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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 May 28;67(Pt 6):m818. doi: 10.1107/S1600536811019520

Poly[(μ2-nitrato-κ2 O:O′)(μ2-pyrimidin­ium-2-carboxyl­ato-κ2 O:O′)lithium(I)]

Wojciech Starosta a, Janusz Leciejewicz a,*
PMCID: PMC3120533  PMID: 21754689

Abstract

In the structure of the title compound, [Li(C5H4N2O2)(NO3)]n, the LiI ion is coordinated by two carboxyl­ate O atoms donated by two ligands and two nitrate O atoms in a distorted tetrahedral geometry. LiI ions, bridged by carboxyl­ate O atoms, form mol­ecular ribbons composed of dimeric units. Two nitrate O atoms link the ribbons into mol­ecular layers parallel to (001). Hydrogen bonds are active between protonated heterocyclic N atoms as donors and carboxyl­ate O atoms as acceptors. The layers are held together by van der Waals inter­actions.

Related literature

For the polymeric structures of some metal complexes with a pyrimidine-2-carboxyl­ate ligand, see: Rodríguez-Diéguez et al. (2007 ▶, 2008 ▶); Zhao & Liu (2010 ▶); Zhang et al. (2008a ▶). For structures built of monomeric mol­ecules, see: Kokunov & Gorbunova (2007 ▶); Antolić et al. (2000 ▶); Zhang et al. (2008b ▶); Suares-Varela et al. (2008 ▶). graphic file with name e-67-0m818-scheme1.jpg

Experimental

Crystal data

  • [Li(C5H4N2O2)(NO3)]

  • M r = 193.05

  • Orthorhombic, Inline graphic

  • a = 12.403 (3) Å

  • b = 9.3290 (19) Å

  • c = 12.810 (3) Å

  • V = 1482.2 (5) Å3

  • Z = 8

  • Mo Kα radiation

  • μ = 0.15 mm−1

  • T = 293 K

  • 0.49 × 0.48 × 0.14 mm

Data collection

  • Kuma KM-4 four-circle diffractometer

  • Absorption correction: analytical (CrysAlis RED; Oxford Diffraction,2008 ▶) T min = 0.782, T max = 0.939

  • 4248 measured reflections

  • 2179 independent reflections

  • 1504 reflections with I > 2σ(I)

  • R int = 0.158

  • 3 standard reflections every 200 reflections intensity decay: 3.8%

Refinement

  • R[F 2 > 2σ(F 2)] = 0.050

  • wR(F 2) = 0.153

  • S = 0.97

  • 2179 reflections

  • 131 parameters

  • H atoms treated by a mixture of independent and constrained refinement

  • Δρmax = 0.43 e Å−3

  • Δρmin = −0.32 e Å−3

Data collection: KM-4 Software (Kuma, 1996 ▶); cell refinement: KM-4 Software; data reduction: DATAPROC (Kuma, 2001 ▶); 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: SHELXTL.

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536811019520/kp2322sup1.cif

e-67-0m818-sup1.cif (13.9KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811019520/kp2322Isup2.hkl

e-67-0m818-Isup2.hkl (107.2KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Selected bond lengths (Å).

O1—Li1 1.978 (3)
O11—Li1 1.967 (3)
Li1—O12i 2.001 (4)
Li1—O2ii 2.019 (3)

Symmetry codes: (i) Inline graphic; (ii) Inline graphic.

Table 2. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A D⋯A D—H⋯A
N2—H2⋯O1iii 0.90 (3) 1.68 (3) 2.5762 (17) 174 (3)

Symmetry code: (iii) Inline graphic.

supplementary crystallographic information

Comment

The structure of the title compound contains LiI ions, each coordinated by two ligand carboxylato and two nitrato O atoms at the apieces of a distorded trigonal pyramid. Its base is composed of coplanar carboxylato O1, nitrato O11 and O12II atoms (Fig. 1). The LiI ion is shifted by 0.0548 (2)Å above this plane. The carboxylato O2III atom is at the apex of the pyramid. The Li—O bond distances fall in the range from 1.967 (3) to 2.019 (3) Å, commonly observed in the structures of Li complexes with carboxylate ligands (Table 1). The Li1—N1 bond distance of 2.467 (3)Å as too long was not allowed for in coordination of the Li ion The pyrimidine ring is planar with r.m.s. of 0.0074 (2) Å]. A hydrogen atom attached to the hetero-ring N2 atom, clearly visible on the Fourier map, maintains the charge balance. It links the N2 atom with the carboxylato OI atom via a hydrogen bond of 2.5762 (17) Å. Bond distances and bond angles within the pyrimidine ring do not differ from those reported earlier in the structures of other metal complexes with the title ligand. The carboxylate group C7/O1/O2 makes with the ring a dihedral angle of 14.81 (2)°. Two LiI ions, one coordinated by the carboxylato O1 atom, the other by the second carboxylato O2 atom of the same ligand form molecular ribbons composed of dimeric units (Fig. 2). The latter bridged by nitrato O11 and O12II atoms give rise to molecular layers. While the nitrato O11 atom coordinates a LiI ion in one ribbon plane, the O12 atom is bonded along the crystal c axis to a LiI ion in an adjacent ribbon; the O11—N11—O12 bond angle is 120.44 (17)°. The third nitrato O13 atomis not involved in the coordination. The NO3 group is planar with r.m.s. of 0.0023 (0) Å. It makes a dihedral angle of 28.8 (2)° with the ribbon plane. Since the bridging nitrate O12 atom is in a terminal position and it is bonded to the LiI ion in the middle of an adjacent ribbon, a layer is formed. A sequence of open channels which propagate along crystal a direction form a layer parallel to the ab plane. The layers stacked along the crystal c direction are held together by van der Waals type interactions. A variety of polymeric molecular patterns have been recently observed in the structures of a number of divalent metal complexes with the title ligand, for example: Mn(II) (Rodríguez-Diéguez et al., 2008; Zhang et al., 2008a); Fe(II) and Co(II) (Rodríguez-Diéguez et al., 2007; Zhao & Liu, 2010); Ca(II) Zhang et al., 2008a), complexes. Structures built of monmeric molecules have been also reported: in a Ag(I) complex by Kokunov & Gorbunova, (2007); in a Cu(II) complex by Suares-Varela et al., (2008) and Zhang et al., (2008a). The structures of two Co(II) complexes have been determined by Antolić et al., (2000) and Zhang et al., (2008b).

Experimental

50 mL of an aqueous solution containing 1 mmol of pyrimidine-2-carbonitrile (Aldrich) and 1 mmol of lithium nitrate hydrate were boiled with constant stirring under reflux for 6 h. After cooling to room temperature 1 N HNO3 was added dropwise until the pH reached 6. Then the solution was stirred for 3 h. After evaporation to dryness the residue was repeatedly dissolved in water and evaporated at room temperature until colourless single crystals of the title compound were deposited. The crystals were washed with cold methanol and dried in the air.

Refinement

H atoms attached to pyridimiine-ring C atoms were placed at calculated positions with C—H=0.93 Å and treated as riding on the parent atoms with Uiso(H)=1.2Ueq(C). The H atom attached to pyrimidine ring N2 atom has been found from the Fourier map and refined isotropically.

Figures

Fig. 1.

Fig. 1.

A fragment of the structure with the atom labeling scheme. Non-hydrogen atoms are shown as 50% elipsoids. Symmetry code: (I) -x + 3/2, y - 1/2, z; (II) -x + 1, -y + 1, -z + 1; (III) -x + 3/2, y + 1/2, z.

Fig. 2.

Fig. 2.

Packing of molecular layers viewed along the a axis.

Crystal data

[Li(C5H4N2O2)(NO3)] F(000) = 784
Mr = 193.05 Dx = 1.730 Mg m−3
Orthorhombic, Pbca Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ac 2ab Cell parameters from 25 reflections
a = 12.403 (3) Å θ = 6–15°
b = 9.3290 (19) Å µ = 0.15 mm−1
c = 12.810 (3) Å T = 293 K
V = 1482.2 (5) Å3 Plates, colorless
Z = 8 0.49 × 0.48 × 0.14 mm

Data collection

Kuma KM-4 four-circle diffractometer 1504 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tube Rint = 0.158
graphite θmax = 30.1°, θmin = 3.2°
profile data from ω/2θ scans h = 0→17
Absorption correction: analytical (CrysAlis RED; Oxford Diffraction,2008) k = 0→13
Tmin = 0.782, Tmax = 0.939 l = −18→18
4248 measured reflections 3 standard reflections every 200 reflections
2179 independent reflections intensity decay: 3.8%

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)] = 0.050 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.153 H atoms treated by a mixture of independent and constrained refinement
S = 0.97 w = 1/[σ2(Fo2) + (0.0702P)2 + 0.2975P] where P = (Fo2 + 2Fc2)/3
2179 reflections (Δ/σ)max < 0.001
131 parameters Δρmax = 0.43 e Å−3
0 restraints Δρmin = −0.32 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
N2 0.61057 (10) 0.04538 (11) 0.35126 (12) 0.0250 (3)
O1 0.71796 (9) 0.39321 (10) 0.32671 (12) 0.0323 (3)
O11 0.47373 (9) 0.63026 (13) 0.36709 (13) 0.0400 (4)
N1 0.52999 (10) 0.27071 (12) 0.37133 (13) 0.0294 (3)
C2 0.61507 (11) 0.18883 (13) 0.35586 (13) 0.0236 (3)
N11 0.38359 (10) 0.62115 (13) 0.40961 (13) 0.0300 (3)
C4 0.51530 (13) −0.02147 (14) 0.35905 (15) 0.0290 (4)
H4 0.5115 −0.1208 0.3538 0.035*
O2 0.80624 (9) 0.18762 (11) 0.35001 (13) 0.0378 (4)
C7 0.72441 (11) 0.26027 (14) 0.34338 (14) 0.0258 (3)
C5 0.42357 (12) 0.05728 (16) 0.37473 (16) 0.0332 (4)
H5 0.3565 0.0135 0.3806 0.040*
C6 0.43471 (12) 0.20546 (16) 0.38159 (17) 0.0350 (4)
H6 0.3737 0.2610 0.3937 0.042*
O12 0.35866 (13) 0.51255 (13) 0.45999 (13) 0.0464 (4)
O13 0.32128 (12) 0.72177 (17) 0.4017 (2) 0.0755 (7)
Li1 0.6045 (2) 0.5149 (3) 0.3893 (3) 0.0362 (7)
H2 0.671 (2) −0.005 (3) 0.339 (2) 0.044 (6)*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
N2 0.0196 (5) 0.0171 (5) 0.0382 (8) −0.0002 (4) −0.0020 (5) −0.0003 (5)
O1 0.0227 (5) 0.0175 (4) 0.0567 (8) −0.0023 (3) 0.0012 (5) 0.0000 (4)
O11 0.0233 (6) 0.0398 (6) 0.0568 (10) 0.0039 (4) 0.0078 (5) 0.0067 (6)
N1 0.0190 (6) 0.0212 (5) 0.0479 (9) 0.0021 (4) −0.0008 (5) −0.0048 (5)
C2 0.0200 (6) 0.0184 (5) 0.0323 (8) −0.0005 (4) −0.0018 (6) −0.0018 (5)
N11 0.0230 (6) 0.0287 (6) 0.0384 (8) −0.0003 (4) −0.0009 (6) 0.0007 (5)
C4 0.0260 (7) 0.0200 (5) 0.0410 (10) −0.0042 (5) −0.0013 (7) 0.0014 (5)
O2 0.0183 (5) 0.0241 (5) 0.0710 (10) 0.0023 (4) 0.0002 (6) 0.0032 (5)
C7 0.0199 (6) 0.0186 (5) 0.0388 (8) −0.0011 (4) −0.0017 (6) −0.0029 (5)
C5 0.0193 (6) 0.0304 (6) 0.0499 (11) −0.0065 (5) −0.0018 (7) 0.0000 (7)
C6 0.0191 (6) 0.0308 (7) 0.0551 (12) 0.0021 (5) 0.0020 (7) −0.0064 (7)
O12 0.0557 (8) 0.0362 (6) 0.0474 (9) −0.0142 (6) 0.0041 (8) 0.0043 (6)
O13 0.0321 (7) 0.0554 (8) 0.139 (2) 0.0210 (6) 0.0136 (10) 0.0267 (11)
Li1 0.0294 (13) 0.0305 (11) 0.0486 (19) 0.0042 (10) 0.0029 (13) 0.0051 (12)

Geometric parameters (Å, °)

N2—C4 1.3399 (19) N11—O12 1.2404 (18)
N2—C2 1.3406 (16) C4—C5 1.369 (2)
N2—H2 0.90 (3) C4—H4 0.9300
O1—C7 1.2610 (16) O2—C7 1.2234 (17)
O1—Li1 1.978 (3) O2—Li1i 2.019 (3)
O11—N11 1.2466 (18) C5—C6 1.392 (2)
O11—Li1 1.967 (3) C5—H5 0.9300
N1—C2 1.3178 (18) C6—H6 0.9300
N1—C6 1.3357 (19) O12—Li1ii 2.001 (4)
N1—Li1 2.469 (3) Li1—O12ii 2.001 (4)
C2—C7 1.5194 (19) Li1—O2iii 2.019 (3)
N11—O13 1.2201 (18)
C4—N2—C2 119.87 (13) O2—C7—C2 119.35 (12)
C4—N2—H2 120.5 (15) O1—C7—C2 113.12 (11)
C2—N2—H2 119.5 (15) C4—C5—C6 117.36 (14)
C7—O1—Li1 122.76 (14) C4—C5—H5 121.3
N11—O11—Li1 129.73 (15) C6—C5—H5 121.3
C2—N1—C6 117.33 (11) N1—C6—C5 122.29 (14)
C2—N1—Li1 104.42 (11) N1—C6—H6 118.9
C6—N1—Li1 137.95 (11) C5—C6—H6 118.9
N1—C2—N2 123.50 (13) N11—O12—Li1ii 123.35 (15)
N1—C2—C7 118.44 (11) O11—Li1—O1 147.4 (2)
N2—C2—C7 118.06 (12) O11—Li1—O12ii 113.43 (18)
O13—N11—O12 120.90 (16) O1—Li1—O12ii 98.94 (15)
O13—N11—O11 118.66 (15) O11—Li1—O2iii 88.82 (12)
O12—N11—O11 120.44 (14) O1—Li1—O2iii 88.11 (14)
N2—C4—C5 119.61 (12) O12ii—Li1—O2iii 102.57 (16)
N2—C4—H4 120.2 O11—Li1—N1 100.51 (13)
C5—C4—H4 120.2 O1—Li1—N1 72.49 (10)
C7—O2—Li1i 156.13 (14) O12ii—Li1—N1 93.28 (13)
O2—C7—O1 127.53 (13) O2iii—Li1—N1 156.71 (19)

Symmetry codes: (i) −x+3/2, y−1/2, z; (ii) −x+1, −y+1, −z+1; (iii) −x+3/2, y+1/2, z.

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N2—H2···O1i 0.90 (3) 1.68 (3) 2.5762 (17) 174 (3)

Symmetry codes: (i) −x+3/2, y−1/2, z.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: KP2322).

References

  1. Antolić, S., Kojić-Prodić, B. & Lovrić, J. (2000). Acta Cryst. C56, e51–e52. [DOI] [PubMed]
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  3. Kuma (1996). KM-4 Software Kuma Diffraction Ltd, Wrocław, Poland.
  4. Kuma (2001). DATAPROC Kuma Diffraction Ltd, Wrocław, Poland.
  5. Oxford Diffraction (2008). CrysAlis RED Oxford Diffraction Ltd, Abingdon, England.
  6. Rodríguez-Diéguez, A., Aouryaghal, H., Mota, A. J. & Colacio, E. (2008). Acta Cryst. E64, m618. [DOI] [PMC free article] [PubMed]
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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 I, global. DOI: 10.1107/S1600536811019520/kp2322sup1.cif

e-67-0m818-sup1.cif (13.9KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811019520/kp2322Isup2.hkl

e-67-0m818-Isup2.hkl (107.2KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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