Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S160053680504064X/xu6059sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S160053680504064X/xu6059Isup2.hkl |
CCDC reference: 296730
To a solution of [H2pyda][pydc] (0.5 g, 1.8 mmol) in water (100 ml) was added a solution of DyCl3·6H2O (0.226 g, 0.6 mmol) in water (20 ml) and the resulting pale-yellow solution was stirred for 30 min. This solution was left to evaporate slowly at room temperature, affording single crystals of (I) after one week; yield 73.4%, m.p. 536–539 K.
H atoms bonded to O and N atoms were located in a difference Fourier map and refined as riding in their as-found relative positions, with Uiso(H) = 1.2Ueq(carrier). Other H atoms were positioned geometrically with C—H = 0.95 Å and refined in a riding-model approximation, with Uiso(H) = 1.2Ueq(C). There is a high positive residual density of 2.75 e Å−3 nearing the Dy1 center (distance 1.12 Å) due to considerable absorption effects which could not be completely corrected.
Data collection: SMART (Bruker, 1998); cell refinement: SAINT-Plus (Bruker, 1998); data reduction: SAINT-Plus; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Sheldrick, 1998); software used to prepare material for publication: SHELXTL.
Fig. 1. The molecular structure of (I),with 30% probability displacement ellipsoids [symmetry codes: (i) −x + 1/2, y, −z + 1/2; (ii) −x − 1/2,+y,-z + 1/2]. |
(H5O2)(C5H8N3)2[Dy(C7H3NO4)3]·2H2O | F(000) = 954 |
Mr = 951.17 | Dx = 1.726 Mg m−3 |
Monoclinic, P2/n | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2yac | Cell parameters from 1024 reflections |
a = 9.654 (2) Å | θ = 3–30° |
b = 10.579 (2) Å | µ = 2.13 mm−1 |
c = 17.972 (4) Å | T = 145 K |
β = 94.483 (4)° | Prism, yellow |
V = 1830.0 (7) Å3 | 0.30 × 0.25 × 0.20 mm |
Z = 2 |
Bruker SMART 1000 CCD area-detector diffractometer | 4508 independent reflections |
Radiation source: fine-focus sealed tube | 3876 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.095 |
ϕ and ω scans | θmax = 28.5°, θmin = 2.2° |
Absorption correction: multi-scan (SADABS; Sheldrick, 1998) | h = −12→12 |
Tmin = 0.406, Tmax = 0.653 | k = −13→13 |
18268 measured reflections | l = −23→23 |
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)] = 0.041 | Hydrogen site location: difference Fourier map |
wR(F2) = 0.101 | H-atom parameters constrained |
S = 1.03 | w = 1/[σ2(Fo2) + (0.053P)2 + 1.585P] where P = (Fo2 + 2Fc2)/3 |
4508 reflections | (Δ/σ)max < 0.001 |
259 parameters | Δρmax = 2.75 e Å−3 |
0 restraints | Δρmin = −1.14 e Å−3 |
(H5O2)(C5H8N3)2[Dy(C7H3NO4)3]·2H2O | V = 1830.0 (7) Å3 |
Mr = 951.17 | Z = 2 |
Monoclinic, P2/n | Mo Kα radiation |
a = 9.654 (2) Å | µ = 2.13 mm−1 |
b = 10.579 (2) Å | T = 145 K |
c = 17.972 (4) Å | 0.30 × 0.25 × 0.20 mm |
β = 94.483 (4)° |
Bruker SMART 1000 CCD area-detector diffractometer | 4508 independent reflections |
Absorption correction: multi-scan (SADABS; Sheldrick, 1998) | 3876 reflections with I > 2σ(I) |
Tmin = 0.406, Tmax = 0.653 | Rint = 0.095 |
18268 measured reflections |
R[F2 > 2σ(F2)] = 0.041 | 0 restraints |
wR(F2) = 0.101 | H-atom parameters constrained |
S = 1.03 | Δρmax = 2.75 e Å−3 |
4508 reflections | Δρmin = −1.14 e Å−3 |
259 parameters |
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. |
x | y | z | Uiso*/Ueq | ||
Dy1 | 0.2500 | 0.47398 (2) | 0.2500 | 0.01906 (9) | |
O1 | 0.3291 (3) | 0.5386 (2) | 0.13321 (14) | 0.0226 (5) | |
O2 | 0.3345 (3) | 0.5190 (3) | 0.00958 (16) | 0.0294 (6) | |
O3 | 0.0843 (3) | 0.3105 (2) | 0.27554 (14) | 0.0251 (5) | |
O4 | −0.0561 (3) | 0.1502 (3) | 0.23905 (15) | 0.0280 (6) | |
O5 | 0.0330 (3) | 0.5742 (3) | 0.20749 (15) | 0.0248 (5) | |
O6 | −0.0928 (3) | 0.7441 (3) | 0.17113 (19) | 0.0382 (7) | |
N1 | 0.1429 (3) | 0.3589 (3) | 0.13878 (16) | 0.0195 (6) | |
N2 | 0.2500 | 0.7096 (4) | 0.2500 | 0.0194 (8) | |
C1 | 0.1723 (4) | 0.3954 (3) | 0.07076 (19) | 0.0202 (7) | |
C2 | 0.1034 (4) | 0.3445 (4) | 0.0067 (2) | 0.0292 (8) | |
H2 | 0.1249 | 0.3715 | −0.0415 | 0.035* | |
C3 | 0.0030 (4) | 0.2539 (4) | 0.0149 (2) | 0.0354 (10) | |
H3 | −0.0468 | 0.2189 | −0.0279 | 0.042* | |
C4 | −0.0253 (4) | 0.2137 (4) | 0.0859 (2) | 0.0296 (8) | |
H4 | −0.0917 | 0.1492 | 0.0925 | 0.036* | |
C5 | 0.0464 (4) | 0.2707 (3) | 0.1464 (2) | 0.0206 (7) | |
C6 | 0.2876 (4) | 0.4916 (3) | 0.0699 (2) | 0.0221 (7) | |
C7 | 0.0209 (4) | 0.2406 (3) | 0.2266 (2) | 0.0214 (7) | |
C8 | 0.1375 (4) | 0.7737 (4) | 0.2232 (2) | 0.0236 (7) | |
C9 | 0.1345 (5) | 0.9060 (4) | 0.2206 (3) | 0.0353 (10) | |
H9 | 0.0551 | 0.9496 | 0.1992 | 0.042* | |
C10 | 0.2500 | 0.9712 (5) | 0.2500 | 0.0391 (15) | |
H10 | 0.2500 | 1.0610 | 0.2500 | 0.047* | |
C11 | 0.0139 (4) | 0.6938 (4) | 0.1978 (2) | 0.0249 (7) | |
N3 | −0.1050 (3) | 0.0922 (3) | 0.38151 (18) | 0.0259 (7) | |
H3N | −0.0765 | 0.1150 | 0.3381 | 0.031* | |
N4 | −0.0386 (4) | 0.2897 (3) | 0.4235 (2) | 0.0339 (8) | |
H4NA | −0.0061 | 0.3054 | 0.3809 | 0.041* | |
H4NB | −0.0542 | 0.3477 | 0.4497 | 0.041* | |
N5 | −0.1513 (5) | −0.1036 (4) | 0.3290 (2) | 0.0430 (10) | |
H5NA | −0.1245 | −0.0767 | 0.2863 | 0.052* | |
H5NB | −0.1999 | −0.1766 | 0.3348 | 0.052* | |
C12 | −0.0969 (4) | 0.1783 (4) | 0.4377 (2) | 0.0272 (8) | |
C13 | −0.1442 (4) | 0.1444 (5) | 0.5065 (2) | 0.0351 (9) | |
H13 | −0.1404 | 0.2025 | 0.5469 | 0.042* | |
C14 | −0.1965 (5) | 0.0243 (4) | 0.5140 (2) | 0.0347 (9) | |
H14 | −0.2291 | 0.0002 | 0.5605 | 0.042* | |
C15 | −0.2032 (5) | −0.0627 (5) | 0.4563 (3) | 0.0367 (10) | |
H15 | −0.2402 | −0.1448 | 0.4629 | 0.044* | |
C16 | −0.1546 (4) | −0.0275 (4) | 0.3885 (2) | 0.0298 (8) | |
O1W | −0.2087 (3) | 0.4599 (3) | 0.18753 (19) | 0.0356 (7) | |
H1WC | −0.2500 | 0.4502 | 0.2500 | 0.043* | |
H1WA | −0.2568 | 0.5022 | 0.1547 | 0.043* | |
H1WB | −0.1315 | 0.5024 | 0.1890 | 0.043* | |
O2W | −0.3942 (3) | −0.3875 (3) | 0.11700 (16) | 0.0352 (7) | |
H2WB | −0.4675 | −0.3997 | 0.1254 | 0.042* | |
H2WA | −0.3771 | −0.4118 | 0.0747 | 0.042* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Dy1 | 0.01921 (13) | 0.01890 (13) | 0.01929 (13) | 0.000 | 0.00300 (8) | 0.000 |
O1 | 0.0227 (13) | 0.0263 (14) | 0.0192 (12) | −0.0043 (10) | 0.0041 (10) | −0.0005 (10) |
O2 | 0.0356 (16) | 0.0329 (15) | 0.0206 (13) | −0.0082 (12) | 0.0083 (11) | 0.0037 (11) |
O3 | 0.0299 (14) | 0.0233 (13) | 0.0224 (12) | −0.0070 (11) | 0.0039 (10) | 0.0017 (10) |
O4 | 0.0317 (15) | 0.0233 (13) | 0.0298 (14) | −0.0066 (11) | 0.0077 (11) | 0.0024 (11) |
O5 | 0.0207 (13) | 0.0216 (12) | 0.0318 (14) | 0.0008 (11) | −0.0005 (10) | −0.0013 (11) |
O6 | 0.0265 (15) | 0.0315 (16) | 0.055 (2) | 0.0065 (12) | −0.0091 (14) | 0.0032 (14) |
N1 | 0.0201 (14) | 0.0187 (14) | 0.0203 (14) | 0.0017 (11) | 0.0044 (11) | 0.0016 (11) |
N2 | 0.018 (2) | 0.022 (2) | 0.0184 (19) | 0.000 | 0.0029 (15) | 0.000 |
C1 | 0.0204 (16) | 0.0192 (16) | 0.0215 (16) | −0.0003 (13) | 0.0036 (13) | −0.0003 (13) |
C2 | 0.030 (2) | 0.036 (2) | 0.0212 (17) | −0.0026 (17) | 0.0023 (15) | −0.0015 (16) |
C3 | 0.037 (2) | 0.048 (3) | 0.0215 (19) | −0.0096 (19) | −0.0005 (17) | −0.0078 (18) |
C4 | 0.029 (2) | 0.031 (2) | 0.029 (2) | −0.0073 (16) | 0.0025 (16) | −0.0039 (16) |
C5 | 0.0197 (17) | 0.0189 (16) | 0.0235 (17) | 0.0001 (13) | 0.0035 (13) | 0.0011 (13) |
C6 | 0.0211 (18) | 0.0239 (17) | 0.0220 (17) | 0.0035 (13) | 0.0070 (14) | 0.0011 (13) |
C7 | 0.0162 (16) | 0.0206 (17) | 0.0277 (18) | 0.0015 (13) | 0.0035 (13) | 0.0014 (14) |
C8 | 0.0241 (19) | 0.0216 (18) | 0.0254 (18) | 0.0009 (14) | 0.0043 (14) | 0.0033 (13) |
C9 | 0.033 (2) | 0.021 (2) | 0.051 (3) | 0.0070 (16) | −0.0002 (19) | 0.0025 (17) |
C10 | 0.038 (3) | 0.014 (2) | 0.065 (4) | 0.000 | 0.004 (3) | 0.000 |
C11 | 0.0246 (18) | 0.0250 (18) | 0.0250 (18) | 0.0038 (15) | 0.0019 (14) | 0.0003 (14) |
N3 | 0.0252 (16) | 0.0242 (16) | 0.0289 (16) | −0.0029 (13) | 0.0062 (13) | 0.0039 (13) |
N4 | 0.039 (2) | 0.0279 (17) | 0.0366 (19) | −0.0045 (15) | 0.0144 (16) | −0.0066 (15) |
N5 | 0.058 (3) | 0.031 (2) | 0.042 (2) | −0.0177 (18) | 0.0138 (18) | −0.0061 (16) |
C12 | 0.0226 (18) | 0.031 (2) | 0.0288 (19) | 0.0012 (15) | 0.0053 (15) | 0.0034 (16) |
C13 | 0.034 (2) | 0.045 (3) | 0.026 (2) | 0.0009 (19) | 0.0044 (17) | −0.0028 (18) |
C14 | 0.030 (2) | 0.046 (3) | 0.029 (2) | 0.0053 (19) | 0.0106 (17) | 0.0115 (18) |
C15 | 0.035 (2) | 0.035 (2) | 0.040 (2) | −0.0055 (19) | 0.0062 (19) | 0.0131 (19) |
C16 | 0.028 (2) | 0.026 (2) | 0.035 (2) | −0.0051 (16) | 0.0047 (16) | 0.0033 (16) |
O1W | 0.0254 (15) | 0.0357 (17) | 0.0453 (18) | −0.0020 (12) | 0.0010 (13) | 0.0005 (13) |
O2W | 0.0303 (15) | 0.0443 (18) | 0.0311 (15) | −0.0090 (13) | 0.0034 (12) | −0.0048 (13) |
Dy1—O1 | 2.389 (3) | C8—C9 | 1.400 (5) |
Dy1—O1i | 2.389 (3) | C8—C11 | 1.505 (5) |
Dy1—O3 | 2.424 (3) | C9—C10 | 1.381 (5) |
Dy1—O3i | 2.424 (3) | C9—H9 | 0.9500 |
Dy1—O5 | 2.418 (3) | C10—C9i | 1.381 (5) |
Dy1—O5i | 2.418 (3) | C10—H10 | 0.9500 |
Dy1—N1 | 2.495 (3) | N3—C12 | 1.358 (5) |
Dy1—N1i | 2.495 (3) | N3—C16 | 1.364 (5) |
Dy1—N2 | 2.492 (4) | N3—H3N | 0.8800 |
O1—C6 | 1.277 (5) | N4—C12 | 1.339 (5) |
O2—C6 | 1.241 (5) | N4—H4NA | 0.8652 |
O3—C7 | 1.269 (4) | N4—H4NB | 0.7955 |
O4—C7 | 1.242 (4) | N5—C16 | 1.342 (6) |
O5—C11 | 1.289 (5) | N5—H5NA | 0.8758 |
O6—C11 | 1.223 (5) | N5—H5NB | 0.9134 |
N1—C5 | 1.333 (4) | C12—C13 | 1.398 (6) |
N1—C1 | 1.333 (4) | C13—C14 | 1.378 (7) |
N2—C8i | 1.338 (4) | C13—H13 | 0.9500 |
N2—C8 | 1.338 (4) | C14—C15 | 1.384 (7) |
C1—C2 | 1.393 (5) | C14—H14 | 0.9500 |
C1—C6 | 1.510 (5) | C15—C16 | 1.390 (6) |
C2—C3 | 1.379 (6) | C15—H15 | 0.9500 |
C2—H2 | 0.9500 | O1W—H1WC | 1.2246 |
C3—C4 | 1.392 (6) | O1W—H1WA | 0.8487 |
C3—H3 | 0.9500 | O1W—H1WB | 0.8689 |
C4—C5 | 1.382 (5) | O2W—H2WB | 0.7462 |
C4—H4 | 0.9500 | O2W—H2WA | 0.8307 |
C5—C7 | 1.516 (5) | ||
O1i—Dy1—O1 | 146.77 (12) | C4—C3—H3 | 120.0 |
O1i—Dy1—O5i | 85.73 (9) | C5—C4—C3 | 117.7 (4) |
O1—Dy1—O5i | 79.85 (9) | C5—C4—H4 | 121.1 |
O1i—Dy1—O5 | 79.85 (9) | C3—C4—H4 | 121.1 |
O1—Dy1—O5 | 85.73 (9) | N1—C5—C4 | 122.4 (3) |
O5i—Dy1—O5 | 128.00 (13) | N1—C5—C7 | 114.3 (3) |
O1i—Dy1—O3 | 77.10 (9) | C4—C5—C7 | 123.3 (3) |
O1—Dy1—O3 | 129.16 (9) | O2—C6—O1 | 125.2 (4) |
O5i—Dy1—O3 | 145.21 (9) | O2—C6—C1 | 119.1 (3) |
O5—Dy1—O3 | 78.72 (9) | O1—C6—C1 | 115.7 (3) |
O1i—Dy1—O3i | 129.16 (9) | O4—C7—O3 | 125.9 (3) |
O1—Dy1—O3i | 77.10 (9) | O4—C7—C5 | 118.5 (3) |
O5i—Dy1—O3i | 78.72 (9) | O3—C7—C5 | 115.6 (3) |
O5—Dy1—O3i | 145.21 (9) | N2—C8—C9 | 122.2 (4) |
O3—Dy1—O3i | 88.95 (13) | N2—C8—C11 | 115.2 (3) |
O1i—Dy1—N2 | 73.38 (6) | C9—C8—C11 | 122.5 (3) |
O1—Dy1—N2 | 73.38 (6) | C10—C9—C8 | 118.2 (4) |
O5i—Dy1—N2 | 64.00 (7) | C10—C9—H9 | 120.9 |
O5—Dy1—N2 | 64.00 (7) | C8—C9—H9 | 120.9 |
O3—Dy1—N2 | 135.53 (7) | C9—C10—C9i | 120.0 (5) |
O3i—Dy1—N2 | 135.53 (7) | C9—C10—H10 | 120.0 |
O1i—Dy1—N1 | 134.65 (9) | C9i—C10—H10 | 120.0 |
O1—Dy1—N1 | 64.94 (9) | O6—C11—O5 | 126.0 (4) |
O5i—Dy1—N1 | 139.62 (9) | O6—C11—C8 | 119.9 (3) |
O5—Dy1—N1 | 70.50 (9) | O5—C11—C8 | 114.1 (3) |
O3—Dy1—N1 | 64.23 (9) | C12—N3—C16 | 123.6 (3) |
O3i—Dy1—N1 | 74.83 (9) | C12—N3—H3N | 118.2 |
N2—Dy1—N1 | 119.21 (7) | C16—N3—H3N | 118.2 |
O1i—Dy1—N1i | 64.94 (9) | C12—N4—H4NA | 121.6 |
O1—Dy1—N1i | 134.65 (9) | C12—N4—H4NB | 117.6 |
O5i—Dy1—N1i | 70.50 (9) | H4NA—N4—H4NB | 118.4 |
O5—Dy1—N1i | 139.62 (9) | C16—N5—H5NA | 122.0 |
O3—Dy1—N1i | 74.83 (9) | C16—N5—H5NB | 111.8 |
O3i—Dy1—N1i | 64.23 (9) | H5NA—N5—H5NB | 124.4 |
N2—Dy1—N1i | 119.21 (7) | N4—C12—N3 | 116.6 (3) |
N1—Dy1—N1i | 121.57 (13) | N4—C12—C13 | 124.5 (4) |
C6—O1—Dy1 | 124.9 (2) | N3—C12—C13 | 118.8 (4) |
C7—O3—Dy1 | 125.0 (2) | C14—C13—C12 | 118.1 (4) |
C11—O5—Dy1 | 125.8 (2) | C14—C13—H13 | 120.9 |
C5—N1—C1 | 119.8 (3) | C12—C13—H13 | 120.9 |
C5—N1—Dy1 | 120.6 (2) | C13—C14—C15 | 122.4 (4) |
C1—N1—Dy1 | 119.3 (2) | C13—C14—H14 | 118.8 |
C8i—N2—C8 | 119.0 (4) | C15—C14—H14 | 118.8 |
C8i—N2—Dy1 | 120.5 (2) | C14—C15—C16 | 118.7 (4) |
C8—N2—Dy1 | 120.5 (2) | C14—C15—H15 | 120.7 |
N1—C1—C2 | 121.6 (3) | C16—C15—H15 | 120.7 |
N1—C1—C6 | 114.5 (3) | N5—C16—N3 | 117.0 (4) |
C2—C1—C6 | 123.9 (3) | N5—C16—C15 | 124.7 (4) |
C3—C2—C1 | 118.3 (4) | N3—C16—C15 | 118.4 (4) |
C3—C2—H2 | 120.8 | H1WC—O1W—H1WA | 118.8 |
C1—C2—H2 | 120.9 | H1WC—O1W—H1WB | 110.8 |
C2—C3—C4 | 120.1 (4) | H1WA—O1W—H1WB | 99.8 |
C2—C3—H3 | 120.0 | H2WB—O2W—H2WA | 113.0 |
O1i—Dy1—O1—C6 | −134.7 (3) | O3i—Dy1—N2—C8 | 139.8 (2) |
O5i—Dy1—O1—C6 | 159.6 (3) | N1—Dy1—N2—C8 | 41.6 (2) |
O5—Dy1—O1—C6 | −70.5 (3) | N1i—Dy1—N2—C8 | −138.4 (2) |
O3—Dy1—O1—C6 | 1.2 (3) | C5—N1—C1—C2 | 0.7 (5) |
O3i—Dy1—O1—C6 | 79.0 (3) | Dy1—N1—C1—C2 | −172.4 (3) |
N2—Dy1—O1—C6 | −134.7 (3) | C5—N1—C1—C6 | −177.5 (3) |
N1—Dy1—O1—C6 | −0.1 (3) | Dy1—N1—C1—C6 | 9.4 (4) |
N1i—Dy1—O1—C6 | 110.4 (3) | N1—C1—C2—C3 | −0.3 (6) |
O1i—Dy1—O3—C7 | 156.8 (3) | C6—C1—C2—C3 | 177.8 (4) |
O1—Dy1—O3—C7 | −0.1 (3) | C1—C2—C3—C4 | −1.2 (6) |
O5i—Dy1—O3—C7 | −140.8 (3) | C2—C3—C4—C5 | 2.3 (6) |
O5—Dy1—O3—C7 | 74.8 (3) | C1—N1—C5—C4 | 0.4 (5) |
O3i—Dy1—O3—C7 | −72.5 (3) | Dy1—N1—C5—C4 | 173.4 (3) |
N2—Dy1—O3—C7 | 107.5 (3) | C1—N1—C5—C7 | −178.5 (3) |
N1—Dy1—O3—C7 | 1.1 (3) | Dy1—N1—C5—C7 | −5.5 (4) |
N1i—Dy1—O3—C7 | −136.0 (3) | C3—C4—C5—N1 | −1.9 (6) |
O1i—Dy1—O5—C11 | 82.0 (3) | C3—C4—C5—C7 | 176.9 (4) |
O1—Dy1—O5—C11 | −67.9 (3) | Dy1—O1—C6—O2 | −175.1 (3) |
O5i—Dy1—O5—C11 | 5.7 (3) | Dy1—O1—C6—C1 | 4.7 (4) |
O3—Dy1—O5—C11 | 160.7 (3) | N1—C1—C6—O2 | 170.7 (3) |
O3i—Dy1—O5—C11 | −127.9 (3) | C2—C1—C6—O2 | −7.5 (6) |
N2—Dy1—O5—C11 | 5.7 (3) | N1—C1—C6—O1 | −9.1 (5) |
N1—Dy1—O5—C11 | −132.8 (3) | C2—C1—C6—O1 | 172.6 (4) |
N1i—Dy1—O5—C11 | 111.0 (3) | Dy1—O3—C7—O4 | 174.1 (3) |
O1i—Dy1—N1—C5 | −31.7 (3) | Dy1—O3—C7—C5 | −4.2 (4) |
O1—Dy1—N1—C5 | −178.4 (3) | N1—C5—C7—O4 | −172.3 (3) |
O5i—Dy1—N1—C5 | 149.8 (2) | C4—C5—C7—O4 | 8.8 (5) |
O5—Dy1—N1—C5 | −83.9 (3) | N1—C5—C7—O3 | 6.2 (5) |
O3—Dy1—N1—C5 | 2.7 (2) | C4—C5—C7—O3 | −172.7 (4) |
O3i—Dy1—N1—C5 | 99.0 (3) | C8i—N2—C8—C9 | 1.5 (3) |
N2—Dy1—N1—C5 | −126.9 (2) | Dy1—N2—C8—C9 | −178.5 (3) |
N1i—Dy1—N1—C5 | 53.1 (2) | C8i—N2—C8—C11 | −177.1 (4) |
O1i—Dy1—N1—C1 | 141.4 (2) | Dy1—N2—C8—C11 | 2.9 (4) |
O1—Dy1—N1—C1 | −5.3 (2) | N2—C8—C9—C10 | −3.0 (6) |
O5i—Dy1—N1—C1 | −37.1 (3) | C11—C8—C9—C10 | 175.6 (3) |
O5—Dy1—N1—C1 | 89.2 (3) | C8—C9—C10—C9i | 1.4 (3) |
O3—Dy1—N1—C1 | 175.7 (3) | Dy1—O5—C11—O6 | 174.3 (3) |
O3i—Dy1—N1—C1 | −88.0 (3) | Dy1—O5—C11—C8 | −6.2 (4) |
N2—Dy1—N1—C1 | 46.1 (3) | N2—C8—C11—O6 | −178.6 (3) |
N1i—Dy1—N1—C1 | −133.9 (3) | C9—C8—C11—O6 | 2.7 (6) |
O1i—Dy1—N2—C8i | 89.30 (19) | N2—C8—C11—O5 | 1.9 (5) |
O1—Dy1—N2—C8i | −90.70 (19) | C9—C8—C11—O5 | −176.8 (4) |
O5i—Dy1—N2—C8i | −4.09 (19) | C16—N3—C12—N4 | 176.4 (4) |
O5—Dy1—N2—C8i | 175.91 (19) | C16—N3—C12—C13 | −1.2 (6) |
O3—Dy1—N2—C8i | 139.8 (2) | N4—C12—C13—C14 | −177.2 (4) |
O3i—Dy1—N2—C8i | −40.2 (2) | N3—C12—C13—C14 | 0.3 (6) |
N1—Dy1—N2—C8i | −138.4 (2) | C12—C13—C14—C15 | 0.1 (7) |
N1i—Dy1—N2—C8i | 41.6 (2) | C13—C14—C15—C16 | 0.4 (7) |
O1i—Dy1—N2—C8 | −90.70 (19) | C12—N3—C16—N5 | −177.5 (4) |
O1—Dy1—N2—C8 | 89.30 (19) | C12—N3—C16—C15 | 1.7 (6) |
O5i—Dy1—N2—C8 | 175.91 (19) | C14—C15—C16—N5 | 177.9 (4) |
O5—Dy1—N2—C8 | −4.09 (19) | C14—C15—C16—N3 | −1.2 (7) |
O3—Dy1—N2—C8 | −40.2 (2) |
Symmetry code: (i) −x+1/2, y, −z+1/2. |
Experimental details
Crystal data | |
Chemical formula | (H5O2)(C5H8N3)2[Dy(C7H3NO4)3]·2H2O |
Mr | 951.17 |
Crystal system, space group | Monoclinic, P2/n |
Temperature (K) | 145 |
a, b, c (Å) | 9.654 (2), 10.579 (2), 17.972 (4) |
β (°) | 94.483 (4) |
V (Å3) | 1830.0 (7) |
Z | 2 |
Radiation type | Mo Kα |
µ (mm−1) | 2.13 |
Crystal size (mm) | 0.30 × 0.25 × 0.20 |
Data collection | |
Diffractometer | Bruker SMART 1000 CCD area-detector diffractometer |
Absorption correction | Multi-scan (SADABS; Sheldrick, 1998) |
Tmin, Tmax | 0.406, 0.653 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 18268, 4508, 3876 |
Rint | 0.095 |
(sin θ/λ)max (Å−1) | 0.671 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.041, 0.101, 1.03 |
No. of reflections | 4508 |
No. of parameters | 259 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 2.75, −1.14 |
Computer programs: SMART (Bruker, 1998), SAINT-Plus (Bruker, 1998), SAINT-Plus, SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), SHELXTL (Sheldrick, 1998), SHELXTL.
Dy1—O1 | 2.389 (3) | Dy1—N1 | 2.495 (3) |
Dy1—O3 | 2.424 (3) | Dy1—N2 | 2.492 (4) |
Dy1—O5 | 2.418 (3) |
We have recently become interested in metal complexes with a pyridine-containing ligand system (Rafizadeh et al., 2004). We present here the structure of the title compound, (I), which includes a pyridinedicaboxylate (pydc) anion and a diaminopyridinium (pyda) cation.
The structure of (I) comprises DyIII complex anions, free pyda cations, dihydronium cations (H5O2)+ and uncoordinted water molecules (Fig. 1). The Dy ion lies on a twofold rotation axis and the nine coordinated-DyIII complex assumes a distorted tricapped trigonal-prismatic geometry, formed by three pydc dianions. This is comparable to the situation found in the Yb analogue (Rafizadeh et al., 2004). The Dy—O and Dy—N bond distances (Table 1) agree with those found in previously reported structures (Fernandes et al., 2001).
Atom H1WC atom of the dihydronium cation lies on a twofold axis. The O1W—H1WC bond distance of 1.225 Å and O1W—H1WC—O1Wii bond angle of 170° [symmetry code: (ii) −x − 1/2,y,-z + 1/2] are comparable to the values found in the Yb analogue (1.218 and 1.221 Å and 170°; Rafizadeh et al., 2004) and in the GdIII analogue [1.216 Å and 164°; Rafizadeh et al., 2005). These also agree with the values deduced from ab initio computations (1.2 Å and 173.5°; Ojamae et al., 1995).