Literature DB >> 21583352

Di-μ-chlorido-bis-({2-[(4-bromo-phen-yl)-imino-meth-yl]pyridine-κN,N'}-chloridomercury(II)).

Ali Mahmoudi, Saeed Dehghanpour, Mehdi Khalaj, Shabnam Pakravan.   

Abstract

The unique Hg(II) ion in the title centrosymmetric dinuclear complex, [Hg(2)Cl(4)(C(12)H(9)BrN(2))(2)], is in a distorted trigonal-bipyramidal coordination environment formed by the bis-chelating N-heterocyclic ligand, two bridging Cl atoms and one terminal Cl atom. One of the bridging Hg-Cl bonds is significantly longer than the other.

Entities:  

Year:  2009        PMID: 21583352      PMCID: PMC2977257          DOI: 10.1107/S1600536809025641

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

For background information on diimine complexes, see: Dehghanpour & Mahmoudi (2007 ▶); Dehghanpour, Mahmoudi, Khalaj & Salmanpour (2007 ▶). For related crystal structures, see: Mahmoudi et al. (2009 ▶); Dehghanpour, Mahmoudi, Khalaj, Salmanpour & Adib (2007 ▶).

Experimental

Crystal data

[Hg2Cl4(C12H9BrN2)2] M = 1065.22 Monoclinic, a = 7.6697 (2) Å b = 15.0247 (4) Å c = 12.2129 (4) Å β = 96.738 (1)° V = 1397.63 (7) Å3 Z = 2 Mo Kα radiation μ = 14.24 mm−1 T = 100 K 0.10 × 0.10 × 0.05 mm

Data collection

Bruker SMART APEXII CCD area-detector diffractometer Absorption correction: multi-scan (APEX2; Bruker, 2005 ▶) T min = 0.280, T max = 0.491 17922 measured reflections 4047 independent reflections 3636 reflections with I > 2σ(I) R int = 0.032

Refinement

R[F 2 > 2σ(F 2)] = 0.019 wR(F 2) = 0.041 S = 1.01 4047 reflections 163 parameters H-atom parameters constrained Δρmax = 0.97 e Å−3 Δρmin = −1.15 e Å−3 Data collection: APEX2 (Bruker, 2005 ▶); cell refinement: APEX2; data reduction: APEX2; program(s) used to solve structure: SHELXTL (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXTL; molecular graphics: PLATON (Spek, 2009 ▶); software used to prepare material for publication: SHELXTL. Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536809025641/lh2844sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536809025641/lh2844Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
[Hg2Cl4(C12H9BrN2)2]F(000) = 976
Mr = 1065.22Dx = 2.531 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 8129 reflections
a = 7.6697 (2) Åθ = 2.2–29.7°
b = 15.0247 (4) ŵ = 14.24 mm1
c = 12.2129 (4) ÅT = 100 K
β = 96.738 (1)°Prism, yellow
V = 1397.63 (7) Å30.10 × 0.10 × 0.05 mm
Z = 2
Bruker SMART APEXII CCD area-detector diffractometer4047 independent reflections
Radiation source: fine-focus sealed tube3636 reflections with I > 2σ(I)
graphiteRint = 0.032
Detector resolution: 0 pixels mm-1θmax = 30.0°, θmin = 2.2°
φ and ω scansh = −10→10
Absorption correction: multi-scan (APEX2; Bruker, 2005)k = −21→20
Tmin = 0.280, Tmax = 0.491l = −17→17
17922 measured reflections
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.019Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.041H-atom parameters constrained
S = 1.01w = 1/[σ2(Fo2) + (0.015P)2 + 1.35P] where P = (Fo2 + 2Fc2)/3
4047 reflections(Δ/σ)max = 0.001
163 parametersΔρmax = 0.97 e Å3
0 restraintsΔρmin = −1.15 e Å3
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.
xyzUiso*/Ueq
Hg10.170956 (13)0.446982 (7)0.108289 (9)0.02080 (3)
Br10.86964 (5)0.10383 (2)−0.01114 (3)0.04340 (9)
Cl10.42148 (9)0.53787 (4)0.15929 (7)0.03126 (16)
Cl20.04621 (9)0.39647 (4)−0.07921 (5)0.02143 (12)
N10.2551 (3)0.29234 (14)0.15931 (18)0.0183 (4)
N2−0.0272 (3)0.38863 (15)0.21855 (18)0.0192 (4)
C1−0.0010 (3)0.30362 (17)0.2535 (2)0.0192 (5)
C2−0.1169 (4)0.26078 (18)0.3146 (2)0.0207 (5)
H2A−0.09740.20060.33660.025*
C3−0.2618 (4)0.30668 (18)0.3433 (2)0.0219 (5)
H3A−0.34200.27880.38610.026*
C4−0.2871 (4)0.39390 (18)0.3083 (2)0.0218 (5)
H4A−0.38420.42720.32750.026*
C5−0.1679 (4)0.43198 (18)0.2445 (2)0.0209 (5)
H5A−0.18780.49110.21840.025*
C60.1522 (4)0.25556 (18)0.2214 (2)0.0212 (5)
H6A0.17520.19650.24710.025*
C70.3966 (3)0.24488 (18)0.1221 (2)0.0194 (5)
C80.4078 (4)0.15213 (19)0.1228 (2)0.0239 (5)
H8A0.31930.11750.15080.029*
C90.5489 (4)0.1107 (2)0.0824 (2)0.0270 (6)
H9A0.55720.04760.08200.032*
C100.6778 (4)0.1622 (2)0.0425 (2)0.0260 (6)
C110.6691 (4)0.25420 (19)0.0398 (2)0.0230 (5)
H11A0.75870.28840.01220.028*
C120.5255 (3)0.29538 (18)0.0786 (2)0.0206 (5)
H12A0.51510.35840.07560.025*
U11U22U33U12U13U23
Hg10.02163 (5)0.01490 (5)0.02590 (6)−0.00157 (4)0.00290 (4)0.00198 (4)
Br10.04489 (19)0.03626 (17)0.0548 (2)0.01823 (15)0.03004 (17)0.01083 (16)
Cl10.0233 (3)0.0157 (3)0.0531 (5)−0.0016 (2)−0.0027 (3)−0.0017 (3)
Cl20.0274 (3)0.0159 (3)0.0210 (3)0.0040 (2)0.0029 (2)0.0000 (2)
N10.0210 (10)0.0147 (10)0.0187 (10)0.0018 (8)0.0009 (8)−0.0002 (8)
N20.0221 (10)0.0163 (10)0.0194 (10)−0.0008 (8)0.0028 (8)0.0005 (8)
C10.0227 (12)0.0171 (12)0.0179 (12)0.0002 (9)0.0025 (10)0.0003 (9)
C20.0278 (13)0.0152 (12)0.0189 (12)−0.0014 (10)0.0027 (10)0.0027 (9)
C30.0248 (13)0.0226 (13)0.0188 (12)−0.0017 (10)0.0043 (10)0.0028 (10)
C40.0234 (12)0.0201 (12)0.0221 (13)0.0042 (10)0.0034 (10)0.0019 (10)
C50.0256 (13)0.0170 (12)0.0203 (12)0.0028 (10)0.0030 (10)0.0031 (10)
C60.0271 (13)0.0162 (12)0.0202 (12)0.0018 (10)0.0030 (10)0.0014 (10)
C70.0201 (11)0.0202 (12)0.0175 (12)0.0025 (10)0.0004 (9)0.0005 (10)
C80.0281 (13)0.0203 (13)0.0244 (13)0.0015 (11)0.0071 (11)0.0030 (11)
C90.0365 (15)0.0199 (13)0.0258 (14)0.0089 (11)0.0086 (12)0.0027 (11)
C100.0283 (13)0.0273 (14)0.0236 (13)0.0088 (11)0.0077 (11)0.0036 (11)
C110.0231 (12)0.0252 (13)0.0209 (12)0.0008 (11)0.0038 (10)0.0014 (11)
C120.0225 (12)0.0204 (12)0.0187 (12)0.0003 (10)0.0017 (10)0.0011 (10)
Hg1—N22.318 (2)C3—H3A0.9500
Hg1—Cl12.3799 (7)C4—C51.392 (4)
Hg1—N12.472 (2)C4—H4A0.9500
Hg1—Cl22.4941 (7)C5—H5A0.9500
Hg1—Cl2i2.8799 (6)C6—H6A0.9500
Br1—C101.894 (3)C7—C81.396 (4)
Cl2—Hg1i2.8799 (6)C7—C121.399 (4)
N1—C61.282 (3)C8—C91.389 (4)
N1—C71.418 (3)C8—H8A0.9500
N2—C51.330 (3)C9—C101.388 (4)
N2—C11.354 (3)C9—H9A0.9500
C1—C21.384 (4)C10—C111.385 (4)
C1—C61.471 (4)C11—C121.394 (4)
C2—C31.387 (4)C11—H11A0.9500
C2—H2A0.9500C12—H12A0.9500
C3—C41.385 (4)
N2—Hg1—Cl1129.00 (6)C3—C4—H4A120.5
N2—Hg1—N170.58 (7)C5—C4—H4A120.5
Cl1—Hg1—N1107.12 (5)N2—C5—C4122.4 (2)
N2—Hg1—Cl2102.20 (6)N2—C5—H5A118.8
Cl1—Hg1—Cl2128.74 (3)C4—C5—H5A118.8
N1—Hg1—Cl290.35 (5)N1—C6—C1120.8 (2)
N2—Hg1—Cl2i88.36 (6)N1—C6—H6A119.6
Cl1—Hg1—Cl2i90.07 (2)C1—C6—H6A119.6
N1—Hg1—Cl2i158.28 (5)C8—C7—C12119.9 (2)
Cl2—Hg1—Cl2i88.926 (19)C8—C7—N1123.3 (2)
Hg1—Cl2—Hg1i91.074 (19)C12—C7—N1116.8 (2)
C6—N1—C7121.4 (2)C9—C8—C7119.7 (3)
C6—N1—Hg1113.18 (17)C9—C8—H8A120.2
C7—N1—Hg1125.39 (17)C7—C8—H8A120.2
C5—N2—C1118.8 (2)C10—C9—C8119.4 (3)
C5—N2—Hg1123.96 (18)C10—C9—H9A120.3
C1—N2—Hg1117.19 (17)C8—C9—H9A120.3
N2—C1—C2121.8 (2)C11—C10—C9122.1 (3)
N2—C1—C6118.2 (2)C11—C10—Br1119.4 (2)
C2—C1—C6119.9 (2)C9—C10—Br1118.5 (2)
C1—C2—C3119.3 (2)C10—C11—C12118.2 (3)
C1—C2—H2A120.4C10—C11—H11A120.9
C3—C2—H2A120.4C12—C11—H11A120.9
C4—C3—C2118.6 (2)C11—C12—C7120.7 (3)
C4—C3—H3A120.7C11—C12—H12A119.7
C2—C3—H3A120.7C7—C12—H12A119.7
C3—C4—C5119.0 (2)
N2—Hg1—Cl2—Hg1i88.09 (6)C6—C1—C2—C3−179.4 (2)
Cl1—Hg1—Cl2—Hg1i−89.22 (3)C1—C2—C3—C40.9 (4)
N1—Hg1—Cl2—Hg1i158.29 (5)C2—C3—C4—C50.8 (4)
Cl2i—Hg1—Cl2—Hg1i0.0C1—N2—C5—C41.5 (4)
N2—Hg1—N1—C6−0.60 (18)Hg1—N2—C5—C4178.0 (2)
Cl1—Hg1—N1—C6125.53 (18)C3—C4—C5—N2−2.1 (4)
Cl2—Hg1—N1—C6−103.42 (18)C7—N1—C6—C1−175.9 (2)
Cl2i—Hg1—N1—C6−15.4 (3)Hg1—N1—C6—C11.6 (3)
N2—Hg1—N1—C7176.8 (2)N2—C1—C6—N1−2.1 (4)
Cl1—Hg1—N1—C7−57.1 (2)C2—C1—C6—N1175.8 (3)
Cl2—Hg1—N1—C773.94 (19)C6—N1—C7—C818.2 (4)
Cl2i—Hg1—N1—C7161.92 (14)Hg1—N1—C7—C8−159.0 (2)
Cl1—Hg1—N2—C586.3 (2)C6—N1—C7—C12−164.6 (2)
N1—Hg1—N2—C5−177.1 (2)Hg1—N1—C7—C1218.3 (3)
Cl2—Hg1—N2—C5−91.0 (2)C12—C7—C8—C91.3 (4)
Cl2i—Hg1—N2—C5−2.5 (2)N1—C7—C8—C9178.5 (3)
Cl1—Hg1—N2—C1−97.14 (19)C7—C8—C9—C100.5 (4)
N1—Hg1—N2—C1−0.46 (18)C8—C9—C10—C11−1.1 (5)
Cl2—Hg1—N2—C185.56 (18)C8—C9—C10—Br1179.6 (2)
Cl2i—Hg1—N2—C1174.10 (18)C9—C10—C11—C120.0 (4)
C5—N2—C1—C20.4 (4)Br1—C10—C11—C12179.3 (2)
Hg1—N2—C1—C2−176.4 (2)C10—C11—C12—C71.8 (4)
C5—N2—C1—C6178.2 (2)C8—C7—C12—C11−2.5 (4)
Hg1—N2—C1—C61.4 (3)N1—C7—C12—C11−179.8 (2)
N2—C1—C2—C3−1.6 (4)
Hg1—N22.318 (2)
Hg1—Cl12.3799 (7)
Hg1—N12.472 (2)
Hg1—Cl22.4941 (7)
Hg1—Cl2i2.8799 (6)
N2—Hg1—Cl1129.00 (6)
N2—Hg1—N170.58 (7)
Cl1—Hg1—N1107.12 (5)
N2—Hg1—Cl2102.20 (6)
Cl1—Hg1—Cl2128.74 (3)
N1—Hg1—Cl290.35 (5)
N2—Hg1—Cl2i88.36 (6)
Cl1—Hg1—Cl2i90.07 (2)
N1—Hg1—Cl2i158.28 (5)
Cl2—Hg1—Cl2i88.926 (19)
Hg1—Cl2—Hg1i91.074 (19)

Symmetry code: (i) .

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