Buy article online - an online subscription or single-article purchase is required to access this article.
Download citation
Download citation
link to html
The title compound, [ZnBr2(C13H23N3)], (3), was readily prepared from the reaction between ZnBr2 and (S,S)-(1–6-[1-(di­methyl­amino)­ethyl]-2-pyridinyl­ethyl)-N,N-di­methyl­amine. (3) exists as a distorted square pyramid and crystallizes with two independent mol­ecules in the asymmetric unit. The apical position of the square pyramid is occupied by one of the Br atoms, with the base of the pyramid consisting of the three N atoms of the ligand and the other Br atom. This is the first reported structure determination of a compound containing the C2-symmetric mol­ecule (S,S)-N-(1-{6-[1-(di­methyl­amino)­ethyl]­pyridin-2-yl}ethyl)-N,N-di­methyl­amine.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536803018920/bt6335sup1.cif
Contains datablocks global, 3

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536803018920/bt63353sup2.hkl
Contains datablock 3

CCDC reference: 222837

Key indicators

  • Single-crystal X-ray study
  • T = 150 K
  • Mean [sigma](C-C) = 0.009 Å
  • R factor = 0.051
  • wR factor = 0.131
  • Data-to-parameter ratio = 21.6

checkCIF/PLATON results

No syntax errors found



Alert level C PLAT029_ALERT_3_C _diffrn_measured_fraction_theta_full Low ....... 0.99 PLAT213_ALERT_2_C Atom C13A has ADP max/min Ratio ............. 3.30 prolat PLAT220_ALERT_2_C Large Non-Solvent C Ueq(max)/Ueq(min) ... 2.86 Ratio PLAT222_ALERT_3_C Large Non-Solvent H Ueq(max)/Ueq(min) ... 3.24 Ratio PLAT250_ALERT_2_C Large U3/U1 ratio for average U(i,j) tensor .... 2.09 PLAT341_ALERT_3_C Low Bond Precision on C-C bonds (x 1000) Ang ... 9 PLAT720_ALERT_4_C Number of Unusual/Non-Standard Label(s) ........ 22
Alert level G REFLT03_ALERT_4_G Please check that the estimate of the number of Friedel pairs is correct. If it is not, please give the correct count in the _publ_section_exptl_refinement section of the submitted CIF. From the CIF: _diffrn_reflns_theta_max 27.54 From the CIF: _reflns_number_total 7418 Count of symmetry unique reflns 4164 Completeness (_total/calc) 178.15% TEST3: Check Friedels for noncentro structure Estimate of Friedel pairs measured 3254 Fraction of Friedel pairs measured 0.781 Are heavy atom types Z>Si present yes
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 7 ALERT level C = Check and explain 1 ALERT level G = General alerts; check 0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 3 ALERT type 2 Indicator that the structure model may be wrong or deficient 3 ALERT type 3 Indicator that the structure quality may be low 2 ALERT type 4 Improvement, methodology, query or suggestion

Comment top

Zinc complexes are important in organic chemistry due to the their central role in many enantioselective reactions (Denmark & Beutner, 2002; Lebel et al., 2003; Soai, 1999) and biological systems (Auld, 2001; Lipscomb & Strater, 1996; Vallee & Auld, 1993). In our ongoing program that aims at developing ligands for molecular recognition of biologically important compounds (Chin et al., 1999; Mancin & Chin, 2002), we wish to report the synthesis and the X-ray analysis of complex (3) from the optically active C2-symmetric ligand (S,S)—N-(1-{6-[1-(dimethylamino)ethyl]pyridin-2-yl}ethyl)-N,N-dimethylamine, (2), and zinc(II) bromide.

Ligand (2) was prepared from the readily available chiral diol (R,R)-(BHEP), (1) (Brown et al., 1997), where BHEP = 2,6-bis(1-hydroxyethyl)pyridine, through its reaction with methanesulfonic anhydride and dimethylamine in acetonitrile (see Scheme). The substitution reaction proceeded through conversion of stereochemistry to afford the (S,S) enantiomer of ligand (2), which was then complexed with zinc(II) bromide to produce compound (3).

In the crystal structure of (3), there are two molecules in the asymmetric unit, A and B (Figs. 1 and 2). The coordination geometry of compound (3) is a distorted square pyramid, with the apical position occupied by a Br atom (Br1). The three N atoms of the ligand and the other Br atom (Br2) occupy the base of the pyramid. The Zn atom is displaced by 0.668 (2) and 0.675 (2) Å in molecules A and B, respectively, towards atom Br1 from the least-squares plane formed by N1/N2/N3/Br2. The maximum deviations from these planes are for atoms N2A [0.027 (3) Å] and N2B [0.103 Å]. An analysis (Cremer & Pople, 1975) of the puckering of the five-membered metallacycle (Zn1/N1/C1/C2/N2), where the C atom (C10) is equatorial to the chelate ring, gives Qt values of 0.412 (5) and 0.424 (5) Å for molecules A and B, respectively. The puckering of the five-membered metallacycle (Zn1/N3/C7/C6/N2), where the C atom (C11) is axial to the chelate ring, gives Qt values of 0.404 (6) and 0.414 (5) Å for molecules A and B, respectively. The conformations of each five-membered ring in both molecules is `envelope' with a local pseudo-twofold axis running along N1 and the mid-point of the C2—N2 bond or N3 and the mid-point of the C6—N2 bond (Duax et al., 1976). The angles N2—Zn1—N1 of 76.00 (17) and 75.61 (19)°, and N2—Zn1—N3 of 74.85 (18) and 74.15 (19)° for molecules A and B, respectively, are considerably smaller than the ideal angle of 90° for a square pyramid. These angles are due to the formation of strained five-membered chelate rings and the distortion in the square pyramid environment around the Zn atom. The Zn—Npyridine bond length in molecules A and B [average 2.106 (5) Å], is comparable to the corresponding bond lengths in other ligands with pyridine complexed to ZnII (Canary et al., 1998; Comba et al., 2002). The only differences between the two molecules in (3) are the values of some of the angles at the Zn center; the most notable of these being N3A—Zn1A—Br1A of 108.90 (16)° and N3B—Zn1B—Br1B of 113.89 (14)°. These differences which may be apparent on viewing Figs. 1 and 2 can only be attributable to packing forces.

Experimental top

2,6-Bis(1-hydroxyethyl)pyridine, (1) (1.21 g, 7.21 mmol), was dissolved in 40 ml dry acetonitrile. Pyridine (3.00 ml, 37.2 mmol) was added to this solution and the mixture was cooled to 273 K in an ice bath. Methanesulfonic anhydride (3.00 g,16.7 mmol) was added to this mixture under an atmosphere of argon. The clear yellow solution turned cloudy after 5 min. This mixture was allowed to stir at room temperature for an additional 30 min and the precipitate was filtered off. Dimethylamine (20 ml, 40.0 mmol) from a 2 M tetrahydrofuran solution was added to the golden brown filtrate and this mixture was allowed to stir at room temperature for 24 h. The precipitate was filtered off and the organic solvents removed under reduced pressure. The remaining residue was partitioned between (30 ml) chloroform and (20 ml) saturated aqueous solution of Na2CO3. The aqueous layer was further extracted with (30 ml) chloroform and the two organic extracts were combined, dried over anhydrous sodium sulfate and the solvent evaporated to afford the crude product, (2), as a brown oil. This oil was chromatographed on silica with dichloromethane/methanol (8:2) as eluant to afford the pure product (2) as a yellow oil (1.31 g, 82%). 1H NMR, 300 MHz (CDCl3): 7.60 (t, J = 7.7 Hz, 1H), 7.21 (d, J = 7.7 Hz, 2H), 3.48 (q, J = 6.6 Hz, 2H), 2.24 (s, 12H), 1.36 (d, J = 6.6 Hz, 6H). 13C NMR, 100 MHz (CDCl3): δ 162.5, 136.6, 119.8, 67.2, 43.1, 19.1. Zinc(II) bromide (183 mg, 0.813 mmol) in 1.5 ml H2O was added to (2) (18.0 mg, 81.3 µmol). The precipitate was collected and dissolved in hot ethanol (2.0 ml). Slow evaporation of the ethanol at room temperature afforded crystals of (3) suitable for X-ray analysis.

Refinement top

All H atoms bonded to C atoms were placed in calculated positions, with C—H distances ranging from 0.95 to 1.00 Å, and included in the refinement in riding-motion approximation, with Uiso = 1.2Ueq (1.5Ueq for methyl) of the carrier atom.

Computing details top

Data collection: COLLECT (Nonius, 1997-2002); cell refinement: DENZO-SMN (Otwinowski & Minor, 1997); data reduction: DENZO-SMN; program(s) used to solve structure: SHELXTL (Sheldrick, 2001); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXT.

Figures top
[Figure 1] Fig. 1. View of molecule A of (3), with the crystallographic labeling scheme. Displacement ellipsoids are at the 30% probability level.
[Figure 2] Fig. 2. View of molecule B of (3), with the crystallographic labeling scheme. Displacement ellipsoids are at the 30% probability level.
[Figure 3] Fig. 3. Packing diagram (Spek, 2002) of (3), viewed bown the b axis. Colour codes: green Br, yellow Zn, blue N, and black C.
[(S,S)—N-(1-{6-[1-(Dimethylamino)ethyl]pyridin-2-yl}ethyl)-N,N- dimethylamine-κ3N]dibromozinc(II) top
Crystal data top
[ZnBr2(C13H23N3)]F(000) = 888
Mr = 446.53Dx = 1.718 Mg m3
Monoclinic, P21Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2ybCell parameters from 24950 reflections
a = 9.9680 (2) Åθ = 2.6–27.5°
b = 11.5077 (2) ŵ = 6.04 mm1
c = 15.4906 (4) ÅT = 150 K
β = 103.712 (1)°Block, colourless
V = 1726.26 (6) Å30.35 × 0.30 × 0.24 mm
Z = 4
Data collection top
Nonius KappaCCD
diffractometer
7418 independent reflections
Radiation source: fine-focus sealed tube6981 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.064
Detector resolution: 9 pixels mm-1θmax = 27.5°, θmin = 3.0°
ϕ scans and ω scans from κ offsetsh = 1212
Absorption correction: multi-scan
(SORTAV; Blessing, 1995)
k = 1414
Tmin = 0.131, Tmax = 0.234l = 1920
12530 measured reflections
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.051 w = 1/[σ2(Fo2) + (0.0848P)2 + 0.0739P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.131(Δ/σ)max < 0.001
S = 1.06Δρmax = 0.91 e Å3
7418 reflectionsΔρmin = 1.64 e Å3
344 parametersExtinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
1 restraintExtinction coefficient: 0.0082 (10)
Primary atom site location: structure-invariant direct methodsAbsolute structure: Flack (1983); 3292 Friedel pairs
Secondary atom site location: difference Fourier mapAbsolute structure parameter: 0.021 (13)
Crystal data top
[ZnBr2(C13H23N3)]V = 1726.26 (6) Å3
Mr = 446.53Z = 4
Monoclinic, P21Mo Kα radiation
a = 9.9680 (2) ŵ = 6.04 mm1
b = 11.5077 (2) ÅT = 150 K
c = 15.4906 (4) Å0.35 × 0.30 × 0.24 mm
β = 103.712 (1)°
Data collection top
Nonius KappaCCD
diffractometer
7418 independent reflections
Absorption correction: multi-scan
(SORTAV; Blessing, 1995)
6981 reflections with I > 2σ(I)
Tmin = 0.131, Tmax = 0.234Rint = 0.064
12530 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.051H-atom parameters constrained
wR(F2) = 0.131Δρmax = 0.91 e Å3
S = 1.06Δρmin = 1.64 e Å3
7418 reflectionsAbsolute structure: Flack (1983); 3292 Friedel pairs
344 parametersAbsolute structure parameter: 0.021 (13)
1 restraint
Special details top

Geometry. 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.

Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Zn1A0.10746 (5)0.63162 (6)0.34857 (4)0.02934 (15)
Br1A0.01456 (6)0.72224 (6)0.20732 (4)0.04120 (16)
Br2A0.07060 (6)0.63257 (6)0.43285 (4)0.04478 (17)
N1A0.2394 (4)0.7659 (4)0.4323 (3)0.0296 (9)
N2A0.3106 (4)0.5837 (4)0.3455 (3)0.0279 (8)
N3A0.1006 (5)0.4383 (5)0.3306 (4)0.0408 (11)
C1A0.3676 (5)0.7783 (5)0.3984 (3)0.0306 (10)
H1AA0.34030.82210.34120.037*
C2A0.4129 (5)0.6591 (5)0.3756 (3)0.0279 (10)
C3A0.5480 (5)0.6280 (5)0.3796 (3)0.0326 (10)
H3AA0.62150.68060.40210.039*
C4A0.5746 (6)0.5185 (6)0.3500 (4)0.0350 (12)
H4AA0.66720.49550.35310.042*
C5A0.4683 (6)0.4430 (6)0.3163 (4)0.0364 (12)
H5AA0.48530.36930.29330.044*
C6A0.3346 (5)0.4782 (5)0.3169 (3)0.0288 (10)
C7A0.2091 (6)0.4037 (6)0.2825 (4)0.0412 (14)
H7AA0.23390.32020.29500.049*
C8A0.1649 (7)0.8779 (6)0.4263 (5)0.0436 (14)
H8AA0.22390.93580.46340.065*
H8AB0.08020.86760.44710.065*
H8AC0.14130.90440.36450.065*
C9A0.2725 (6)0.7248 (7)0.5252 (4)0.0433 (14)
H9AA0.33040.78240.56330.065*
H9AB0.32220.65080.52930.065*
H9AC0.18680.71380.54480.065*
C10A0.4842 (6)0.8475 (6)0.4581 (4)0.0428 (14)
H10A0.44940.92370.47080.064*
H10B0.55940.85790.42800.064*
H10C0.51860.80530.51390.064*
C11A0.1618 (8)0.4226 (8)0.1811 (5)0.059 (2)
H11A0.23560.39880.15290.088*
H11B0.14070.50500.16880.088*
H11C0.07900.37600.15720.088*
C12A0.1414 (8)0.3859 (8)0.4199 (6)0.063 (2)
H12A0.13940.30110.41460.095*
H12B0.07700.41070.45520.095*
H12C0.23500.41130.44920.095*
C13A0.0395 (7)0.3935 (8)0.2854 (8)0.080 (3)
H13A0.03570.30880.27950.120*
H13B0.06890.42870.22630.120*
H13C0.10560.41360.32080.120*
Zn1B0.46597 (6)0.08880 (6)0.16004 (4)0.03171 (16)
Br1B0.40421 (6)0.10618 (5)0.30084 (4)0.03968 (16)
Br2B0.48588 (7)0.28215 (6)0.09799 (4)0.04563 (17)
N1B0.2658 (5)0.0407 (5)0.0663 (3)0.0349 (10)
N2B0.4752 (5)0.0928 (4)0.1491 (3)0.0322 (9)
N3B0.6917 (5)0.0456 (5)0.1721 (3)0.0370 (10)
C1B0.2287 (5)0.0774 (6)0.0917 (4)0.0336 (11)
H1BA0.18920.06760.14490.040*
C2B0.3572 (6)0.1511 (5)0.1211 (3)0.0315 (11)
C3B0.3569 (6)0.2715 (6)0.1221 (3)0.0357 (11)
H3BA0.27300.31320.10240.043*
C4B0.4806 (7)0.3302 (6)0.1524 (4)0.0391 (12)
H4BA0.48220.41270.15320.047*
C5B0.6025 (6)0.2677 (5)0.1815 (4)0.0369 (11)
H5BA0.68830.30630.20240.044*
C6B0.5951 (6)0.1472 (5)0.1792 (4)0.0323 (11)
C7B0.7193 (6)0.0704 (5)0.2124 (4)0.0377 (12)
H7BA0.80050.10510.19430.045*
C8B0.1588 (7)0.1260 (7)0.0706 (5)0.0489 (15)
H8BA0.07210.10360.02930.073*
H8BB0.18730.20280.05420.073*
H8BC0.14520.12880.13120.073*
C9B0.2938 (7)0.0430 (7)0.0233 (4)0.0465 (14)
H9BA0.20950.02250.06770.070*
H9BB0.36670.01320.02590.070*
H9BC0.32370.12110.03570.070*
C10B0.1171 (7)0.1370 (7)0.0203 (5)0.0523 (17)
H10D0.03640.08590.00360.078*
H10E0.09010.21020.04380.078*
H10F0.15340.15290.03200.078*
C11B0.7505 (7)0.0655 (6)0.3156 (4)0.0451 (14)
H11D0.83130.01610.33810.068*
H11E0.76940.14410.33980.068*
H11F0.67060.03330.33400.068*
C12B0.7049 (7)0.0362 (7)0.0761 (5)0.0480 (15)
H12D0.80060.01750.07550.072*
H12E0.67910.11040.04560.072*
H12F0.64360.02520.04550.072*
C13B0.7874 (7)0.1340 (7)0.2166 (5)0.0507 (16)
H13D0.88230.10910.21920.076*
H13E0.77560.14520.27710.076*
H13F0.76890.20720.18370.076*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Zn1A0.0165 (2)0.0351 (3)0.0365 (3)0.0002 (2)0.0066 (2)0.0004 (2)
Br1A0.0310 (3)0.0512 (4)0.0404 (3)0.0109 (2)0.0063 (2)0.0049 (2)
Br2A0.0252 (2)0.0551 (4)0.0593 (4)0.0052 (2)0.0205 (2)0.0018 (3)
N1A0.0207 (19)0.036 (2)0.034 (2)0.0004 (16)0.0103 (16)0.0060 (17)
N2A0.0164 (17)0.035 (2)0.0325 (19)0.0017 (16)0.0055 (14)0.0016 (17)
N3A0.020 (2)0.038 (3)0.064 (3)0.0025 (18)0.010 (2)0.002 (2)
C1A0.023 (2)0.036 (3)0.034 (2)0.003 (2)0.0086 (19)0.005 (2)
C2A0.017 (2)0.039 (3)0.029 (2)0.0009 (18)0.0075 (16)0.002 (2)
C3A0.019 (2)0.044 (3)0.036 (2)0.000 (2)0.0080 (17)0.007 (2)
C4A0.021 (2)0.048 (3)0.038 (3)0.004 (2)0.0108 (19)0.007 (2)
C5A0.026 (2)0.047 (3)0.037 (3)0.011 (2)0.010 (2)0.003 (2)
C6A0.020 (2)0.031 (3)0.035 (2)0.0055 (18)0.0064 (18)0.001 (2)
C7A0.026 (3)0.035 (3)0.058 (4)0.005 (2)0.001 (2)0.012 (3)
C8A0.037 (3)0.040 (3)0.056 (4)0.002 (3)0.015 (3)0.011 (3)
C9A0.034 (3)0.067 (4)0.032 (3)0.015 (3)0.015 (2)0.006 (3)
C10A0.029 (3)0.050 (4)0.050 (3)0.012 (2)0.010 (2)0.012 (3)
C11A0.042 (3)0.074 (5)0.051 (4)0.015 (3)0.007 (3)0.022 (4)
C12A0.042 (4)0.059 (5)0.095 (6)0.011 (3)0.028 (4)0.036 (4)
C13A0.022 (3)0.058 (5)0.150 (9)0.014 (3)0.003 (4)0.038 (5)
Zn1B0.0298 (3)0.0307 (3)0.0364 (3)0.0015 (2)0.0114 (2)0.0000 (2)
Br1B0.0444 (3)0.0414 (3)0.0361 (3)0.0076 (2)0.0152 (2)0.0001 (2)
Br2B0.0551 (4)0.0352 (3)0.0513 (3)0.0008 (3)0.0221 (3)0.0061 (2)
N1B0.031 (2)0.039 (2)0.035 (2)0.0029 (19)0.0061 (18)0.0015 (19)
N2B0.029 (2)0.035 (2)0.035 (2)0.0039 (18)0.0125 (18)0.0042 (18)
N3B0.028 (2)0.038 (3)0.046 (3)0.0029 (19)0.0108 (19)0.004 (2)
C1B0.024 (2)0.046 (3)0.030 (2)0.001 (2)0.0047 (18)0.000 (2)
C2B0.035 (3)0.037 (3)0.025 (2)0.002 (2)0.0109 (19)0.0000 (19)
C3B0.039 (3)0.040 (3)0.029 (2)0.012 (2)0.011 (2)0.003 (2)
C4B0.050 (3)0.032 (3)0.038 (3)0.007 (2)0.017 (2)0.001 (2)
C5B0.042 (3)0.031 (3)0.042 (3)0.004 (2)0.018 (2)0.004 (2)
C6B0.032 (3)0.030 (3)0.036 (3)0.003 (2)0.013 (2)0.003 (2)
C7B0.028 (2)0.039 (3)0.048 (3)0.006 (2)0.012 (2)0.000 (2)
C8B0.036 (3)0.058 (4)0.052 (3)0.014 (3)0.009 (2)0.004 (3)
C9B0.045 (3)0.056 (4)0.038 (3)0.001 (3)0.009 (3)0.004 (3)
C10B0.037 (3)0.057 (4)0.053 (4)0.010 (3)0.008 (3)0.007 (3)
C11B0.037 (3)0.051 (4)0.043 (3)0.000 (3)0.003 (2)0.006 (3)
C12B0.042 (3)0.059 (4)0.051 (3)0.005 (3)0.026 (3)0.001 (3)
C13B0.034 (3)0.050 (4)0.065 (4)0.012 (3)0.006 (3)0.001 (3)
Geometric parameters (Å, º) top
Zn1A—N2A2.110 (4)Zn1B—N2B2.101 (5)
Zn1A—N1A2.234 (4)Zn1B—N1B2.241 (5)
Zn1A—N3A2.241 (6)Zn1B—N3B2.269 (5)
Zn1A—Br1A2.4025 (8)Zn1B—Br1B2.4109 (8)
Zn1A—Br2A2.4401 (8)Zn1B—Br2B2.4504 (9)
N1A—C9A1.477 (7)N1B—C8B1.462 (8)
N1A—C8A1.479 (8)N1B—C9B1.480 (8)
N1A—C1A1.499 (6)N1B—C1B1.486 (8)
N2A—C6A1.334 (7)N2B—C6B1.332 (7)
N2A—C2A1.336 (7)N2B—C2B1.334 (7)
N3A—C12A1.475 (10)N3B—C13B1.452 (8)
N3A—C13A1.498 (8)N3B—C7B1.472 (8)
N3A—C7A1.504 (8)N3B—C12B1.527 (8)
C1A—C2A1.512 (8)C1B—C2B1.514 (8)
C1A—C10A1.526 (7)C1B—C10B1.531 (8)
C1A—H1AA1.0000C1B—H1BA1.0000
C2A—C3A1.381 (7)C2B—C3B1.385 (9)
C3A—C4A1.388 (9)C3B—C4B1.387 (9)
C3A—H3AA0.9500C3B—H3BA0.9500
C4A—C5A1.374 (9)C4B—C5B1.392 (9)
C4A—H4AA0.9500C4B—H4BA0.9500
C5A—C6A1.395 (7)C5B—C6B1.388 (8)
C5A—H5AA0.9500C5B—H5BA0.9500
C6A—C7A1.506 (8)C6B—C7B1.508 (8)
C7A—C11A1.546 (10)C7B—C11B1.556 (9)
C7A—H7AA1.0000C7B—H7BA1.0000
C8A—H8AA0.9800C8B—H8BA0.9800
C8A—H8AB0.9800C8B—H8BB0.9800
C8A—H8AC0.9800C8B—H8BC0.9800
C9A—H9AA0.9800C9B—H9BA0.9800
C9A—H9AB0.9800C9B—H9BB0.9800
C9A—H9AC0.9800C9B—H9BC0.9800
C10A—H10A0.9800C10B—H10D0.9800
C10A—H10B0.9800C10B—H10E0.9800
C10A—H10C0.9800C10B—H10F0.9800
C11A—H11A0.9800C11B—H11D0.9800
C11A—H11B0.9800C11B—H11E0.9800
C11A—H11C0.9800C11B—H11F0.9800
C12A—H12A0.9800C12B—H12D0.9800
C12A—H12B0.9800C12B—H12E0.9800
C12A—H12C0.9800C12B—H12F0.9800
C13A—H13A0.9800C13B—H13D0.9800
C13A—H13B0.9800C13B—H13E0.9800
C13A—H13C0.9800C13B—H13F0.9800
N2A—Zn1A—N1A76.00 (17)N2B—Zn1B—N1B75.61 (19)
N2A—Zn1A—N3A74.85 (18)N2B—Zn1B—N3B74.15 (19)
N1A—Zn1A—N3A139.05 (18)N1B—Zn1B—N3B135.45 (19)
N2A—Zn1A—Br1A104.93 (12)N2B—Zn1B—Br1B100.44 (13)
N1A—Zn1A—Br1A105.97 (13)N1B—Zn1B—Br1B103.14 (13)
N3A—Zn1A—Br1A108.90 (16)N3B—Zn1B—Br1B113.89 (14)
N2A—Zn1A—Br2A146.82 (12)N2B—Zn1B—Br2B149.60 (13)
N1A—Zn1A—Br2A95.11 (11)N1B—Zn1B—Br2B96.46 (14)
N3A—Zn1A—Br2A93.81 (14)N3B—Zn1B—Br2B93.45 (14)
Br1A—Zn1A—Br2A108.25 (3)Br1B—Zn1B—Br2B109.96 (3)
C9A—N1A—C8A109.5 (5)C8B—N1B—C9B109.4 (5)
C9A—N1A—C1A111.1 (4)C8B—N1B—C1B111.8 (5)
C8A—N1A—C1A110.6 (5)C9B—N1B—C1B112.2 (5)
C9A—N1A—Zn1A108.0 (4)C8B—N1B—Zn1B110.6 (4)
C8A—N1A—Zn1A110.4 (3)C9B—N1B—Zn1B105.5 (4)
C1A—N1A—Zn1A107.2 (3)C1B—N1B—Zn1B107.1 (3)
C6A—N2A—C2A121.7 (4)C6B—N2B—C2B121.8 (5)
C6A—N2A—Zn1A119.6 (3)C6B—N2B—Zn1B119.5 (4)
C2A—N2A—Zn1A118.7 (4)C2B—N2B—Zn1B118.3 (4)
C12A—N3A—C13A108.5 (7)C13B—N3B—C7B113.5 (5)
C12A—N3A—C7A106.6 (5)C13B—N3B—C12B108.3 (5)
C13A—N3A—C7A112.2 (6)C7B—N3B—C12B107.4 (5)
C12A—N3A—Zn1A107.2 (5)C13B—N3B—Zn1B114.4 (4)
C13A—N3A—Zn1A113.4 (5)C7B—N3B—Zn1B108.4 (4)
C7A—N3A—Zn1A108.7 (4)C12B—N3B—Zn1B104.4 (4)
N1A—C1A—C2A108.8 (4)N1B—C1B—C2B110.3 (4)
N1A—C1A—C10A115.3 (4)N1B—C1B—C10B113.7 (5)
C2A—C1A—C10A112.8 (5)C2B—C1B—C10B112.6 (5)
N1A—C1A—H1AA106.4N1B—C1B—H1BA106.6
C2A—C1A—H1AA106.4C2B—C1B—H1BA106.6
C10A—C1A—H1AA106.4C10B—C1B—H1BA106.6
N2A—C2A—C3A120.2 (5)N2B—C2B—C3B120.2 (6)
N2A—C2A—C1A115.2 (4)N2B—C2B—C1B115.8 (5)
C3A—C2A—C1A124.6 (5)C3B—C2B—C1B124.0 (5)
C2A—C3A—C4A118.8 (5)C2B—C3B—C4B119.1 (5)
C2A—C3A—H3AA120.6C2B—C3B—H3BA120.4
C4A—C3A—H3AA120.6C4B—C3B—H3BA120.4
C5A—C4A—C3A120.6 (5)C3B—C4B—C5B119.7 (6)
C5A—C4A—H4AA119.7C3B—C4B—H4BA120.1
C3A—C4A—H4AA119.7C5B—C4B—H4BA120.1
C4A—C5A—C6A117.7 (6)C6B—C5B—C4B118.1 (6)
C4A—C5A—H5AA121.1C6B—C5B—H5BA120.9
C6A—C5A—H5AA121.1C4B—C5B—H5BA120.9
N2A—C6A—C5A120.9 (5)N2B—C6B—C5B121.1 (6)
N2A—C6A—C7A115.8 (4)N2B—C6B—C7B116.1 (5)
C5A—C6A—C7A123.2 (5)C5B—C6B—C7B122.8 (5)
N3A—C7A—C6A108.0 (5)N3B—C7B—C6B109.4 (5)
N3A—C7A—C11A112.6 (5)N3B—C7B—C11B112.0 (5)
C6A—C7A—C11A107.9 (6)C6B—C7B—C11B108.7 (5)
N3A—C7A—H7AA109.4N3B—C7B—H7BA108.9
C6A—C7A—H7AA109.4C6B—C7B—H7BA108.9
C11A—C7A—H7AA109.4C11B—C7B—H7BA108.9
N1A—C8A—H8AA109.5N1B—C8B—H8BA109.5
N1A—C8A—H8AB109.5N1B—C8B—H8BB109.5
H8AA—C8A—H8AB109.5H8BA—C8B—H8BB109.5
N1A—C8A—H8AC109.5N1B—C8B—H8BC109.5
H8AA—C8A—H8AC109.5H8BA—C8B—H8BC109.5
H8AB—C8A—H8AC109.5H8BB—C8B—H8BC109.5
N1A—C9A—H9AA109.5N1B—C9B—H9BA109.5
N1A—C9A—H9AB109.5N1B—C9B—H9BB109.5
H9AA—C9A—H9AB109.5H9BA—C9B—H9BB109.5
N1A—C9A—H9AC109.5N1B—C9B—H9BC109.5
H9AA—C9A—H9AC109.5H9BA—C9B—H9BC109.5
H9AB—C9A—H9AC109.5H9BB—C9B—H9BC109.5
C1A—C10A—H10A109.5C1B—C10B—H10D109.5
C1A—C10A—H10B109.5C1B—C10B—H10E109.5
H10A—C10A—H10B109.5H10D—C10B—H10E109.5
C1A—C10A—H10C109.5C1B—C10B—H10F109.5
H10A—C10A—H10C109.5H10D—C10B—H10F109.5
H10B—C10A—H10C109.5H10E—C10B—H10F109.5
C7A—C11A—H11A109.5C7B—C11B—H11D109.5
C7A—C11A—H11B109.5C7B—C11B—H11E109.5
H11A—C11A—H11B109.5H11D—C11B—H11E109.5
C7A—C11A—H11C109.5C7B—C11B—H11F109.5
H11A—C11A—H11C109.5H11D—C11B—H11F109.5
H11B—C11A—H11C109.5H11E—C11B—H11F109.5
N3A—C12A—H12A109.5N3B—C12B—H12D109.5
N3A—C12A—H12B109.5N3B—C12B—H12E109.5
H12A—C12A—H12B109.5H12D—C12B—H12E109.5
N3A—C12A—H12C109.5N3B—C12B—H12F109.5
H12A—C12A—H12C109.5H12D—C12B—H12F109.5
H12B—C12A—H12C109.5H12E—C12B—H12F109.5
N3A—C13A—H13A109.5N3B—C13B—H13D109.5
N3A—C13A—H13B109.5N3B—C13B—H13E109.5
H13A—C13A—H13B109.5H13D—C13B—H13E109.5
N3A—C13A—H13C109.5N3B—C13B—H13F109.5
H13A—C13A—H13C109.5H13D—C13B—H13F109.5
H13B—C13A—H13C109.5H13E—C13B—H13F109.5

Experimental details

Crystal data
Chemical formula[ZnBr2(C13H23N3)]
Mr446.53
Crystal system, space groupMonoclinic, P21
Temperature (K)150
a, b, c (Å)9.9680 (2), 11.5077 (2), 15.4906 (4)
β (°) 103.712 (1)
V3)1726.26 (6)
Z4
Radiation typeMo Kα
µ (mm1)6.04
Crystal size (mm)0.35 × 0.30 × 0.24
Data collection
DiffractometerNonius KappaCCD
diffractometer
Absorption correctionMulti-scan
(SORTAV; Blessing, 1995)
Tmin, Tmax0.131, 0.234
No. of measured, independent and
observed [I > 2σ(I)] reflections
12530, 7418, 6981
Rint0.064
(sin θ/λ)max1)0.651
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.051, 0.131, 1.06
No. of reflections7418
No. of parameters344
No. of restraints1
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.91, 1.64
Absolute structureFlack (1983); 3292 Friedel pairs
Absolute structure parameter0.021 (13)

Computer programs: COLLECT (Nonius, 1997-2002), DENZO-SMN (Otwinowski & Minor, 1997), DENZO-SMN, SHELXTL (Sheldrick, 2001), SHELXTL, SHELXT.

Selected geometric parameters (Å, º) top
Zn1A—N2A2.110 (4)Zn1B—N2B2.101 (5)
Zn1A—N1A2.234 (4)Zn1B—N1B2.241 (5)
Zn1A—N3A2.241 (6)Zn1B—N3B2.269 (5)
Zn1A—Br1A2.4025 (8)Zn1B—Br1B2.4109 (8)
Zn1A—Br2A2.4401 (8)Zn1B—Br2B2.4504 (9)
N2A—Zn1A—N1A76.00 (17)N2B—Zn1B—N1B75.61 (19)
N2A—Zn1A—N3A74.85 (18)N2B—Zn1B—N3B74.15 (19)
N1A—Zn1A—N3A139.05 (18)N1B—Zn1B—N3B135.45 (19)
N2A—Zn1A—Br1A104.93 (12)N2B—Zn1B—Br1B100.44 (13)
N1A—Zn1A—Br1A105.97 (13)N1B—Zn1B—Br1B103.14 (13)
N3A—Zn1A—Br1A108.90 (16)N3B—Zn1B—Br1B113.89 (14)
N2A—Zn1A—Br2A146.82 (12)N2B—Zn1B—Br2B149.60 (13)
N1A—Zn1A—Br2A95.11 (11)N1B—Zn1B—Br2B96.46 (14)
N3A—Zn1A—Br2A93.81 (14)N3B—Zn1B—Br2B93.45 (14)
Br1A—Zn1A—Br2A108.25 (3)Br1B—Zn1B—Br2B109.96 (3)
 

Subscribe to Acta Crystallographica Section E: Crystallographic Communications

The full text of this article is available to subscribers to the journal.

If you have already registered and are using a computer listed in your registration details, please email support@iucr.org for assistance.

Buy online

You may purchase this article in PDF and/or HTML formats. For purchasers in the European Community who do not have a VAT number, VAT will be added at the local rate. Payments to the IUCr are handled by WorldPay, who will accept payment by credit card in several currencies. To purchase the article, please complete the form below (fields marked * are required), and then click on `Continue'.
E-mail address* 
Repeat e-mail address* 
(for error checking) 

Format*   PDF (US $40)
   HTML (US $40)
   PDF+HTML (US $50)
In order for VAT to be shown for your country javascript needs to be enabled.

VAT number 
(non-UK EC countries only) 
Country* 
 

Terms and conditions of use
Contact us

Follow Acta Cryst. E
Sign up for e-alerts
Follow Acta Cryst. on Twitter
Follow us on facebook
Sign up for RSS feeds