Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S2053229616006458/wq3112sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S2053229616006458/wq3112Isup2.hkl | |
Structure factor file (CIF format) https://doi.org/10.1107/S2053229616006458/wq3112IIsup3.hkl | |
Structure factor file (CIF format) https://doi.org/10.1107/S2053229616006458/wq3112IIIsup4.hkl | |
Structure factor file (CIF format) https://doi.org/10.1107/S2053229616006458/wq3112IVsup5.hkl | |
Structure factor file (CIF format) https://doi.org/10.1107/S2053229616006458/wq3112Vsup6.hkl | |
Portable Document Format (PDF) file https://doi.org/10.1107/S2053229616006458/wq3112sup7.pdf |
CCDC references: 1474849; 1474848; 1474847; 1474846; 1474845
The chemistry of organically templated metal sulfates (OTMS) has attracted extensive interest of the materials science community. Recently, increasing attention has been paid to the development of synthetic strategies for the preparation of organic–inorganic hybrid materials with novel structures and special properties. Sulfur–oxygen–metal (S—O—M) linkages provide the possibility of using SO42- tetrahedra as a building unit to form new solid-state materials with novel topological structures and interesting physical properties (Rao et al., 2006).
The 2-aminopyridinium (2ap) cation has received little attention as a template agent in OTMS. In the case of double metal and 2ap sulfates, only one representative is known up to now (Lukianova et al., 2015). The crystal structure of bis(2-aminopyridinium) sulfate has also been reported (Jebas et al., 2006a). In the literature, there are reports where simple inorganic–organic hybrids with the 2ap cation and various halogen salts characterized by interesting supramolecular networks (Luque et al., 1997; Su et al., 2002; Kumar et al., 2005; Jebas et al., 2006b; Zhang et al., 2006; Fun et al., 2008; Gelmboldt et al., 2009; Cai & Fu, 2010; Jin et al., 2011; Rao et al., 2011; Mhadhbi et al., 2016) and dielectric properties are discussed (Kulicka et al., 2004).
In general, protonated aminopyridinium cations act mainly as template agents as they directly contribute to the dimensionality of the hydrogen-bonding network in the crystal structures of hybrid organic–inorganic materials. The presence of electrostatic interactions, i.e. weak interactions such as C—H···O and π–π interactions, in these solids suggests that these weak interactions play a significant role in shaping the resultant supramolecular assemblies and stabilization of these organic–inorganic hybrid materials.
In this paper, we have directed our efforts towards the synthesis and crystal structure determination, complemented by Hirshfeld surface analysis, of five new 2-aminopyridinium metal sulfates, namely (2ap)[Al(H2O)6](SO4)2·4H2O, (I), (2ap)2[Co(H2O)6]3(SO4)4·2H2O, (II), (2ap)2[Mg(H2O)6]3(SO4)4·2H2O, (III), (2ap)2[Ni(H2O)6](SO4)2, (IV), and (2ap)2[Zn(H2O)6](SO4)2, (V), along with the previously reported copper analogue, (VI) (Lukianova et al., 2015).
The title compounds were synthesized according to the previously described method of Lukianova et al. (2015). An aqueous solution (4 ml) of 2-aminopyridine (0.19 g, 2.0 mmol), the pH of which was adjusted to 2.5 by admixing 30% sulfuric acid, was added slowly to an aqueous solution (3 ml) containing the appropriate metal sulfate [2.0 mmol for (I), 3.0 mmol for (II), 3.0 mmol for (III), 1.0 mmol for (IV) and 1.0 mmol for (V)]. Single crystals of a suitable size were obtained by slow solvent evaporation under ambient conditions for a period of several weeks.
The three-dimensional Hirshfeld surfaces (HSs) and two-dimensional fingerprint plots of (I), (II), (IV) and the copper analogue were generated using the CrystalExplorer software (Wolff et al., 2012).
Crystal data, data collection and structure refinement details are summarized in Table 1. The positions of the amine H atoms were located initially in difference Fourier maps but were subsequently allowed to ride in the refinement, with C—H = 0.96 Å and N—H = 0.91 Å. The isotropic atomic displacement parameters of the H atoms were evaluated as 1.2Ueq of the parent atom. Water H atoms were located firstly in a difference Fourier map and then fixed, with O—H = 0.840 (2) Å and Uiso(H) = 1.5Ueq(O).
Compound (I) crystallizes in the triclinic P1 space group. The asymmetric unit is composed of two halves of two crystallographically independent AlIII cations, both lying on special positions, one protonated 2-aminopyridinium cation, two isolated sulfate anions and four noncoordinated water molecules. As shown in Fig. 1, two metal ions occupy inversion centres, both of them are hexacoordinated by six water molecules, adopting a slightly distorted octahedral coordination geometry. Selected bond lengths and angles are presented below in Table S1 (see Supporting information). The lengths of the Al1—OW and Al2—OW bonds vary from 1.8739 (14) to 1.8896 (15) Å and from 1.8760 (13) to 1.8930 (14) Å, respectively. The values of cis-OW—Al—OW angles are in the range 89.07 (6)–90.93 (6)° in the Al1 octahedron and 89.63 (6)–90.37 (6)° in the Al2 octahedron. These values are comparable with those reported for AlIII complexes with a six-coordinated octahedral geometry (Bataille, 2003). Each centrosymmetric [Al(H2O)6]3+ cation donates ten hydrogen bonds to eight sulfate anions and two hydrogen bonds to two uncoordinated water molecules (Fig. 2). The first sulfate anion accepts a total of nine hydrogen bonds, i.e. five from four hexaaquaaluminium complex cations, three from three solvent water molecules and one N—H···O hydrogen bond from one 2ap cation. The second sulfate anion accepts eight hydrogen bonds, i.e. five from five [Al(H2O)6]3+ cations, one from a free water molecule and two from one 2ap cation. The 2ap cation donates three N—H···O hydrogen bonds to the O atoms of two sulfate anions. One of the carbon-bound H atoms is involved in a weak hydrogen-bond interaction with an O atom of a solvent water molecule. Four free water molecules, namely O1W, O2W, O3W and O4W, are involved in 14 multidirectional O—H···O hydrogen bonds between coordinated water molecules of the [Al(H2O)6]3+ cations, sulfate O atoms and uncoordinated water molecules, forming an inorganic network parallel to the ab plane (Fig. 3a). The O1W molecule donates one hydrogen bond to O2W and one bond to a sulfate anion, and accepts one bond from the O22W atom. O2W donates two hydrogen bonds, i.e. one to O3W and another to a sulfate anion, and accepts two bonds from two solvation water molecules (O2W and O4W). O3W donates two hydrogen bonds to two sulfate anions and accepts two hydrogen bonds from two free water molecules (O4W and O2W). O4W donates two hydrogen bonds to two uncoordinated water molecules (O3W and O2W) and accepts one bond from the O11W atom.
In the crystal structure of (I), a three-dimensional supramolecular network is built from N—H···O, O—H···O and weak C—H···O hydrogen bonds involving the inorganic and organic parts of the structure (Table 2). Organic layers are built of π–π interacting stacks of 2ap cations (Table 3) connected to inorganic layers through N—H···O and C—H···O hydrogen bonds (Table 2 and Figs. 3b/c). The planes of all the 2ap rings are perpendicular to the [100] direction.
Isostructural compounds (II) and (III) (structure type 2) crystallize in the triclinic P1 space group. The asymmetric part of the unit cell contains two hexaaqua-coordinated MII ions (one of them lies on a centre of inversion with half occupancy), one protonated amine group which is disordered over two sites, two sulfate anions and one solvent water molecule (Fig. 4). Each MII atom is located at the centre of a distorted octahedron formed by six O atoms from six water molecules. The M—OW bond lengths are in the ranges 2.0343 (18)–2.1852 (17), 2.0513 (18)–2.1074 (17), 2.0178 (19)–2.1321 (18) and 2.0391 (17)–2.0961 (19) Å for Co1—OW, Co2—OW, Mg1—OW and Mg2—OW, respectively. The cis- and trans-OW—M—OW angles are 81.14 (7)–94.50 (7) and 172.42 (7)–178.16 (6)°, respectively, in the Co1 octahedron, 89.61 (8)–90.39 (8) and 180° in the Co2 octahedron, 85.29 (8)–98.30 (7) and 172.81 (9)–174.89 (8)° in the Mg1 octahedron, and 89.59 (8)–90.41 (8) and 180° (due to inversion symmetry) in the Mg2 octahedron Significant distortions in the coordination polyhedra of (II) and (III) are clearly evident (see Tables S2 and S3 in the Supporting information) and the most considerable distortions are observed in the case of the M1 environment, which does not lie on a centre of inversion.
The M1 octahedron donates eleven hydrogen bonds to six sulfate anions, donates one hydrogen bond to the O13W atom and accepts one hydrogen bond from the O11W water molecule (Fig. 5a), while the M2 octahedron donates eight hydrogen bonds to six sulfate anions and four hydrogen bonds to four solvent water molecules (Fig. 5b). The 2ap cations donate three N—H···O hydrogen bonds to O atoms in the main disordered part and three N—H···O hydrogen bonds in minor disordered part also. The orientationally disordered NH2 group has the minor disordered part attached to the C6 atom, instead of to C2. Reorientation from the first to the second position appears to be impossible due to the environment of the 2ap cation, and most likely is a result of incorrect alignment during the growth of the crystal. The NH2 groups are distributed between two positions with site occupancies equal to 0.121 (5) in the minor part of both (II) and (III).
Uncoordinated water molecule O1W donates two hydrogen bonds to two crystallographically independent sulfate anions and accepts two hydrogen bonds from two [MII(H2O)6]2+ cations. The first sulfate anion accepts ten hydrogen bonds, i.e. seven from four hexaaqua complexes, one from a free water molecule and two N—H···O hydrogen bonds from one 2ap cation. The second sulfate anion accepts eleven hydrogen bonds, i.e. eight from five [MII(H2O)6]2+ cations, one from a free water molecule and two from two 2ap cations. As a result, an inorganic network is formed through O—H···O hydrogen bonds between water molecules, sulfate anions and inorganic cations, and lies parallel to the ac plane (Tables 4 and 5, and Fig. 6a). Significant parallel π–π interactions between pairs of pyridinium rings (Table 3) assist in the formation of a supramolecular association along the a-axis direction and make the overall framework more stable (Fig. 6b). C—H···O hydrogen bonds are not observed in structure type 2.
Isostructural compounds (IV) and (V) crystallize in the triclinic P1 space group. In contrast to compounds (I)–(III), type 3, is characterized by the absence of noncoordinated water molecules. One half of an [M(H2O)6]2+ cation (located on an inversion centre), one sulfate anion and one 2ap cation form the asymmetric unit (see Fig. 7). The MII atom occupies the centre of a slightly distorted octahedron built by the coordination of six water molecules. The crystal packing reveals a layered arrangement of the inorganic and organic parts of the structure.
The M—OW bond lengths (see Tables S4 and S5 in the Supporting information) are 2.0503 (13)–2.0590 (17) and 2.0813 (19)–2.0996 (18) Å for salts (IV) and (V), respectively. The cis bond angles around the MII centres range from 86.63 (6) to 93.37 (6)° for (IV), and from 86.88 (8) to 93.12 (8)° for (IV). The trans angles are all equal to 180°. Geometric parameters are in accord with those reported for other Ni and Zn analogs (Fleck et al., 2004).
The [M(H2O)6]2+ cation donates twelve hydrogen bonds to six sulfate anions (see Fig. 8a). The SO42- anion accepts nine hydrogen bonds, i.e. six from three hexaaqua complexes and three N—H···O hydrogen bonds from two 2ap cations. The [M(H2O)6]2+ cation in salts (IV) and (V) are connected via hydrogen bonds from water molecules to sulfate anions, forming inorganic networks parallel to the ab plane (Fig. 8b). As inferred in Fig. 9, the crystal structure is represented by a series of successive layers: inorganic layers of [M(H2O)6]2+ cations connected to sulfate anions by hydrogen bonds and organic layers of 2ap cations, both being parallel to bc plane. The organic and inorganic layers are linked to each other by two types of hydrogen bonding, i.e. N—H···O and weak C—H···O, present in the crystal structure (Tables 5 and 6, and Fig. 9). This hydrogen-bonding interaction directs the infinite condensation of the respective building units. The crystal packings are further extended via π–π interactions between the 2ap rings in the a-axis direction (Table 3). Moreover, the C—H···O interactions result in the final three-dimensional supramolecular arrangement in type 3.
Hirshfeld surfaces (with dnorm mapped) and fingerprints (de versus di) were generated using Crystal Explorer for the 2ap cations in all of the reported structures along with the earlier studied copper-containing analog (VI) (Lukianova et al., 2015). Analysis of the Hirshfeld surfaces (Fig. 10) reveals several common features of the 2ap cations and highlights their roles in the crystal packing organization. The cation is characterized by the presence of three strong hydrogen-bond donors, while its planar structure provides the possibility for the existence of π–π interactions. The closest [immediate?] environment of the 2ap cation in all the structures is constructed in a similar manner. The cations are involved in strong double hydrogen-bond formation with the sulfate anion in order to produce a charge-assisted pair of composition [2ap···SO4]-. The pair is formed by two H atoms of the pyridinium ring (N1—H) and the amino group (N2—H) hydrogen bonded to two O atoms of the same sulfate anion. The fitted image reveals the distribution of sufate anions with respect to the 2ap cations (Fig. 11). It is worth noting that the remaining H atom of the amino group is hydrogen bonded to another sulfate anion in all of the reported structures. Thus, in hydrogen bonds of the N—H···O type, the role of the acceptor is played by the sulfate O atoms only. The weakest hydrogen bonds formed by the 2ap cations are of the C—H···O type, in which the acceptor O atoms belong to all possible oxygen-containing groups, viz. sulfate anions and coordinated and noncoordinated water molecules.
Another common feature of all the 2ap cations is their involvement in the formation of π–π interacting columns (Table 3) composed of antiparallel oriented cations. In all the structures, these columns propagate along the a axis. The mutual arrangement of these columns results in two different types of crystal packing. In structure types 1 [observed for Al analog (I)] and 2 [observed for Co analog (II) and Mg analog (III)], the columns are isolated and surrounded by inorganic sublattices (Figs. 3b/c and 6b). The second type of crystal packing is governed by the presence of π–π stacked columns aggregated into layers (Fig. 9) and is seen in structure types 3 [observed for Ni analog (IV) and Zn analog (V)] and 4 [observed for Cu analog (VI)]. As a result, alternating organic and inorganic layers are formed.
The fingerprint plots of the 2ap cations are all similar in shape (see Figs. S1–S4 in the Supporting information). They are characterized by the presence of spike pointing at around (di = 0.7, de = 1.1), which corresponds to hydrogen bonds of the N—H···O type. In all the plots, the contacts of inner H atoms dominate the surface area, with around 30% of the area corresponding to H···O contacts, around 40% to H···H contacts and 10–15% to π–π interactions. The strongest of the π–π interactions is illustrated by a presence of a red dot in the fingerprint plot of structure (VI) (Table 3).
In the current work, the results of structural studies of 2-aminopyridinium-templated metal (Al, Co, Mg, Ni and Zn) sulfate hydrates are reported for the first time. The templating role of 2ap is governed by the formation of characteristic charge-assisted hydrogen-bond pairs with sulfate anions and the presence of π–π interactions between the cations. In all of the studied compounds, as well as in the previously reported Cu analog, π–π interactions between the 2ap cations lead to the formation of columns with an antiparallel orientation of the cations. Another common feature of the compounds is the presence of hexaaqua-coordinated metal centres. Sulfate anions do not coordinate to the metal centres and are incorporated in diverse three-dimentional hydrogen-bonding networks, together with hexaaquametal octahedra and uncoordinated water molecules (if present). The mutual arrangement of π–π-interacting columns results in the formation of two modes of crystal packing, i.e. the first with isolated organic columns surrounded by the inorganic counterpart (structural types 1 and 2) and the second characterized by alternate organic–inorganic layers (structural types 3 and 4).
The chemistry of organically templated metal sulfates (OTMS) has attracted extensive interest of the materials science community. Recently, increasing attention has been paid to the development of synthetic strategies for the preparation of organic–inorganic hybrid materials with novel structures and special properties. Sulfur–oxygen–metal (S—O—M) linkages provide the possibility of using SO42- tetrahedra as a building unit to form new solid-state materials with novel topological structures and interesting physical properties (Rao et al., 2006).
The 2-aminopyridinium (2ap) cation has received little attention as a template agent in OTMS. In the case of double metal and 2ap sulfates, only one representative is known up to now (Lukianova et al., 2015). The crystal structure of bis(2-aminopyridinium) sulfate has also been reported (Jebas et al., 2006a). In the literature, there are reports where simple inorganic–organic hybrids with the 2ap cation and various halogen salts characterized by interesting supramolecular networks (Luque et al., 1997; Su et al., 2002; Kumar et al., 2005; Jebas et al., 2006b; Zhang et al., 2006; Fun et al., 2008; Gelmboldt et al., 2009; Cai & Fu, 2010; Jin et al., 2011; Rao et al., 2011; Mhadhbi et al., 2016) and dielectric properties are discussed (Kulicka et al., 2004).
In general, protonated aminopyridinium cations act mainly as template agents as they directly contribute to the dimensionality of the hydrogen-bonding network in the crystal structures of hybrid organic–inorganic materials. The presence of electrostatic interactions, i.e. weak interactions such as C—H···O and π–π interactions, in these solids suggests that these weak interactions play a significant role in shaping the resultant supramolecular assemblies and stabilization of these organic–inorganic hybrid materials.
In this paper, we have directed our efforts towards the synthesis and crystal structure determination, complemented by Hirshfeld surface analysis, of five new 2-aminopyridinium metal sulfates, namely (2ap)[Al(H2O)6](SO4)2·4H2O, (I), (2ap)2[Co(H2O)6]3(SO4)4·2H2O, (II), (2ap)2[Mg(H2O)6]3(SO4)4·2H2O, (III), (2ap)2[Ni(H2O)6](SO4)2, (IV), and (2ap)2[Zn(H2O)6](SO4)2, (V), along with the previously reported copper analogue, (VI) (Lukianova et al., 2015).
The three-dimensional Hirshfeld surfaces (HSs) and two-dimensional fingerprint plots of (I), (II), (IV) and the copper analogue were generated using the CrystalExplorer software (Wolff et al., 2012).
Compound (I) crystallizes in the triclinic P1 space group. The asymmetric unit is composed of two halves of two crystallographically independent AlIII cations, both lying on special positions, one protonated 2-aminopyridinium cation, two isolated sulfate anions and four noncoordinated water molecules. As shown in Fig. 1, two metal ions occupy inversion centres, both of them are hexacoordinated by six water molecules, adopting a slightly distorted octahedral coordination geometry. Selected bond lengths and angles are presented below in Table S1 (see Supporting information). The lengths of the Al1—OW and Al2—OW bonds vary from 1.8739 (14) to 1.8896 (15) Å and from 1.8760 (13) to 1.8930 (14) Å, respectively. The values of cis-OW—Al—OW angles are in the range 89.07 (6)–90.93 (6)° in the Al1 octahedron and 89.63 (6)–90.37 (6)° in the Al2 octahedron. These values are comparable with those reported for AlIII complexes with a six-coordinated octahedral geometry (Bataille, 2003). Each centrosymmetric [Al(H2O)6]3+ cation donates ten hydrogen bonds to eight sulfate anions and two hydrogen bonds to two uncoordinated water molecules (Fig. 2). The first sulfate anion accepts a total of nine hydrogen bonds, i.e. five from four hexaaquaaluminium complex cations, three from three solvent water molecules and one N—H···O hydrogen bond from one 2ap cation. The second sulfate anion accepts eight hydrogen bonds, i.e. five from five [Al(H2O)6]3+ cations, one from a free water molecule and two from one 2ap cation. The 2ap cation donates three N—H···O hydrogen bonds to the O atoms of two sulfate anions. One of the carbon-bound H atoms is involved in a weak hydrogen-bond interaction with an O atom of a solvent water molecule. Four free water molecules, namely O1W, O2W, O3W and O4W, are involved in 14 multidirectional O—H···O hydrogen bonds between coordinated water molecules of the [Al(H2O)6]3+ cations, sulfate O atoms and uncoordinated water molecules, forming an inorganic network parallel to the ab plane (Fig. 3a). The O1W molecule donates one hydrogen bond to O2W and one bond to a sulfate anion, and accepts one bond from the O22W atom. O2W donates two hydrogen bonds, i.e. one to O3W and another to a sulfate anion, and accepts two bonds from two solvation water molecules (O2W and O4W). O3W donates two hydrogen bonds to two sulfate anions and accepts two hydrogen bonds from two free water molecules (O4W and O2W). O4W donates two hydrogen bonds to two uncoordinated water molecules (O3W and O2W) and accepts one bond from the O11W atom.
In the crystal structure of (I), a three-dimensional supramolecular network is built from N—H···O, O—H···O and weak C—H···O hydrogen bonds involving the inorganic and organic parts of the structure (Table 2). Organic layers are built of π–π interacting stacks of 2ap cations (Table 3) connected to inorganic layers through N—H···O and C—H···O hydrogen bonds (Table 2 and Figs. 3b/c). The planes of all the 2ap rings are perpendicular to the [100] direction.
Isostructural compounds (II) and (III) (structure type 2) crystallize in the triclinic P1 space group. The asymmetric part of the unit cell contains two hexaaqua-coordinated MII ions (one of them lies on a centre of inversion with half occupancy), one protonated amine group which is disordered over two sites, two sulfate anions and one solvent water molecule (Fig. 4). Each MII atom is located at the centre of a distorted octahedron formed by six O atoms from six water molecules. The M—OW bond lengths are in the ranges 2.0343 (18)–2.1852 (17), 2.0513 (18)–2.1074 (17), 2.0178 (19)–2.1321 (18) and 2.0391 (17)–2.0961 (19) Å for Co1—OW, Co2—OW, Mg1—OW and Mg2—OW, respectively. The cis- and trans-OW—M—OW angles are 81.14 (7)–94.50 (7) and 172.42 (7)–178.16 (6)°, respectively, in the Co1 octahedron, 89.61 (8)–90.39 (8) and 180° in the Co2 octahedron, 85.29 (8)–98.30 (7) and 172.81 (9)–174.89 (8)° in the Mg1 octahedron, and 89.59 (8)–90.41 (8) and 180° (due to inversion symmetry) in the Mg2 octahedron Significant distortions in the coordination polyhedra of (II) and (III) are clearly evident (see Tables S2 and S3 in the Supporting information) and the most considerable distortions are observed in the case of the M1 environment, which does not lie on a centre of inversion.
The M1 octahedron donates eleven hydrogen bonds to six sulfate anions, donates one hydrogen bond to the O13W atom and accepts one hydrogen bond from the O11W water molecule (Fig. 5a), while the M2 octahedron donates eight hydrogen bonds to six sulfate anions and four hydrogen bonds to four solvent water molecules (Fig. 5b). The 2ap cations donate three N—H···O hydrogen bonds to O atoms in the main disordered part and three N—H···O hydrogen bonds in minor disordered part also. The orientationally disordered NH2 group has the minor disordered part attached to the C6 atom, instead of to C2. Reorientation from the first to the second position appears to be impossible due to the environment of the 2ap cation, and most likely is a result of incorrect alignment during the growth of the crystal. The NH2 groups are distributed between two positions with site occupancies equal to 0.121 (5) in the minor part of both (II) and (III).
Uncoordinated water molecule O1W donates two hydrogen bonds to two crystallographically independent sulfate anions and accepts two hydrogen bonds from two [MII(H2O)6]2+ cations. The first sulfate anion accepts ten hydrogen bonds, i.e. seven from four hexaaqua complexes, one from a free water molecule and two N—H···O hydrogen bonds from one 2ap cation. The second sulfate anion accepts eleven hydrogen bonds, i.e. eight from five [MII(H2O)6]2+ cations, one from a free water molecule and two from two 2ap cations. As a result, an inorganic network is formed through O—H···O hydrogen bonds between water molecules, sulfate anions and inorganic cations, and lies parallel to the ac plane (Tables 4 and 5, and Fig. 6a). Significant parallel π–π interactions between pairs of pyridinium rings (Table 3) assist in the formation of a supramolecular association along the a-axis direction and make the overall framework more stable (Fig. 6b). C—H···O hydrogen bonds are not observed in structure type 2.
Isostructural compounds (IV) and (V) crystallize in the triclinic P1 space group. In contrast to compounds (I)–(III), type 3, is characterized by the absence of noncoordinated water molecules. One half of an [M(H2O)6]2+ cation (located on an inversion centre), one sulfate anion and one 2ap cation form the asymmetric unit (see Fig. 7). The MII atom occupies the centre of a slightly distorted octahedron built by the coordination of six water molecules. The crystal packing reveals a layered arrangement of the inorganic and organic parts of the structure.
The M—OW bond lengths (see Tables S4 and S5 in the Supporting information) are 2.0503 (13)–2.0590 (17) and 2.0813 (19)–2.0996 (18) Å for salts (IV) and (V), respectively. The cis bond angles around the MII centres range from 86.63 (6) to 93.37 (6)° for (IV), and from 86.88 (8) to 93.12 (8)° for (IV). The trans angles are all equal to 180°. Geometric parameters are in accord with those reported for other Ni and Zn analogs (Fleck et al., 2004).
The [M(H2O)6]2+ cation donates twelve hydrogen bonds to six sulfate anions (see Fig. 8a). The SO42- anion accepts nine hydrogen bonds, i.e. six from three hexaaqua complexes and three N—H···O hydrogen bonds from two 2ap cations. The [M(H2O)6]2+ cation in salts (IV) and (V) are connected via hydrogen bonds from water molecules to sulfate anions, forming inorganic networks parallel to the ab plane (Fig. 8b). As inferred in Fig. 9, the crystal structure is represented by a series of successive layers: inorganic layers of [M(H2O)6]2+ cations connected to sulfate anions by hydrogen bonds and organic layers of 2ap cations, both being parallel to bc plane. The organic and inorganic layers are linked to each other by two types of hydrogen bonding, i.e. N—H···O and weak C—H···O, present in the crystal structure (Tables 5 and 6, and Fig. 9). This hydrogen-bonding interaction directs the infinite condensation of the respective building units. The crystal packings are further extended via π–π interactions between the 2ap rings in the a-axis direction (Table 3). Moreover, the C—H···O interactions result in the final three-dimensional supramolecular arrangement in type 3.
Hirshfeld surfaces (with dnorm mapped) and fingerprints (de versus di) were generated using Crystal Explorer for the 2ap cations in all of the reported structures along with the earlier studied copper-containing analog (VI) (Lukianova et al., 2015). Analysis of the Hirshfeld surfaces (Fig. 10) reveals several common features of the 2ap cations and highlights their roles in the crystal packing organization. The cation is characterized by the presence of three strong hydrogen-bond donors, while its planar structure provides the possibility for the existence of π–π interactions. The closest [immediate?] environment of the 2ap cation in all the structures is constructed in a similar manner. The cations are involved in strong double hydrogen-bond formation with the sulfate anion in order to produce a charge-assisted pair of composition [2ap···SO4]-. The pair is formed by two H atoms of the pyridinium ring (N1—H) and the amino group (N2—H) hydrogen bonded to two O atoms of the same sulfate anion. The fitted image reveals the distribution of sufate anions with respect to the 2ap cations (Fig. 11). It is worth noting that the remaining H atom of the amino group is hydrogen bonded to another sulfate anion in all of the reported structures. Thus, in hydrogen bonds of the N—H···O type, the role of the acceptor is played by the sulfate O atoms only. The weakest hydrogen bonds formed by the 2ap cations are of the C—H···O type, in which the acceptor O atoms belong to all possible oxygen-containing groups, viz. sulfate anions and coordinated and noncoordinated water molecules.
Another common feature of all the 2ap cations is their involvement in the formation of π–π interacting columns (Table 3) composed of antiparallel oriented cations. In all the structures, these columns propagate along the a axis. The mutual arrangement of these columns results in two different types of crystal packing. In structure types 1 [observed for Al analog (I)] and 2 [observed for Co analog (II) and Mg analog (III)], the columns are isolated and surrounded by inorganic sublattices (Figs. 3b/c and 6b). The second type of crystal packing is governed by the presence of π–π stacked columns aggregated into layers (Fig. 9) and is seen in structure types 3 [observed for Ni analog (IV) and Zn analog (V)] and 4 [observed for Cu analog (VI)]. As a result, alternating organic and inorganic layers are formed.
The fingerprint plots of the 2ap cations are all similar in shape (see Figs. S1–S4 in the Supporting information). They are characterized by the presence of spike pointing at around (di = 0.7, de = 1.1), which corresponds to hydrogen bonds of the N—H···O type. In all the plots, the contacts of inner H atoms dominate the surface area, with around 30% of the area corresponding to H···O contacts, around 40% to H···H contacts and 10–15% to π–π interactions. The strongest of the π–π interactions is illustrated by a presence of a red dot in the fingerprint plot of structure (VI) (Table 3).
In the current work, the results of structural studies of 2-aminopyridinium-templated metal (Al, Co, Mg, Ni and Zn) sulfate hydrates are reported for the first time. The templating role of 2ap is governed by the formation of characteristic charge-assisted hydrogen-bond pairs with sulfate anions and the presence of π–π interactions between the cations. In all of the studied compounds, as well as in the previously reported Cu analog, π–π interactions between the 2ap cations lead to the formation of columns with an antiparallel orientation of the cations. Another common feature of the compounds is the presence of hexaaqua-coordinated metal centres. Sulfate anions do not coordinate to the metal centres and are incorporated in diverse three-dimentional hydrogen-bonding networks, together with hexaaquametal octahedra and uncoordinated water molecules (if present). The mutual arrangement of π–π-interacting columns results in the formation of two modes of crystal packing, i.e. the first with isolated organic columns surrounded by the inorganic counterpart (structural types 1 and 2) and the second characterized by alternate organic–inorganic layers (structural types 3 and 4).
The title compounds were synthesized according to the previously described method of Lukianova et al. (2015). An aqueous solution (4 ml) of 2-aminopyridine (0.19 g, 2.0 mmol), the pH of which was adjusted to 2.5 by admixing 30% sulfuric acid, was added slowly to an aqueous solution (3 ml) containing the appropriate metal sulfate [2.0 mmol for (I), 3.0 mmol for (II), 3.0 mmol for (III), 1.0 mmol for (IV) and 1.0 mmol for (V)]. Single crystals of a suitable size were obtained by slow solvent evaporation under ambient conditions for a period of several weeks.
Crystal data, data collection and structure refinement details are summarized in Table 1. The positions of the amine H atoms were located initially in difference Fourier maps but were subsequently allowed to ride in the refinement, with C—H = 0.96 Å and N—H = 0.91 Å. The isotropic atomic displacement parameters of the H atoms were evaluated as 1.2Ueq of the parent atom. Water H atoms were located firstly in a difference Fourier map and then fixed, with O—H = 0.840 (2) Å and Uiso(H) = 1.5Ueq(O).
For all compounds, data collection: CrysAlis PRO (Rigaku Oxford Diffraction, 2015); cell refinement: CrysAlis PRO (Rigaku Oxford Diffraction, 2015); data reduction: CrysAlis PRO (Rigaku Oxford Diffraction, 2015). Program(s) used to solve structure: SHELXT (Sheldrick, 2015a) for (I), (III), (IV); SHELXS97 (Sheldrick, 2008) for (II), (V). For all compounds, program(s) used to refine structure: SHELXL2014 (Sheldrick, 2015b); molecular graphics: DIAMOND (Brandenburg, 1997); software used to prepare material for publication: OLEX2 (Dolomanov et al., 2009).
(C5H7N2)[Al(H2O)6](SO4)2·4H2O | Z = 2 |
Mr = 494.38 | F(000) = 520 |
Triclinic, P1 | Dx = 1.668 Mg m−3 |
a = 6.667 (3) Å | Mo Kα radiation, λ = 0.71073 Å |
b = 12.160 (4) Å | Cell parameters from 5322 reflections |
c = 12.911 (4) Å | θ = 2.2–29.5° |
α = 72.30 (3)° | µ = 0.41 mm−1 |
β = 81.03 (3)° | T = 100 K |
γ = 85.57 (3)° | Block, colourless |
V = 984.5 (7) Å3 | 0.50 × 0.33 × 0.20 mm |
Rigaku Oxford Diffraction Xcalibur Atlas diffractometer | 4751 independent reflections |
Radiation source: fine-focus sealed X-ray tube, Enhance (Mo) X-ray Source | 3685 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.027 |
Detector resolution: 10.6249 pixels mm-1 | θmax = 29.4°, θmin = 2.8° |
ω scans | h = −9→8 |
Absorption correction: analytical [CrysAlis PRO (Rigaku Oxford Diffraction, 2015), based on expressions derived by Clark & Reid (1995)] | k = −15→15 |
Tmin = 0.869, Tmax = 0.930 | l = −17→17 |
14826 measured reflections |
Refinement on F2 | 20 restraints |
Least-squares matrix: full | Hydrogen site location: mixed |
R[F2 > 2σ(F2)] = 0.036 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.093 | w = 1/[σ2(Fo2) + (0.042P)2 + 0.452P] where P = (Fo2 + 2Fc2)/3 |
S = 1.02 | (Δ/σ)max = 0.001 |
4751 reflections | Δρmax = 0.32 e Å−3 |
316 parameters | Δρmin = −0.62 e Å−3 |
(C5H7N2)[Al(H2O)6](SO4)2·4H2O | γ = 85.57 (3)° |
Mr = 494.38 | V = 984.5 (7) Å3 |
Triclinic, P1 | Z = 2 |
a = 6.667 (3) Å | Mo Kα radiation |
b = 12.160 (4) Å | µ = 0.41 mm−1 |
c = 12.911 (4) Å | T = 100 K |
α = 72.30 (3)° | 0.50 × 0.33 × 0.20 mm |
β = 81.03 (3)° |
Rigaku Oxford Diffraction Xcalibur Atlas diffractometer | 4751 independent reflections |
Absorption correction: analytical [CrysAlis PRO (Rigaku Oxford Diffraction, 2015), based on expressions derived by Clark & Reid (1995)] | 3685 reflections with I > 2σ(I) |
Tmin = 0.869, Tmax = 0.930 | Rint = 0.027 |
14826 measured reflections |
R[F2 > 2σ(F2)] = 0.036 | 20 restraints |
wR(F2) = 0.093 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.02 | Δρmax = 0.32 e Å−3 |
4751 reflections | Δρmin = −0.62 e Å−3 |
316 parameters |
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. |
x | y | z | Uiso*/Ueq | ||
Al1 | 0.5000 | 0.0000 | 0.5000 | 0.00796 (16) | |
O11W | 0.64761 (18) | 0.08727 (10) | 0.36697 (11) | 0.0105 (3) | |
H11A | 0.640 (3) | 0.0781 (18) | 0.3073 (14) | 0.016* | |
H11B | 0.762 (2) | 0.1150 (17) | 0.3618 (17) | 0.016* | |
O12W | 0.38678 (18) | 0.13785 (10) | 0.52461 (11) | 0.0105 (3) | |
H12A | 0.284 (3) | 0.1365 (18) | 0.5739 (15) | 0.016* | |
H12B | 0.361 (3) | 0.1918 (15) | 0.4703 (15) | 0.016* | |
O13W | 0.71181 (18) | 0.00732 (10) | 0.57732 (11) | 0.0105 (3) | |
H13A | 0.812 (3) | −0.0391 (16) | 0.5869 (17) | 0.016* | |
H13B | 0.726 (3) | 0.0623 (16) | 0.6018 (17) | 0.016* | |
Al2 | 0.5000 | 0.5000 | 0.5000 | 0.00801 (16) | |
O21W | 0.62866 (18) | 0.36833 (10) | 0.46954 (11) | 0.0105 (3) | |
H21A | 0.651 (3) | 0.3090 (15) | 0.5199 (15) | 0.016* | |
H21B | 0.729 (3) | 0.3711 (18) | 0.4194 (15) | 0.016* | |
O22W | 0.65215 (18) | 0.59526 (11) | 0.37401 (11) | 0.0118 (3) | |
H22A | 0.613 (3) | 0.6341 (17) | 0.3134 (14) | 0.018* | |
H22B | 0.762 (3) | 0.6215 (17) | 0.3759 (18) | 0.018* | |
O23W | 0.70379 (18) | 0.50546 (11) | 0.58517 (11) | 0.0114 (3) | |
H23A | 0.801 (3) | 0.4575 (16) | 0.5978 (17) | 0.017* | |
H23B | 0.718 (3) | 0.5610 (16) | 0.6071 (18) | 0.017* | |
S1 | 0.91029 (6) | 0.20997 (3) | 0.68614 (4) | 0.00876 (11) | |
O11 | 0.84308 (18) | 0.20057 (10) | 0.80334 (10) | 0.0121 (3) | |
O12 | 0.98659 (18) | 0.32749 (10) | 0.62760 (11) | 0.0129 (3) | |
O13 | 0.73407 (18) | 0.19311 (10) | 0.63619 (10) | 0.0116 (3) | |
O14 | 1.06889 (18) | 0.12046 (10) | 0.67919 (11) | 0.0139 (3) | |
S2 | 0.09053 (6) | 0.28132 (3) | 0.31390 (4) | 0.00884 (11) | |
O21 | 0.00743 (17) | 0.16827 (10) | 0.38119 (10) | 0.0124 (3) | |
O22 | 0.27136 (18) | 0.30327 (10) | 0.35807 (10) | 0.0120 (3) | |
O23 | −0.06040 (18) | 0.37597 (10) | 0.31594 (11) | 0.0142 (3) | |
O24 | 0.15050 (19) | 0.27888 (10) | 0.19974 (10) | 0.0139 (3) | |
N1 | 0.2134 (2) | 0.47940 (12) | 0.03559 (13) | 0.0134 (3) | |
H1 | 0.1694 | 0.4196 | 0.0875 | 0.016* | |
C2 | 0.1898 (3) | 0.58361 (15) | 0.05441 (15) | 0.0131 (4) | |
N2 | 0.0992 (2) | 0.58848 (13) | 0.15262 (13) | 0.0173 (3) | |
H2A | 0.0574 | 0.5264 | 0.2021 | 0.021* | |
H2B | 0.0825 | 0.6537 | 0.1665 | 0.021* | |
C3 | 0.2632 (3) | 0.68047 (15) | −0.03180 (16) | 0.0155 (4) | |
H3 | 0.2504 | 0.7535 | −0.0220 | 0.019* | |
C4 | 0.3527 (3) | 0.66674 (16) | −0.12932 (17) | 0.0180 (4) | |
H4 | 0.4009 | 0.7309 | −0.1860 | 0.022* | |
C5 | 0.3737 (3) | 0.55711 (17) | −0.14604 (16) | 0.0174 (4) | |
H5 | 0.4341 | 0.5481 | −0.2131 | 0.021* | |
C6 | 0.3037 (3) | 0.46511 (16) | −0.06194 (16) | 0.0150 (4) | |
H6 | 0.3173 | 0.3917 | −0.0707 | 0.018* | |
O1W | 0.4378 (2) | 0.27903 (11) | 0.81670 (11) | 0.0156 (3) | |
H1WA | 0.555 (3) | 0.2484 (18) | 0.8117 (19) | 0.023* | |
H1WB | 0.360 (3) | 0.2229 (16) | 0.8478 (18) | 0.023* | |
O2W | 0.1749 (2) | 0.10078 (12) | 0.92133 (12) | 0.0181 (3) | |
H2WA | 0.061 (3) | 0.1135 (19) | 0.9014 (19) | 0.027* | |
H2WB | 0.164 (4) | 0.091 (2) | 0.9861 (14) | 0.027* | |
O3W | 0.1666 (2) | 0.07501 (12) | 0.14593 (12) | 0.0180 (3) | |
H3WA | 0.089 (3) | 0.0290 (17) | 0.1929 (16) | 0.027* | |
H3WB | 0.141 (3) | 0.1356 (16) | 0.1639 (19) | 0.027* | |
O4W | 0.5926 (2) | 0.05318 (12) | 0.18214 (12) | 0.0189 (3) | |
H4WA | 0.471 (3) | 0.0479 (19) | 0.1738 (19) | 0.028* | |
H4WB | 0.665 (3) | 0.0103 (18) | 0.1544 (19) | 0.028* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Al1 | 0.0075 (3) | 0.0073 (3) | 0.0095 (4) | −0.0004 (3) | −0.0019 (3) | −0.0027 (3) |
O11W | 0.0096 (6) | 0.0129 (6) | 0.0095 (7) | −0.0033 (5) | −0.0007 (5) | −0.0038 (5) |
O12W | 0.0113 (6) | 0.0093 (6) | 0.0098 (7) | 0.0009 (5) | −0.0012 (5) | −0.0016 (5) |
O13W | 0.0103 (6) | 0.0084 (6) | 0.0155 (7) | 0.0014 (5) | −0.0055 (5) | −0.0060 (5) |
Al2 | 0.0078 (3) | 0.0071 (3) | 0.0089 (4) | −0.0005 (3) | −0.0018 (3) | −0.0017 (3) |
O21W | 0.0112 (6) | 0.0088 (6) | 0.0107 (7) | 0.0010 (5) | −0.0013 (5) | −0.0019 (5) |
O22W | 0.0095 (6) | 0.0127 (6) | 0.0120 (7) | −0.0026 (5) | −0.0026 (5) | −0.0011 (5) |
O23W | 0.0118 (6) | 0.0088 (6) | 0.0159 (7) | 0.0011 (5) | −0.0052 (5) | −0.0059 (5) |
S1 | 0.0083 (2) | 0.0082 (2) | 0.0099 (2) | 0.00001 (15) | −0.00166 (16) | −0.00276 (17) |
O11 | 0.0130 (6) | 0.0146 (6) | 0.0095 (6) | 0.0005 (5) | −0.0013 (5) | −0.0049 (5) |
O12 | 0.0112 (6) | 0.0090 (6) | 0.0165 (7) | −0.0023 (5) | −0.0036 (5) | 0.0003 (5) |
O13 | 0.0120 (6) | 0.0108 (6) | 0.0134 (7) | −0.0013 (5) | −0.0039 (5) | −0.0045 (5) |
O14 | 0.0128 (6) | 0.0128 (6) | 0.0141 (7) | 0.0041 (5) | −0.0007 (5) | −0.0031 (5) |
S2 | 0.0086 (2) | 0.0083 (2) | 0.0096 (2) | −0.00033 (15) | −0.00152 (16) | −0.00245 (17) |
O21 | 0.0103 (6) | 0.0098 (6) | 0.0157 (7) | −0.0020 (5) | −0.0022 (5) | −0.0009 (5) |
O22 | 0.0123 (6) | 0.0097 (6) | 0.0143 (7) | −0.0024 (5) | −0.0037 (5) | −0.0025 (5) |
O23 | 0.0134 (6) | 0.0120 (6) | 0.0147 (7) | 0.0029 (5) | −0.0006 (5) | −0.0018 (5) |
O24 | 0.0187 (6) | 0.0131 (6) | 0.0105 (7) | −0.0003 (5) | −0.0011 (5) | −0.0048 (5) |
N1 | 0.0142 (7) | 0.0108 (7) | 0.0150 (8) | −0.0015 (6) | −0.0031 (6) | −0.0025 (6) |
C2 | 0.0100 (8) | 0.0147 (9) | 0.0160 (10) | −0.0004 (7) | −0.0049 (7) | −0.0050 (8) |
N2 | 0.0261 (9) | 0.0110 (7) | 0.0157 (9) | −0.0030 (6) | −0.0005 (7) | −0.0059 (7) |
C3 | 0.0156 (9) | 0.0108 (8) | 0.0196 (10) | −0.0002 (7) | −0.0058 (8) | −0.0024 (8) |
C4 | 0.0142 (9) | 0.0177 (9) | 0.0168 (10) | −0.0016 (7) | −0.0038 (8) | 0.0038 (8) |
C5 | 0.0135 (9) | 0.0252 (10) | 0.0134 (10) | 0.0014 (7) | −0.0036 (7) | −0.0051 (8) |
C6 | 0.0119 (8) | 0.0184 (9) | 0.0178 (10) | 0.0025 (7) | −0.0052 (7) | −0.0091 (8) |
O1W | 0.0119 (6) | 0.0159 (7) | 0.0168 (7) | 0.0010 (5) | −0.0001 (6) | −0.0032 (6) |
O2W | 0.0168 (7) | 0.0233 (7) | 0.0145 (7) | −0.0002 (6) | −0.0040 (6) | −0.0050 (6) |
O3W | 0.0265 (7) | 0.0128 (7) | 0.0153 (8) | −0.0023 (5) | −0.0023 (6) | −0.0049 (6) |
O4W | 0.0195 (7) | 0.0206 (7) | 0.0196 (8) | 0.0015 (6) | −0.0043 (6) | −0.0098 (6) |
Al1—O11Wi | 1.8896 (15) | S1—O14 | 1.4707 (13) |
Al1—O11W | 1.8896 (15) | S2—O21 | 1.4808 (14) |
Al1—O12Wi | 1.8799 (13) | S2—O22 | 1.4855 (13) |
Al1—O12W | 1.8799 (13) | S2—O23 | 1.4728 (13) |
Al1—O13Wi | 1.8739 (14) | S2—O24 | 1.4745 (14) |
Al1—O13W | 1.8740 (14) | N1—H1 | 0.8600 |
O11W—H11A | 0.821 (15) | N1—C2 | 1.354 (2) |
O11W—H11B | 0.841 (15) | N1—C6 | 1.363 (2) |
O12W—H12A | 0.859 (15) | C2—N2 | 1.333 (2) |
O12W—H12B | 0.833 (15) | C2—C3 | 1.410 (3) |
O13W—H13A | 0.842 (15) | N2—H2A | 0.8600 |
O13W—H13B | 0.839 (15) | N2—H2B | 0.8600 |
Al2—O21Wii | 1.8760 (13) | C3—H3 | 0.9300 |
Al2—O21W | 1.8760 (13) | C3—C4 | 1.359 (3) |
Al2—O22Wii | 1.8810 (16) | C4—H4 | 0.9300 |
Al2—O22W | 1.8810 (16) | C4—C5 | 1.407 (3) |
Al2—O23Wii | 1.8930 (14) | C5—H5 | 0.9300 |
Al2—O23W | 1.8930 (14) | C5—C6 | 1.354 (3) |
O21W—H21A | 0.833 (15) | C6—H6 | 0.9300 |
O21W—H21B | 0.852 (15) | O1W—H1WA | 0.841 (15) |
O22W—H22A | 0.850 (15) | O1W—H1WB | 0.849 (16) |
O22W—H22B | 0.830 (15) | O2W—H2WA | 0.825 (16) |
O23W—H23A | 0.837 (15) | O2W—H2WB | 0.800 (16) |
O23W—H23B | 0.825 (15) | O3W—H3WA | 0.831 (16) |
S1—O11 | 1.4815 (14) | O3W—H3WB | 0.836 (16) |
S1—O12 | 1.4859 (14) | O4W—H4WA | 0.845 (16) |
S1—O13 | 1.4806 (13) | O4W—H4WB | 0.808 (16) |
O11Wi—Al1—O11W | 180.0 | Al2—O22W—H22B | 122.3 (15) |
O12W—Al1—O11W | 89.45 (6) | H22A—O22W—H22B | 107 (2) |
O12Wi—Al1—O11Wi | 89.45 (6) | Al2—O23W—H23A | 125.2 (14) |
O12Wi—Al1—O11W | 90.54 (6) | Al2—O23W—H23B | 123.8 (15) |
O12W—Al1—O11Wi | 90.55 (6) | H23A—O23W—H23B | 110 (2) |
O12Wi—Al1—O12W | 180.0 | O11—S1—O12 | 109.44 (8) |
O13W—Al1—O11Wi | 89.07 (6) | O13—S1—O11 | 108.96 (8) |
O13W—Al1—O11W | 90.93 (6) | O13—S1—O12 | 108.18 (8) |
O13Wi—Al1—O11Wi | 90.93 (6) | O14—S1—O11 | 108.71 (8) |
O13Wi—Al1—O11W | 89.07 (6) | O14—S1—O12 | 111.37 (8) |
O13W—Al1—O12W | 89.22 (6) | O14—S1—O13 | 110.15 (7) |
O13Wi—Al1—O12W | 90.78 (6) | O21—S2—O22 | 109.45 (8) |
O13W—Al1—O12Wi | 90.78 (6) | O23—S2—O21 | 111.23 (8) |
O13Wi—Al1—O12Wi | 89.22 (6) | O23—S2—O22 | 108.31 (7) |
O13Wi—Al1—O13W | 180.0 | O23—S2—O24 | 109.38 (8) |
Al1—O11W—H11A | 123.1 (15) | O24—S2—O21 | 109.05 (8) |
Al1—O11W—H11B | 124.4 (15) | O24—S2—O22 | 109.40 (8) |
H11A—O11W—H11B | 107 (2) | C2—N1—H1 | 118.5 |
Al1—O12W—H12A | 120.6 (14) | C2—N1—C6 | 122.95 (16) |
Al1—O12W—H12B | 117.7 (14) | C6—N1—H1 | 118.5 |
H12A—O12W—H12B | 105 (2) | N1—C2—C3 | 117.53 (16) |
Al1—O13W—H13A | 126.0 (14) | N2—C2—N1 | 118.35 (17) |
Al1—O13W—H13B | 123.9 (14) | N2—C2—C3 | 124.12 (16) |
H13A—O13W—H13B | 109.8 (19) | C2—N2—H2A | 120.0 |
O21Wii—Al2—O21W | 180.00 (4) | C2—N2—H2B | 120.0 |
O21Wii—Al2—O22W | 89.68 (6) | H2A—N2—H2B | 120.0 |
O21W—Al2—O22Wii | 89.68 (6) | C2—C3—H3 | 120.1 |
O21Wii—Al2—O22Wii | 90.32 (6) | C4—C3—C2 | 119.75 (16) |
O21W—Al2—O22W | 90.32 (6) | C4—C3—H3 | 120.1 |
O21Wii—Al2—O23Wii | 90.26 (6) | C3—C4—H4 | 119.4 |
O21W—Al2—O23W | 90.26 (6) | C3—C4—C5 | 121.12 (18) |
O21Wii—Al2—O23W | 89.74 (6) | C5—C4—H4 | 119.4 |
O21W—Al2—O23Wii | 89.74 (6) | C4—C5—H5 | 120.9 |
O22W—Al2—O22Wii | 180.0 | C6—C5—C4 | 118.21 (18) |
O22W—Al2—O23Wii | 89.63 (6) | C6—C5—H5 | 120.9 |
O22Wii—Al2—O23Wii | 90.37 (6) | N1—C6—H6 | 119.8 |
O22W—Al2—O23W | 90.37 (6) | C5—C6—N1 | 120.44 (16) |
O22Wii—Al2—O23W | 89.63 (6) | C5—C6—H6 | 119.8 |
O23Wii—Al2—O23W | 180.0 | H1WA—O1W—H1WB | 105 (2) |
Al2—O21W—H21A | 121.2 (14) | H2WA—O2W—H2WB | 109 (2) |
Al2—O21W—H21B | 123.4 (14) | H3WA—O3W—H3WB | 102 (2) |
H21A—O21W—H21B | 105 (2) | H4WA—O4W—H4WB | 109 (2) |
Al2—O22W—H22A | 128.9 (15) | ||
N1—C2—C3—C4 | 0.3 (3) | C3—C4—C5—C6 | −0.5 (3) |
C2—N1—C6—C5 | −0.5 (3) | C4—C5—C6—N1 | 0.8 (3) |
C2—C3—C4—C5 | 0.0 (3) | C6—N1—C2—N2 | 179.93 (16) |
N2—C2—C3—C4 | −179.69 (17) | C6—N1—C2—C3 | −0.1 (2) |
Symmetry codes: (i) −x+1, −y, −z+1; (ii) −x+1, −y+1, −z+1. |
D—H···A | D—H | H···A | D···A | D—H···A |
O11W—H11A···O4W | 0.82 (2) | 1.81 (2) | 2.626 (2) | 173 (2) |
O11W—H11B···O21iii | 0.84 (2) | 1.89 (2) | 2.715 (2) | 168 (2) |
O12W—H12A···O14iv | 0.86 (2) | 1.79 (2) | 2.648 (2) | 175 (2) |
O12W—H12B···O22 | 0.83 (2) | 1.80 (2) | 2.628 (2) | 173 (2) |
O13W—H13A···O21i | 0.84 (2) | 1.88 (2) | 2.711 (2) | 167 (2) |
O13W—H13B···O13 | 0.84 (2) | 1.78 (2) | 2.6144 (18) | 171 (2) |
O21W—H21A···O13 | 0.83 (2) | 1.84 (2) | 2.667 (2) | 170 (2) |
O21W—H21B···O23iii | 0.85 (2) | 1.77 (2) | 2.622 (2) | 180 (3) |
O22W—H22A···O1Wii | 0.85 (2) | 1.76 (2) | 2.606 (2) | 173 (2) |
O22W—H22B···O12v | 0.83 (2) | 1.82 (2) | 2.647 (2) | 175 (2) |
O23W—H23A···O12 | 0.84 (2) | 1.91 (2) | 2.740 (2) | 169 (2) |
O23W—H23B···O22ii | 0.83 (2) | 1.85 (2) | 2.6660 (18) | 172 (2) |
N1—H1···O24 | 0.86 | 1.87 | 2.711 (2) | 164 |
N2—H2A···O23 | 0.86 | 2.09 | 2.944 (2) | 176 |
N2—H2B···O11ii | 0.86 | 2.04 | 2.856 (2) | 159 |
C6—H6···O1Wvi | 0.93 | 2.30 | 3.127 (2) | 147 |
O1W—H1WA···O11 | 0.84 (2) | 1.96 (2) | 2.792 (2) | 170 (2) |
O1W—H1WB···O2W | 0.85 (2) | 1.92 (2) | 2.768 (2) | 177 (2) |
O2W—H2WA···O11iv | 0.83 (2) | 2.09 (2) | 2.864 (2) | 156 (2) |
O2W—H2WB···O3Wvii | 0.80 (2) | 2.02 (2) | 2.812 (2) | 173 (2) |
O3W—H3WA···O14i | 0.83 (2) | 2.25 (2) | 3.069 (2) | 169 (2) |
O3W—H3WB···O24 | 0.84 (2) | 1.94 (2) | 2.7609 (19) | 166 (2) |
O4W—H4WA···O3W | 0.85 (2) | 2.10 (2) | 2.929 (2) | 167 (2) |
O4W—H4WB···O2Wi | 0.81 (2) | 2.04 (2) | 2.849 (2) | 175 (2) |
Symmetry codes: (i) −x+1, −y, −z+1; (ii) −x+1, −y+1, −z+1; (iii) x+1, y, z; (iv) x−1, y, z; (v) −x+2, −y+1, −z+1; (vi) x, y, z−1; (vii) x, y, z+1. |
(C5H7N2)2[Co(H2O)6]3(SO4)4·2H2O | Z = 1 |
Mr = 1111.60 | F(000) = 575 |
Triclinic, P1 | Dx = 1.812 Mg m−3 |
a = 6.640 (3) Å | Mo Kα radiation, λ = 0.71073 Å |
b = 11.710 (4) Å | Cell parameters from 5917 reflections |
c = 14.294 (4) Å | θ = 3.1–29.1° |
α = 67.97 (3)° | µ = 1.53 mm−1 |
β = 81.57 (3)° | T = 100 K |
γ = 85.39 (3)° | Plate, red |
V = 1018.8 (7) Å3 | 0.42 × 0.27 × 0.08 mm |
Rigaku Oxford Diffraction Xcalibur Atlas diffractometer | 4878 independent reflections |
Radiation source: fine-focus sealed X-ray tube, Enhance (Mo) X-ray Source | 4072 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.025 |
Detector resolution: 10.6249 pixels mm-1 | θmax = 29.6°, θmin = 2.8° |
ω scans | h = −8→8 |
Absorption correction: analytical [CrysAlis PRO (Rigaku Oxford Diffraction, 2015), based on expressions derived by Clark & Reid (1995)] | k = −15→15 |
Tmin = 0.609, Tmax = 0.891 | l = −18→19 |
14070 measured reflections |
Refinement on F2 | 20 restraints |
Least-squares matrix: full | Hydrogen site location: mixed |
R[F2 > 2σ(F2)] = 0.031 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.069 | w = 1/[σ2(Fo2) + (0.024P)2 + 0.719P] where P = (Fo2 + 2Fc2)/3 |
S = 1.06 | (Δ/σ)max = 0.001 |
4878 reflections | Δρmax = 0.42 e Å−3 |
321 parameters | Δρmin = −0.44 e Å−3 |
(C5H7N2)2[Co(H2O)6]3(SO4)4·2H2O | γ = 85.39 (3)° |
Mr = 1111.60 | V = 1018.8 (7) Å3 |
Triclinic, P1 | Z = 1 |
a = 6.640 (3) Å | Mo Kα radiation |
b = 11.710 (4) Å | µ = 1.53 mm−1 |
c = 14.294 (4) Å | T = 100 K |
α = 67.97 (3)° | 0.42 × 0.27 × 0.08 mm |
β = 81.57 (3)° |
Rigaku Oxford Diffraction Xcalibur Atlas diffractometer | 4878 independent reflections |
Absorption correction: analytical [CrysAlis PRO (Rigaku Oxford Diffraction, 2015), based on expressions derived by Clark & Reid (1995)] | 4072 reflections with I > 2σ(I) |
Tmin = 0.609, Tmax = 0.891 | Rint = 0.025 |
14070 measured reflections |
R[F2 > 2σ(F2)] = 0.031 | 20 restraints |
wR(F2) = 0.069 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.06 | Δρmax = 0.42 e Å−3 |
4878 reflections | Δρmin = −0.44 e Å−3 |
321 parameters |
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. |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
Co1 | 0.81730 (4) | 0.24175 (2) | 0.48940 (2) | 0.01270 (8) | |
O11W | 1.0930 (2) | 0.15648 (15) | 0.54025 (13) | 0.0193 (3) | |
H11A | 1.117 (4) | 0.0828 (16) | 0.550 (2) | 0.029* | |
H11B | 1.148 (4) | 0.173 (2) | 0.5808 (17) | 0.029* | |
O12W | 0.5454 (2) | 0.33969 (14) | 0.44448 (12) | 0.0163 (3) | |
H12A | 0.482 (3) | 0.327 (2) | 0.4027 (16) | 0.024* | |
H12B | 0.557 (4) | 0.4142 (16) | 0.4194 (19) | 0.024* | |
O13W | 0.8355 (2) | 0.11152 (13) | 0.41171 (12) | 0.0154 (3) | |
H13A | 0.928 (3) | 0.133 (2) | 0.3645 (16) | 0.023* | |
H13B | 0.736 (3) | 0.117 (2) | 0.3823 (18) | 0.023* | |
O14W | 0.8099 (2) | 0.36353 (15) | 0.56340 (13) | 0.0213 (4) | |
H14A | 0.905 (3) | 0.370 (2) | 0.5927 (19) | 0.032* | |
H14B | 0.701 (3) | 0.373 (2) | 0.5938 (19) | 0.032* | |
O15W | 0.6390 (2) | 0.12358 (14) | 0.60913 (12) | 0.0195 (3) | |
H15A | 0.618 (4) | 0.0507 (16) | 0.621 (2) | 0.029* | |
H15B | 0.530 (3) | 0.151 (2) | 0.6307 (19) | 0.029* | |
O16W | 0.9640 (2) | 0.36329 (14) | 0.35903 (13) | 0.0235 (4) | |
H16A | 1.089 (3) | 0.356 (3) | 0.341 (2) | 0.035* | |
H16B | 0.950 (4) | 0.4385 (17) | 0.350 (2) | 0.035* | |
Co2 | 1.0000 | 0.5000 | 0.0000 | 0.01264 (10) | |
O21W | 1.0568 (2) | 0.57791 (18) | 0.09997 (14) | 0.0279 (4) | |
H21A | 0.968 (4) | 0.614 (3) | 0.126 (2) | 0.042* | |
H21B | 1.163 (3) | 0.578 (3) | 0.122 (2) | 0.042* | |
O22W | 0.8877 (3) | 0.34331 (17) | 0.12342 (14) | 0.0354 (5) | |
H22A | 0.946 (4) | 0.314 (3) | 0.1730 (18) | 0.053* | |
H22B | 0.766 (3) | 0.322 (3) | 0.139 (2) | 0.053* | |
O23W | 0.7093 (2) | 0.57899 (16) | −0.00391 (12) | 0.0239 (4) | |
H23A | 0.626 (4) | 0.563 (2) | 0.0473 (16) | 0.036* | |
H23B | 0.661 (4) | 0.625 (2) | −0.0543 (16) | 0.036* | |
S1 | 0.26050 (7) | 0.32185 (5) | 0.71193 (4) | 0.01344 (11) | |
O11 | 0.2389 (2) | 0.28812 (14) | 0.82416 (11) | 0.0227 (4) | |
O12 | 0.4429 (2) | 0.39702 (14) | 0.66754 (13) | 0.0240 (4) | |
O13 | 0.0779 (2) | 0.39364 (13) | 0.67393 (12) | 0.0199 (3) | |
O14 | 0.2811 (2) | 0.20808 (13) | 0.68886 (11) | 0.0158 (3) | |
S2 | 0.37373 (7) | 0.21252 (5) | 0.26165 (4) | 0.01285 (11) | |
O21 | 0.3555 (2) | 0.31783 (13) | 0.29681 (11) | 0.0160 (3) | |
O22 | 0.4874 (2) | 0.11002 (13) | 0.33098 (11) | 0.0181 (3) | |
O23 | 0.1693 (2) | 0.17496 (14) | 0.25939 (11) | 0.0175 (3) | |
O24 | 0.4888 (2) | 0.25378 (13) | 0.15788 (11) | 0.0163 (3) | |
N1 | 0.2263 (3) | 0.06643 (18) | 0.97837 (15) | 0.0226 (4) | |
H1 | 0.2200 | 0.1354 | 0.9280 | 0.027* | |
C2 | 0.2830 (3) | −0.0361 (2) | 0.95853 (18) | 0.0218 (5) | |
H2 | 0.3148 | −0.0327 | 0.8920 | 0.026* | 0.121 (5) |
N2 | 0.3252 (3) | −0.0250 (2) | 0.86323 (16) | 0.0204 (6) | 0.879 (5) |
H2A | 0.3163 | 0.0461 | 0.8156 | 0.024* | 0.879 (5) |
H2B | 0.3618 | −0.0889 | 0.8483 | 0.024* | 0.879 (5) |
C3 | 0.2927 (3) | −0.1489 (2) | 1.04194 (19) | 0.0251 (5) | |
H3 | 0.3328 | −0.2213 | 1.0311 | 0.030* | |
C4 | 0.2426 (3) | −0.1506 (2) | 1.13858 (18) | 0.0261 (5) | |
H4 | 0.2474 | −0.2249 | 1.1935 | 0.031* | |
C5 | 0.1840 (3) | −0.0419 (2) | 1.15618 (19) | 0.0284 (6) | |
H5 | 0.1498 | −0.0432 | 1.2220 | 0.034* | |
C6 | 0.1785 (3) | 0.0660 (2) | 1.07421 (19) | 0.0257 (5) | |
H6 | 0.1418 | 0.1394 | 1.0840 | 0.031* | 0.879 (5) |
O1W | 0.5638 (2) | 0.45007 (14) | 0.83619 (11) | 0.0165 (3) | |
H1WA | 0.5340 | 0.4310 | 0.7882 | 0.025* | |
H1WB | 0.5789 | 0.5279 | 0.7883 | 0.025* | |
N2A | 0.1513 (18) | 0.1596 (12) | 1.0656 (10) | 0.009 (4)* | 0.121 (5) |
H2AA | 0.1622 | 0.2162 | 1.0058 | 0.011* | 0.121 (5) |
H2AB | 0.1184 | 0.1789 | 1.1184 | 0.011* | 0.121 (5) |
U11 | U22 | U33 | U12 | U13 | U23 | |
Co1 | 0.01207 (14) | 0.01120 (15) | 0.01479 (15) | 0.00019 (10) | −0.00248 (11) | −0.00455 (11) |
O11W | 0.0188 (8) | 0.0158 (8) | 0.0283 (9) | 0.0050 (6) | −0.0122 (7) | −0.0116 (7) |
O12W | 0.0176 (8) | 0.0140 (8) | 0.0189 (8) | 0.0016 (6) | −0.0085 (6) | −0.0061 (7) |
O13W | 0.0127 (7) | 0.0169 (8) | 0.0162 (8) | −0.0010 (6) | −0.0018 (6) | −0.0057 (6) |
O14W | 0.0131 (8) | 0.0274 (9) | 0.0323 (10) | 0.0012 (7) | −0.0052 (7) | −0.0205 (8) |
O15W | 0.0197 (8) | 0.0128 (8) | 0.0225 (8) | 0.0001 (6) | 0.0047 (7) | −0.0054 (7) |
O16W | 0.0171 (8) | 0.0126 (8) | 0.0342 (10) | 0.0004 (6) | 0.0065 (7) | −0.0048 (7) |
Co2 | 0.00979 (18) | 0.0159 (2) | 0.0120 (2) | −0.00087 (14) | −0.00193 (15) | −0.00457 (16) |
O21W | 0.0177 (8) | 0.0449 (11) | 0.0370 (10) | 0.0075 (8) | −0.0107 (8) | −0.0320 (9) |
O22W | 0.0212 (9) | 0.0399 (11) | 0.0271 (10) | −0.0156 (8) | −0.0124 (8) | 0.0146 (8) |
O23W | 0.0129 (8) | 0.0377 (10) | 0.0156 (8) | 0.0077 (7) | −0.0028 (6) | −0.0048 (8) |
S1 | 0.0124 (2) | 0.0121 (3) | 0.0173 (3) | 0.00063 (18) | −0.0042 (2) | −0.0064 (2) |
O11 | 0.0365 (9) | 0.0174 (8) | 0.0170 (8) | 0.0074 (7) | −0.0087 (7) | −0.0092 (7) |
O12 | 0.0168 (8) | 0.0189 (8) | 0.0397 (10) | −0.0058 (6) | 0.0030 (7) | −0.0161 (8) |
O13 | 0.0191 (8) | 0.0145 (8) | 0.0290 (9) | 0.0040 (6) | −0.0122 (7) | −0.0090 (7) |
O14 | 0.0169 (7) | 0.0129 (7) | 0.0195 (8) | −0.0003 (6) | −0.0029 (6) | −0.0079 (6) |
S2 | 0.0113 (2) | 0.0132 (3) | 0.0146 (3) | −0.00040 (18) | −0.0019 (2) | −0.0056 (2) |
O21 | 0.0166 (7) | 0.0138 (7) | 0.0190 (8) | 0.0005 (6) | −0.0033 (6) | −0.0075 (6) |
O22 | 0.0195 (8) | 0.0124 (7) | 0.0205 (8) | 0.0006 (6) | −0.0061 (6) | −0.0031 (6) |
O23 | 0.0130 (7) | 0.0229 (8) | 0.0202 (8) | −0.0039 (6) | −0.0010 (6) | −0.0116 (7) |
O24 | 0.0135 (7) | 0.0191 (8) | 0.0155 (8) | −0.0007 (6) | 0.0007 (6) | −0.0063 (6) |
N1 | 0.0182 (9) | 0.0191 (10) | 0.0247 (11) | −0.0016 (7) | −0.0063 (8) | 0.0001 (8) |
C2 | 0.0089 (10) | 0.0292 (13) | 0.0210 (12) | −0.0040 (9) | −0.0030 (9) | −0.0009 (10) |
N2 | 0.0238 (12) | 0.0161 (11) | 0.0208 (12) | 0.0019 (8) | −0.0013 (9) | −0.0073 (9) |
C3 | 0.0165 (11) | 0.0203 (12) | 0.0299 (14) | −0.0002 (9) | −0.0031 (10) | 0.0005 (10) |
C4 | 0.0187 (11) | 0.0288 (14) | 0.0211 (12) | −0.0044 (9) | −0.0039 (10) | 0.0030 (10) |
C5 | 0.0199 (12) | 0.0374 (15) | 0.0231 (13) | −0.0077 (10) | −0.0056 (10) | −0.0033 (11) |
C6 | 0.0208 (12) | 0.0300 (14) | 0.0268 (13) | −0.0058 (10) | −0.0065 (10) | −0.0087 (11) |
O1W | 0.0183 (7) | 0.0168 (8) | 0.0166 (8) | −0.0018 (6) | −0.0043 (6) | −0.0075 (6) |
Co1—O11W | 2.1042 (17) | O23W—H23B | 0.811 (17) |
Co1—O12W | 2.1074 (17) | S1—O11 | 1.4888 (17) |
Co1—O13W | 2.1852 (17) | S1—O12 | 1.4735 (17) |
Co1—O14W | 2.0640 (17) | S1—O13 | 1.4689 (16) |
Co1—O15W | 2.0343 (18) | S1—O14 | 1.4797 (16) |
Co1—O16W | 2.0368 (19) | S2—O21 | 1.4869 (16) |
O11W—H11A | 0.827 (17) | S2—O22 | 1.4744 (16) |
O11W—H11B | 0.813 (17) | S2—O23 | 1.4687 (16) |
O12W—H12A | 0.838 (16) | S2—O24 | 1.4855 (16) |
O12W—H12B | 0.815 (16) | N1—H1 | 0.8600 |
O13W—H13A | 0.819 (16) | N1—C2 | 1.347 (3) |
O13W—H13B | 0.819 (16) | N1—C6 | 1.358 (3) |
O14W—H14A | 0.828 (17) | C2—H2 | 0.9300 |
O14W—H14B | 0.810 (17) | C2—N2 | 1.309 (3) |
O15W—H15A | 0.824 (17) | C2—C3 | 1.414 (3) |
O15W—H15B | 0.830 (16) | N2—H2A | 0.8600 |
O16W—H16A | 0.840 (17) | N2—H2B | 0.8600 |
O16W—H16B | 0.839 (17) | C3—H3 | 0.9300 |
Co2—O21Wi | 2.0513 (18) | C3—C4 | 1.366 (4) |
Co2—O21W | 2.0513 (18) | C4—H4 | 0.9300 |
Co2—O22Wi | 2.1073 (19) | C4—C5 | 1.402 (4) |
Co2—O22W | 2.1073 (19) | C5—H5 | 0.9300 |
Co2—O23Wi | 2.0715 (17) | C5—C6 | 1.365 (3) |
Co2—O23W | 2.0715 (17) | C6—H6 | 0.9300 |
O21W—H21A | 0.817 (17) | C6—N2A | 1.060 (13) |
O21W—H21B | 0.818 (17) | O1W—H1WA | 0.8493 |
O22W—H22A | 0.804 (18) | O1W—H1WB | 0.9143 |
O22W—H22B | 0.837 (17) | N2A—H2AA | 0.8600 |
O23W—H23A | 0.819 (17) | N2A—H2AB | 0.8600 |
O11W—Co1—O12W | 174.53 (6) | Co2—O21W—H21B | 129 (2) |
O11W—Co1—O13W | 84.79 (6) | H21A—O21W—H21B | 109 (3) |
O12W—Co1—O13W | 100.63 (6) | Co2—O22W—H22A | 121 (2) |
O14W—Co1—O11W | 93.44 (7) | Co2—O22W—H22B | 126 (2) |
O14W—Co1—O12W | 81.14 (7) | H22A—O22W—H22B | 109 (3) |
O14W—Co1—O13W | 178.16 (6) | Co2—O23W—H23A | 121.8 (19) |
O15W—Co1—O11W | 94.50 (7) | Co2—O23W—H23B | 126 (2) |
O15W—Co1—O12W | 86.37 (7) | H23A—O23W—H23B | 112 (3) |
O15W—Co1—O13W | 89.76 (7) | O12—S1—O11 | 107.67 (10) |
O15W—Co1—O14W | 90.88 (7) | O12—S1—O14 | 110.99 (9) |
O15W—Co1—O16W | 172.42 (7) | O13—S1—O11 | 108.34 (10) |
O16W—Co1—O11W | 92.29 (7) | O13—S1—O12 | 110.29 (10) |
O16W—Co1—O12W | 87.18 (7) | O13—S1—O14 | 110.26 (9) |
O16W—Co1—O13W | 87.52 (7) | O14—S1—O11 | 109.22 (9) |
O16W—Co1—O14W | 92.06 (7) | O22—S2—O21 | 109.09 (9) |
Co1—O11W—H11A | 120.5 (18) | O22—S2—O24 | 109.28 (9) |
Co1—O11W—H11B | 123.0 (19) | O23—S2—O21 | 109.29 (9) |
H11A—O11W—H11B | 108 (3) | O23—S2—O22 | 110.95 (9) |
Co1—O12W—H12A | 121.8 (17) | O23—S2—O24 | 110.13 (9) |
Co1—O12W—H12B | 113.8 (18) | O24—S2—O21 | 108.03 (9) |
H12A—O12W—H12B | 102 (2) | C2—N1—H1 | 118.5 |
Co1—O13W—H13A | 107.7 (18) | C2—N1—C6 | 123.1 (2) |
Co1—O13W—H13B | 112.8 (18) | C6—N1—H1 | 118.5 |
H13A—O13W—H13B | 102 (2) | N1—C2—H2 | 121.0 |
Co1—O14W—H14A | 123.3 (19) | N1—C2—C3 | 118.0 (2) |
Co1—O14W—H14B | 116 (2) | N2—C2—N1 | 118.0 (2) |
H14A—O14W—H14B | 111 (3) | N2—C2—C3 | 124.1 (2) |
Co1—O15W—H15A | 128.3 (19) | C3—C2—H2 | 121.0 |
Co1—O15W—H15B | 118.3 (19) | C2—N2—H2A | 120.0 |
H15A—O15W—H15B | 105 (3) | C2—N2—H2B | 120.0 |
Co1—O16W—H16A | 122.2 (19) | H2A—N2—H2B | 120.0 |
Co1—O16W—H16B | 117.5 (19) | C2—C3—H3 | 120.3 |
H16A—O16W—H16B | 102 (3) | C4—C3—C2 | 119.4 (2) |
O21W—Co2—O21Wi | 180.0 | C4—C3—H3 | 120.3 |
O21W—Co2—O22W | 89.77 (9) | C3—C4—H4 | 119.5 |
O21Wi—Co2—O22W | 90.23 (9) | C3—C4—C5 | 121.0 (2) |
O21W—Co2—O22Wi | 90.23 (9) | C5—C4—H4 | 119.5 |
O21Wi—Co2—O22Wi | 89.77 (9) | C4—C5—H5 | 120.8 |
O21W—Co2—O23W | 90.11 (7) | C6—C5—C4 | 118.3 (2) |
O21W—Co2—O23Wi | 89.89 (7) | C6—C5—H5 | 120.8 |
O21Wi—Co2—O23Wi | 90.11 (7) | N1—C6—C5 | 120.3 (2) |
O21Wi—Co2—O23W | 89.89 (7) | N1—C6—H6 | 119.9 |
O22W—Co2—O22Wi | 180.00 (10) | C5—C6—H6 | 119.9 |
O23W—Co2—O22Wi | 90.39 (8) | N2A—C6—N1 | 105.6 (8) |
O23Wi—Co2—O22W | 90.39 (8) | N2A—C6—C5 | 134.0 (8) |
O23Wi—Co2—O22Wi | 89.61 (8) | H1WA—O1W—H1WB | 85.4 |
O23W—Co2—O22W | 89.61 (8) | C6—N2A—H2AA | 120.0 |
O23W—Co2—O23Wi | 180.0 | C6—N2A—H2AB | 120.0 |
Co2—O21W—H21A | 122 (2) | H2AA—N2A—H2AB | 120.0 |
N1—C2—C3—C4 | 0.8 (3) | C3—C4—C5—C6 | −0.1 (3) |
C2—N1—C6—C5 | −0.8 (3) | C4—C5—C6—N1 | 0.9 (3) |
C2—N1—C6—N2A | 175.9 (7) | C4—C5—C6—N2A | −174.7 (10) |
C2—C3—C4—C5 | −0.7 (3) | C6—N1—C2—N2 | 179.8 (2) |
N2—C2—C3—C4 | −179.1 (2) | C6—N1—C2—C3 | 0.0 (3) |
Symmetry code: (i) −x+2, −y+1, −z. |
D—H···A | D—H | H···A | D···A | D—H···A |
O11W—H11A···O13Wii | 0.83 (2) | 2.14 (2) | 2.964 (2) | 175 (3) |
O11W—H11B···O14iii | 0.81 (2) | 2.07 (2) | 2.881 (2) | 178 (3) |
O12W—H12A···O21 | 0.84 (2) | 1.88 (2) | 2.711 (2) | 173 (3) |
O12W—H12B···O12iv | 0.82 (2) | 2.09 (2) | 2.894 (3) | 169 (3) |
O13W—H13A···O23iii | 0.82 (2) | 1.98 (2) | 2.800 (2) | 175 (2) |
O13W—H13B···O22 | 0.82 (2) | 1.92 (2) | 2.735 (2) | 172 (3) |
O14W—H14A···O13iii | 0.83 (2) | 1.85 (2) | 2.671 (2) | 169 (3) |
O14W—H14B···O12 | 0.81 (2) | 1.93 (2) | 2.744 (2) | 179 (3) |
O15W—H15A···O22v | 0.82 (2) | 1.90 (2) | 2.706 (2) | 166 (3) |
O15W—H15B···O14 | 0.83 (2) | 1.93 (2) | 2.756 (2) | 177 (3) |
O16W—H16A···O21iii | 0.84 (2) | 1.87 (2) | 2.699 (2) | 171 (3) |
O16W—H16B···O13iv | 0.84 (2) | 1.86 (2) | 2.703 (2) | 179 (3) |
O21W—H21A···O11iv | 0.82 (2) | 1.95 (2) | 2.766 (2) | 175 (3) |
O21W—H21B···O1Wvi | 0.82 (2) | 1.95 (2) | 2.758 (2) | 168 (3) |
O22W—H22A···O23iii | 0.80 (2) | 2.24 (2) | 2.959 (3) | 150 (3) |
O22W—H22B···O24 | 0.84 (2) | 2.01 (2) | 2.835 (2) | 169 (3) |
O23W—H23A···O1Wiv | 0.82 (2) | 1.90 (2) | 2.714 (2) | 171 (3) |
O23W—H23B···O24vii | 0.81 (2) | 1.96 (2) | 2.759 (2) | 169 (3) |
N1—H1···O11 | 0.86 | 1.85 | 2.701 (3) | 172 |
N2—H2A···O14 | 0.86 | 2.10 | 2.955 (3) | 173 |
N2—H2B···O24v | 0.86 | 2.12 | 2.959 (3) | 164 |
O1W—H1WA···O12 | 0.85 | 2.09 | 2.935 (2) | 175 |
O1W—H1WB···O21iv | 0.91 | 1.80 | 2.711 (2) | 171 |
Symmetry codes: (ii) −x+2, −y, −z+1; (iii) x+1, y, z; (iv) −x+1, −y+1, −z+1; (v) −x+1, −y, −z+1; (vi) −x+2, −y+1, −z+1; (vii) −x+1, −y+1, −z. |
(C5H7N2)2[Mg(H2O)6]3(SO4)4·2H2O | Z = 1 |
Mr = 1007.74 | F(000) = 530 |
Triclinic, P1 | Dx = 1.613 Mg m−3 |
a = 6.682 (3) Å | Mo Kα radiation, λ = 0.71073 Å |
b = 11.807 (4) Å | Cell parameters from 4995 reflections |
c = 14.309 (4) Å | θ = 2.8–29.2° |
α = 68.23 (3)° | µ = 0.39 mm−1 |
β = 82.13 (3)° | T = 100 K |
γ = 84.76 (3)° | Block, colourless |
V = 1037.5 (7) Å3 | 0.43 × 0.36 × 0.23 mm |
Rigaku Oxford Diffraction Xcalibur Atlas diffractometer | 4884 independent reflections |
Radiation source: fine-focus sealed X-ray tube, Enhance (Mo) X-ray Source | 3875 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.026 |
Detector resolution: 10.6249 pixels mm-1 | θmax = 29.3°, θmin = 1.9° |
ω scans | h = −8→9 |
Absorption correction: analytical [CrysAlis PRO (Rigaku Oxford Diffraction, 2015), based on expressions derived by Clark & Reid (1995)] | k = −15→14 |
Tmin = 0.892, Tmax = 0.928 | l = −19→18 |
11467 measured reflections |
Refinement on F2 | 20 restraints |
Least-squares matrix: full | Hydrogen site location: mixed |
R[F2 > 2σ(F2)] = 0.040 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.089 | w = 1/[σ2(Fo2) + (0.030P)2 + 0.790P] where P = (Fo2 + 2Fc2)/3 |
S = 1.03 | (Δ/σ)max = 0.001 |
4884 reflections | Δρmax = 0.45 e Å−3 |
324 parameters | Δρmin = −0.40 e Å−3 |
(C5H7N2)2[Mg(H2O)6]3(SO4)4·2H2O | γ = 84.76 (3)° |
Mr = 1007.74 | V = 1037.5 (7) Å3 |
Triclinic, P1 | Z = 1 |
a = 6.682 (3) Å | Mo Kα radiation |
b = 11.807 (4) Å | µ = 0.39 mm−1 |
c = 14.309 (4) Å | T = 100 K |
α = 68.23 (3)° | 0.43 × 0.36 × 0.23 mm |
β = 82.13 (3)° |
Rigaku Oxford Diffraction Xcalibur Atlas diffractometer | 4884 independent reflections |
Absorption correction: analytical [CrysAlis PRO (Rigaku Oxford Diffraction, 2015), based on expressions derived by Clark & Reid (1995)] | 3875 reflections with I > 2σ(I) |
Tmin = 0.892, Tmax = 0.928 | Rint = 0.026 |
11467 measured reflections |
R[F2 > 2σ(F2)] = 0.040 | 20 restraints |
wR(F2) = 0.089 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.03 | Δρmax = 0.45 e Å−3 |
4884 reflections | Δρmin = −0.40 e Å−3 |
324 parameters |
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. |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
Mg1 | 0.81378 (10) | 0.23692 (6) | 0.49397 (5) | 0.01481 (16) | |
O11W | 1.0598 (2) | 0.13517 (16) | 0.56102 (15) | 0.0275 (4) | |
H11A | 1.101 (4) | 0.0690 (19) | 0.560 (2) | 0.041* | |
H11B | 1.124 (4) | 0.155 (3) | 0.596 (2) | 0.041* | |
O12W | 0.5724 (2) | 0.35023 (14) | 0.43273 (13) | 0.0200 (3) | |
H12A | 0.508 (4) | 0.337 (2) | 0.3931 (18) | 0.030* | |
H12B | 0.577 (4) | 0.4250 (16) | 0.411 (2) | 0.030* | |
O13W | 0.8425 (2) | 0.12786 (14) | 0.40247 (12) | 0.0169 (3) | |
H13A | 0.937 (3) | 0.149 (2) | 0.3562 (16) | 0.025* | |
H13B | 0.744 (3) | 0.126 (2) | 0.3752 (18) | 0.025* | |
O14W | 0.7913 (2) | 0.32636 (17) | 0.59110 (15) | 0.0302 (4) | |
H14A | 0.883 (4) | 0.353 (3) | 0.610 (2) | 0.045* | |
H14B | 0.681 (3) | 0.350 (3) | 0.615 (2) | 0.045* | |
O15W | 0.5991 (2) | 0.12192 (15) | 0.58580 (14) | 0.0262 (4) | |
H15A | 0.592 (4) | 0.0455 (16) | 0.613 (2) | 0.039* | |
H15B | 0.507 (3) | 0.151 (2) | 0.616 (2) | 0.039* | |
O16W | 1.0006 (3) | 0.36017 (16) | 0.39053 (17) | 0.0397 (5) | |
H16A | 1.113 (3) | 0.346 (3) | 0.361 (2) | 0.060* | |
H16B | 0.974 (5) | 0.4362 (17) | 0.366 (2) | 0.060* | |
Mg2 | 1.0000 | 0.5000 | 0.0000 | 0.0143 (2) | |
O21W | 1.0623 (2) | 0.57333 (16) | 0.10139 (14) | 0.0261 (4) | |
H21A | 0.982 (4) | 0.613 (2) | 0.128 (2) | 0.039* | |
H21B | 1.169 (3) | 0.572 (3) | 0.123 (2) | 0.039* | |
O22W | 0.8941 (2) | 0.34472 (16) | 0.12053 (14) | 0.0303 (4) | |
H22A | 0.958 (4) | 0.299 (2) | 0.1654 (18) | 0.045* | |
H22B | 0.775 (3) | 0.321 (3) | 0.137 (2) | 0.045* | |
O23W | 0.7155 (2) | 0.57895 (15) | −0.00078 (12) | 0.0213 (3) | |
H23A | 0.641 (4) | 0.566 (2) | 0.0525 (15) | 0.032* | |
H23B | 0.661 (4) | 0.623 (2) | −0.0509 (16) | 0.032* | |
S1 | 0.24947 (7) | 0.31939 (5) | 0.71412 (4) | 0.01455 (12) | |
O11 | 0.2178 (2) | 0.28429 (14) | 0.82576 (12) | 0.0229 (4) | |
O12 | 0.4330 (2) | 0.39112 (14) | 0.67622 (13) | 0.0221 (4) | |
O13 | 0.0741 (2) | 0.39470 (13) | 0.67063 (13) | 0.0237 (4) | |
O14 | 0.2744 (2) | 0.20773 (13) | 0.68906 (11) | 0.0169 (3) | |
S2 | 0.37973 (7) | 0.21759 (5) | 0.25672 (4) | 0.01327 (12) | |
O21 | 0.3611 (2) | 0.31962 (13) | 0.29477 (11) | 0.0165 (3) | |
O22 | 0.4965 (2) | 0.11450 (13) | 0.32351 (11) | 0.0182 (3) | |
O23 | 0.1764 (2) | 0.18145 (13) | 0.25324 (11) | 0.0175 (3) | |
O24 | 0.4911 (2) | 0.25977 (13) | 0.15362 (11) | 0.0173 (3) | |
N1 | 0.2287 (3) | 0.06416 (17) | 0.97674 (16) | 0.0236 (4) | |
H1 | 0.2199 | 0.1327 | 0.9271 | 0.028* | |
C2 | 0.2799 (3) | −0.0381 (2) | 0.95590 (18) | 0.0229 (5) | |
H2 | 0.3055 | −0.0348 | 0.8894 | 0.027* | 0.121 (5) |
N2 | 0.3134 (3) | −0.0267 (2) | 0.86029 (17) | 0.0216 (6) | 0.879 (5) |
H2A | 0.3024 | 0.0440 | 0.8134 | 0.026* | 0.879 (5) |
H2B | 0.3462 | −0.0901 | 0.8445 | 0.026* | 0.879 (5) |
C3 | 0.2935 (3) | −0.1499 (2) | 1.03795 (19) | 0.0268 (5) | |
H3 | 0.3296 | −0.2219 | 1.0264 | 0.032* | |
C4 | 0.2530 (3) | −0.1514 (2) | 1.13463 (19) | 0.0284 (6) | |
H4 | 0.2599 | −0.2252 | 1.1888 | 0.034* | |
C5 | 0.2012 (3) | −0.0435 (2) | 1.15349 (19) | 0.0292 (6) | |
H5 | 0.1747 | −0.0447 | 1.2194 | 0.035* | |
C6 | 0.1906 (3) | 0.0631 (2) | 1.07281 (19) | 0.0263 (5) | |
H6 | 0.1570 | 0.1359 | 1.0835 | 0.032* | 0.879 (5) |
N2A | 0.1625 (19) | 0.1588 (13) | 1.0646 (11) | 0.013 (4)* | 0.121 (5) |
H2AA | 0.1679 | 0.2149 | 1.0052 | 0.015* | 0.121 (5) |
H2AB | 0.1351 | 0.1781 | 1.1174 | 0.015* | 0.121 (5) |
O1W | 0.5554 (2) | 0.45065 (14) | 0.83503 (12) | 0.0176 (3) | |
H1WA | 0.513 (4) | 0.425 (2) | 0.7954 (17) | 0.026* | |
H1WB | 0.570 (4) | 0.5230 (16) | 0.7977 (17) | 0.026* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Mg1 | 0.0141 (3) | 0.0132 (4) | 0.0172 (4) | 0.0001 (3) | −0.0025 (3) | −0.0054 (3) |
O11W | 0.0259 (9) | 0.0244 (10) | 0.0417 (11) | 0.0086 (7) | −0.0184 (8) | −0.0201 (9) |
O12W | 0.0231 (8) | 0.0160 (8) | 0.0226 (9) | 0.0017 (6) | −0.0104 (7) | −0.0069 (7) |
O13W | 0.0153 (8) | 0.0183 (8) | 0.0168 (8) | −0.0017 (6) | −0.0019 (6) | −0.0059 (7) |
O14W | 0.0169 (8) | 0.0446 (11) | 0.0475 (12) | 0.0042 (7) | −0.0091 (8) | −0.0373 (10) |
O15W | 0.0291 (9) | 0.0134 (8) | 0.0308 (10) | −0.0017 (7) | 0.0097 (7) | −0.0063 (8) |
O16W | 0.0292 (10) | 0.0135 (9) | 0.0625 (14) | −0.0010 (7) | 0.0235 (9) | −0.0075 (9) |
Mg2 | 0.0114 (5) | 0.0162 (5) | 0.0142 (5) | 0.0001 (4) | −0.0030 (4) | −0.0039 (4) |
O21W | 0.0181 (8) | 0.0371 (10) | 0.0341 (10) | 0.0073 (7) | −0.0101 (7) | −0.0251 (9) |
O22W | 0.0182 (8) | 0.0321 (10) | 0.0269 (10) | −0.0085 (7) | −0.0083 (7) | 0.0089 (8) |
O23W | 0.0152 (8) | 0.0301 (10) | 0.0141 (9) | 0.0049 (6) | −0.0028 (6) | −0.0039 (7) |
S1 | 0.0142 (2) | 0.0126 (3) | 0.0179 (3) | 0.00057 (17) | −0.0040 (2) | −0.0063 (2) |
O11 | 0.0326 (9) | 0.0173 (8) | 0.0186 (9) | 0.0025 (6) | −0.0019 (7) | −0.0075 (7) |
O12 | 0.0182 (8) | 0.0182 (8) | 0.0321 (10) | −0.0048 (6) | 0.0013 (7) | −0.0122 (7) |
O13 | 0.0232 (8) | 0.0145 (8) | 0.0379 (10) | 0.0051 (6) | −0.0172 (7) | −0.0113 (7) |
O14 | 0.0189 (7) | 0.0137 (8) | 0.0197 (8) | −0.0004 (5) | −0.0029 (6) | −0.0078 (6) |
S2 | 0.0123 (2) | 0.0130 (3) | 0.0146 (3) | −0.00053 (17) | −0.00170 (19) | −0.0050 (2) |
O21 | 0.0160 (7) | 0.0154 (8) | 0.0199 (8) | −0.0002 (5) | −0.0022 (6) | −0.0086 (7) |
O22 | 0.0190 (8) | 0.0139 (8) | 0.0199 (8) | 0.0008 (5) | −0.0060 (6) | −0.0032 (7) |
O23 | 0.0137 (7) | 0.0210 (8) | 0.0198 (8) | −0.0036 (6) | −0.0011 (6) | −0.0093 (7) |
O24 | 0.0149 (7) | 0.0206 (8) | 0.0151 (8) | −0.0007 (6) | −0.0006 (6) | −0.0053 (7) |
N1 | 0.0199 (10) | 0.0190 (10) | 0.0264 (11) | −0.0028 (7) | −0.0049 (8) | −0.0006 (9) |
C2 | 0.0113 (10) | 0.0327 (14) | 0.0206 (12) | −0.0045 (9) | −0.0016 (9) | −0.0042 (11) |
N2 | 0.0266 (12) | 0.0179 (12) | 0.0197 (12) | 0.0020 (8) | −0.0012 (9) | −0.0073 (10) |
C3 | 0.0192 (12) | 0.0244 (13) | 0.0286 (14) | −0.0005 (9) | −0.0021 (10) | −0.0006 (11) |
C4 | 0.0216 (12) | 0.0312 (14) | 0.0216 (13) | −0.0033 (9) | −0.0020 (10) | 0.0031 (11) |
C5 | 0.0223 (12) | 0.0386 (15) | 0.0218 (13) | −0.0061 (10) | −0.0026 (10) | −0.0041 (12) |
C6 | 0.0223 (12) | 0.0313 (15) | 0.0257 (14) | −0.0043 (9) | −0.0049 (10) | −0.0093 (11) |
O1W | 0.0197 (8) | 0.0169 (8) | 0.0173 (9) | −0.0029 (6) | −0.0049 (6) | −0.0058 (7) |
Mg1—O11W | 2.069 (2) | O23W—H23B | 0.824 (17) |
Mg1—O12W | 2.0695 (19) | S1—O11 | 1.4836 (17) |
Mg1—O13W | 2.1321 (18) | S1—O12 | 1.4774 (16) |
Mg1—O14W | 2.0178 (19) | S1—O13 | 1.4661 (16) |
Mg1—O15W | 2.036 (2) | S1—O14 | 1.4794 (15) |
Mg1—O16W | 2.023 (2) | S2—O21 | 1.4845 (15) |
O11W—H11A | 0.808 (17) | S2—O22 | 1.4735 (16) |
O11W—H11B | 0.810 (17) | S2—O23 | 1.4733 (15) |
O12W—H12A | 0.821 (17) | S2—O24 | 1.4834 (16) |
O12W—H12B | 0.822 (17) | N1—H1 | 0.8600 |
O13W—H13A | 0.831 (16) | N1—C2 | 1.352 (3) |
O13W—H13B | 0.815 (16) | N1—C6 | 1.359 (3) |
O14W—H14A | 0.830 (17) | C2—H2 | 0.9300 |
O14W—H14B | 0.840 (17) | C2—N2 | 1.314 (3) |
O15W—H15A | 0.843 (17) | C2—C3 | 1.409 (3) |
O15W—H15B | 0.831 (17) | N2—H2A | 0.8600 |
O16W—H16A | 0.845 (18) | N2—H2B | 0.8600 |
O16W—H16B | 0.846 (18) | C3—H3 | 0.9300 |
Mg2—O21W | 2.0471 (17) | C3—C4 | 1.367 (4) |
Mg2—O21Wi | 2.0471 (17) | C4—H4 | 0.9300 |
Mg2—O22Wi | 2.0961 (19) | C4—C5 | 1.401 (4) |
Mg2—O22W | 2.0961 (19) | C5—H5 | 0.9300 |
Mg2—O23Wi | 2.0391 (17) | C5—C6 | 1.360 (4) |
Mg2—O23W | 2.0391 (17) | C6—H6 | 0.9300 |
O21W—H21A | 0.825 (17) | C6—N2A | 1.093 (14) |
O21W—H21B | 0.816 (17) | N2A—H2AA | 0.8600 |
O22W—H22A | 0.813 (17) | N2A—H2AB | 0.8600 |
O22W—H22B | 0.841 (17) | O1W—H1WA | 0.822 (16) |
O23W—H23A | 0.821 (17) | O1W—H1WB | 0.829 (16) |
O11W—Mg1—O12W | 174.72 (7) | Mg2—O21W—H21B | 129 (2) |
O11W—Mg1—O13W | 86.78 (7) | H21A—O21W—H21B | 105 (3) |
O12W—Mg1—O13W | 98.30 (7) | Mg2—O22W—H22A | 126 (2) |
O14W—Mg1—O11W | 89.41 (8) | Mg2—O22W—H22B | 128 (2) |
O14W—Mg1—O12W | 85.60 (8) | H22A—O22W—H22B | 105 (3) |
O14W—Mg1—O13W | 174.89 (8) | Mg2—O23W—H23A | 120.2 (19) |
O14W—Mg1—O15W | 89.96 (8) | Mg2—O23W—H23B | 126.7 (19) |
O14W—Mg1—O16W | 92.37 (9) | H23A—O23W—H23B | 113 (3) |
O15W—Mg1—O11W | 96.46 (9) | O12—S1—O11 | 107.82 (10) |
O15W—Mg1—O12W | 85.29 (8) | O12—S1—O14 | 110.69 (9) |
O15W—Mg1—O13W | 87.08 (7) | O13—S1—O11 | 108.86 (10) |
O16W—Mg1—O11W | 90.37 (9) | O13—S1—O12 | 109.67 (10) |
O16W—Mg1—O12W | 88.10 (8) | O13—S1—O14 | 110.53 (9) |
O16W—Mg1—O13W | 91.06 (8) | O14—S1—O11 | 109.20 (9) |
O16W—Mg1—O15W | 172.81 (9) | O22—S2—O21 | 109.23 (9) |
Mg1—O11W—H11A | 126 (2) | O22—S2—O24 | 108.69 (9) |
Mg1—O11W—H11B | 124 (2) | O23—S2—O21 | 109.36 (8) |
H11A—O11W—H11B | 110 (3) | O23—S2—O22 | 111.04 (9) |
Mg1—O12W—H12A | 122.0 (18) | O23—S2—O24 | 110.01 (9) |
Mg1—O12W—H12B | 121.8 (18) | O24—S2—O21 | 108.47 (9) |
H12A—O12W—H12B | 104 (3) | C2—N1—H1 | 118.6 |
Mg1—O13W—H13A | 111.6 (17) | C2—N1—C6 | 122.7 (2) |
Mg1—O13W—H13B | 117.3 (18) | C6—N1—H1 | 118.6 |
H13A—O13W—H13B | 106 (2) | N1—C2—H2 | 121.0 |
Mg1—O14W—H14A | 129 (2) | N1—C2—C3 | 118.0 (2) |
Mg1—O14W—H14B | 123 (2) | N2—C2—N1 | 117.7 (2) |
H14A—O14W—H14B | 108 (3) | N2—C2—C3 | 124.3 (2) |
Mg1—O15W—H15A | 135.0 (19) | C3—C2—H2 | 121.0 |
Mg1—O15W—H15B | 117 (2) | C2—N2—H2A | 120.0 |
H15A—O15W—H15B | 106 (3) | C2—N2—H2B | 120.0 |
Mg1—O16W—H16A | 127 (2) | H2A—N2—H2B | 120.0 |
Mg1—O16W—H16B | 125 (2) | C2—C3—H3 | 120.3 |
H16A—O16W—H16B | 108 (3) | C4—C3—C2 | 119.4 (2) |
O21Wi—Mg2—O21W | 180.0 | C4—C3—H3 | 120.3 |
O21Wi—Mg2—O22Wi | 89.74 (8) | C3—C4—H4 | 119.4 |
O21Wi—Mg2—O22W | 90.26 (8) | C3—C4—C5 | 121.1 (2) |
O21W—Mg2—O22Wi | 90.26 (8) | C5—C4—H4 | 119.4 |
O21W—Mg2—O22W | 89.73 (8) | C4—C5—H5 | 120.9 |
O22Wi—Mg2—O22W | 180.00 (8) | C6—C5—C4 | 118.2 (2) |
O23Wi—Mg2—O21W | 90.06 (7) | C6—C5—H5 | 120.9 |
O23W—Mg2—O21Wi | 90.06 (7) | N1—C6—C5 | 120.6 (2) |
O23W—Mg2—O21W | 89.94 (7) | N1—C6—H6 | 119.7 |
O23Wi—Mg2—O21Wi | 89.94 (7) | C5—C6—H6 | 119.7 |
O23W—Mg2—O22W | 89.59 (8) | N2A—C6—N1 | 105.2 (8) |
O23W—Mg2—O22Wi | 90.41 (8) | N2A—C6—C5 | 134.1 (8) |
O23Wi—Mg2—O22W | 90.41 (8) | C6—N2A—H2AA | 120.0 |
O23Wi—Mg2—O22Wi | 89.59 (8) | C6—N2A—H2AB | 120.0 |
O23W—Mg2—O23Wi | 180.0 | H2AA—N2A—H2AB | 120.0 |
Mg2—O21W—H21A | 126 (2) | H1WA—O1W—H1WB | 99 (2) |
N1—C2—C3—C4 | 0.6 (3) | C3—C4—C5—C6 | 0.5 (3) |
C2—N1—C6—C5 | −0.6 (3) | C4—C5—C6—N1 | 0.2 (3) |
C2—N1—C6—N2A | 176.8 (7) | C4—C5—C6—N2A | −176.3 (10) |
C2—C3—C4—C5 | −0.9 (3) | C6—N1—C2—N2 | 179.9 (2) |
N2—C2—C3—C4 | −179.2 (2) | C6—N1—C2—C3 | 0.1 (3) |
Symmetry code: (i) −x+2, −y+1, −z. |
D—H···A | D—H | H···A | D···A | D—H···A |
O11W—H11A···O13Wii | 0.81 (2) | 2.19 (2) | 2.977 (2) | 164 (3) |
O11W—H11B···O14iii | 0.81 (2) | 2.06 (2) | 2.873 (2) | 177 (3) |
O12W—H12A···O21 | 0.82 (2) | 1.90 (2) | 2.722 (2) | 176 (3) |
O12W—H12B···O12iv | 0.82 (2) | 2.07 (2) | 2.867 (2) | 165 (3) |
O13W—H13A···O23iii | 0.83 (2) | 1.98 (2) | 2.809 (2) | 173 (3) |
O13W—H13B···O22 | 0.82 (2) | 1.94 (2) | 2.750 (2) | 174 (3) |
O14W—H14A···O13iii | 0.83 (2) | 1.83 (2) | 2.658 (2) | 172 (3) |
O14W—H14B···O12 | 0.84 (2) | 1.88 (2) | 2.713 (2) | 175 (3) |
O15W—H15A···O22v | 0.84 (2) | 1.88 (2) | 2.701 (2) | 165 (3) |
O15W—H15B···O14 | 0.83 (2) | 1.96 (2) | 2.783 (2) | 174 (3) |
O16W—H16A···O21iii | 0.85 (2) | 1.85 (2) | 2.698 (2) | 178 (3) |
O16W—H16B···O13iv | 0.85 (2) | 1.88 (2) | 2.714 (2) | 172 (3) |
O21W—H21A···O11iv | 0.83 (2) | 1.94 (2) | 2.758 (2) | 173 (3) |
O21W—H21B···O1Wvi | 0.82 (2) | 1.98 (2) | 2.783 (2) | 171 (3) |
O22W—H22A···O23iii | 0.81 (2) | 2.12 (2) | 2.912 (3) | 166 (3) |
O22W—H22B···O24 | 0.84 (2) | 2.05 (2) | 2.876 (2) | 170 (3) |
O23W—H23A···O1Wiv | 0.82 (2) | 1.90 (2) | 2.711 (2) | 173 (3) |
O23W—H23B···O24vii | 0.82 (2) | 1.94 (2) | 2.752 (2) | 170 (3) |
N1—H1···O11 | 0.86 | 1.84 | 2.697 (3) | 175 |
N2—H2A···O14 | 0.86 | 2.10 | 2.957 (3) | 174 |
N2—H2B···O24v | 0.86 | 2.18 | 2.999 (3) | 158 |
O1W—H1WA···O12 | 0.82 (2) | 2.04 (2) | 2.850 (2) | 169 (2) |
O1W—H1WB···O21iv | 0.83 (2) | 1.89 (2) | 2.716 (2) | 172 (3) |
Symmetry codes: (ii) −x+2, −y, −z+1; (iii) x+1, y, z; (iv) −x+1, −y+1, −z+1; (v) −x+1, −y, −z+1; (vi) −x+2, −y+1, −z+1; (vii) −x+1, −y+1, −z. |
(C5H7N2)2[Ni(H2O)6](SO4)2 | Z = 1 |
Mr = 549.18 | F(000) = 286 |
Triclinic, P1 | Dx = 1.710 Mg m−3 |
a = 6.970 (3) Å | Mo Kα radiation, λ = 0.71073 Å |
b = 7.913 (3) Å | Cell parameters from 6242 reflections |
c = 11.391 (4) Å | θ = 3.0–29.1° |
α = 72.31 (3)° | µ = 1.18 mm−1 |
β = 89.57 (3)° | T = 100 K |
γ = 64.20 (3)° | Block, light green |
V = 533.2 (4) Å3 | 0.15 × 0.12 × 0.1 mm |
Rigaku Oxford Diffraction Xcalibur Atlas diffractometer | 2662 independent reflections |
Radiation source: fine-focus sealed X-ray tube, Enhance (Mo) X-ray Source | 2341 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.026 |
Detector resolution: 10.6249 pixels mm-1 | θmax = 29.6°, θmin = 3.0° |
ω scans | h = −9→9 |
Absorption correction: analytical [CrysAlis PRO (Rigaku Oxford Diffraction, 2015), based on expressions derived by Clark & Reid (1995)] | k = −10→11 |
Tmin = 0.879, Tmax = 0.909 | l = −15→15 |
11780 measured reflections |
Refinement on F2 | 6 restraints |
Least-squares matrix: full | Hydrogen site location: mixed |
R[F2 > 2σ(F2)] = 0.026 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.060 | w = 1/[σ2(Fo2) + (0.022P)2 + 0.338P] where P = (Fo2 + 2Fc2)/3 |
S = 1.07 | (Δ/σ)max < 0.001 |
2662 reflections | Δρmax = 0.31 e Å−3 |
160 parameters | Δρmin = −0.44 e Å−3 |
(C5H7N2)2[Ni(H2O)6](SO4)2 | γ = 64.20 (3)° |
Mr = 549.18 | V = 533.2 (4) Å3 |
Triclinic, P1 | Z = 1 |
a = 6.970 (3) Å | Mo Kα radiation |
b = 7.913 (3) Å | µ = 1.18 mm−1 |
c = 11.391 (4) Å | T = 100 K |
α = 72.31 (3)° | 0.15 × 0.12 × 0.1 mm |
β = 89.57 (3)° |
Rigaku Oxford Diffraction Xcalibur Atlas diffractometer | 2662 independent reflections |
Absorption correction: analytical [CrysAlis PRO (Rigaku Oxford Diffraction, 2015), based on expressions derived by Clark & Reid (1995)] | 2341 reflections with I > 2σ(I) |
Tmin = 0.879, Tmax = 0.909 | Rint = 0.026 |
11780 measured reflections |
R[F2 > 2σ(F2)] = 0.026 | 6 restraints |
wR(F2) = 0.060 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.07 | Δρmax = 0.31 e Å−3 |
2662 reflections | Δρmin = −0.44 e Å−3 |
160 parameters |
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. |
x | y | z | Uiso*/Ueq | ||
Ni1 | 0.5000 | 1.0000 | 0.0000 | 0.01038 (8) | |
O1W | 0.81801 (19) | 0.79924 (18) | 0.06654 (11) | 0.0149 (2) | |
H1WA | 0.836 (3) | 0.687 (2) | 0.1100 (18) | 0.022* | |
H1WB | 0.912 (3) | 0.782 (3) | 0.0206 (18) | 0.022* | |
O2W | 0.40209 (19) | 0.78550 (17) | 0.07618 (11) | 0.0143 (2) | |
H2WA | 0.504 (3) | 0.674 (2) | 0.1164 (18) | 0.021* | |
H2WB | 0.323 (3) | 0.769 (3) | 0.0309 (18) | 0.021* | |
O3W | 0.51634 (19) | 0.95526 (18) | −0.16941 (11) | 0.0149 (2) | |
H3WA | 0.448 (3) | 0.903 (3) | −0.1925 (19) | 0.022* | |
H3WB | 0.639 (3) | 0.908 (3) | −0.1889 (19) | 0.022* | |
S1 | 0.86679 (6) | 0.26220 (6) | 0.19837 (3) | 0.01136 (9) | |
O1 | 0.78367 (19) | 0.46560 (17) | 0.20867 (11) | 0.0165 (2) | |
O2 | 0.84333 (19) | 0.28270 (18) | 0.06561 (10) | 0.0171 (2) | |
O3 | 0.74195 (18) | 0.16573 (17) | 0.26770 (11) | 0.0158 (2) | |
O4 | 1.09523 (18) | 0.14692 (17) | 0.25389 (10) | 0.0149 (2) | |
N1 | 0.7453 (2) | 0.5110 (2) | 0.43941 (13) | 0.0147 (3) | |
H1 | 0.7428 | 0.5000 | 0.3667 | 0.018* | |
C2 | 0.7799 (3) | 0.3513 (2) | 0.53979 (15) | 0.0139 (3) | |
N2 | 0.8077 (2) | 0.1831 (2) | 0.52350 (13) | 0.0176 (3) | |
H2A | 0.8035 | 0.1768 | 0.4496 | 0.021* | |
H2B | 0.8298 | 0.0806 | 0.5869 | 0.021* | |
C3 | 0.7865 (3) | 0.3701 (3) | 0.65929 (15) | 0.0172 (3) | |
H3 | 0.8124 | 0.2625 | 0.7305 | 0.021* | |
C4 | 0.7541 (3) | 0.5491 (3) | 0.66851 (17) | 0.0199 (4) | |
H4 | 0.7567 | 0.5630 | 0.7466 | 0.024* | |
C5 | 0.7170 (3) | 0.7119 (3) | 0.56133 (17) | 0.0209 (4) | |
H5 | 0.6949 | 0.8332 | 0.5679 | 0.025* | |
C6 | 0.7140 (3) | 0.6890 (3) | 0.44846 (17) | 0.0185 (3) | |
H6 | 0.6906 | 0.7950 | 0.3767 | 0.022* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Ni1 | 0.01129 (15) | 0.01018 (15) | 0.00950 (14) | −0.00459 (12) | 0.00164 (10) | −0.00349 (11) |
O1W | 0.0136 (6) | 0.0133 (6) | 0.0144 (6) | −0.0046 (5) | 0.0030 (5) | −0.0027 (5) |
O2W | 0.0156 (6) | 0.0134 (6) | 0.0142 (6) | −0.0076 (5) | −0.0001 (5) | −0.0035 (5) |
O3W | 0.0141 (6) | 0.0198 (6) | 0.0151 (6) | −0.0091 (5) | 0.0042 (5) | −0.0093 (5) |
S1 | 0.01211 (19) | 0.01263 (19) | 0.00994 (18) | −0.00585 (16) | 0.00185 (14) | −0.00423 (14) |
O1 | 0.0198 (6) | 0.0120 (6) | 0.0157 (6) | −0.0053 (5) | 0.0027 (5) | −0.0048 (5) |
O2 | 0.0183 (6) | 0.0259 (7) | 0.0112 (5) | −0.0125 (5) | 0.0032 (4) | −0.0079 (5) |
O3 | 0.0162 (6) | 0.0200 (6) | 0.0149 (6) | −0.0113 (5) | 0.0038 (5) | −0.0061 (5) |
O4 | 0.0130 (6) | 0.0168 (6) | 0.0142 (5) | −0.0067 (5) | 0.0015 (4) | −0.0043 (5) |
N1 | 0.0153 (7) | 0.0158 (7) | 0.0114 (6) | −0.0058 (6) | 0.0011 (5) | −0.0044 (5) |
C2 | 0.0101 (7) | 0.0165 (8) | 0.0144 (7) | −0.0052 (6) | 0.0024 (6) | −0.0055 (6) |
N2 | 0.0224 (7) | 0.0178 (7) | 0.0129 (7) | −0.0095 (6) | 0.0031 (6) | −0.0050 (6) |
C3 | 0.0163 (8) | 0.0216 (9) | 0.0118 (7) | −0.0079 (7) | 0.0026 (6) | −0.0043 (7) |
C4 | 0.0153 (8) | 0.0275 (10) | 0.0185 (8) | −0.0075 (7) | 0.0016 (7) | −0.0132 (7) |
C5 | 0.0166 (8) | 0.0183 (9) | 0.0286 (9) | −0.0066 (7) | 0.0000 (7) | −0.0108 (7) |
C6 | 0.0149 (8) | 0.0143 (8) | 0.0224 (9) | −0.0046 (7) | −0.0005 (7) | −0.0040 (7) |
Ni1—O1W | 2.0590 (17) | S1—O4 | 1.4722 (14) |
Ni1—O1Wi | 2.0590 (17) | N1—H1 | 0.8600 |
Ni1—O2Wi | 2.0503 (14) | N1—C2 | 1.350 (2) |
Ni1—O2W | 2.0503 (13) | N1—C6 | 1.365 (2) |
Ni1—O3W | 2.0588 (13) | C2—N2 | 1.331 (2) |
Ni1—O3Wi | 2.0588 (13) | C2—C3 | 1.417 (2) |
O1W—H1WA | 0.830 (15) | N2—H2A | 0.8600 |
O1W—H1WB | 0.825 (15) | N2—H2B | 0.8600 |
O2W—H2WA | 0.841 (15) | C3—H3 | 0.9300 |
O2W—H2WB | 0.832 (15) | C3—C4 | 1.371 (3) |
O3W—H3WA | 0.839 (15) | C4—H4 | 0.9300 |
O3W—H3WB | 0.829 (15) | C4—C5 | 1.406 (3) |
S1—O1 | 1.4973 (13) | C5—H5 | 0.9300 |
S1—O2 | 1.4737 (13) | C5—C6 | 1.354 (3) |
S1—O3 | 1.4714 (13) | C6—H6 | 0.9300 |
O1Wi—Ni1—O1W | 180.0 | O3—S1—O2 | 111.20 (7) |
O2W—Ni1—O1W | 91.67 (6) | O3—S1—O4 | 109.79 (8) |
O2Wi—Ni1—O1Wi | 91.67 (6) | O4—S1—O1 | 108.40 (7) |
O2Wi—Ni1—O1W | 88.33 (6) | O4—S1—O2 | 110.39 (8) |
O2W—Ni1—O1Wi | 88.33 (6) | C2—N1—H1 | 118.6 |
O2Wi—Ni1—O2W | 180.0 | C2—N1—C6 | 122.79 (15) |
O2W—Ni1—O3Wi | 87.04 (5) | C6—N1—H1 | 118.6 |
O2Wi—Ni1—O3W | 87.04 (5) | N1—C2—C3 | 118.16 (15) |
O2Wi—Ni1—O3Wi | 92.96 (5) | N2—C2—N1 | 119.33 (15) |
O2W—Ni1—O3W | 92.96 (5) | N2—C2—C3 | 122.50 (15) |
O3W—Ni1—O1W | 93.37 (6) | C2—N2—H2A | 120.0 |
O3Wi—Ni1—O1Wi | 93.37 (6) | C2—N2—H2B | 120.0 |
O3W—Ni1—O1Wi | 86.63 (6) | H2A—N2—H2B | 120.0 |
O3Wi—Ni1—O1W | 86.63 (6) | C2—C3—H3 | 120.4 |
O3Wi—Ni1—O3W | 180.000 (10) | C4—C3—C2 | 119.10 (16) |
Ni1—O1W—H1WA | 113.6 (14) | C4—C3—H3 | 120.4 |
Ni1—O1W—H1WB | 122.0 (15) | C3—C4—H4 | 119.6 |
H1WA—O1W—H1WB | 107 (2) | C3—C4—C5 | 120.78 (16) |
Ni1—O2W—H2WA | 113.4 (14) | C5—C4—H4 | 119.6 |
Ni1—O2W—H2WB | 118.8 (14) | C4—C5—H5 | 120.6 |
H2WA—O2W—H2WB | 109 (2) | C6—C5—C4 | 118.80 (17) |
Ni1—O3W—H3WA | 122.5 (14) | C6—C5—H5 | 120.6 |
Ni1—O3W—H3WB | 115.8 (15) | N1—C6—H6 | 119.8 |
H3WA—O3W—H3WB | 108 (2) | C5—C6—N1 | 120.34 (16) |
O2—S1—O1 | 108.62 (8) | C5—C6—H6 | 119.8 |
O3—S1—O1 | 108.37 (7) | ||
N1—C2—C3—C4 | 1.1 (2) | C3—C4—C5—C6 | −0.1 (3) |
C2—N1—C6—C5 | 0.1 (2) | C4—C5—C6—N1 | 0.4 (3) |
C2—C3—C4—C5 | −0.7 (2) | C6—N1—C2—N2 | 179.58 (15) |
N2—C2—C3—C4 | −179.32 (15) | C6—N1—C2—C3 | −0.8 (2) |
Symmetry code: (i) −x+1, −y+2, −z. |
D—H···A | D—H | H···A | D···A | D—H···A |
O1W—H1WA···O1 | 0.83 (2) | 1.95 (2) | 2.756 (2) | 163 (2) |
O1W—H1WB···O2ii | 0.83 (2) | 1.91 (2) | 2.732 (2) | 172 (2) |
O2W—H2WA···O1 | 0.84 (2) | 1.95 (2) | 2.764 (2) | 162 (2) |
O2W—H2WB···O2iii | 0.83 (2) | 1.85 (2) | 2.6834 (18) | 177 (2) |
O3W—H3WA···O3iii | 0.84 (2) | 1.93 (2) | 2.7556 (18) | 169 (2) |
O3W—H3WB···O4ii | 0.83 (2) | 1.91 (2) | 2.727 (2) | 168 (2) |
N1—H1···O1 | 0.86 | 1.90 | 2.755 (2) | 171 |
N2—H2A···O3 | 0.86 | 2.15 | 3.006 (2) | 171 |
N2—H2B···O4iv | 0.86 | 2.00 | 2.858 (2) | 172 |
C6—H6···O3Wi | 0.93 | 2.51 | 3.363 (3) | 153 |
Symmetry codes: (i) −x+1, −y+2, −z; (ii) −x+2, −y+1, −z; (iii) −x+1, −y+1, −z; (iv) −x+2, −y, −z+1. |
(C5H7N2)2[Zn(H2O)6](SO4)2 | Z = 1 |
Mr = 555.84 | F(000) = 288 |
Triclinic, P1 | Dx = 1.715 Mg m−3 |
a = 6.977 (3) Å | Mo Kα radiation, λ = 0.71073 Å |
b = 7.929 (3) Å | Cell parameters from 3000 reflections |
c = 11.441 (4) Å | θ = 3.0–28.3° |
α = 72.25 (3)° | µ = 1.41 mm−1 |
β = 89.53 (3)° | T = 100 K |
γ = 64.45 (3)° | Plate, colourless |
V = 538.2 (4) Å3 | 0.33 × 0.25 × 0.07 mm |
Rigaku Oxford Diffraction Xcalibur Atlas diffractometer | 2563 independent reflections |
Radiation source: fine-focus sealed X-ray tube, Enhance (Mo) X-ray Source | 2120 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.032 |
Detector resolution: 10.6249 pixels mm-1 | θmax = 29.7°, θmin = 3.0° |
ω scans | h = −9→8 |
Absorption correction: analytical [CrysAlis PRO (Rigaku Oxford Diffraction, 2015), based on expressions derived by Clark & Reid (1995)] | k = −10→10 |
Tmin = 0.694, Tmax = 0.921 | l = −15→14 |
7323 measured reflections |
Refinement on F2 | 6 restraints |
Least-squares matrix: full | Hydrogen site location: mixed |
R[F2 > 2σ(F2)] = 0.037 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.078 | w = 1/[σ2(Fo2) + (0.023P)2 + 0.501P] where P = (Fo2 + 2Fc2)/3 |
S = 1.08 | (Δ/σ)max < 0.001 |
2563 reflections | Δρmax = 0.38 e Å−3 |
160 parameters | Δρmin = −0.56 e Å−3 |
(C5H7N2)2[Zn(H2O)6](SO4)2 | γ = 64.45 (3)° |
Mr = 555.84 | V = 538.2 (4) Å3 |
Triclinic, P1 | Z = 1 |
a = 6.977 (3) Å | Mo Kα radiation |
b = 7.929 (3) Å | µ = 1.41 mm−1 |
c = 11.441 (4) Å | T = 100 K |
α = 72.25 (3)° | 0.33 × 0.25 × 0.07 mm |
β = 89.53 (3)° |
Rigaku Oxford Diffraction Xcalibur Atlas diffractometer | 2563 independent reflections |
Absorption correction: analytical [CrysAlis PRO (Rigaku Oxford Diffraction, 2015), based on expressions derived by Clark & Reid (1995)] | 2120 reflections with I > 2σ(I) |
Tmin = 0.694, Tmax = 0.921 | Rint = 0.032 |
7323 measured reflections |
R[F2 > 2σ(F2)] = 0.037 | 6 restraints |
wR(F2) = 0.078 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.08 | Δρmax = 0.38 e Å−3 |
2563 reflections | Δρmin = −0.56 e Å−3 |
160 parameters |
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. |
x | y | z | Uiso*/Ueq | ||
Zn1 | 0.5000 | 1.0000 | 0.0000 | 0.01411 (12) | |
O1W | 0.8228 (3) | 0.7965 (3) | 0.06621 (16) | 0.0178 (4) | |
H1WA | 0.840 (5) | 0.684 (3) | 0.108 (2) | 0.027* | |
H1WB | 0.919 (4) | 0.781 (4) | 0.020 (2) | 0.027* | |
O2W | 0.4015 (3) | 0.7817 (3) | 0.07706 (16) | 0.0166 (4) | |
H2WA | 0.508 (4) | 0.678 (3) | 0.114 (2) | 0.025* | |
H2WB | 0.327 (4) | 0.763 (4) | 0.031 (2) | 0.025* | |
O3W | 0.5158 (3) | 0.9549 (3) | −0.17208 (16) | 0.0181 (4) | |
H3WA | 0.443 (4) | 0.913 (4) | −0.200 (3) | 0.027* | |
H3WB | 0.636 (3) | 0.915 (4) | −0.195 (3) | 0.027* | |
S1 | 0.86634 (10) | 0.26278 (9) | 0.19970 (5) | 0.01418 (15) | |
O1 | 0.7842 (3) | 0.4652 (3) | 0.21008 (16) | 0.0189 (4) | |
O2 | 0.8423 (3) | 0.2834 (3) | 0.06753 (15) | 0.0197 (4) | |
O3 | 0.7418 (3) | 0.1661 (3) | 0.26976 (15) | 0.0181 (4) | |
O4 | 1.0947 (3) | 0.1480 (3) | 0.25429 (15) | 0.0179 (4) | |
N1 | 0.7456 (3) | 0.5091 (3) | 0.44013 (19) | 0.0169 (4) | |
H1 | 0.7426 | 0.4984 | 0.3677 | 0.020* | |
C2 | 0.7808 (4) | 0.3492 (4) | 0.5403 (2) | 0.0160 (5) | |
N2 | 0.8090 (3) | 0.1814 (3) | 0.52404 (19) | 0.0188 (5) | |
H2A | 0.8047 | 0.1753 | 0.4504 | 0.023* | |
H2B | 0.8315 | 0.0790 | 0.5872 | 0.023* | |
C3 | 0.7865 (4) | 0.3698 (4) | 0.6584 (2) | 0.0187 (5) | |
H3 | 0.8115 | 0.2628 | 0.7295 | 0.022* | |
C4 | 0.7552 (4) | 0.5472 (4) | 0.6681 (2) | 0.0216 (6) | |
H4 | 0.7589 | 0.5606 | 0.7459 | 0.026* | |
C5 | 0.7172 (4) | 0.7100 (4) | 0.5609 (3) | 0.0229 (6) | |
H5 | 0.6944 | 0.8314 | 0.5671 | 0.027* | |
C6 | 0.7147 (4) | 0.6865 (4) | 0.4490 (2) | 0.0201 (6) | |
H6 | 0.6916 | 0.7921 | 0.3775 | 0.024* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Zn1 | 0.0148 (2) | 0.0157 (2) | 0.0116 (2) | −0.00715 (17) | 0.00165 (15) | −0.00385 (16) |
O1W | 0.0166 (9) | 0.0184 (10) | 0.0147 (9) | −0.0068 (8) | 0.0032 (7) | −0.0023 (8) |
O2W | 0.0166 (10) | 0.0178 (10) | 0.0151 (9) | −0.0089 (8) | −0.0013 (7) | −0.0030 (8) |
O3W | 0.0170 (10) | 0.0258 (10) | 0.0156 (9) | −0.0118 (8) | 0.0037 (7) | −0.0093 (8) |
S1 | 0.0151 (3) | 0.0168 (3) | 0.0112 (3) | −0.0079 (3) | 0.0016 (2) | −0.0044 (2) |
O1 | 0.0220 (10) | 0.0168 (9) | 0.0166 (9) | −0.0078 (8) | 0.0026 (7) | −0.0052 (7) |
O2 | 0.0194 (9) | 0.0301 (11) | 0.0132 (9) | −0.0136 (8) | 0.0040 (7) | −0.0085 (8) |
O3 | 0.0184 (9) | 0.0244 (10) | 0.0165 (9) | −0.0135 (8) | 0.0047 (7) | −0.0077 (8) |
O4 | 0.0160 (9) | 0.0220 (10) | 0.0150 (9) | −0.0091 (8) | 0.0013 (7) | −0.0043 (7) |
N1 | 0.0165 (11) | 0.0220 (12) | 0.0115 (10) | −0.0078 (9) | 0.0015 (8) | −0.0058 (9) |
C2 | 0.0115 (12) | 0.0188 (13) | 0.0162 (12) | −0.0063 (10) | 0.0020 (9) | −0.0048 (10) |
N2 | 0.0252 (12) | 0.0203 (12) | 0.0112 (10) | −0.0113 (10) | 0.0036 (9) | −0.0045 (9) |
C3 | 0.0152 (13) | 0.0237 (14) | 0.0162 (13) | −0.0085 (11) | 0.0025 (10) | −0.0059 (11) |
C4 | 0.0170 (13) | 0.0308 (16) | 0.0204 (13) | −0.0104 (12) | 0.0029 (10) | −0.0135 (12) |
C5 | 0.0194 (14) | 0.0225 (15) | 0.0274 (15) | −0.0088 (12) | 0.0007 (11) | −0.0102 (12) |
C6 | 0.0159 (13) | 0.0169 (14) | 0.0225 (14) | −0.0060 (11) | −0.0019 (10) | −0.0022 (11) |
Zn1—O1Wi | 2.097 (2) | S1—O4 | 1.475 (2) |
Zn1—O1W | 2.097 (2) | N1—H1 | 0.8600 |
Zn1—O2W | 2.0813 (19) | N1—C2 | 1.353 (3) |
Zn1—O2Wi | 2.0813 (19) | N1—C6 | 1.364 (3) |
Zn1—O3W | 2.0996 (18) | C2—N2 | 1.330 (3) |
Zn1—O3Wi | 2.0996 (18) | C2—C3 | 1.413 (3) |
O1W—H1WA | 0.828 (17) | N2—H2A | 0.8600 |
O1W—H1WB | 0.844 (17) | N2—H2B | 0.8600 |
O2W—H2WA | 0.820 (17) | C3—H3 | 0.9300 |
O2W—H2WB | 0.833 (17) | C3—C4 | 1.367 (4) |
O3W—H3WA | 0.823 (17) | C4—H4 | 0.9300 |
O3W—H3WB | 0.828 (17) | C4—C5 | 1.410 (4) |
S1—O1 | 1.4971 (18) | C5—H5 | 0.9300 |
S1—O2 | 1.4736 (18) | C5—C6 | 1.350 (4) |
S1—O3 | 1.4744 (18) | C6—H6 | 0.9300 |
O1Wi—Zn1—O1W | 180.0 | O2—S1—O4 | 110.26 (11) |
O1W—Zn1—O3Wi | 86.88 (8) | O3—S1—O1 | 108.21 (10) |
O1W—Zn1—O3W | 93.12 (8) | O3—S1—O4 | 109.74 (11) |
O1Wi—Zn1—O3Wi | 93.12 (8) | O4—S1—O1 | 108.48 (11) |
O1Wi—Zn1—O3W | 86.88 (8) | C2—N1—H1 | 118.5 |
O2W—Zn1—O1Wi | 88.54 (8) | C2—N1—C6 | 122.9 (2) |
O2W—Zn1—O1W | 91.46 (8) | C6—N1—H1 | 118.5 |
O2Wi—Zn1—O1W | 88.54 (8) | N1—C2—C3 | 117.6 (2) |
O2Wi—Zn1—O1Wi | 91.46 (8) | N2—C2—N1 | 119.4 (2) |
O2W—Zn1—O2Wi | 180.0 | N2—C2—C3 | 123.1 (2) |
O2W—Zn1—O3Wi | 87.20 (7) | C2—N2—H2A | 120.0 |
O2Wi—Zn1—O3Wi | 92.80 (7) | C2—N2—H2B | 120.0 |
O2W—Zn1—O3W | 92.80 (7) | H2A—N2—H2B | 120.0 |
O2Wi—Zn1—O3W | 87.20 (7) | C2—C3—H3 | 120.1 |
O3Wi—Zn1—O3W | 180.000 (15) | C4—C3—C2 | 119.9 (2) |
Zn1—O1W—H1WA | 113 (2) | C4—C3—H3 | 120.1 |
Zn1—O1W—H1WB | 122 (2) | C3—C4—H4 | 119.8 |
H1WA—O1W—H1WB | 107 (3) | C3—C4—C5 | 120.4 (2) |
Zn1—O2W—H2WA | 108 (2) | C5—C4—H4 | 119.8 |
Zn1—O2W—H2WB | 118 (2) | C4—C5—H5 | 120.6 |
H2WA—O2W—H2WB | 111 (3) | C6—C5—C4 | 118.7 (3) |
Zn1—O3W—H3WA | 125 (2) | C6—C5—H5 | 120.6 |
Zn1—O3W—H3WB | 117 (2) | N1—C6—H6 | 119.7 |
H3WA—O3W—H3WB | 110 (3) | C5—C6—N1 | 120.5 (2) |
O2—S1—O1 | 108.64 (11) | C5—C6—H6 | 119.7 |
O2—S1—O3 | 111.43 (10) | ||
N1—C2—C3—C4 | 0.5 (4) | C3—C4—C5—C6 | −0.7 (4) |
C2—N1—C6—C5 | −0.3 (4) | C4—C5—C6—N1 | 0.8 (4) |
C2—C3—C4—C5 | 0.0 (4) | C6—N1—C2—N2 | 179.8 (2) |
N2—C2—C3—C4 | −179.7 (2) | C6—N1—C2—C3 | −0.4 (3) |
Symmetry code: (i) −x+1, −y+2, −z. |
D—H···A | D—H | H···A | D···A | D—H···A |
O1W—H1WA···O1 | 0.83 (2) | 1.97 (2) | 2.765 (3) | 162 (3) |
O1W—H1WB···O2ii | 0.84 (2) | 1.89 (2) | 2.731 (3) | 172 (3) |
O2W—H2WA···O1 | 0.82 (2) | 1.97 (2) | 2.775 (3) | 169 (3) |
O2W—H2WB···O2iii | 0.83 (2) | 1.85 (2) | 2.687 (3) | 178 (3) |
O3W—H3WA···O3iii | 0.82 (2) | 1.93 (2) | 2.752 (3) | 176 (3) |
O3W—H3WB···O4ii | 0.83 (2) | 1.91 (2) | 2.729 (3) | 174 (3) |
N1—H1···O1 | 0.86 | 1.90 | 2.754 (3) | 171 |
N2—H2A···O3 | 0.86 | 2.15 | 2.997 (3) | 171 |
N2—H2B···O4iv | 0.86 | 2.01 | 2.860 (3) | 173 |
C6—H6···O3Wi | 0.93 | 2.51 | 3.370 (4) | 153 |
Symmetry codes: (i) −x+1, −y+2, −z; (ii) −x+2, −y+1, −z; (iii) −x+1, −y+1, −z; (iv) −x+2, −y, −z+1. |
Experimental details
(I) | (II) | (III) | |
Crystal data | |||
Chemical formula | (C5H7N2)[Al(H2O)6](SO4)2·4H2O | (C5H7N2)2[Co(H2O)6]3(SO4)4·2H2O | (C5H7N2)2[Mg(H2O)6]3(SO4)4·2H2O |
Mr | 494.38 | 1111.60 | 1007.74 |
Crystal system, space group | Triclinic, P1 | Triclinic, P1 | Triclinic, P1 |
Temperature (K) | 100 | 100 | 100 |
a, b, c (Å) | 6.667 (3), 12.160 (4), 12.911 (4) | 6.640 (3), 11.710 (4), 14.294 (4) | 6.682 (3), 11.807 (4), 14.309 (4) |
α, β, γ (°) | 72.30 (3), 81.03 (3), 85.57 (3) | 67.97 (3), 81.57 (3), 85.39 (3) | 68.23 (3), 82.13 (3), 84.76 (3) |
V (Å3) | 984.5 (7) | 1018.8 (7) | 1037.5 (7) |
Z | 2 | 1 | 1 |
Radiation type | Mo Kα | Mo Kα | Mo Kα |
µ (mm−1) | 0.41 | 1.53 | 0.39 |
Crystal size (mm) | 0.50 × 0.33 × 0.20 | 0.42 × 0.27 × 0.08 | 0.43 × 0.36 × 0.23 |
Data collection | |||
Diffractometer | Rigaku Oxford Diffraction Xcalibur Atlas | Rigaku Oxford Diffraction Xcalibur Atlas | Rigaku Oxford Diffraction Xcalibur Atlas |
Absorption correction | Analytical [CrysAlis PRO (Rigaku Oxford Diffraction, 2015), based on expressions derived by Clark & Reid (1995)] | Analytical [CrysAlis PRO (Rigaku Oxford Diffraction, 2015), based on expressions derived by Clark & Reid (1995)] | Analytical [CrysAlis PRO (Rigaku Oxford Diffraction, 2015), based on expressions derived by Clark & Reid (1995)] |
Tmin, Tmax | 0.869, 0.930 | 0.609, 0.891 | 0.892, 0.928 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 14826, 4751, 3685 | 14070, 4878, 4072 | 11467, 4884, 3875 |
Rint | 0.027 | 0.025 | 0.026 |
(sin θ/λ)max (Å−1) | 0.691 | 0.695 | 0.689 |
Refinement | |||
R[F2 > 2σ(F2)], wR(F2), S | 0.036, 0.093, 1.02 | 0.031, 0.069, 1.06 | 0.040, 0.089, 1.03 |
No. of reflections | 4751 | 4878 | 4884 |
No. of parameters | 316 | 321 | 324 |
No. of restraints | 20 | 20 | 20 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement | H atoms treated by a mixture of independent and constrained refinement | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.32, −0.62 | 0.42, −0.44 | 0.45, −0.40 |
(IV) | (V) | |
Crystal data | ||
Chemical formula | (C5H7N2)2[Ni(H2O)6](SO4)2 | (C5H7N2)2[Zn(H2O)6](SO4)2 |
Mr | 549.18 | 555.84 |
Crystal system, space group | Triclinic, P1 | Triclinic, P1 |
Temperature (K) | 100 | 100 |
a, b, c (Å) | 6.970 (3), 7.913 (3), 11.391 (4) | 6.977 (3), 7.929 (3), 11.441 (4) |
α, β, γ (°) | 72.31 (3), 89.57 (3), 64.20 (3) | 72.25 (3), 89.53 (3), 64.45 (3) |
V (Å3) | 533.2 (4) | 538.2 (4) |
Z | 1 | 1 |
Radiation type | Mo Kα | Mo Kα |
µ (mm−1) | 1.18 | 1.41 |
Crystal size (mm) | 0.15 × 0.12 × 0.1 | 0.33 × 0.25 × 0.07 |
Data collection | ||
Diffractometer | Rigaku Oxford Diffraction Xcalibur Atlas | Rigaku Oxford Diffraction Xcalibur Atlas |
Absorption correction | Analytical [CrysAlis PRO (Rigaku Oxford Diffraction, 2015), based on expressions derived by Clark & Reid (1995)] | Analytical [CrysAlis PRO (Rigaku Oxford Diffraction, 2015), based on expressions derived by Clark & Reid (1995)] |
Tmin, Tmax | 0.879, 0.909 | 0.694, 0.921 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 11780, 2662, 2341 | 7323, 2563, 2120 |
Rint | 0.026 | 0.032 |
(sin θ/λ)max (Å−1) | 0.695 | 0.696 |
Refinement | ||
R[F2 > 2σ(F2)], wR(F2), S | 0.026, 0.060, 1.07 | 0.037, 0.078, 1.08 |
No. of reflections | 2662 | 2563 |
No. of parameters | 160 | 160 |
No. of restraints | 6 | 6 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.31, −0.44 | 0.38, −0.56 |
Computer programs: CrysAlis PRO (Rigaku Oxford Diffraction, 2015), SHELXT (Sheldrick, 2015a), SHELXS97 (Sheldrick, 2008), SHELXL2014 (Sheldrick, 2015b), DIAMOND (Brandenburg, 1997), OLEX2 (Dolomanov et al., 2009).
D—H···A | D—H | H···A | D···A | D—H···A |
O11W—H11A···O4W | 0.821 (15) | 1.810 (15) | 2.626 (2) | 173 (2) |
O11W—H11B···O21iii | 0.841 (15) | 1.885 (16) | 2.715 (2) | 168 (2) |
O12W—H12A···O14iv | 0.859 (15) | 1.791 (16) | 2.648 (2) | 175 (2) |
O12W—H12B···O22 | 0.833 (15) | 1.800 (16) | 2.628 (2) | 173 (2) |
O13W—H13A···O21i | 0.842 (15) | 1.884 (16) | 2.711 (2) | 167 (2) |
O13W—H13B···O13 | 0.839 (15) | 1.783 (15) | 2.6144 (18) | 171 (2) |
O21W—H21A···O13 | 0.833 (15) | 1.843 (16) | 2.667 (2) | 170 (2) |
O21W—H21B···O23iii | 0.852 (15) | 1.770 (16) | 2.622 (2) | 180 (3) |
O22W—H22A···O1Wii | 0.850 (15) | 1.760 (16) | 2.606 (2) | 173 (2) |
O22W—H22B···O12v | 0.830 (15) | 1.819 (16) | 2.647 (2) | 175 (2) |
O23W—H23A···O12 | 0.837 (15) | 1.913 (16) | 2.740 (2) | 169 (2) |
O23W—H23B···O22ii | 0.825 (15) | 1.847 (16) | 2.6660 (18) | 172 (2) |
N1—H1···O24 | 0.86 | 1.87 | 2.711 (2) | 164 |
N2—H2A···O23 | 0.86 | 2.09 | 2.944 (2) | 176 |
N2—H2B···O11ii | 0.86 | 2.04 | 2.856 (2) | 159 |
C6—H6···O1Wvi | 0.93 | 2.30 | 3.127 (2) | 147 |
O1W—H1WA···O11 | 0.841 (15) | 1.959 (16) | 2.792 (2) | 170 (2) |
O1W—H1WB···O2W | 0.849 (16) | 1.920 (16) | 2.768 (2) | 177 (2) |
O2W—H2WA···O11iv | 0.825 (16) | 2.089 (18) | 2.864 (2) | 156 (2) |
O2W—H2WB···O3Wvii | 0.800 (16) | 2.016 (16) | 2.812 (2) | 173 (2) |
O3W—H3WA···O14i | 0.831 (16) | 2.250 (17) | 3.069 (2) | 169 (2) |
O3W—H3WB···O24 | 0.836 (16) | 1.942 (16) | 2.7609 (19) | 166 (2) |
O4W—H4WA···O3W | 0.845 (16) | 2.099 (17) | 2.929 (2) | 167 (2) |
O4W—H4WB···O2Wi | 0.808 (16) | 2.044 (16) | 2.849 (2) | 175 (2) |
Symmetry codes: (i) −x+1, −y, −z+1; (ii) −x+1, −y+1, −z+1; (iii) x+1, y, z; (iv) x−1, y, z; (v) −x+2, −y+1, −z+1; (vi) x, y, z−1; (vii) x, y, z+1. |
Compound | CgI | CgJ | Distance between ring centroids (Å) | Perpendicular distance between rings (Å) | Offset (Å) |
(I) | Cg1 | Cg1i | 4.130 (2) | 3.0792 (8) | 2.753 |
(I) | Cg1 | Cg1ii | 3.454 (2) | 3.2134 (8) | 1.265 |
(II) | Cg1 | Cg1iii | 3.634 (2) | 3.2118 (8) | 1.700 |
(II) | Cg1 | Cg1iv | 3.706 (2) | 3.3228 (8) | 1.640 |
(III) | Cg1 | Cg1iii | 3.677 (2) | 3.2564 (8) | 1.708 |
(III) | Cg1 | Cg1iv | 3.666 (2) | 3.3574 (8) | 1.471 |
(IV) | Cg1 | Cg1v | 3.955 (2) | 3.3426 (9) | 2.114 |
(IV) | Cg1 | Cg1vi | 3.564 (2) | 3.3101 (9) | 1.321 |
(V) | Cg1 | Cg1v | 3.950 (2) | 3.3531 (12) | 2.088 |
(V) | Cg1 | Cg1vi | 3.569 (2) | 3.3166 (12) | 1.318 |
(VI) | Cg1 | Cg1vi | 3.414 (3) | 3.4028 (15) | 0.276 |
(VI) | Cg1 | Cg1vii | 3.958 (3) | 3.4079 (15) | 2.013 |
Symmetry codes: (i) -x, -y+1, -z; (ii) -x+1, -y+1, -z; (iii) -x, -y, -z+2; (iv) -x+1, -y, -z+2; (v) -x+1, -y+1, -z+1; (vi) -x+2, -y+1, -z+1; (vii) -x+1, -y+1, -z+2. |
D—H···A | D—H | H···A | D···A | D—H···A |
O11W—H11A···O13Wii | 0.827 (17) | 2.139 (17) | 2.964 (2) | 175 (3) |
O11W—H11B···O14iii | 0.813 (17) | 2.068 (17) | 2.881 (2) | 178 (3) |
O12W—H12A···O21 | 0.838 (16) | 1.878 (17) | 2.711 (2) | 173 (3) |
O12W—H12B···O12iv | 0.815 (16) | 2.090 (17) | 2.894 (3) | 169 (3) |
O13W—H13A···O23iii | 0.819 (16) | 1.984 (17) | 2.800 (2) | 175 (2) |
O13W—H13B···O22 | 0.819 (16) | 1.921 (17) | 2.735 (2) | 172 (3) |
O14W—H14A···O13iii | 0.828 (17) | 1.853 (18) | 2.671 (2) | 169 (3) |
O14W—H14B···O12 | 0.810 (17) | 1.934 (17) | 2.744 (2) | 179 (3) |
O15W—H15A···O22v | 0.824 (17) | 1.899 (17) | 2.706 (2) | 166 (3) |
O15W—H15B···O14 | 0.830 (16) | 1.928 (17) | 2.756 (2) | 177 (3) |
O16W—H16A···O21iii | 0.840 (17) | 1.867 (18) | 2.699 (2) | 171 (3) |
O16W—H16B···O13iv | 0.839 (17) | 1.864 (17) | 2.703 (2) | 179 (3) |
O21W—H21A···O11iv | 0.817 (17) | 1.951 (18) | 2.766 (2) | 175 (3) |
O21W—H21B···O1Wvi | 0.818 (17) | 1.953 (18) | 2.758 (2) | 168 (3) |
O22W—H22A···O23iii | 0.804 (18) | 2.24 (2) | 2.959 (3) | 150 (3) |
O22W—H22B···O24 | 0.837 (17) | 2.009 (19) | 2.835 (2) | 169 (3) |
O23W—H23A···O1Wiv | 0.819 (17) | 1.901 (18) | 2.714 (2) | 171 (3) |
O23W—H23B···O24vii | 0.811 (17) | 1.958 (18) | 2.759 (2) | 169 (3) |
N1—H1···O11 | 0.86 | 1.85 | 2.701 (3) | 172 |
N2—H2A···O14 | 0.86 | 2.10 | 2.955 (3) | 173 |
N2—H2B···O24v | 0.86 | 2.12 | 2.959 (3) | 164 |
O1W—H1WA···O12 | 0.85 | 2.09 | 2.935 (2) | 175 |
O1W—H1WB···O21iv | 0.91 | 1.80 | 2.711 (2) | 171 |
Symmetry codes: (ii) −x+2, −y, −z+1; (iii) x+1, y, z; (iv) −x+1, −y+1, −z+1; (v) −x+1, −y, −z+1; (vi) −x+2, −y+1, −z+1; (vii) −x+1, −y+1, −z. |
D—H···A | D—H | H···A | D···A | D—H···A |
O11W—H11A···O13Wii | 0.808 (17) | 2.192 (19) | 2.977 (2) | 164 (3) |
O11W—H11B···O14iii | 0.810 (17) | 2.063 (18) | 2.873 (2) | 177 (3) |
O12W—H12A···O21 | 0.821 (17) | 1.903 (17) | 2.722 (2) | 176 (3) |
O12W—H12B···O12iv | 0.822 (17) | 2.065 (18) | 2.867 (2) | 165 (3) |
O13W—H13A···O23iii | 0.831 (16) | 1.982 (17) | 2.809 (2) | 173 (3) |
O13W—H13B···O22 | 0.815 (16) | 1.938 (17) | 2.750 (2) | 174 (3) |
O14W—H14A···O13iii | 0.830 (17) | 1.834 (18) | 2.658 (2) | 172 (3) |
O14W—H14B···O12 | 0.840 (17) | 1.875 (18) | 2.713 (2) | 175 (3) |
O15W—H15A···O22v | 0.843 (17) | 1.877 (18) | 2.701 (2) | 165 (3) |
O15W—H15B···O14 | 0.831 (17) | 1.955 (17) | 2.783 (2) | 174 (3) |
O16W—H16A···O21iii | 0.845 (18) | 1.853 (18) | 2.698 (2) | 178 (3) |
O16W—H16B···O13iv | 0.846 (18) | 1.875 (19) | 2.714 (2) | 172 (3) |
O21W—H21A···O11iv | 0.825 (17) | 1.937 (18) | 2.758 (2) | 173 (3) |
O21W—H21B···O1Wvi | 0.816 (17) | 1.975 (18) | 2.783 (2) | 171 (3) |
O22W—H22A···O23iii | 0.813 (17) | 2.116 (19) | 2.912 (3) | 166 (3) |
O22W—H22B···O24 | 0.841 (17) | 2.045 (18) | 2.876 (2) | 170 (3) |
O23W—H23A···O1Wiv | 0.821 (17) | 1.895 (17) | 2.711 (2) | 173 (3) |
O23W—H23B···O24vii | 0.824 (17) | 1.936 (17) | 2.752 (2) | 170 (3) |
N1—H1···O11 | 0.86 | 1.84 | 2.697 (3) | 174.9 |
N2—H2A···O14 | 0.86 | 2.10 | 2.957 (3) | 174.3 |
N2—H2B···O24v | 0.86 | 2.18 | 2.999 (3) | 158.2 |
O1W—H1WA···O12 | 0.822 (16) | 2.039 (17) | 2.850 (2) | 169 (2) |
O1W—H1WB···O21iv | 0.829 (16) | 1.893 (17) | 2.716 (2) | 172 (3) |
Symmetry codes: (ii) −x+2, −y, −z+1; (iii) x+1, y, z; (iv) −x+1, −y+1, −z+1; (v) −x+1, −y, −z+1; (vi) −x+2, −y+1, −z+1; (vii) −x+1, −y+1, −z. |
D—H···A | D—H | H···A | D···A | D—H···A |
O1W—H1WA···O1 | 0.830 (15) | 1.953 (16) | 2.756 (2) | 163 (2) |
O1W—H1WB···O2ii | 0.825 (15) | 1.913 (16) | 2.732 (2) | 172 (2) |
O2W—H2WA···O1 | 0.841 (15) | 1.951 (16) | 2.764 (2) | 162 (2) |
O2W—H2WB···O2iii | 0.832 (15) | 1.852 (16) | 2.6834 (18) | 177 (2) |
O3W—H3WA···O3iii | 0.839 (15) | 1.927 (16) | 2.7556 (18) | 169 (2) |
O3W—H3WB···O4ii | 0.829 (15) | 1.910 (16) | 2.727 (2) | 168 (2) |
N1—H1···O1 | 0.86 | 1.90 | 2.755 (2) | 171.1 |
N2—H2A···O3 | 0.86 | 2.15 | 3.006 (2) | 170.8 |
N2—H2B···O4iv | 0.86 | 2.00 | 2.858 (2) | 172.3 |
C6—H6···O3Wi | 0.93 | 2.51 | 3.363 (3) | 152.8 |
Symmetry codes: (i) −x+1, −y+2, −z; (ii) −x+2, −y+1, −z; (iii) −x+1, −y+1, −z; (iv) −x+2, −y, −z+1. |
D—H···A | D—H | H···A | D···A | D—H···A |
O1W—H1WA···O1 | 0.828 (17) | 1.966 (19) | 2.765 (3) | 162 (3) |
O1W—H1WB···O2ii | 0.844 (17) | 1.893 (18) | 2.731 (3) | 172 (3) |
O2W—H2WA···O1 | 0.820 (17) | 1.966 (18) | 2.775 (3) | 169 (3) |
O2W—H2WB···O2iii | 0.833 (17) | 1.854 (18) | 2.687 (3) | 178 (3) |
O3W—H3WA···O3iii | 0.823 (17) | 1.930 (18) | 2.752 (3) | 176 (3) |
O3W—H3WB···O4ii | 0.828 (17) | 1.905 (18) | 2.729 (3) | 174 (3) |
N1—H1···O1 | 0.86 | 1.90 | 2.754 (3) | 171 |
N2—H2A···O3 | 0.86 | 2.15 | 2.997 (3) | 171 |
N2—H2B···O4iv | 0.86 | 2.01 | 2.860 (3) | 173 |
C6—H6···O3Wi | 0.93 | 2.51 | 3.370 (4) | 153 |
Symmetry codes: (i) −x+1, −y+2, −z; (ii) −x+2, −y+1, −z; (iii) −x+1, −y+1, −z; (iv) −x+2, −y, −z+1. |