a 6.7895(2) _cell_length_b 14.5013(4) _cell_length_c 24.8565(8) _cell_angle_alpha 90 _cell_angle_beta 90 _cell_angle_gamma 90 _cell_volume 2447.29(13) _cell_formula_units_Z 4 _cell_measurement_temperature 294(2) _cell_measurement_reflns_used 19448 _cell_measurement_theta_min 3.0 _cell_measurement_theta_max 27.5 _exptl_crystal_description prism _exptl_crystal_colour 'translucent pale-brown' _exptl_crystal_size_max 0.42 _exptl_crystal_size_mid 0.39 _exptl_crystal_size_min 0.28 _exptl_crystal_density_meas ? _exptl_crystal_density_diffrn 1.619 _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 1208 _exptl_absorpt_coefficient_mu 1.999 _exptl_absorpt_correction_type multi-scan _exptl_absorpt_correction_T_min 0.466 _exptl_absorpt_correction_T_max 0.57 _exptl_absorpt_process_details 'ABSCOR (Higashi, 1995)' _exptl_special_details ; ? ; _diffrn_ambient_temperature 294(2) _diffrn_radiation_wavelength 0.71073 _diffrn_radiation_type MoK\a _diffrn_radiation_source 'long-fine-focus sealed tube' _diffrn_radiation_monochromator graphite _diffrn_measurement_device_type 'Rigaku SCXmini' _diffrn_measurement_method \w-scans _diffrn_detector_area_resol_mean 6.85 _diffrn_standards_number 0 _diffrn_standards_interval_count ? _diffrn_standards_interval_time 0 _diffrn_standards_decay_% <0.2 _diffrn_reflns_number 19627 _diffrn_reflns_av_R_equivalents 0.029 _diffrn_reflns_av_sigmaI/netI 0.027 _diffrn_reflns_limit_h_min -8 _diffrn_reflns_limit_h_max 8 _diffrn_reflns_limit_k_min -13 _diffrn_reflns_limit_k_max 18 _diffrn_reflns_limit_l_min -30 _diffrn_reflns_limit_l_max 32 _diffrn_reflns_theta_min 3.1 _diffrn_reflns_theta_max 27.5 _reflns_number_total 5482 _reflns_number_gt 5172 _reflns_threshold_expression 'I>2\s(I)' _computing_data_collection 'SCXmini (Rigaku, 2006)' _computing_cell_refinement 'Process-Auto (Rigaku, 1998)' _computing_data_reduction 'Process-Auto' _computing_structure_solution 'SIR92 (Altomare et al., 1994)' _computing_structure_refinement 'SHELXL-97 (Sheldrick, 1997)' _computing_molecular_graphics 'CrystalStructure V3.7 (Rigaku, 2005)' _computing_publication_material 'SHELXL-97 (Sheldrick, 1997)' _refine_special_details ; Refinement of F^2^ against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F^2^, conventional R-factors R are based on F, with F set to zero for negative F^2^. The threshold expression of F^2^ > 2sigma(F^2^) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F^2^ are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger. ; _refine_ls_structure_factor_coef Fsqd _refine_ls_matrix_type full _refine_ls_weighting_scheme calc _refine_ls_weighting_details 'calc w=1/[\s^2^(Fo^2^)+(0.022P)^2^+P] where P=(Fo^2^+2Fc^2^)/3' _atom_sites_solution_primary direct _atom_sites_solution_secondary difmap _atom_sites_solution_hydrogens geom _refine_ls_hydrogen_treatment mixed _refine_ls_extinction_method none _refine_ls_extinction_coef ? _refine_ls_abs_structure_details '(Flack, 1983)' _refine_ls_abs_structure_Flack 0.007(14) _refine_ls_number_reflns 5482 _refine_ls_number_parameters 291 _refine_ls_number_restraints 215 _refine_ls_R_factor_all 0.030 _refine_ls_R_factor_gt 0.027 _refine_ls_wR_factor_ref 0.062 _refine_ls_wR_factor_gt 0.061 _refine_ls_goodness_of_fit_ref 1.10 _refine_ls_restrained_S_all 1.08 _refine_ls_shift/su_max 0.003 _refine_ls_shift/su_mean 0.000 loop_ _atom_site_label _atom_site_type_symbol _atom_site_fract_x _atom_site_fract_y _atom_site_fract_z _atom_site_U_iso_or_equiv _atom_site_adp_type _atom_site_occupancy _atom_site_symmetry_multiplicity _atom_site_calc_flag _atom_site_refinement_flags _atom_site_disorder_assembly _atom_site_disorder_group I1 I 0.24806(3) 1.289623(13) 0.701876(8) 0.05308(7) Uani 1 1 d . . . Co1 Co 0.21430(5) 0.93696(2) 0.673829(13) 0.02590(7) Uani 1 1 d . . . O4 O 0.8157(3) 1.08284(14) 0.62835(8) 0.0383(4) Uani 1 1 d DU . . H4 H 0.930(3) 1.062(2) 0.6145(12) 0.042(8) Uiso 1 1 d D . . O5 O 0.6808(5) 1.1481(2) 0.72736(12) 0.0804(9) Uani 1 1 d D . . H2W H 0.739(7) 1.151(4) 0.6947(11) 0.121 Uiso 1 1 d D . . H1W H 0.571(5) 1.175(3) 0.740(2) 0.121 Uiso 1 1 d D . . O1 O 0.3046(2) 0.83092(11) 0.63805(7) 0.0294(4) Uani 1 1 d U A . O3 O -0.3187(3) 0.81759(15) 0.60232(9) 0.0474(5) Uani 1 1 d DU A . H3 H -0.441(3) 0.809(3) 0.6175(14) 0.071 Uiso 1 1 d D . . O2 O 0.1432(2) 0.99710(12) 0.60874(7) 0.0301(4) Uani 1 1 d U A . N1A N 0.2831(3) 0.88261(14) 0.74411(8) 0.0357(5) Uani 0.657(6) 1 d PU A 1 H1A1 H 0.1910 0.8413 0.7540 0.043 Uiso 0.657(6) 1 calc PR A 1 H1A2 H 0.3999 0.8535 0.7419 0.043 Uiso 0.657(6) 1 calc PR A 1 N3A N 0.1217(3) 1.04309(15) 0.71760(9) 0.0369(5) Uani 0.657(6) 1 d PU A 1 H3A1 H 0.2014 1.0917 0.7119 0.044 Uiso 0.657(6) 1 calc PR A 1 H3A2 H -0.0006 1.0589 0.7072 0.044 Uiso 0.657(6) 1 calc PR A 1 N1B N 0.2831(3) 0.88261(14) 0.74411(8) 0.0357(5) Uani 0.343(6) 1 d PU A 2 H1B1 H 0.2280 0.8263 0.7463 0.043 Uiso 0.343(6) 1 calc PR A 2 H1B2 H 0.4146 0.8751 0.7455 0.043 Uiso 0.343(6) 1 calc PR A 2 N3B N 0.1217(3) 1.04309(15) 0.71760(9) 0.0369(5) Uani 0.343(6) 1 d PU A 2 H3B1 H 0.1555 1.0966 0.7017 0.044 Uiso 0.343(6) 1 calc PR A 2 H3B2 H -0.0101 1.0415 0.7211 0.044 Uiso 0.343(6) 1 calc PR A 2 N2 N -0.0417(3) 0.87671(13) 0.67324(9) 0.0286(4) Uani 1 1 d U A . H2A H -0.0911 0.8754 0.7068 0.034 Uiso 1 1 calc R . . H2B H -0.1254 0.9089 0.6523 0.034 Uiso 1 1 calc R . . N4 N 0.4763(3) 0.98935(14) 0.66224(8) 0.0282(4) Uani 1 1 d U A . H4A H 0.5135 1.0216 0.6915 0.034 Uiso 1 1 calc R . . H4B H 0.5641 0.9438 0.6570 0.034 Uiso 1 1 calc R . . C1 C 0.1466(3) 0.78521(18) 0.61191(10) 0.0288(5) Uani 1 1 d U . . H1 H 0.1054 0.8216 0.5806 0.035 Uiso 1 1 calc R A . C2 C -0.0230(3) 0.78085(17) 0.65230(11) 0.0293(5) Uani 1 1 d U A . H2 H 0.0169 0.7408 0.6821 0.035 Uiso 1 1 calc R . . C15 C 0.2218(4) 0.69206(16) 0.59293(10) 0.0312(5) Uani 1 1 d U A . C16 C 0.2528(5) 0.61960(17) 0.62874(11) 0.0431(6) Uani 1 1 d U . . H16 H 0.2211 0.6266 0.6649 0.052 Uiso 1 1 calc R A . C17 C 0.3307(5) 0.5371(2) 0.61045(15) 0.0540(9) Uani 1 1 d U A . H17 H 0.3467 0.4882 0.6343 0.065 Uiso 1 1 calc R . . C18 C 0.3844(5) 0.5268(2) 0.55766(15) 0.0560(9) Uani 1 1 d U . . H18 H 0.4380 0.4713 0.5458 0.067 Uiso 1 1 calc R A . C19 C 0.3591(6) 0.5977(2) 0.52268(15) 0.0568(9) Uani 1 1 d U A . H19 H 0.3981 0.5909 0.4870 0.068 Uiso 1 1 calc R . . C20 C 0.2757(5) 0.67989(19) 0.53957(11) 0.0453(7) Uani 1 1 d U . . H20 H 0.2558 0.7273 0.5150 0.054 Uiso 1 1 calc R A . C5 C 0.4717(3) 1.05122(18) 0.61421(10) 0.0271(5) Uani 1 1 d U . . H5 H 0.4302 1.1130 0.6255 0.033 Uiso 1 1 calc R A . C3 C -0.2219(4) 0.74665(18) 0.63105(12) 0.0403(6) Uani 1 1 d U . . H3A H -0.2014 0.6941 0.6076 0.048 Uiso 1 1 calc R A . H3B H -0.3036 0.7270 0.6609 0.048 Uiso 1 1 calc R . . C9 C 0.2787(4) 1.07077(16) 0.52822(9) 0.0294(5) Uani 1 1 d U . . C14 C 0.1607(4) 1.14859(19) 0.52991(12) 0.0371(6) Uani 1 1 d U A . H14 H 0.0962 1.1642 0.5616 0.045 Uiso 1 1 calc R . . C13 C 0.1378(4) 1.2035(2) 0.48459(14) 0.0465(7) Uani 1 1 d U . . H13 H 0.0554 1.2547 0.4859 0.056 Uiso 1 1 calc R A . C12 C 0.2360(5) 1.1829(2) 0.43779(12) 0.0512(8) Uani 1 1 d U A . H12 H 0.2208 1.2201 0.4076 0.061 Uiso 1 1 calc R . . C11 C 0.3566(5) 1.1070(2) 0.43583(12) 0.0500(8) Uani 1 1 d U . . H11 H 0.4257 1.0937 0.4045 0.060 Uiso 1 1 calc R A . C10 C 0.3762(4) 1.0500(2) 0.48032(11) 0.0404(6) Uani 1 1 d U A . H10 H 0.4548 0.9976 0.4782 0.048 Uiso 1 1 calc R . . C6 C 0.6744(3) 1.05765(19) 0.58866(10) 0.0317(5) Uani 1 1 d U A . H6A H 0.7098 0.9987 0.5730 0.038 Uiso 1 1 calc R . . H6B H 0.6729 1.1034 0.5602 0.038 Uiso 1 1 calc R . . C4 C 0.3141(3) 1.01045(16) 0.57716(10) 0.0279(5) Uani 1 1 d U A . H4C H 0.3600 0.9500 0.5647 0.034 Uiso 1 1 calc R . . C7A C 0.2942(8) 0.9589(3) 0.78466(19) 0.0429(10) Uiso 0.657(6) 1 d PDU A 1 H7A1 H 0.4162 0.9929 0.7806 0.051 Uiso 0.657(6) 1 calc PR A 1 H7A2 H 0.2886 0.9340 0.8209 0.051 Uiso 0.657(6) 1 calc PR A 1 C8A C 0.1202(9) 1.0209(4) 0.77437(19) 0.0448(10) Uiso 0.657(6) 1 d PDU A 1 H8A1 H -0.0013 0.9897 0.7839 0.054 Uiso 0.657(6) 1 calc PR A 1 H8A2 H 0.1307 1.0766 0.7957 0.054 Uiso 0.657(6) 1 calc PR A 1 C7B C 0.2222(16) 0.9357(6) 0.7904(3) 0.0429(10) Uiso 0.343(6) 1 d PDU A 2 H7B1 H 0.3118 0.9252 0.8201 0.051 Uiso 0.343(6) 1 calc PR A 2 H7B2 H 0.0909 0.9175 0.8015 0.051 Uiso 0.343(6) 1 calc PR A 2 C8B C 0.2241(19) 1.0347(5) 0.7749(3) 0.0448(10) Uiso 0.343(6) 1 d PDU A 2 H8B1 H 0.3585 1.0573 0.7731 0.054 Uiso 0.343(6) 1 calc PR A 2 H8B2 H 0.1528 1.0711 0.8012 0.054 Uiso 0.343(6) 1 calc PR A 2 loop_ _atom_site_aniso_label _atom_site_aniso_U_11 _atom_site_aniso_U_22 _atom_site_aniso_U_33 _atom_site_aniso_U_23 _atom_site_aniso_U_13 _atom_site_aniso_U_12 I1 0.05905(14) 0.04394(11) 0.05623(12) -0.00782(8) 0.01004(12) -0.00603(12) Co1 0.02083(15) 0.02368(14) 0.03319(15) 0.00319(12) 0.00077(13) 0.00013(13) O4 0.0212(9) 0.0493(11) 0.0442(11) 0.0009(9) -0.0001(8) -0.0008(8) O5 0.071(2) 0.102(2) 0.0673(18) -0.0235(17) 0.0020(15) 0.0044(17) O1 0.0201(9) 0.0284(8) 0.0397(9) -0.0011(7) 0.0017(7) 0.0000(7) O3 0.0312(11) 0.0498(12) 0.0613(13) 0.0091(10) -0.0030(10) -0.0049(9) O2 0.0182(8) 0.0349(10) 0.0374(10) 0.0081(8) -0.0008(7) -0.0007(7) N1A 0.0300(12) 0.0387(11) 0.0383(11) 0.0069(9) 0.0025(10) -0.0002(11) N3A 0.0307(12) 0.0318(12) 0.0481(14) 0.0005(10) 0.0028(10) 0.0000(9) N1B 0.0300(12) 0.0387(11) 0.0383(11) 0.0069(9) 0.0025(10) -0.0002(11) N3B 0.0307(12) 0.0318(12) 0.0481(14) 0.0005(10) 0.0028(10) 0.0000(9) N2 0.0212(10) 0.0273(10) 0.0375(11) 0.0019(9) 0.0039(9) 0.0016(8) N4 0.0236(10) 0.0272(10) 0.0337(11) 0.0036(9) -0.0006(8) -0.0013(8) C1 0.0241(12) 0.0294(12) 0.0328(13) 0.0054(11) 0.0012(10) -0.0006(11) C2 0.0235(12) 0.0246(11) 0.0397(14) 0.0022(11) 0.0006(10) 0.0001(10) C15 0.0246(12) 0.0334(11) 0.0357(12) -0.0017(9) 0.0001(11) -0.0017(11) C16 0.0481(17) 0.0389(13) 0.0422(14) 0.0038(11) 0.0066(16) 0.0119(16) C17 0.056(2) 0.0372(16) 0.069(2) 0.0037(15) 0.0014(16) 0.0143(14) C18 0.0459(19) 0.0424(17) 0.080(3) -0.0226(18) 0.0101(17) 0.0035(15) C19 0.063(2) 0.059(2) 0.0489(19) -0.0207(16) 0.0134(16) -0.0081(17) C20 0.0544(19) 0.0433(14) 0.0380(14) -0.0040(11) 0.0038(15) -0.0080(16) C5 0.0192(11) 0.0264(12) 0.0358(13) 0.0054(11) 0.0016(9) 0.0003(10) C3 0.0271(14) 0.0319(12) 0.0619(17) 0.0002(12) 0.0009(14) -0.0030(12) C9 0.0228(11) 0.0331(11) 0.0325(11) 0.0023(9) -0.0034(10) -0.0017(12) C14 0.0344(14) 0.0350(14) 0.0420(15) 0.0076(12) 0.0035(12) 0.0013(11) C13 0.0398(16) 0.0389(16) 0.061(2) 0.0165(15) -0.0013(14) 0.0048(14) C12 0.053(2) 0.0556(17) 0.0450(16) 0.0191(13) -0.0038(16) 0.0007(18) C11 0.0536(19) 0.065(2) 0.0309(15) 0.0038(14) 0.0015(13) 0.0033(17) C10 0.0395(15) 0.0459(16) 0.0356(14) -0.0006(13) -0.0034(12) 0.0052(13) C6 0.0227(12) 0.0356(13) 0.0367(14) 0.0055(11) 0.0016(10) -0.0001(11) C4 0.0204(12) 0.0270(11) 0.0364(13) 0.0022(10) 0.0007(10) 0.0007(10) _geom_special_details ; All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes. ; loop_ _geom_bond_atom_site_label_1 _geom_bond_atom_site_label_2 _geom_bond_distance _geom_bond_site_symmetry_2 _geom_bond_publ_flag Co1 O1 1.8793(17) . y Co1 O2 1.9002(18) . y Co1 N2 1.9456(19) . y Co1 N4 1.955(2) . y Co1 N1A 1.973(2) . y Co1 N3A 1.987(2) . y O4 C6 1.424(3) . y O4 H4 0.899(17) . y O5 H2W 0.91(2) . y O5 H1W 0.90(3) . y O1 C1 1.419(3) . y O3 C3 1.414(3) . y O3 H3 0.919(18) . y O2 C4 1.415(3) . y N1A C7A 1.498(5) . y N1A H1A1 0.9000 . ? N1A H1A2 0.9000 . ? N3A C8A 1.448(5) . y N3A H3A1 0.9000 . ? N3A H3A2 0.9000 . ? N2 C2 1.490(3) . y N2 H2A 0.9000 . ? N2 H2B 0.9000 . ? N4 C5 1.494(3) . y N4 H4A 0.9000 . ? N4 H4B 0.9000 . ? C1 C15 1.519(3) . y C1 C2 1.529(3) . y C1 H1 0.9800 . ? C2 C3 1.532(4) . y C2 H2 0.9800 . ? C15 C20 1.387(4) . y C15 C16 1.393(3) . y C16 C17 1.385(4) . y C16 H16 0.9300 . ? C17 C18 1.370(5) . y C17 H17 0.9300 . ? C18 C19 1.357(5) . y C18 H18 0.9300 . ? C19 C20 1.385(4) . y C19 H19 0.9300 . ? C20 H20 0.9300 . ? C5 C6 1.519(3) . y C5 C4 1.531(3) . y C5 H5 0.9800 . ? C3 H3A 0.9700 . ? C3 H3B 0.9700 . ? C9 C14 1.384(4) . y C9 C10 1.395(4) . y C9 C4 1.517(3) . y C14 C13 1.389(4) . y C14 H14 0.9300 . ? C13 C12 1.374(4) . y C13 H13 0.9300 . ? C12 C11 1.373(4) . y C12 H12 0.9300 . ? C11 C10 1.387(4) . y C11 H11 0.9300 . ? C10 H10 0.9300 . ? C6 H6A 0.9700 . ? C6 H6B 0.9700 . ? C4 H4C 0.9800 . ? C7A C8A 1.506(6) . y C7A H7A1 0.9700 . ? C7A H7A2 0.9700 . ? C8A H8A1 0.9700 . ? C8A H8A2 0.9700 . ? C7B C8B 1.487(10) . y C7B H7B1 0.9700 . ? C7B H7B2 0.9700 . ? C8B H8B1 0.9700 . ? C8B H8B2 0.9700 . ? loop_ _geom_angle_atom_site_label_1 _geom_angle_atom_site_label_2 _geom_angle_atom_site_label_3 _geom_angle _geom_angle_site_symmetry_1 _geom_angle_site_symmetry_3 _geom_angle_publ_flag O1 Co1 O2 93.18(8) . . y O1 Co1 N2 85.45(8) . . y O2 Co1 N2 88.43(8) . . y O1 Co1 N4 87.21(8) . . y O2 Co1 N4 85.83(8) . . y N2 Co1 N4 170.41(9) . . y O1 Co1 N1A 90.85(8) . . y O2 Co1 N1A 175.95(9) . . y N2 Co1 N1A 92.23(10) . . y N4 Co1 N1A 94.03(9) . . y O1 Co1 N3A 175.03(9) . . y O2 Co1 N3A 91.74(9) . . y N2 Co1 N3A 93.98(9) . . y N4 Co1 N3A 93.87(9) . . y N1A Co1 N3A 84.23(9) . . y C6 O4 H4 103(2) . . y H2W O5 H1W 131(5) . . y C1 O1 Co1 110.63(14) . . y C3 O3 H3 96(2) . . y C4 O2 Co1 109.08(14) . . y C7A N1A Co1 108.2(2) . . y C7A N1A H1A1 110.1 . . ? Co1 N1A H1A1 110.1 . . ? C7A N1A H1A2 110.1 . . ? Co1 N1A H1A2 110.1 . . ? H1A1 N1A H1A2 108.4 . . ? C8A N3A Co1 111.3(2) . . y C8A N3A H3A1 109.4 . . ? Co1 N3A H3A1 109.4 . . ? C8A N3A H3A2 109.4 . . ? Co1 N3A H3A2 109.4 . . ? H3A1 N3A H3A2 108.0 . . ? C2 N2 Co1 110.22(14) . . y C2 N2 H2A 109.6 . . ? Co1 N2 H2A 109.6 . . ? C2 N2 H2B 109.6 . . ? Co1 N2 H2B 109.6 . . ? H2A N2 H2B 108.1 . . ? C5 N4 Co1 109.41(14) . . y C5 N4 H4A 109.8 . . ? Co1 N4 H4A 109.8 . . ? C5 N4 H4B 109.8 . . ? Co1 N4 H4B 109.8 . . ? H4A N4 H4B 108.2 . . ? O1 C1 C15 107.69(19) . . ? O1 C1 C2 106.8(2) . . ? C15 C1 C2 114.8(2) . . ? O1 C1 H1 109.1 . . ? C15 C1 H1 109.1 . . ? C2 C1 H1 109.1 . . ? N2 C2 C1 104.8(2) . . ? N2 C2 C3 110.3(2) . . ? C1 C2 C3 116.8(2) . . ? N2 C2 H2 108.2 . . ? C1 C2 H2 108.2 . . ? C3 C2 H2 108.2 . . ? C20 C15 C16 118.4(2) . . ? C20 C15 C1 119.9(2) . . ? C16 C15 C1 121.5(2) . . ? C17 C16 C15 120.0(3) . . ? C17 C16 H16 120.0 . . ? C15 C16 H16 120.0 . . ? C18 C17 C16 120.7(3) . . ? C18 C17 H17 119.6 . . ? C16 C17 H17 119.6 . . ? C19 C18 C17 119.8(3) . . ? C19 C18 H18 120.1 . . ? C17 C18 H18 120.1 . . ? C18 C19 C20 120.6(3) . . ? C18 C19 H19 119.7 . . ? C20 C19 H19 119.7 . . ? C19 C20 C15 120.5(3) . . ? C19 C20 H20 119.8 . . ? C15 C20 H20 119.8 . . ? N4 C5 C6 110.6(2) . . ? N4 C5 C4 105.27(19) . . ? C6 C5 C4 113.9(2) . . ? N4 C5 H5 109.0 . . ? C6 C5 H5 109.0 . . ? C4 C5 H5 109.0 . . ? O3 C3 C2 110.4(2) . . ? O3 C3 H3A 109.6 . . ? C2 C3 H3A 109.6 . . ? O3 C3 H3B 109.6 . . ? C2 C3 H3B 109.6 . . ? H3A C3 H3B 108.1 . . ? C14 C9 C10 118.4(2) . . ? C14 C9 C4 122.5(2) . . ? C10 C9 C4 119.0(2) . . ? C9 C14 C13 120.5(3) . . ? C9 C14 H14 119.7 . . ? C13 C14 H14 119.7 . . ? C12 C13 C14 120.5(3) . . ? C12 C13 H13 119.7 . . ? C14 C13 H13 119.7 . . ? C11 C12 C13 119.6(3) . . ? C11 C12 H12 120.2 . . ? C13 C12 H12 120.2 . . ? C12 C11 C10 120.4(3) . . ? C12 C11 H11 119.8 . . ? C10 C11 H11 119.8 . . ? C11 C10 C9 120.4(3) . . ? C11 C10 H10 119.8 . . ? C9 C10 H10 119.8 . . ? O4 C6 C5 109.7(2) . . ? O4 C6 H6A 109.7 . . ? C5 C6 H6A 109.7 . . ? O4 C6 H6B 109.7 . . ? C5 C6 H6B 109.7 . . ? H6A C6 H6B 108.2 . . ? O2 C4 C9 113.18(19) . . ? O2 C4 C5 107.0(2) . . ? C9 C4 C5 111.8(2) . . ? O2 C4 H4C 108.3 . . ? C9 C4 H4C 108.3 . . ? C5 C4 H4C 108.3 . . ? N1A C7A C8A 106.7(4) . . ? N1A C7A H7A1 110.4 . . ? C8A C7A H7A1 110.4 . . ? N1A C7A H7A2 110.4 . . ? C8A C7A H7A2 110.4 . . ? H7A1 C7A H7A2 108.6 . . ? N3A C8A C7A 107.0(4) . . ? N3A C8A H8A1 110.3 . . ? C7A C8A H8A1 110.3 . . ? N3A C8A H8A2 110.3 . . ? C7A C8A H8A2 110.3 . . ? H8A1 C8A H8A2 108.6 . . ? C8B C7B H7B1 110.1 . . ? C8B C7B H7B2 110.1 . . ? H7B1 C7B H7B2 108.5 . . ? C7B C8B H8B1 110.2 . . ? C7B C8B H8B2 110.2 . . ? H8B1 C8B H8B2 108.5 . . ? loop_ _geom_hbond_atom_site_label_D _geom_hbond_atom_site_label_H _geom_hbond_atom_site_label_A _geom_hbond_distance_DH _geom_hbond_distance_HA _geom_hbond_distance_DA _geom_hbond_angle_DHA _geom_hbond_site_symmetry_A O4 H4 O2 0.899(17) 1.73(2) 2.594(2) 159(3) 1_655 O5 H2W O4 0.906(19) 1.99(3) 2.792(3) 146(5) . O5 H1W I1 0.90(3) 2.91(4) 3.639(3) 140(5) . O3 H3 O1 0.919(18) 1.83(2) 2.714(3) 160(4) 1_455 N1A H1A1 I1 0.90 3.26 4.078(2) 152 3_546 N1A H1A2 I1 0.90 2.92 3.709(2) 147 3_646 N3A H3A1 I1 0.90 2.90 3.697(2) 149 . N3A H3A2 O4 0.90 2.35 3.094(3) 140 1_455 N3A H3A2 O5 0.90 2.57 3.368(4) 148 1_455 N1B H1B2 I1 0.90 2.91 3.709(2) 148 3_646 N3B H3B1 I1 0.90 2.87 3.697(2) 154 . N3B H3B2 O5 0.90 2.61 3.368(4) 142 1_455 N3B H3B2 O4 0.90 2.66 3.094(3) 111 1_455 N2 H2A I1 0.90 2.80 3.632(2) 155 3_546 N4 H4A O5 0.90 2.34 3.139(4) 149 . N4 H4B O3 0.90 2.41 3.219(3) 149 1_655 _diffrn_measured_fraction_theta_max 0.994 _diffrn_reflns_theta_full 27.5 _diffrn_measured_fraction_theta_full 0.994 _refine_diff_density_max 0.58 _refine_diff_density_min -0.69 _refine_diff_density_rms 0.054