Literature DB >> 28638648

An infinite two-dimensional hybrid water-chloride network in a 4'-(furan-2-yl)-2,2':6',2''-terpyridine nickel(II) matrix.

Wei-Wei Fu1, Ya-Qian Li1, Yang Liu1, Man-Sheng Chen1, Wei Li1, Ying-Qun Yang1.   

Abstract

A new complex, namely bis-[4'-(furan-2-yl)-2,2':6',2''-terpyridine]-nickel(II) dichloride deca-hydrate, [Ni(C19H13N3O)2]Cl2·10H2O, has been crystallized by solvent evaporation and characterized by single-crystal X-ray diffraction. The coordination environment of the NiII cation is distorted octa-hedral with slight deviations from an idealized geometry. The most intriguing structural feature is an infinite two-dimensional hybrid water-chloride network parallel to (011) constructed by O-H⋯O and O-H⋯Cl hydrogen bonds involving two independent chloride ions and ten independent solvent water mol-ecules with an l-shaped pattern. One of the furyl rings is disordered with a refined occupancy ratio of 0.786 (13):0.214 (13).

Entities:  

Keywords:  NiII; crystal structure; hydrogen bonds; terpyridine; water cluster; water–chloride network

Year:  2017        PMID: 28638648      PMCID: PMC5458313          DOI: 10.1107/S2056989017007095

Source DB:  PubMed          Journal:  Acta Crystallogr E Crystallogr Commun


Chemical context

Water has received much scientific inter­est as it is a major chemical constituent on the earth’s surface and it is also the source of life. Many discrete water clusters and polymeric water aggregates, with different types of hydrogen bonds and in diverse sizes and shapes, captured in the crystal lattice of an organic or metal coordination complex during crystallization have been found and investigated experimentally and theoretically (Dutta et al., 2015 ▸; Ganguly & Mondal, 2015 ▸; Han et al., 2014 ▸; Hundal et al., 2014 ▸; Pati et al., 2014 ▸). Hybrid waterchloride associates incorporated in various crystal matrixes are one of the most inter­esting combinations in water clusters research due to their fundamental importance for understanding waterhalide inter­actions in the atmosphere, the ocean and in biological systems (Inumaru et al., 2008 ▸; Kumar et al., 2011 ▸; Lakshminarayanan et al., 2006 ▸; Li et al., 2008 ▸). According to a search of the Cambridge Structural Database (CSD Version 5.37, May 2016; Groom et al., 2016 ▸), there are about nine examples with waterchloride hydrogen bonds forming one-dimensional tapes (Boyer et al., 2011 ▸; van Holst et al., 2008 ▸; Kepert et al., 1999 ▸; Jitsukawa et al., 1994 ▸), two-dimensional (Kepert et al., 1994 ▸; Chowdhury et al., 2011 ▸; Duan et al., 2016 ▸) and three-dimensional (Figgis et al., 1983 ▸; Pruchnik et al., 1996 ▸) networks from 2,2′:6′,2′′-terpyridine ligands. When 4′-substituted terpyridines with phenyl, pyridyl, imidazolyl rings were considered, two-dimensional and three-dimensional waterchloride networks with two chloride ions and at least six water mol­ecules were found (Constable et al., 1990 ▸; Kou et al., 2008 ▸; Chen et al., 2013 ▸; Fernandes et al., 2008 ▸; McMurtrie & Dance, 2010 ▸; Padhi et al., 2010 ▸; Indumathy et al., 2008 ▸; Mahendiran et al., 2016 ▸). The hydro­phobic and hydro­philic layers are further linked by two kinds of C—H⋯O hydrogen bonds into three-dimensional networks. In this context, a ftpy–NiII complex [ftpy = 4′-(furan-2-yl)-2,2′:6′,2′′-terpyridine] (Fig. 1 ▸) with two chlorides as counter-ions and ten solvent water mol­ecules (1) is described herein.
Figure 1

The mol­ecular structure of [Ni(ftpy)2]2+ in 1, with displacement ellipsoids drawn at the 30% probability level.

Structural commentary

The asymmetric unit of 1 is composed of a cationic [Ni(ftpy)2]2+ part, two chloride anions, and ten water mol­ecules of crystallization. The distances between Ni1 and the N atoms of the central pyridyl rings [1.974 (3) and 1.977 (3) Å] are slightly shorter than those between Ni1 and the N atoms of outer pyridyl rings [2.093 (3) −2.099 (3) Å; Table 1 ▸]. The angles involving Ni1 can be divided into two sets, viz. three transoid angles [178.36 (10), 155.38 (11) and 155.89 (11)°] and 12 cisoid angles, which range from 77.74 (11) to 103.80 (10)°. The differences in the bond lengths and angles indicate a distorted octa­hedral geometry (Constable et al., 1990 ▸; Logacheva et al., 2009 ▸; Padhi et al., 2010 ▸; Fu et al., 2013 ▸). The terpyridyl ring systems [maximum deviations of ±0.058 (4) Å for C27/C31 and 0.192 (4) Å for C17] are almost perpendicular to each other, subtending a dihedral angle of 87.35 (6)°. The furyl rings are almost coplanar with the terpyridyl ring systems, making dihedral angles of 8.1 (2) and 3.2 (3)° for the O1- and O2-containing rings, respectively.
Table 1

Selected geometric parameters (Å, °)

Ni1—N51.974 (3)Ni1—N32.096 (3)
Ni1—N21.977 (3)Ni1—N12.098 (3)
Ni1—N62.093 (3)Ni1—N42.099 (3)
    
N5—Ni1—N2178.36 (10)N2—Ni1—N177.77 (11)
N5—Ni1—N677.81 (11)N6—Ni1—N193.13 (11)
N2—Ni1—N6102.65 (11)N3—Ni1—N1155.38 (11)
N5—Ni1—N3100.71 (11)N5—Ni1—N478.10 (11)
N2—Ni1—N377.74 (11)N2—Ni1—N4101.46 (12)
N6—Ni1—N389.84 (11)N6—Ni1—N4155.89 (11)
N5—Ni1—N1103.80 (10)N3—Ni1—N495.46 (11)

Supra­molecular features

In the crystal, there are hydro­phobic layers composed of [Ni(ftpy)2]2+ dications and hydro­philic layers composed of water mol­ecules and chloride anions (Fig. 2 ▸). In the hydro­phobic layers, shown in Fig. 3 ▸, [Ni(ftpy)2]2+ dications are linked by two kinds of face-to-face π–π inter­actions with centroid–centroid distances of 3.530 (4) and 3.760 (4) Å between the furyl and outer pyridyl rings, forming one-dimensional (1D) chains. These 1D chains are linked by further π–π inter­actions with centroid distances of 4.367 (4) Å between furyl rings and 4.405 (4) Å between furyl and central pyridyl rings, forming two-dimensional networks. The water mol­ecules and chloride anions form a two-dimensional network parallel to (011) via O—H⋯O and O—H⋯Cl hydrogen bonds (Table 2 ▸), as shown in Fig. 4 ▸.
Figure 2

View of the hydro­phobic (represented by wireframes) and hydro­philic (represented by spheres) layers in 1.

Figure 3

A view of the two-dimensional undulating sheet of hydro­phobic layers, with π–π inter­actions highlighted by dashed lines [purple for 3.533 (5) and 3.761 (4) Å, and green for 4.338 (14) and 4.405 (4) Å].

Table 2

Hydrogen-bond geometry (Å, °)

D—H⋯A D—HH⋯A DA D—H⋯A
O1W—H1WA⋯Cl10.872.253.113 (4)169
O1W—H1WB⋯O9W i 0.872.062.923 (6)175
O2W—H2WB⋯O5W ii 0.831.992.813 (7)172
O2W—H2WA⋯Cl10.842.393.215 (4)168
O3W—H3WC⋯O4W 0.862.052.760 (9)140
O3W—H3WA⋯O6W iii 0.882.353.134 (7)148
O4W—H4WB⋯Cl20.882.583.107 (5)119
O4W—H4WA⋯Cl20.872.563.107 (5)122
O5W—H5WA⋯Cl20.872.373.079 (4)138
O5W—H5WB⋯O9W 0.892.162.991 (6)156
O6W—H6WC⋯O2W ii 0.832.112.929 (6)167
O6W—H6WA⋯O7W 0.832.182.838 (6)136
O7W—H7WA⋯Cl20.872.343.190 (4)167
O7W—H7WB⋯O4W ii 0.871.932.798 (5)172
O8W—H8WC⋯O3W ii 0.852.062.856 (8)155
O8W—H8WD⋯Cl2iv 0.852.403.204 (6)157
O9W—H9WA⋯O10W v 0.861.932.756 (6)159
O9W—H9WB⋯O1W vi 0.862.112.878 (5)147
O10W—H10A⋯Cl1vii 0.882.273.141 (4)171
O10W—H10B⋯Cl1viii 0.872.383.225 (4)165

Symmetry codes: (i) ; (ii) ; (iii) ; (iv) ; (v) ; (vi) ; (vii) ; (viii) .

Figure 4

A view of the hybrid water–chloride hydrogen-bonded assemblies in 1, with water mol­ecules and chloride anions shown as coloured balls and hydrogen bonds as dashed lines.

The multicyclic {[(H2O)10Cl2]2−} fragments in the hydro­philic layers are constructed by means of 11 non-equivalent O—H⋯O hydrogen bonds with O⋯O distances ranging from 2.756 (6) to 3.134 (7) Å and nine O—H⋯Cl hydrogen bonds with O⋯Cl distances ranging from 3.079 (4) to 3.225 (4) Å (Table 2 ▸, Fig. 4 ▸). Both the O⋯O and O⋯Cl distances are comparable with those found in various types of water clusters and waterchloride associates (Safin et al., 2015 ▸; Bhat & Revankar, 2016 ▸; Ris et al., 2016 ▸). The resulting two-dimensional network can be considered as a set of alternating cyclic fragments with three tetra­nuclear, three penta­nuclear, one hexa­nuclear and two octa­nuclear fragments, as shown in Fig. 5 ▸ a. Two of these fragments are composed only of water mol­ecules, whereas the other seven rings are waterchloride hybrids with one or two Cl− anions. Most of the rings are non-planar, contributing to the formation of an intricate relief geometry of the waterchloride layer. Using the method described by Infantes and co-workers (Infantes & Motherwell, 2002 ▸; Infantes et al., 2003 ▸), this two-dimensional waterchloride network can be described as having an L4(6)4(6)4(6)5(5)5(6)5(6)6(8)8(8)8(10) pattern.
Figure 5

Multicyclic {[(H2O)10Cl2]2−} fragments with repeating units of two-dimensional water–chloride networks in (a) 1, (b) 2, (c) 3, (d) 4 and (e) 5.

Comparison with other terpyridine complexes possessing 10 solvent water mol­ecules

It is inter­esting to make a comparison of the two-dimensional waterchloride networks in 1 and those found in other terpyridine complexes possessing 10 solvent water mol­ecules, viz. [Fe(phtpy)2]Cl2·10H2O (2; refcode: VOBKON; Fernandes et al., 2008 ▸), [Ni(phtpy)2]Cl2·10H2O, (3; refcode: SIXLIU01; Chen et al., 2013 ▸), [Ru(phtpy)2]Cl2·10H2O (4; refcode: FAFFID; McMurtrie & Dance, 2010 ▸) and [Ru(pytpy)2]Cl2·10H2O (5; refcode: TUXGUP; Padhi et al., 2010 ▸) [phtpy = 4′-phenyl-2,2′:6′,2′′-terpyridine and pytpy = 4′-(2-pyrid­yl)-2,2′:6′,2′′-terpyridine]. In spite of the differences in the metal ions and terpyridine ligands, the crystal parameters are almost the same for compounds 2–5. Where a five-membered furyl ring is involved instead of a six-membered phenyl or pyridyl ring, the size of the crystal cell decreases with reduction in the cell volume of about 4.5% from 2200 to 2100 Å3. Considering the O⋯O and O⋯Cl distances within the two-dimensional waterchloride networks, a different number of trinuclear, tetra­nuclear, penta­nuclear, hexa­nuclear and octa­nuclear rings have been determined, giving an L4(6)4(6)4(6)4(6)4(6)5(6)5(6)5(6)6(8)8(12) pattern for 2, an L4(6)4(6)4(6)5(7)5(7)5(8)5(8)6(7)6(9)6(9)8(12) pattern for 3, an L4(6)4(6)4(6)4(6)4(6)4(6)5(6)5(6)5(7)6(7)8(12) pattern for 4 and an L3(6)4(6)5(5)5(6)5(6)6(8)6(8)8(8)8(10) pattern for 5 (Fig. 5 ▸ b–e). These results illustrate how a waterchloride assembly could be fine-tuned by adopting diverse ligands and different metal ions. It is potentially useful for future studies of waterwater or waterchloride inter­actions for chemists as well as theoreticians.

Synthesis and crystallization

4′-Furyl-2,2′:6′,2′′-terpyridine was prepared by a literature method (Wang & Hanan, 2005 ▸). Other reagents and solvents used in reactions were purchased from Aladdin Chemical and used without purification, unless otherwise indicated. NiCl2·6H2O (0.1 mmol, 0.024g) and ftpy (0.2 mmol, 0.060 g) were dissolved in 10 ml distilled water and 10 ml methanol. The solution was left alone for slow evaporation without disturbance for about one month and reddish brown crystals of (1) suitable for X-ray analysis were obtained.

Refinement

Crystal data, data collection and structure refinement details are summarized in Table 3 ▸. All hydrogen atoms except those of water mol­ecules were generated geometrically and refined isotropically using a riding model, with C—H = 0.93 Å and U iso(H) = 1.2U eq(C). The hydrogen atoms of solvent water mol­ecules were located in difference-Fourier maps, refined with DFIX restraints of O—H distances and finally fixed at those positions using AFIX 3 in SHELXL (Sheldrick, 2015b ▸). Atoms C36, C37, C38 and O2 were found to be disordered over two sets of sites with a refined occupancy ratio of 0.786 (13):0.214 (13) for C36/C36A, C37/C37A, C38/C38A, and O2/O2A. In order to model the disorder of this furyl ring, various restraints (DFIX, FLAT, ISOR, DELU, EADP) were applied in the refinement.
Table 3

Experimental details

Crystal data
Chemical formula[Ni(C19H13N3O)2]Cl2·10H2O
M r 908.42
Crystal system, space groupTriclinic, P
Temperature (K)296
a, b, c (Å)10.351 (7), 11.894 (8), 19.070 (13)
α, β, γ (°)76.33 (1), 88.582 (12), 67.077 (11)
V3)2095 (2)
Z 2
Radiation typeMo Kα
μ (mm−1)0.66
Crystal size (mm)0.23 × 0.18 × 0.15
 
Data collection
DiffractometerBruker SMART CCD area-detector
Absorption correctionMulti-scan (SADABS; Bruker, 2012)
T min, T max 0.864, 0.908
No. of measured, independent and observed [I > 2σ(I)] reflections10779, 7382, 5322
R int 0.029
(sin θ/λ)max−1)0.597
 
Refinement
R[F 2 > 2σ(F 2)], wR(F 2), S 0.050, 0.144, 1.07
No. of reflections7382
No. of parameters546
No. of restraints75
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å−3)0.42, −0.53

Computer programs: SMART and SAINT (Bruker, 2012 ▸), SHELXT (Sheldrick, 2015a ▸); SHELXL2014 (Sheldrick, 2015b ▸), OLEX2(Dolomanov et al., 2009 ▸), DIAMOND (Brandenburg & Putz, 2008 ▸) and publCIF (Westrip, 2010 ▸).

Crystal structure: contains datablock(s) I. DOI: 10.1107/S2056989017007095/lh5845sup1.cif Structure factors: contains datablock(s) I. DOI: 10.1107/S2056989017007095/lh5845Isup2.hkl CCDC reference: 1498201 Additional supporting information: crystallographic information; 3D view; checkCIF report
[Ni(C19H13N3O)2]Cl2·10H2OZ = 2
Mr = 908.42F(000) = 948
Triclinic, P1Dx = 1.440 Mg m3
a = 10.351 (7) ÅMo Kα radiation, λ = 0.71073 Å
b = 11.894 (8) ÅCell parameters from 3615 reflections
c = 19.070 (13) Åθ = 2.2–24.0°
α = 76.33 (1)°µ = 0.66 mm1
β = 88.582 (12)°T = 296 K
γ = 67.077 (11)°Block, brown
V = 2095 (2) Å30.23 × 0.18 × 0.15 mm
Bruker SMART CCD area-detector diffractometer5322 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.029
phi and ω scansθmax = 25.1°, θmin = 1.9°
Absorption correction: multi-scan (SADABS; Bruker, 2012)h = −12→8
Tmin = 0.864, Tmax = 0.908k = −14→13
10779 measured reflectionsl = −22→19
7382 independent 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)] = 0.050Hydrogen site location: mixed
wR(F2) = 0.144H-atom parameters constrained
S = 1.07w = 1/[σ2(Fo2) + (0.0689P)2] where P = (Fo2 + 2Fc2)/3
7382 reflections(Δ/σ)max < 0.001
546 parametersΔρmax = 0.42 e Å3
75 restraintsΔρmin = −0.53 e Å3
Geometry. 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.
xyzUiso*/UeqOcc. (<1)
Ni10.97894 (4)0.78241 (4)0.74747 (2)0.03697 (15)
Cl10.30308 (10)0.17463 (10)0.94851 (6)0.0626 (3)
Cl20.28593 (15)0.70315 (14)0.37352 (7)0.0975 (4)
N10.9435 (3)0.6158 (2)0.77056 (14)0.0395 (6)
N21.0808 (3)0.6936 (2)0.84370 (14)0.0371 (6)
N31.0524 (3)0.9124 (2)0.76977 (14)0.0402 (6)
N41.1361 (3)0.7137 (2)0.67860 (15)0.0404 (6)
N50.8802 (3)0.8743 (2)0.65098 (14)0.0363 (6)
N60.7778 (3)0.8893 (3)0.77339 (14)0.0399 (6)
O1W0.0399 (3)0.1312 (3)1.0094 (2)0.1017 (12)
H1WA0.10690.14790.98650.153*
H1WB−0.01840.12830.97850.153*
O11.3786 (3)0.5497 (3)1.07455 (16)0.0771 (8)
O2W0.3405 (4)0.3554 (3)0.8020 (2)0.1191 (14)
H2WB0.42560.33900.79970.179*
H2WA0.32800.31790.84310.179*
O20.7323 (4)1.0325 (5)0.38766 (18)0.0652 (12)0.786 (13)
O2A0.5318 (13)1.1546 (17)0.4459 (8)0.0652 (12)0.214 (13)
O3W0.0344 (6)0.4187 (5)0.4364 (3)0.161 (2)
H3WC0.12420.38490.43770.241*
H3WA−0.00040.47920.39670.241*
O4W0.2936 (5)0.4343 (4)0.4358 (2)0.1321 (15)
H4WB0.23660.50980.44010.198*
H4WA0.35340.46580.41680.198*
O5W0.3714 (4)0.7092 (4)0.21731 (19)0.1075 (12)
H5WA0.32290.74840.24840.161*
H5WB0.30790.77510.18660.161*
O6W0.8002 (4)0.6442 (4)0.3295 (2)0.1187 (14)
H6WC0.75940.65590.28980.178*
H6WA0.73390.69820.34420.178*
O7W0.5809 (3)0.6957 (3)0.42459 (18)0.0892 (10)
H7WA0.50690.68420.41370.134*
H7WB0.61690.65000.46800.134*
O8W0.9848 (5)0.7051 (5)0.4183 (3)0.165 (2)
H8WC0.97410.69100.46340.247*
H8WD1.05410.72660.40860.247*
O9W0.1697 (4)0.8720 (3)0.08918 (18)0.0972 (11)
H9WA0.23280.85960.05830.146*
H9WB0.13810.95270.08240.146*
O10W0.6127 (3)0.1247 (3)−0.00361 (17)0.0790 (9)
H10A0.52440.1474−0.01820.119*
H10B0.61770.04790.01110.119*
C11.4491 (5)0.4603 (6)1.1365 (3)0.0893 (16)
H1A1.49700.47321.17240.107*
C21.4381 (5)0.3551 (6)1.1366 (2)0.0892 (16)
H2A1.47850.28001.17190.107*
C31.3555 (4)0.3735 (4)1.0750 (2)0.0629 (10)
H3A1.32840.31491.06180.075*
C41.3234 (4)0.4928 (4)1.03888 (19)0.0502 (8)
C51.2401 (3)0.5626 (3)0.97208 (18)0.0439 (8)
C61.2338 (3)0.6820 (3)0.93761 (18)0.0450 (8)
H61.28420.71840.95750.054*
C71.1634 (3)0.5118 (3)0.93943 (18)0.0435 (8)
H71.16570.43220.96100.052*
C81.0858 (3)0.5796 (3)0.87613 (17)0.0400 (7)
C91.1521 (3)0.7449 (3)0.87409 (17)0.0386 (7)
C101.1305 (3)0.8734 (3)0.83215 (18)0.0405 (8)
C111.1802 (4)0.9497 (4)0.8570 (2)0.0519 (9)
H111.23590.92010.90030.062*
C121.1457 (4)1.0711 (4)0.8163 (2)0.0591 (10)
H121.17721.12500.83190.071*
C131.0652 (4)1.1115 (4)0.7531 (2)0.0574 (10)
H131.04101.19320.72510.069*
C141.0200 (4)1.0298 (3)0.7311 (2)0.0506 (9)
H140.96491.05770.68770.061*
C150.9995 (3)0.5383 (3)0.83507 (18)0.0384 (7)
C160.9774 (4)0.4297 (3)0.8607 (2)0.0485 (9)
H161.01660.37740.90600.058*
C170.8971 (4)0.3996 (4)0.8187 (2)0.0568 (10)
H170.87940.32740.83560.068*
C180.8430 (4)0.4757 (4)0.7518 (2)0.0557 (10)
H180.79000.45500.72230.067*
C190.8678 (4)0.5830 (3)0.7287 (2)0.0491 (9)
H190.83150.63470.68280.059*
C201.2646 (4)0.6268 (3)0.6978 (2)0.0507 (9)
H201.29240.59210.74680.061*
C211.3586 (4)0.5861 (4)0.6483 (2)0.0624 (11)
H211.44830.52460.66350.075*
C221.3193 (4)0.6362 (4)0.5779 (2)0.0605 (10)
H221.38210.61040.54350.073*
C231.1853 (4)0.7262 (4)0.5561 (2)0.0515 (9)
H231.15650.76150.50730.062*
C241.0956 (3)0.7623 (3)0.60840 (18)0.0389 (7)
C250.9482 (3)0.8536 (3)0.59157 (17)0.0383 (7)
C260.8800 (4)0.9120 (3)0.52461 (18)0.0438 (8)
H260.92710.89580.48360.053*
C270.7407 (4)0.9953 (3)0.51755 (18)0.0421 (8)
C280.6734 (4)1.0179 (3)0.57974 (18)0.0423 (8)
H280.58031.07460.57670.051*
C290.7472 (3)0.9549 (3)0.64582 (17)0.0367 (7)
C300.6892 (3)0.9652 (3)0.71648 (17)0.0378 (7)
C310.5555 (4)1.0467 (3)0.7236 (2)0.0488 (8)
H310.49601.09970.68310.059*
C320.5115 (4)1.0483 (4)0.7922 (2)0.0551 (10)
H320.42111.10210.79870.066*
C330.6021 (4)0.9698 (4)0.8509 (2)0.0549 (10)
H330.57430.96940.89770.066*
C340.7340 (4)0.8921 (3)0.83933 (19)0.0499 (9)
H340.79560.83910.87910.060*
C350.6651 (4)1.0581 (3)0.44799 (17)0.0473 (8)
C360.5368 (6)1.1455 (5)0.4263 (4)0.0530 (14)0.786 (13)
H360.46931.18070.45660.064*0.786 (13)
C36A0.695 (2)1.046 (2)0.3801 (7)0.0530 (14)0.214 (13)
H36A0.77790.98940.36720.064*0.214 (13)
C370.5193 (7)1.1758 (6)0.3518 (4)0.0582 (16)0.786 (13)
H370.43901.23380.32310.070*0.786 (13)
C37A0.585 (3)1.130 (2)0.3344 (7)0.0582 (16)0.214 (13)
H37A0.57931.13930.28460.070*0.214 (13)
C380.6383 (8)1.1068 (6)0.3293 (2)0.0593 (15)0.786 (13)
H380.65611.10810.28110.071*0.786 (13)
C38A0.4838 (19)1.198 (2)0.3714 (10)0.0593 (15)0.214 (13)
H38A0.39801.26200.35160.071*0.214 (13)
U11U22U33U12U13U23
Ni10.0399 (3)0.0386 (3)0.0332 (2)−0.01552 (19)0.00434 (16)−0.01032 (18)
Cl10.0538 (6)0.0650 (6)0.0640 (6)−0.0216 (5)−0.0007 (4)−0.0095 (5)
Cl20.1043 (10)0.1146 (11)0.0714 (9)−0.0447 (9)0.0106 (7)−0.0168 (8)
N10.0398 (15)0.0438 (16)0.0373 (16)−0.0172 (13)0.0044 (12)−0.0131 (13)
N20.0400 (15)0.0369 (15)0.0358 (15)−0.0158 (12)0.0047 (11)−0.0110 (12)
N30.0430 (16)0.0411 (16)0.0405 (16)−0.0189 (13)0.0082 (12)−0.0138 (13)
N40.0399 (16)0.0407 (15)0.0411 (17)−0.0147 (13)0.0069 (12)−0.0136 (13)
N50.0383 (15)0.0357 (14)0.0361 (15)−0.0151 (12)0.0085 (11)−0.0106 (12)
N60.0434 (15)0.0457 (16)0.0337 (15)−0.0192 (13)0.0088 (12)−0.0132 (13)
O1W0.075 (2)0.106 (3)0.121 (3)−0.032 (2)0.034 (2)−0.033 (2)
O10.080 (2)0.091 (2)0.0604 (19)−0.0284 (18)−0.0039 (15)−0.0255 (17)
O2W0.153 (4)0.072 (2)0.096 (3)−0.015 (2)0.047 (3)−0.008 (2)
O20.054 (2)0.083 (3)0.0378 (19)−0.010 (2)−0.0021 (15)−0.0050 (18)
O2A0.054 (2)0.083 (3)0.0378 (19)−0.010 (2)−0.0021 (15)−0.0050 (18)
O3W0.202 (5)0.220 (6)0.127 (4)−0.143 (5)0.047 (4)−0.068 (4)
O4W0.120 (3)0.150 (4)0.113 (4)−0.051 (3)−0.009 (3)−0.011 (3)
O5W0.149 (4)0.128 (3)0.073 (2)−0.083 (3)0.012 (2)−0.025 (2)
O6W0.114 (3)0.157 (4)0.141 (4)−0.090 (3)0.056 (3)−0.079 (3)
O7W0.085 (2)0.081 (2)0.084 (2)−0.0156 (18)−0.0003 (17)−0.0184 (18)
O8W0.163 (5)0.214 (6)0.121 (4)−0.081 (4)0.011 (3)−0.034 (4)
O9W0.097 (2)0.104 (3)0.092 (3)−0.049 (2)0.031 (2)−0.015 (2)
O10W0.0620 (18)0.094 (2)0.085 (2)−0.0325 (17)−0.0038 (15)−0.0244 (18)
C10.064 (3)0.129 (5)0.055 (3)−0.010 (3)−0.018 (2)−0.034 (3)
C20.089 (4)0.093 (4)0.042 (2)0.003 (3)−0.0113 (18)−0.003 (2)
C30.075 (3)0.0587 (19)0.050 (2)−0.022 (2)0.0019 (17)−0.0116 (17)
C40.047 (2)0.0585 (18)0.0374 (19)−0.0128 (18)0.0000 (14)−0.0124 (14)
C50.0400 (19)0.048 (2)0.0362 (19)−0.0093 (16)0.0054 (14)−0.0112 (16)
C60.0435 (19)0.051 (2)0.044 (2)−0.0188 (17)0.0034 (15)−0.0183 (17)
C70.050 (2)0.0385 (19)0.0375 (19)−0.0151 (16)0.0043 (15)−0.0055 (15)
C80.0401 (18)0.0429 (19)0.0377 (19)−0.0152 (16)0.0080 (14)−0.0135 (16)
C90.0388 (18)0.0428 (19)0.0337 (18)−0.0132 (15)0.0066 (13)−0.0141 (15)
C100.0414 (18)0.0447 (19)0.042 (2)−0.0201 (16)0.0089 (14)−0.0181 (16)
C110.055 (2)0.058 (2)0.052 (2)−0.0278 (19)0.0027 (17)−0.0200 (19)
C120.064 (3)0.056 (2)0.073 (3)−0.034 (2)0.014 (2)−0.028 (2)
C130.071 (3)0.043 (2)0.063 (3)−0.027 (2)0.007 (2)−0.0150 (19)
C140.055 (2)0.045 (2)0.048 (2)−0.0179 (18)0.0037 (16)−0.0072 (17)
C150.0359 (17)0.0386 (18)0.0415 (19)−0.0134 (15)0.0070 (14)−0.0139 (15)
C160.048 (2)0.041 (2)0.054 (2)−0.0163 (17)0.0054 (16)−0.0071 (17)
C170.059 (2)0.046 (2)0.073 (3)−0.0288 (19)0.007 (2)−0.016 (2)
C180.054 (2)0.055 (2)0.068 (3)−0.029 (2)0.0026 (19)−0.022 (2)
C190.051 (2)0.053 (2)0.047 (2)−0.0222 (18)−0.0010 (16)−0.0158 (18)
C200.044 (2)0.049 (2)0.056 (2)−0.0134 (18)0.0049 (17)−0.0156 (18)
C210.038 (2)0.064 (3)0.077 (3)−0.0086 (19)0.0091 (19)−0.023 (2)
C220.050 (2)0.067 (3)0.066 (3)−0.018 (2)0.024 (2)−0.030 (2)
C230.050 (2)0.059 (2)0.047 (2)−0.0196 (19)0.0147 (16)−0.0205 (18)
C240.0402 (18)0.0378 (18)0.043 (2)−0.0171 (15)0.0103 (14)−0.0145 (15)
C250.0433 (19)0.0414 (18)0.0358 (18)−0.0197 (16)0.0114 (14)−0.0154 (15)
C260.051 (2)0.049 (2)0.0360 (19)−0.0231 (18)0.0153 (15)−0.0148 (16)
C270.050 (2)0.0430 (19)0.0353 (19)−0.0212 (17)0.0044 (14)−0.0087 (15)
C280.0429 (19)0.0409 (19)0.040 (2)−0.0133 (16)0.0039 (14)−0.0102 (15)
C290.0415 (19)0.0349 (17)0.0358 (18)−0.0157 (15)0.0086 (14)−0.0121 (14)
C300.0422 (19)0.0366 (18)0.0377 (19)−0.0169 (15)0.0076 (14)−0.0128 (15)
C310.047 (2)0.047 (2)0.048 (2)−0.0144 (17)0.0088 (16)−0.0121 (17)
C320.051 (2)0.059 (2)0.060 (3)−0.0197 (19)0.0225 (19)−0.027 (2)
C330.063 (2)0.063 (2)0.044 (2)−0.025 (2)0.0233 (18)−0.023 (2)
C340.061 (2)0.056 (2)0.0343 (19)−0.0238 (19)0.0103 (16)−0.0136 (17)
C350.058 (2)0.057 (2)0.0349 (19)−0.029 (2)0.0046 (16)−0.0142 (17)
C360.057 (3)0.050 (3)0.049 (3)−0.016 (2)0.016 (3)−0.019 (3)
C36A0.057 (3)0.050 (3)0.049 (3)−0.016 (2)0.016 (3)−0.019 (3)
C370.045 (3)0.057 (3)0.060 (3)−0.010 (3)−0.003 (3)−0.010 (3)
C37A0.045 (3)0.057 (3)0.060 (3)−0.010 (3)−0.003 (3)−0.010 (3)
C380.056 (3)0.074 (4)0.033 (2)−0.014 (3)−0.004 (2)−0.005 (2)
C38A0.056 (3)0.074 (4)0.033 (2)−0.014 (3)−0.004 (2)−0.005 (2)
Ni1—N51.974 (3)C7—H70.9300
Ni1—N21.977 (3)C8—C151.487 (4)
Ni1—N62.093 (3)C9—C101.480 (4)
Ni1—N32.096 (3)C10—C111.376 (5)
Ni1—N12.098 (3)C11—C121.378 (5)
Ni1—N42.099 (3)C11—H110.9300
N1—C151.335 (4)C12—C131.356 (6)
N1—C191.350 (4)C12—H120.9300
N2—C81.331 (4)C13—C141.377 (5)
N2—C91.339 (4)C13—H130.9300
N3—C141.329 (4)C14—H140.9300
N3—C101.333 (4)C15—C161.373 (5)
N4—C201.322 (4)C16—C171.364 (5)
N4—C241.332 (4)C16—H160.9300
N5—C291.326 (4)C17—C181.361 (5)
N5—C251.340 (4)C17—H170.9300
N6—C341.329 (4)C18—C191.368 (5)
N6—C301.332 (4)C18—H180.9300
O1W—H1WA0.8732C19—H190.9300
O1W—H1WB0.8701C20—C211.370 (5)
O1—C41.336 (4)C20—H200.9300
O1—C11.379 (6)C21—C221.336 (6)
O2W—H2WB0.8275C21—H210.9300
O2W—H2WA0.8393C22—C231.379 (5)
O2—C351.364 (4)C22—H220.9300
O2—C381.373 (5)C23—C241.373 (4)
O2A—C351.404 (9)C23—H230.9300
O2A—C38A1.421 (9)C24—C251.476 (5)
O3W—H3WC0.8556C25—C261.362 (5)
O3W—H3WA0.8797C26—C271.383 (5)
O4W—H4WB0.8839C26—H260.9300
O4W—H4WA0.8729C27—C281.389 (4)
O5W—H5WA0.8692C27—C351.435 (5)
O5W—H5WB0.8890C28—C291.374 (5)
O6W—H6WC0.8315C28—H280.9300
O6W—H6WA0.8339C29—C301.474 (4)
O7W—H7WA0.8667C30—C311.372 (5)
O7W—H7WB0.8744C31—C321.375 (5)
O8W—H8WC0.8502C31—H310.9300
O8W—H8WD0.8528C32—C331.372 (5)
O9W—H9WA0.8616C32—H320.9300
O9W—H9WB0.8629C33—C341.365 (5)
O10W—H10A0.8785C33—H330.9300
O10W—H10B0.8705C34—H340.9300
C1—C21.299 (7)C35—C361.328 (6)
C1—H1A0.9300C35—C36A1.352 (9)
C2—C31.394 (6)C36—C371.378 (6)
C2—H2A0.9300C36—H360.9300
C3—C41.334 (5)C36A—C37A1.344 (10)
C3—H3A0.9300C36A—H36A0.9300
C4—C51.432 (5)C37—C381.315 (6)
C5—C61.394 (5)C37—H370.9300
C5—C71.400 (5)C37A—C38A1.351 (9)
C6—C91.368 (5)C37A—H37A0.9300
C6—H60.9300C38—H380.9300
C7—C81.355 (5)C38A—H38A0.9300
N5—Ni1—N2178.36 (10)N3—C14—H14118.9
N5—Ni1—N677.81 (11)C13—C14—H14118.9
N2—Ni1—N6102.65 (11)N1—C15—C16121.9 (3)
N5—Ni1—N3100.71 (11)N1—C15—C8114.7 (3)
N2—Ni1—N377.74 (11)C16—C15—C8123.5 (3)
N6—Ni1—N389.84 (11)C17—C16—C15119.0 (4)
N5—Ni1—N1103.80 (10)C17—C16—H16120.5
N2—Ni1—N177.77 (11)C15—C16—H16120.5
N6—Ni1—N193.13 (11)C18—C17—C16119.8 (3)
N3—Ni1—N1155.38 (11)C18—C17—H17120.1
N5—Ni1—N478.10 (11)C16—C17—H17120.1
N2—Ni1—N4101.46 (12)C17—C18—C19119.1 (3)
N6—Ni1—N4155.89 (11)C17—C18—H18120.5
N3—Ni1—N495.46 (11)C19—C18—H18120.5
N1—Ni1—N491.74 (10)N1—C19—C18121.7 (4)
C15—N1—C19118.5 (3)N1—C19—H19119.1
C15—N1—Ni1114.5 (2)C18—C19—H19119.1
C19—N1—Ni1126.9 (2)N4—C20—C21122.5 (4)
C8—N2—C9120.0 (3)N4—C20—H20118.8
C8—N2—Ni1120.1 (2)C21—C20—H20118.8
C9—N2—Ni1119.7 (2)C22—C21—C20118.9 (4)
C14—N3—C10118.6 (3)C22—C21—H21120.6
C14—N3—Ni1126.4 (2)C20—C21—H21120.6
C10—N3—Ni1114.8 (2)C21—C22—C23119.9 (4)
C20—N4—C24118.8 (3)C21—C22—H22120.0
C20—N4—Ni1127.0 (3)C23—C22—H22120.0
C24—N4—Ni1114.1 (2)C24—C23—C22118.4 (4)
C29—N5—C25120.9 (3)C24—C23—H23120.8
C29—N5—Ni1119.5 (2)C22—C23—H23120.8
C25—N5—Ni1119.6 (2)N4—C24—C23121.5 (3)
C34—N6—C30118.6 (3)N4—C24—C25115.4 (3)
C34—N6—Ni1126.8 (2)C23—C24—C25123.1 (3)
C30—N6—Ni1114.5 (2)N5—C25—C26120.4 (3)
H1WA—O1W—H1WB109.3N5—C25—C24112.8 (3)
C4—O1—C1105.9 (4)C26—C25—C24126.8 (3)
H2WB—O2W—H2WA108.4C25—C26—C27120.0 (3)
C35—O2—C38106.7 (4)C25—C26—H26120.0
C35—O2A—C38A104.3 (8)C27—C26—H26120.0
H3WC—O3W—H3WA110.8C26—C27—C28118.7 (3)
H4WB—O4W—H4WA89.3C26—C27—C35121.7 (3)
H5WA—O5W—H5WB81.1C28—C27—C35119.7 (3)
H6WC—O6W—H6WA96.0C29—C28—C27118.6 (3)
H7WA—O7W—H7WB110.0C29—C28—H28120.7
H8WC—O8W—H8WD111.3C27—C28—H28120.7
H9WA—O9W—H9WB101.0N5—C29—C28121.4 (3)
H10A—O10W—H10B87.7N5—C29—C30113.5 (3)
C2—C1—O1109.2 (4)C28—C29—C30125.1 (3)
C2—C1—H1A125.4N6—C30—C31122.3 (3)
O1—C1—H1A125.4N6—C30—C29114.5 (3)
C1—C2—C3108.6 (5)C31—C30—C29123.1 (3)
C1—C2—H2A125.7C30—C31—C32118.4 (3)
C3—C2—H2A125.7C30—C31—H31120.8
C4—C3—C2105.5 (4)C32—C31—H31120.8
C4—C3—H3A127.3C33—C32—C31119.4 (3)
C2—C3—H3A127.3C33—C32—H32120.3
C3—C4—O1110.8 (3)C31—C32—H32120.3
C3—C4—C5129.7 (4)C34—C33—C32118.7 (3)
O1—C4—C5119.5 (3)C34—C33—H33120.7
C6—C5—C7118.2 (3)C32—C33—H33120.7
C6—C5—C4121.2 (3)N6—C34—C33122.6 (3)
C7—C5—C4120.6 (3)N6—C34—H34118.7
C9—C6—C5118.8 (3)C33—C34—H34118.7
C9—C6—H6120.6C36—C35—O2107.6 (4)
C5—C6—H6120.6C36A—C35—O2A109.5 (8)
C8—C7—C5119.4 (3)C36—C35—C27133.6 (4)
C8—C7—H7120.3C36A—C35—C27133.4 (8)
C5—C7—H7120.3O2—C35—C27118.8 (3)
N2—C8—C7121.8 (3)O2A—C35—C27117.1 (7)
N2—C8—C15112.6 (3)C35—C36—C37109.4 (4)
C7—C8—C15125.6 (3)C35—C36—H36125.3
N2—C9—C6121.7 (3)C37—C36—H36125.3
N2—C9—C10112.7 (3)C37A—C36A—C35108.2 (9)
C6—C9—C10125.5 (3)C37A—C36A—H36A125.9
N3—C10—C11122.2 (3)C35—C36A—H36A125.9
N3—C10—C9114.7 (3)C38—C37—C36106.7 (4)
C11—C10—C9122.9 (3)C38—C37—H37126.7
C10—C11—C12118.4 (4)C36—C37—H37126.7
C10—C11—H11120.8C36A—C37A—C38A110.1 (10)
C12—C11—H11120.8C36A—C37A—H37A124.9
C13—C12—C11119.5 (3)C38A—C37A—H37A124.9
C13—C12—H12120.3C37—C38—O2109.6 (4)
C11—C12—H12120.3C37—C38—H38125.2
C12—C13—C14119.1 (4)O2—C38—H38125.2
C12—C13—H13120.4C37A—C38A—O2A107.8 (9)
C14—C13—H13120.4C37A—C38A—H38A126.1
N3—C14—C13122.1 (4)O2A—C38A—H38A126.1
D—H···AD—HH···AD···AD—H···A
O1W—H1WA···Cl10.872.253.113 (4)169
O1W—H1WB···O9Wi0.872.062.923 (6)175
O2W—H2WB···O5Wii0.831.992.813 (7)172
O2W—H2WA···Cl10.842.393.215 (4)168
O3W—H3WC···O4W0.862.052.760 (9)140
O3W—H3WA···O6Wiii0.882.353.134 (7)148
O4W—H4WB···Cl20.882.583.107 (5)119
O4W—H4WA···Cl20.872.563.107 (5)122
O5W—H5WA···Cl20.872.373.079 (4)138
O5W—H5WB···O9W0.892.162.991 (6)156
O6W—H6WC···O2Wii0.832.112.929 (6)167
O6W—H6WA···O7W0.832.182.838 (6)136
O7W—H7WA···Cl20.872.343.190 (4)167
O7W—H7WB···O4Wii0.871.932.798 (5)172
O8W—H8WC···O3Wii0.852.062.856 (8)155
O8W—H8WD···Cl2iv0.852.403.204 (6)157
O9W—H9WA···O10Wv0.861.932.756 (6)159
O9W—H9WB···O1Wvi0.862.112.878 (5)147
O10W—H10A···Cl1vii0.882.273.141 (4)171
O10W—H10B···Cl1viii0.872.383.225 (4)165
  15 in total

1.  New Rhodium(II) Complexes with 2,2':6',2"-Terpyridine.

Authors:  Florian P. Pruchnik; Francis Robert; Yves Jeannin; Suzanne Jeannin
Journal:  Inorg Chem       Date:  1996-07-03       Impact factor: 5.165

2.  A hybrid water-chloride structure with discrete undecameric water moieties self-assembled in a heptaprotonated octaamino cryptand.

Authors:  P S Lakshminarayanan; Eringathodi Suresh; Pradyut Ghosh
Journal:  Angew Chem Int Ed Engl       Date:  2006-06-02       Impact factor: 15.336

3.  Reversible emergence of a self-assembled layered structure from three-dimensional isotropic ionic crystal of a cluster compound (4-HNC5H4OH)2Mo6Cl14 driven by absorption of water and alcohols.

Authors:  Kei Inumaru; Takashi Kikudome; Hiroshi Fukuoka; Shoji Yamanaka
Journal:  J Am Chem Soc       Date:  2008-07-10       Impact factor: 15.419

4.  Impact of metal on the DNA photo-induced cleavage activity of a family of Phterpy complexes.

Authors:  Gong-Jun Chen; Zhi-Gang Wang; Ying-Ying Kou; Jin-Lei Tian; Shi-Ping Yan
Journal:  J Inorg Biochem       Date:  2013-01-26       Impact factor: 4.155

5.  Encapsulation of [(SO₄)₄(H₂O)1₁₂]⁸⁻ clusters in a metal organic framework of pyridyl functionalized cyanuric acid based tris-urea.

Authors:  Ranjan Dutta; Bidyut Akhuli; Pradyut Ghosh
Journal:  Dalton Trans       Date:  2015-09-14       Impact factor: 4.390

6.  Simultaneous encapsulation of an infinite T4(0)A(0)6(0) water tape and discrete water hexamers in a hydrogen-bonded Ag(I) supramolecular framework.

Authors:  Lu-Lu Han; Tuo-Ping Hu; Jiang-Shan Chen; Zhong-Hui Li; Xing-Po Wang; Ya-Qin Zhao; Xiao-Yu Li; Di Sun
Journal:  Dalton Trans       Date:  2014-06-21       Impact factor: 4.390

7.  Ni(II), Co(II), Cu(II), Zn(II) and Na(I) complexes of a hybrid ligand 4'-(4'''-benzo-15-crown-5)-methyloxy-2,2':6',2''-terpyridine.

Authors:  Nadezhda M Logacheva; Vladimir E Baulin; Aslan Yu Tsivadze; Elena N Pyatova; Irina S Ivanova; Yurii A Velikodny; Vladimir V Chernyshev
Journal:  Dalton Trans       Date:  2009-02-11       Impact factor: 4.390

8.  SHELXT - integrated space-group and crystal-structure determination.

Authors:  George M Sheldrick
Journal:  Acta Crystallogr A Found Adv       Date:  2015-01-01       Impact factor: 2.290

9.  Crystal structure refinement with SHELXL.

Authors:  George M Sheldrick
Journal:  Acta Crystallogr C Struct Chem       Date:  2015-01-01       Impact factor: 1.172

10.  The Cambridge Structural Database.

Authors:  Colin R Groom; Ian J Bruno; Matthew P Lightfoot; Suzanna C Ward
Journal:  Acta Crystallogr B Struct Sci Cryst Eng Mater       Date:  2016-04-01
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