Abstract
In the title compound, C16H28N4O8·2H2O, the 12-membered macrocycle has twofold crystallographic symmetry and the asymmetric unit comprises one half-molecule. The four carboxyl/carboxylate groups reside on the same side of the macrocycle. The molecule is a double zwitterion with two of the carboxylic acid H atoms transferred to the two N atoms on the opposite sides of the macrocycle, resulting in both N atoms having positive charges and leaving the two resulting carboxylate groups with negative charges. The two remaining carboxylic acid groups and the carboxylate groups form O—H⋯O hydrogen bonds with the crystal water molecules. The H atoms bound to the N atoms within the macrocyle are engaged in two equivalent hydrogen bonds with the adjacent N atoms.
Related literature
Kumagai et al. (2002 ▶) describe different coordinations for carboxylate groups. For background information about the title compound and its metal complexes, see: Viola-Villegas & Doyle (2009 ▶). For macrocycle configurations, see: Bosnich et al. (1965 ▶); Dale (1973 ▶, 1976 ▶, 1980 ▶); Meyer et al. (1998 ▶).
Experimental
Crystal data
C16H28N4O8·2H2O
M r = 440.46
Orthorhombic,
a = 17.183 (2) Å
b = 6.5826 (9) Å
c = 17.983 (2) Å
V = 2034.0 (5) Å3
Z = 4
Mo Kα radiation
μ = 0.12 mm−1
T = 100 K
0.43 × 0.27 × 0.27 mm
Data collection
Bruker SMART APEX CCD diffractometer
Absorption correction: multi-scan (SADABS; Bruker 2003 ▶) T min = 0.810, T max = 1.000
19408 measured reflections
2520 independent reflections
2236 reflections with I > 2σ(I)
R int = 0.037
Refinement
R[F 2 > 2σ(F 2)] = 0.042
wR(F 2) = 0.112
S = 1.08
2520 reflections
144 parameters
2 restraints
H atoms treated by a mixture of independent and constrained refinement
Δρmax = 0.70 e Å−3
Δρmin = −0.19 e Å−3
Data collection: SMART (Bruker, 2001 ▶); cell refinement: SAINT-Plus (Bruker, 2001 ▶); data reduction: SAINT-Plus; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: SHELXTL (Sheldrick, 2008 ▶); software used to prepare material for publication: SHELXL97 and PLATON Spek (2009) ▶.
Supplementary Material
Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536811004843/kp2290sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811004843/kp2290Isup2.hkl
Table 1. Hydrogen-bond geometry (Å, °).
D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
---|---|---|---|---|
O3—H3⋯O5 | 0.84 | 1.71 | 2.5295 (14) | 166 |
N1—H1⋯N2 | 0.93 | 2.44 | 2.8940 (14) | 110 |
O5—H5D⋯O1i | 0.86 (1) | 1.78 (2) | 2.6380 (14) | 173 (2) |
O5—H5C⋯O1ii | 0.84 (1) | 1.85 (2) | 2.6776 (14) | 170 (2) |
Symmetry codes: (i) ; (ii) .
Acknowledgments
MZ was supported by NSF grant 0111511. The diffractometer was funded by NSF grant 0087210, by the Ohio Board of Regents grant CAP-491 and by Youngstown State University.
supplementary crystallographic information
Comment
In the course of our studies to prepare coordination polymer and metal-organic framework type compounds we investigated the title compound as a potentional building block. The molecule 1,4,7,10-tetraazacyclodecane-1,4,7,10-tetraacetic acid DOTAH4 and its deprotonated analogs, [DOTAH2]2- and [DOTA]4- have several features desirable in coordination chemistry. The ligand offers a macrocycle with four neutral nitrogen donor sites as well as four dangling carboxylic acid groups. Carboxylate groups when deprotonated have been shown to exhibit nine different coordination modes with metal ions, seven of which coordinate two or more metal ions (Kumagai et al., 2002). Therefore, the potential for forming molecular species as well as coordination polymers or metal-organic framework type compounds exists for this organic building block. For numerous examples of metal containing DOTAH4 compounds and its charged analogues see Viola-Villegas & Doyle (2009).
Only half of DOTAH4 molecule (Fig. 1) in the structure is an asymmetric unit. The other half of the macrocycle is generated by a twofold rotation axis parallel to the b axis. There is no significant ring strain based on an analysis of the bond angles withing the ring. The ring is composed of eight methylene carbons (C1—C4, C1i—C4i), two ammonium N atoms (N1, N1i) and two tertiary N atoms (N2, N2i) (symmetry operator (i): -x + 1, y, -z + 3/2). The bond angles between them range from 110–112°. The configuration has all four N atoms located above the eight methylene carbons along the direction of the twofold axis in the centre of the ring producing a basket-like shape that would be able to coordinate a metal without large changes of the overall structure of the molecule. According to the system outlined by Dale this arrangement would be described as (3,3,3,3)-B (Dale, 1973, 1976, 1980, Meyer et al., 1998). This system uses numbers to indicate the number of chemical bonds between the genuinie corners in the macrocycle. Genuine corners are the central atoms in an anti-gauche-gauche-anti bond sequence. In the title compound the atoms C1, C3, C1A, and C3A constitute genuine corners which are separated from each other along the macrocycle by three bonds. The "B" designation indicates that the four heteroatoms in this 12-membered macrocylce reside in a square planar arrangement above the methylene carbons (as described above). Using the terminology of Bosnich et al. (1965) the configuration of the macrocycle would be cis-I since all of the carboxylate containing groups project in the same direction.
The weighted average ring bond distance is 1.503 Å (PLATON, Spek (2009)). The weighted average absolute torsion angle is 100.45°. The total puckering amplitude of the ring is 1.526 Å. The four carboxylic acid and carboxylate groups are bound to the N atoms and also all reside above the macrocycle. This arrangement leads to well separated hydrophobic and hydrophilic parts within the molecule. The H atoms bound to the N atoms within the macrocyle are engaged in two equivalent hydrogen bonds with the adjacent nitrogen atoms (N1—H1···N2, N1i—H1i···N2i, Table 1). The N1—H1 and H1···N2 distances are 0.93 Å and 2.44 Å respectively. The angle between the donor and acceptor is 110.1° in accord with the donor and acceptor both residing within the ring and being separated by two atoms.
The crystal packing (Figs. 2 and 3) is dominated by hydrogen bonding between the crystal water molecules and the carboxylic acid and carboxylate groups. Each water molecule forms three hydrogen bonding interactions with the two hydrogen atoms oriented towards carboxylate groups (O5—H5D···O1ii, O5—H5C···O1iii, Table 1) and the oxygen directed towards a carboxylic acid group (O3—H3···O5, Table 1).
Experimental
The title compound 1,4,7,10-tetraazacyclodecane-1,4,7,10-tetraacetic acid was purchased from Strem Chemicals and used without further purification.
The compound was crystallized from a saturated DMSO solution. A DMSO solution (2 mL) was saturated with DOTAH4 at 323 K. Upon cooling to room temperature and sitting for four days colourless block shaped crystals were formed.
Refinement
The oxygen to hydrogen bond distances in the solvent water molecule were restrained to be 0.84 Å with a standard deviation of 0.02 Å. They were set to have an isotropic displacement parameter of 1.5 times that of the adjacent oxygen atom. The same displacement parameter was used for the hydrogen bound to the carboxylic acid, which were placed in calculated positions at a distance of 0.84 Å from the O atom but that were allowed to freely rotate at a fixed angle around the C—O bond to best fit the experimental electron density. All other hydrogen atoms in the structure were placed in calculated positions with X—H distances of 0.99 (methylene) or 0.93 Å (amine) with Uiso(H) = 1.2 Ueq(X).
The highest residual electron density peak in the final Fourier map, with a heigth of 0.70 e-×Å-3, is located at the center of the macrocylce. An electron density difference Fourier map cutting through the protonated amine N atoms and the center of the residual electron density in the middle of the ring (with the protic amine H atoms removed prior to generation of the map) shows electron densities in the positions of the amine H atoms that are substantially larger than that of the residual electron density in the center of the ring, thus indicating that the amine H atoms are indeed fully protonated (which is supported by a refinement of the amine H atom occupancy, which yielded full occupancy). The residual density in the center of the ring refines to about 60% of one electron and it is located on a special position (site symmetry of 4c).
Figures
Crystal data
C16H28N4O8·2H2O | Dx = 1.438 Mg m−3 |
Mr = 440.46 | Mo Kα radiation, λ = 0.71073 Å |
Orthorhombic, Pbcn | Cell parameters from 13988 reflections |
a = 17.183 (2) Å | θ = 1.0–28.3° |
b = 6.5826 (9) Å | µ = 0.12 mm−1 |
c = 17.983 (2) Å | T = 100 K |
V = 2034.0 (5) Å3 | Block, colourless |
Z = 4 | 0.43 × 0.27 × 0.27 mm |
F(000) = 944 |
Data collection
Bruker SMART APEX CCD diffractometer | 2520 independent reflections |
Radiation source: fine-focus sealed tube | 2236 reflections with I > 2σ(I) |
graphite | Rint = 0.037 |
ω scans | θmax = 28.3°, θmin = 2.3° |
Absorption correction: multi-scan (SADABS; Bruker 2003) | h = −22→22 |
Tmin = 0.810, Tmax = 1.000 | k = −8→8 |
19408 measured reflections | l = −23→23 |
Refinement
Refinement on F2 | Primary atom site location: structure-invariant direct methods |
Least-squares matrix: full | Secondary atom site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.042 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.112 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.08 | w = 1/[σ2(Fo2) + (0.0616P)2 + 0.8651P] where P = (Fo2 + 2Fc2)/3 |
2520 reflections | (Δ/σ)max = 0.003 |
144 parameters | Δρmax = 0.70 e Å−3 |
2 restraints | Δρmin = −0.19 e Å−3 |
Special details
Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes. |
Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger. |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)
x | y | z | Uiso*/Ueq | ||
C1 | 0.52319 (7) | 0.29809 (18) | 0.59684 (7) | 0.0172 (2) | |
H1A | 0.5484 | 0.1817 | 0.5716 | 0.021* | |
H1B | 0.5118 | 0.4028 | 0.5588 | 0.021* | |
C2 | 0.44727 (7) | 0.22770 (18) | 0.63205 (7) | 0.0169 (2) | |
H2A | 0.4101 | 0.1899 | 0.5923 | 0.020* | |
H2B | 0.4573 | 0.1052 | 0.6625 | 0.020* | |
C3 | 0.35164 (7) | 0.29561 (18) | 0.72810 (7) | 0.0161 (2) | |
H3A | 0.3257 | 0.1827 | 0.7015 | 0.019* | |
H3B | 0.3118 | 0.3994 | 0.7398 | 0.019* | |
C4 | 0.61331 (7) | 0.21651 (18) | 0.70032 (7) | 0.0165 (2) | |
H4A | 0.6542 | 0.1467 | 0.6711 | 0.020* | |
H4B | 0.5724 | 0.1157 | 0.7123 | 0.020* | |
C5 | 0.64046 (7) | 0.50850 (18) | 0.61660 (7) | 0.0175 (2) | |
H5A | 0.6619 | 0.4297 | 0.5744 | 0.021* | |
H5B | 0.6833 | 0.5319 | 0.6524 | 0.021* | |
C6 | 0.61183 (7) | 0.71385 (19) | 0.58773 (7) | 0.0190 (3) | |
C7 | 0.37872 (7) | 0.54695 (18) | 0.63298 (7) | 0.0167 (2) | |
H7A | 0.3332 | 0.4922 | 0.6058 | 0.020* | |
H7B | 0.4178 | 0.5900 | 0.5957 | 0.020* | |
C8 | 0.35349 (7) | 0.73022 (18) | 0.67787 (7) | 0.0187 (3) | |
N1 | 0.57832 (6) | 0.38475 (15) | 0.65388 (5) | 0.0147 (2) | |
H1 | 0.5502 | 0.4699 | 0.6852 | 0.018* | |
N2 | 0.41201 (5) | 0.38638 (15) | 0.67930 (6) | 0.0156 (2) | |
O1 | 0.66535 (6) | 0.81050 (15) | 0.55408 (6) | 0.0293 (2) | |
O2 | 0.54404 (5) | 0.76758 (14) | 0.59796 (6) | 0.0248 (2) | |
O3 | 0.31304 (5) | 0.86834 (13) | 0.64068 (5) | 0.0201 (2) | |
H3 | 0.3110 | 0.8356 | 0.5956 | 0.030* | |
O4 | 0.36798 (7) | 0.75428 (15) | 0.74325 (5) | 0.0286 (2) | |
O5 | 0.29964 (6) | 0.82984 (15) | 0.50131 (5) | 0.0218 (2) | |
H5C | 0.2571 (9) | 0.800 (3) | 0.4810 (9) | 0.033* | |
H5D | 0.3139 (11) | 0.942 (2) | 0.4806 (10) | 0.033* |
Atomic displacement parameters (Å2)
U11 | U22 | U33 | U12 | U13 | U23 | |
C1 | 0.0153 (5) | 0.0185 (5) | 0.0176 (5) | −0.0004 (4) | −0.0003 (4) | −0.0007 (4) |
C2 | 0.0144 (5) | 0.0160 (5) | 0.0204 (6) | −0.0006 (4) | −0.0001 (4) | −0.0015 (4) |
C3 | 0.0124 (5) | 0.0153 (5) | 0.0205 (6) | −0.0014 (4) | −0.0004 (4) | −0.0014 (4) |
C4 | 0.0159 (5) | 0.0127 (5) | 0.0209 (6) | 0.0024 (4) | −0.0001 (4) | 0.0018 (4) |
C5 | 0.0141 (5) | 0.0164 (5) | 0.0219 (6) | −0.0006 (4) | 0.0033 (4) | 0.0026 (4) |
C6 | 0.0210 (6) | 0.0160 (5) | 0.0201 (6) | −0.0001 (4) | −0.0001 (4) | 0.0014 (4) |
C7 | 0.0148 (5) | 0.0157 (5) | 0.0195 (5) | 0.0005 (4) | −0.0017 (4) | 0.0005 (4) |
C8 | 0.0183 (6) | 0.0143 (5) | 0.0236 (6) | −0.0037 (4) | 0.0004 (4) | 0.0004 (4) |
N1 | 0.0132 (4) | 0.0137 (5) | 0.0173 (5) | 0.0007 (3) | 0.0010 (3) | 0.0008 (4) |
N2 | 0.0127 (4) | 0.0142 (5) | 0.0198 (5) | 0.0004 (3) | 0.0003 (4) | 0.0010 (4) |
O1 | 0.0287 (5) | 0.0212 (5) | 0.0381 (6) | 0.0002 (4) | 0.0111 (4) | 0.0102 (4) |
O2 | 0.0187 (5) | 0.0196 (4) | 0.0361 (5) | 0.0025 (4) | −0.0007 (4) | 0.0035 (4) |
O3 | 0.0218 (4) | 0.0158 (4) | 0.0227 (4) | 0.0021 (3) | 0.0013 (3) | −0.0007 (3) |
O4 | 0.0445 (6) | 0.0186 (5) | 0.0227 (5) | −0.0021 (4) | −0.0053 (4) | −0.0026 (4) |
O5 | 0.0234 (5) | 0.0173 (4) | 0.0246 (5) | 0.0009 (4) | −0.0023 (4) | 0.0023 (3) |
Geometric parameters (Å, °)
C1—N1 | 1.5082 (15) | C5—C6 | 1.5294 (17) |
C1—C2 | 1.5223 (16) | C5—H5A | 0.9900 |
C1—H1A | 0.9900 | C5—H5B | 0.9900 |
C1—H1B | 0.9900 | C6—O2 | 1.2312 (16) |
C2—N2 | 1.4765 (15) | C6—O1 | 1.2715 (16) |
C2—H2A | 0.9900 | C7—N2 | 1.4622 (15) |
C2—H2B | 0.9900 | C7—C8 | 1.5149 (17) |
C3—N2 | 1.4844 (15) | C7—H7A | 0.9900 |
C3—C4i | 1.5136 (16) | C7—H7B | 0.9900 |
C3—H3A | 0.9900 | C8—O4 | 1.2122 (16) |
C3—H3B | 0.9900 | C8—O3 | 1.3255 (15) |
C4—N1 | 1.5117 (15) | N1—H1 | 0.9300 |
C4—C3i | 1.5136 (17) | O3—H3 | 0.8400 |
C4—H4A | 0.9900 | O5—H5C | 0.840 (15) |
C4—H4B | 0.9900 | O5—H5D | 0.865 (15) |
C5—N1 | 1.5011 (15) | ||
N1—C1—C2 | 111.75 (10) | N1—C5—H5B | 108.8 |
N1—C1—H1A | 109.3 | C6—C5—H5B | 108.8 |
C2—C1—H1A | 109.3 | H5A—C5—H5B | 107.7 |
N1—C1—H1B | 109.3 | O2—C6—O1 | 127.71 (12) |
C2—C1—H1B | 109.3 | O2—C6—C5 | 120.50 (11) |
H1A—C1—H1B | 107.9 | O1—C6—C5 | 111.78 (11) |
N2—C2—C1 | 112.06 (10) | N2—C7—C8 | 112.59 (10) |
N2—C2—H2A | 109.2 | N2—C7—H7A | 109.1 |
C1—C2—H2A | 109.2 | C8—C7—H7A | 109.1 |
N2—C2—H2B | 109.2 | N2—C7—H7B | 109.1 |
C1—C2—H2B | 109.2 | C8—C7—H7B | 109.1 |
H2A—C2—H2B | 107.9 | H7A—C7—H7B | 107.8 |
N2—C3—C4i | 111.30 (9) | O4—C8—O3 | 120.49 (12) |
N2—C3—H3A | 109.4 | O4—C8—C7 | 124.21 (12) |
C4i—C3—H3A | 109.4 | O3—C8—C7 | 115.30 (11) |
N2—C3—H3B | 109.4 | C5—N1—C1 | 110.39 (9) |
C4i—C3—H3B | 109.4 | C5—N1—C4 | 111.18 (9) |
H3A—C3—H3B | 108.0 | C1—N1—C4 | 110.39 (9) |
N1—C4—C3i | 112.09 (9) | C5—N1—H1 | 108.3 |
N1—C4—H4A | 109.2 | C1—N1—H1 | 108.3 |
C3i—C4—H4A | 109.2 | C4—N1—H1 | 108.3 |
N1—C4—H4B | 109.2 | C7—N2—C2 | 110.13 (9) |
C3i—C4—H4B | 109.2 | C7—N2—C3 | 110.75 (9) |
H4A—C4—H4B | 107.9 | C2—N2—C3 | 110.02 (9) |
N1—C5—C6 | 113.73 (10) | C8—O3—H3 | 109.5 |
N1—C5—H5A | 108.8 | H5C—O5—H5D | 105.1 (18) |
C6—C5—H5A | 108.8 | ||
N1—C1—C2—N2 | 51.11 (13) | C3i—C4—N1—C5 | 74.84 (12) |
N1—C5—C6—O2 | 2.30 (17) | C3i—C4—N1—C1 | −162.30 (9) |
N1—C5—C6—O1 | −177.48 (11) | C8—C7—N2—C2 | −170.60 (9) |
N2—C7—C8—O4 | 8.99 (17) | C8—C7—N2—C3 | 67.48 (12) |
N2—C7—C8—O3 | −170.88 (10) | C1—C2—N2—C7 | 73.24 (12) |
C6—C5—N1—C1 | 73.84 (12) | C1—C2—N2—C3 | −164.40 (10) |
C6—C5—N1—C4 | −163.30 (10) | C4i—C3—N2—C7 | −150.74 (10) |
C2—C1—N1—C5 | −162.75 (9) | C4i—C3—N2—C2 | 87.27 (11) |
C2—C1—N1—C4 | 73.93 (12) |
Symmetry codes: (i) −x+1, y, −z+3/2.
Hydrogen-bond geometry (Å, °)
D—H···A | D—H | H···A | D···A | D—H···A |
O3—H3···O5 | 0.84 | 1.71 | 2.5295 (14) | 166 |
N1—H1···N2 | 0.93 | 2.44 | 2.8940 (14) | 110 |
O5—H5D···O1ii | 0.86 (1) | 1.78 (2) | 2.6380 (14) | 173.(2) |
O5—H5C···O1iii | 0.84 (1) | 1.85 (2) | 2.6776 (14) | 170.(2) |
Symmetry codes: (ii) −x+1, −y+2, −z+1; (iii) x−1/2, −y+3/2, −z+1.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: KP2290).
References
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Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536811004843/kp2290sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811004843/kp2290Isup2.hkl