############################################################################## ### ### ### Electronic paper (Acta Crystallographica Section E) ### ### ### ############################################################################## # # # This CIF contains the data in a paper accepted for publication in Acta # # Crystallographica Section E. It conforms to the requirements of Notes # # for Authors for Section E, and has been peer reviewed under the auspices # # of the IUCr Commission on Journals. # # # # Full details of the Crystallographic Information File format # # are given in the paper "The Crystallographic Information File (CIF): # # a New Standard Archive File for Crystallography" by S. R. Hall, F. H. # # Allen and I. D. Brown [Acta Cryst. (1991), A47, 655-685]. # # # # The current version of the core CIF dictionary is obtainable from # # ftp://ftp.iucr.org/pub/cif_core.dic. The current version number is 2.4. # # # # Software is freely available for graphical display of the structure(s) in # # this CIF. For information consult the CIF home page http://www.iucr.org/ # # cif/home.html # # # # This file may be used for bona fide research purposes within the # # scientific community so long as proper attribution is given to the journal # # article from which it was obtained. # # # ############################################################################## data_I _audit_creation_method SHELXL-97 _chemical_name_systematic ; L-Alanine hydrochloride monohydrate ; _chemical_name_common 'L-Alanine hydrochloride monohydrate' _chemical_formula_moiety 'C3 H8 N O2 +, Cl -, H2 O' _chemical_formula_sum 'C3 H10 Cl N O3' _chemical_formula_iupac 'C3 H8 N O2 +, Cl -, H2 O' _chemical_formula_weight 143.57 _chemical_melting_point ? _symmetry_cell_setting orthorhombic _symmetry_space_group_name_H-M 'P 21 21 21' _symmetry_space_group_name_Hall 'P 2ac 2ab' loop_ _symmetry_equiv_pos_as_xyz 'x, y, z' '-x+1/2, -y, z+1/2' '-x, y+1/2, -z+1/2' 'x+1/2, -y+1/2, -z' _cell_length_a 6.1925(13) _cell_length_b 9.929(2) _cell_length_c 11.759(3) _cell_angle_alpha 90.0 _cell_angle_beta 90.0 _cell_angle_gamma 90.0 _cell_volume 723.0(3) _cell_formula_units_Z 4 _cell_measurement_reflns_used 902 _cell_measurement_theta_min 7.44 _cell_measurement_theta_max 53.94 _cell_measurement_temperature 150(2) _exptl_crystal_description 'plate' _exptl_crystal_colour 'colourless' _exptl_crystal_size_max 0.45 _exptl_crystal_size_mid 0.40 _exptl_crystal_size_min 0.35 _exptl_crystal_density_diffrn 1.319 _exptl_crystal_density_meas ? _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 304 _exptl_absorpt_coefficient_mu 0.462 _exptl_absorpt_correction_type multi-scan _exptl_absorpt_process_details '(SADABS; Bruker 2001)' _exptl_absorpt_correction_T_min 0.8189 _exptl_absorpt_correction_T_max 0.8549 _exptl_special_details ; ; _diffrn_ambient_temperature 293(2) _diffrn_radiation_type MoK\a _diffrn_radiation_wavelength 0.71073 _diffrn_radiation_source 'fine-focus sealed tube' _diffrn_radiation_monochromator graphite _diffrn_measurement_device_type 'Bruker SMART APEX CCD area-detector' _diffrn_measurement_method \w _diffrn_detector_area_resol_mean ? _diffrn_reflns_number 5762 _diffrn_reflns_av_R_equivalents 0.0218 _diffrn_reflns_av_sigmaI/netI 0.0168 _diffrn_reflns_theta_min 2.68 _diffrn_reflns_theta_max 27.00 _diffrn_reflns_theta_full 27.00 _diffrn_measured_fraction_theta_max 0.961 _diffrn_measured_fraction_theta_full 0.961 _diffrn_reflns_limit_h_min -7 _diffrn_reflns_limit_h_max 7 _diffrn_reflns_limit_k_min -11 _diffrn_reflns_limit_k_max 12 _diffrn_reflns_limit_l_min -14 _diffrn_reflns_limit_l_max 14 _diffrn_standards_number 263 _diffrn_standards_interval_count ? _diffrn_standards_interval_time ? _diffrn_standards_decay_% 0.0 _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^ > \s(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. ; _reflns_number_total 1467 _reflns_number_gt 1452 _reflns_threshold_expression I>2\s(I) _refine_ls_structure_factor_coef Fsqd _refine_ls_matrix_type full _refine_ls_R_factor_all 0.0195 _refine_ls_R_factor_gt 0.0193 _refine_ls_wR_factor_gt 0.0532 _refine_ls_wR_factor_ref 0.0533 _refine_ls_goodness_of_fit_ref 1.114 _refine_ls_restrained_S_all 1.114 _refine_ls_number_reflns 1467 _refine_ls_number_parameters 84 _refine_ls_number_restraints 0 _refine_ls_hydrogen_treatment mixed _refine_ls_weighting_scheme calc _refine_ls_weighting_details 'calc w=1/[\s^2^(Fo^2^)+(0.0308P)^2^+0.0901P] where P=(Fo^2^+2Fc^2^)/3' _atom_sites_solution_hydrogens geom _atom_sites_solution_primary direct _atom_sites_solution_secondary difmap _refine_ls_shift/su_max 0.001 _refine_ls_shift/su_mean 0.000 _refine_diff_density_max 0.194 _refine_diff_density_min -0.199 _refine_ls_extinction_method none _refine_ls_extinction_coef ? _refine_ls_abs_structure_details 'Flack (1983), 533 Friedel pairs' _refine_ls_abs_structure_Flack 0.02(6) 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' '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' 'Cl' 'Cl' 0.1484 0.1585 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4' _computing_data_collection ; SMART for WNT/2000 (Bruker, 2001) ; _computing_cell_refinement ; SAINT-Plus (Bruker, 2001) ; _computing_data_reduction ; SAINT-Plus (Bruker, 2001) ; _computing_structure_solution 'SHELXS97 (Sheldrick, 2008)' _computing_structure_refinement 'SHELXL97 (Sheldrick, 2008)' _computing_molecular_graphics 'ORTEP-3 for Windows (Farrugia, 1997)' _computing_publication_material 'SHELXL97 (Sheldrick, 2008)' loop_ _atom_site_type_symbol _atom_site_label _atom_site_fract_x _atom_site_fract_y _atom_site_fract_z _atom_site_U_iso_or_equiv _atom_site_adp_type _atom_site_calc_flag _atom_site_refinement_flags _atom_site_occupancy _atom_site_disorder_assembly _atom_site_disorder_group Cl Cl 0.19971(4) 0.55991(3) 1.25180(2) 0.02475(10) Uani d . 1 . . C C1 0.8057(2) 0.60202(13) 0.88317(11) 0.0295(3) Uani d . 1 . . H H1A 0.9301 0.6167 0.8360 0.044 Uiso calc R 1 . . H H1B 0.7483 0.6872 0.9073 0.044 Uiso calc R 1 . . H H1C 0.6979 0.5540 0.8407 0.044 Uiso calc R 1 . . C C2 0.6780(2) 0.49201(12) 1.06398(10) 0.0249(2) Uani d . 1 . . N N 0.96092(17) 0.38728(10) 0.95162(8) 0.0230(2) Uani d . 1 . . H HA 1.0116 0.3443 1.0124 0.034 Uiso calc R 1 . . H HB 1.0676 0.4003 0.9021 0.034 Uiso calc R 1 . . H HC 0.8577 0.3381 0.9193 0.034 Uiso calc R 1 . . O O3 1.13229(15) 0.26883(10) 1.15289(8) 0.0261(2) Uani d . 1 . . O O1 0.60730(17) 0.38141(9) 1.08180(8) 0.0342(2) Uani d . 1 . . O O2 0.60094(18) 0.60494(10) 1.10708(9) 0.0374(2) Uani d . 1 . . H H2 0.4967 0.5880 1.1476 0.056 Uiso calc R 1 . . C C3 0.87031(18) 0.51981(12) 0.98686(10) 0.0228(2) Uani d . 1 . . H H3 0.9801 0.5694 1.0299 0.027 Uiso calc R 1 . . H H4 1.159(3) 0.335(2) 1.1930(16) 0.047(5) Uiso d . 1 . . H H5 1.050(3) 0.2271(18) 1.1882(14) 0.036(5) Uiso d . 1 . . loop_ _atom_site_aniso_label _atom_site_aniso_U_11 _atom_site_aniso_U_22 _atom_site_aniso_U_33 _atom_site_aniso_U_12 _atom_site_aniso_U_13 _atom_site_aniso_U_23 Cl 0.02114(14) 0.02522(15) 0.02790(15) 0.00128(9) 0.00012(12) -0.00516(12) C1 0.0308(6) 0.0239(6) 0.0337(6) 0.0021(5) 0.0026(5) 0.0073(5) C2 0.0260(5) 0.0230(5) 0.0256(5) 0.0013(5) 0.0015(5) -0.0018(5) N 0.0232(5) 0.0200(5) 0.0257(5) 0.0019(4) 0.0028(4) 0.0023(4) O3 0.0281(5) 0.0235(4) 0.0268(5) -0.0044(4) 0.0023(4) -0.0008(4) O1 0.0398(5) 0.0238(4) 0.0389(5) -0.0059(4) 0.0160(4) -0.0029(4) O2 0.0384(5) 0.0244(4) 0.0494(6) 0.0011(4) 0.0183(5) -0.0046(4) C3 0.0227(5) 0.0183(5) 0.0274(6) -0.0003(4) 0.0011(5) -0.0002(4) _geom_special_details ; All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes. ; loop_ _geom_bond_atom_site_label_1 _geom_bond_atom_site_label_2 _geom_bond_site_symmetry_2 _geom_bond_distance _geom_bond_publ_flag C1 C3 . 1.5209(17) ? C1 H1A . 0.9600 ? C1 H1B . 0.9600 ? C1 H1C . 0.9600 ? C2 O1 . 1.2006(16) yes C2 O2 . 1.3196(15) yes C2 C3 . 1.5223(16) yes N C3 . 1.4893(15) yes N HA . 0.8900 ? N HB . 0.8900 ? N HC . 0.8900 ? O3 H4 . 0.82(2) ? O3 H5 . 0.78(2) ? O2 H2 . 0.8200 ? C3 H3 . 0.9800 ? loop_ _geom_angle_atom_site_label_1 _geom_angle_atom_site_label_2 _geom_angle_atom_site_label_3 _geom_angle_site_symmetry_1 _geom_angle_site_symmetry_3 _geom_angle _geom_angle_publ_flag C3 C1 H1A . . 109.5 ? C3 C1 H1B . . 109.5 ? H1A C1 H1B . . 109.5 ? C3 C1 H1C . . 109.5 ? H1A C1 H1C . . 109.5 ? H1B C1 H1C . . 109.5 ? O1 C2 O2 . . 125.34(11) yes O1 C2 C3 . . 123.71(11) yes O2 C2 C3 . . 110.95(10) yes C3 N HA . . 109.5 ? C3 N HB . . 109.5 ? HA N HB . . 109.5 ? C3 N HC . . 109.5 ? HA N HC . . 109.5 ? HB N HC . . 109.5 ? H4 O3 H5 . . 104.4(17) ? C2 O2 H2 . . 109.5 ? N C3 C1 . . 110.50(10) ? N C3 C2 . . 107.48(9) ? C1 C3 C2 . . 111.65(11) ? N C3 H3 . . 109.1 ? C1 C3 H3 . . 109.1 ? C2 C3 H3 . . 109.1 ? loop_ _geom_torsion_atom_site_label_1 _geom_torsion_atom_site_label_2 _geom_torsion_atom_site_label_3 _geom_torsion_atom_site_label_4 _geom_torsion_site_symmetry_1 _geom_torsion_site_symmetry_2 _geom_torsion_site_symmetry_3 _geom_torsion_site_symmetry_4 _geom_torsion _geom_torsion_publ_flag O1 C2 C3 N . . . . -6.06(18) yes O2 C2 C3 N . . . . 174.26(9) yes O1 C2 C3 C1 . . . . 115.28(14) yes O2 C2 C3 C1 . . . . -64.39(14) yes loop_ _geom_hbond_atom_site_label_D _geom_hbond_atom_site_label_H _geom_hbond_atom_site_label_A _geom_hbond_site_symmetry_A _geom_hbond_distance_DH _geom_hbond_distance_HA _geom_hbond_distance_DA _geom_hbond_angle_DHA N HA O3 . 0.89 1.96 2.8479(14) 173.8 N HB Cl 2_664 0.89 2.31 3.1957(11) 170.6 N HC O3 4_457 0.89 1.95 2.8380(15) 179.5 O2 H2 Cl . 0.82 2.23 3.0446(11) 174.6 O3 H4 Cl 1_655 0.82(2) 2.35(2) 3.1432(12) 161.0(17) O3 H5 Cl 3_647 0.78(2) 2.38(2) 3.1283(11) 163.3(16) data_global _journal_date_recd_electronic 2008-03-06 _journal_date_accepted 2008-04-01 _journal_name_full 'Acta Crystallographica, Section E' _journal_year 2008 _journal_volume 64 _journal_issue 5 _journal_page_first o806 _journal_page_last o806 _journal_paper_category QO _journal_coeditor_code HG2382 _publ_contact_author_name 'Kazuhiko Yamada' _publ_contact_author_address ; National Institute for Materials Science 3-13 Sakura Tsukuba 305-0003 Japan ; _publ_contact_author_email yamada.kazuhiko@nims.go.jp _publ_contact_author_fax '+81-29-863-5571' _publ_contact_author_phone '+81-29-863-5483' _publ_section_title ; L-Alanine hydrochloride monohydrate ; loop_ _publ_author_name _publ_author_footnote _publ_author_address 'Yamada, Kazuhiko' . ; National Institute for Materials Science 3-13 Sakura Tsukuba 305-0003 Japan ; 'Sato, Akira' . ; National Institute for Materials Science 3-13 Sakura Tsukuba 305-0003 Japan ; 'Shimizu, Tadashi' . ; National Institute for Materials Science 3-13 Sakura Tsukuba 305-0003 Japan ; 'Yamazaki, Toshio' . ; Protein Research Group, Genomic Sciences Center, Yokohama Institute, RIKEN, 1-7-22 Suehiro, Tsurumi, Yokohama 230-0045, Japan ; 'Yokoyama, Shigeyuki' . ; Protein Research Group, Genomic Sciences Center, Yokohama Institute, RIKEN, 1-7-22 Suehiro, Tsurumi, Yokohama 230-0045, Japan ;