Literature DB >> 23476164

Bis(2,6-diamino-4-chloro-pyrimidin-1-ium) fumarate.

Kaliyaperumal Thanigaimani1, Nuridayanti Che Khalib, Abbas Farhadikoutenaei, Suhana Arshad, Ibrahim Abdul Razak.   

Abstract

In the title salt, 2C4H6ClN4(+)·C4H2O4(2-), the complete fumarate dianion is generated by crystallographic inversion symmetry. The cation is essentially planar, with a maximum deviation of 0.018 (1) Å. In the anion, the carboxyl-ate group is twisted slightly away from the attached plane, the dihedral angle between the carboxyl-ate and (E)-but-2-ene planes being 12.78 (13)°. In the crystal, the protonated N atom and the 2-amino group of the cation are hydrogen bonded to the carboxyl-ate O atoms of the anion via a pair of N-H⋯O hydrogen bonds, forming an R2(2)(8) ring motif. In addition, another type of R2(2)(8) motif is formed by centrosymmetrically related pyrimidinium cations via N-H⋯N hydrogen bonds. These two combined motifs form a heterotetra-mer. The crystal structure is further stabilized by stong N-H⋯O, N-H⋯Cl and weak C-H⋯O hydrogen bonds, resulting a three-dimensional network.

Entities:  

Year:  2012        PMID: 23476164      PMCID: PMC3588928          DOI: 10.1107/S1600536812045308

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

For applications of pyrimidine derivatives, see: Condon et al. (1993 ▶); Maeno et al. (1990 ▶); Gilchrist (1997 ▶). For details of fumaric acid, see: Batchelor et al. (2000 ▶). For hydrogen-bonded synthons, see: Thakur & Desiraju (2008 ▶). For hydrogen-bond motifs, see: Bernstein et al. (1995 ▶). For bond-length data, see: Allen et al. (1987 ▶). For stability of the temperature controller used for the data collection, see: Cosier & Glazer (1986 ▶).

Experimental

Crystal data

C4H6ClN4 +·0.5C4H2O4 2− M = 202.61 Monoclinic, a = 5.4478 (7) Å b = 10.5187 (14) Å c = 14.8171 (18) Å β = 100.990 (4)° V = 833.50 (18) Å3 Z = 4 Mo Kα radiation μ = 0.43 mm−1 T = 100 K 0.71 × 0.31 × 0.17 mm

Data collection

Bruker SMART APEXII DUO CCD area-detector diffractometer Absorption correction: multi-scan (SADABS; Bruker, 2009 ▶) T min = 0.749, T max = 0.931 9206 measured reflections 2984 independent reflections 2708 reflections with I > 2σ(I) R int = 0.033

Refinement

R[F 2 > 2σ(F 2)] = 0.042 wR(F 2) = 0.127 S = 1.08 2984 reflections 138 parameters 1 restraint H atoms treated by a mixture of independent and constrained refinement Δρmax = 0.78 e Å−3 Δρmin = −0.78 e Å−3 Data collection: APEX2 (Bruker, 2009 ▶); cell refinement: SAINT (Bruker, 2009 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL and PLATON (Spek, 2009 ▶). Click here for additional data file. Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536812045308/rz5019sup1.cif Click here for additional data file. Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812045308/rz5019Isup2.hkl Click here for additional data file. Supplementary material file. DOI: 10.1107/S1600536812045308/rz5019Isup3.cml Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C4H6ClN4+·0.5C4H2O42F(000) = 416
Mr = 202.61Dx = 1.615 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 6512 reflections
a = 5.4478 (7) Åθ = 3.4–32.6°
b = 10.5187 (14) ŵ = 0.43 mm1
c = 14.8171 (18) ÅT = 100 K
β = 100.990 (4)°Block, colourless
V = 833.50 (18) Å30.71 × 0.31 × 0.17 mm
Z = 4
Bruker SMART APEXII DUO CCD area-detector diffractometer2984 independent reflections
Radiation source: fine-focus sealed tube2708 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.033
φ and ω scansθmax = 32.6°, θmin = 2.4°
Absorption correction: multi-scan (SADABS; Bruker, 2009)h = −8→8
Tmin = 0.749, Tmax = 0.931k = −15→11
9206 measured reflectionsl = −22→20
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.042Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.127H atoms treated by a mixture of independent and constrained refinement
S = 1.08w = 1/[σ2(Fo2) + (0.0781P)2 + 0.3432P] where P = (Fo2 + 2Fc2)/3
2984 reflections(Δ/σ)max < 0.001
138 parametersΔρmax = 0.78 e Å3
1 restraintΔρmin = −0.78 e Å3
Experimental. The crystal was placed in the cold stream of an Oxford Cryosystems Cobra open-flow nitrogen cryostat (Cosier & Glazer, 1986) operating at 100.0 (1) K.
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.
xyzUiso*/Ueq
Cl10.40235 (6)0.33920 (3)0.76706 (2)0.01926 (11)
N10.60987 (19)0.49304 (10)0.89510 (7)0.0145 (2)
N20.94266 (19)0.63383 (10)0.88172 (7)0.01248 (19)
N30.7774 (2)0.62835 (11)1.01344 (8)0.0172 (2)
N41.1199 (2)0.64457 (11)0.75251 (8)0.0155 (2)
C10.7751 (2)0.58432 (11)0.92934 (8)0.0128 (2)
C20.9508 (2)0.59135 (11)0.79616 (8)0.0121 (2)
C30.7835 (2)0.49584 (11)0.75646 (8)0.0139 (2)
H3A0.78270.46270.69680.017*
C40.6220 (2)0.45442 (11)0.81056 (8)0.0138 (2)
O10.1038 (2)0.65131 (9)0.56049 (7)0.0197 (2)
O20.2393 (2)0.68272 (9)0.42877 (7)0.0196 (2)
C50.2377 (2)0.62262 (11)0.50395 (8)0.0145 (2)
C60.4095 (2)0.51141 (11)0.52358 (8)0.0148 (2)
H6A0.38940.45470.57150.018*
H11.054 (4)0.688 (2)0.9060 (19)0.054 (8)*
H20.874 (4)0.685 (2)1.0338 (16)0.031 (6)*
H30.662 (4)0.597 (2)1.0383 (16)0.035 (6)*
H41.118 (4)0.629 (2)0.7009 (16)0.024 (5)*
H51.208 (4)0.697 (2)0.7770 (15)0.025 (5)*
U11U22U33U12U13U23
Cl10.01810 (17)0.01552 (16)0.02516 (18)−0.00602 (9)0.00670 (12)−0.00792 (10)
N10.0156 (4)0.0128 (4)0.0160 (5)−0.0033 (3)0.0054 (3)−0.0023 (3)
N20.0156 (4)0.0097 (4)0.0130 (4)−0.0027 (3)0.0050 (3)−0.0008 (3)
N30.0212 (5)0.0169 (5)0.0153 (5)−0.0072 (4)0.0082 (4)−0.0037 (4)
N40.0205 (5)0.0133 (4)0.0138 (4)−0.0028 (4)0.0063 (4)−0.0010 (4)
C10.0144 (5)0.0103 (5)0.0145 (5)−0.0017 (4)0.0047 (4)0.0002 (4)
C20.0139 (5)0.0094 (4)0.0135 (5)0.0008 (3)0.0041 (4)0.0004 (3)
C30.0155 (5)0.0114 (5)0.0154 (5)−0.0015 (4)0.0047 (4)−0.0020 (4)
C40.0141 (5)0.0101 (4)0.0178 (5)−0.0014 (4)0.0040 (4)−0.0022 (4)
O10.0235 (5)0.0206 (5)0.0174 (4)0.0087 (3)0.0096 (4)0.0032 (3)
O20.0270 (5)0.0178 (4)0.0159 (4)0.0112 (4)0.0089 (4)0.0055 (3)
C50.0167 (5)0.0132 (5)0.0138 (5)0.0039 (4)0.0039 (4)0.0004 (4)
C60.0179 (5)0.0126 (5)0.0143 (5)0.0049 (4)0.0039 (4)0.0023 (4)
Cl1—C41.7385 (12)N4—H40.78 (2)
N1—C41.3305 (15)N4—H50.77 (2)
N1—C11.3474 (15)C2—C31.4076 (16)
N2—C21.3529 (15)C3—C41.3695 (16)
N2—C11.3592 (14)C3—H3A0.9500
N2—H10.862 (10)O1—C51.2482 (14)
N3—C11.3273 (15)O2—C51.2824 (14)
N3—H20.81 (2)C5—C61.4919 (16)
N3—H30.85 (2)C6—C6i1.334 (2)
N4—C21.3444 (15)C6—H6A0.9500
C4—N1—C1114.99 (10)N4—C2—C3122.99 (11)
C2—N2—C1120.34 (10)N2—C2—C3119.54 (10)
C2—N2—H1118 (2)C4—C3—C2114.80 (10)
C1—N2—H1122 (2)C4—C3—H3A122.6
C1—N3—H2119.5 (17)C2—C3—H3A122.6
C1—N3—H3113.3 (16)N1—C4—C3127.36 (11)
H2—N3—H3127 (2)N1—C4—Cl1114.05 (9)
C2—N4—H4120.1 (17)C3—C4—Cl1118.59 (9)
C2—N4—H5119.4 (16)O1—C5—O2124.44 (11)
H4—N4—H5120 (2)O1—C5—C6118.95 (11)
N3—C1—N1119.22 (10)O2—C5—C6116.61 (10)
N3—C1—N2117.81 (11)C6i—C6—C5122.53 (14)
N1—C1—N2122.97 (10)C6i—C6—H6A118.7
N4—C2—N2117.47 (11)C5—C6—H6A118.7
C4—N1—C1—N3−179.71 (11)N2—C2—C3—C40.33 (17)
C4—N1—C1—N2−0.05 (17)C1—N1—C4—C30.85 (19)
C2—N2—C1—N3179.15 (11)C1—N1—C4—Cl1−178.65 (9)
C2—N2—C1—N1−0.51 (18)C2—C3—C4—N1−0.99 (19)
C1—N2—C2—N4179.70 (11)C2—C3—C4—Cl1178.50 (9)
C1—N2—C2—C30.34 (17)O1—C5—C6—C6i−167.18 (16)
N4—C2—C3—C4−178.98 (11)O2—C5—C6—C6i12.7 (2)
D—H···AD—HH···AD···AD—H···A
N2—H1···O2ii0.86 (1)1.69 (1)2.5281 (14)165 (3)
N3—H2···O1ii0.81 (2)2.12 (2)2.9233 (15)168 (2)
N3—H3···N1iii0.85 (2)2.15 (2)3.0014 (16)176 (2)
N4—H4···O1iv0.78 (2)2.08 (2)2.8307 (16)161 (2)
N4—H5···Cl1v0.77 (2)2.78 (2)3.3671 (13)135.0 (19)
N4—H5···O2ii0.77 (2)2.56 (2)3.1458 (15)134.2 (19)
C3—H3A···O2i0.952.393.3085 (16)162
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯A D—HH⋯A DA D—H⋯A
N2—H1⋯O2i 0.86 (1)1.69 (1)2.5281 (14)165 (3)
N3—H2⋯O1i 0.81 (2)2.12 (2)2.9233 (15)168 (2)
N3—H3⋯N1ii 0.85 (2)2.15 (2)3.0014 (16)176 (2)
N4—H4⋯O1iii 0.78 (2)2.08 (2)2.8307 (16)161 (2)
N4—H5⋯Cl1iv 0.77 (2)2.78 (2)3.3671 (13)135.0 (19)
N4—H5⋯O2i 0.77 (2)2.56 (2)3.1458 (15)134.2 (19)
C3—H3A⋯O2v 0.952.393.3085 (16)162

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

  2 in total

1.  A short history of SHELX.

Authors:  George M Sheldrick
Journal:  Acta Crystallogr A       Date:  2007-12-21       Impact factor: 2.290

2.  Structure validation in chemical crystallography.

Authors:  Anthony L Spek
Journal:  Acta Crystallogr D Biol Crystallogr       Date:  2009-01-20
  2 in total
  2 in total

1.  Supra-molecular inter-actions in 2,6-di-amino-4-chloro-pyrimidin-1-ium 5-chloro-salicylate and bis-(2,6-di-amino-4-chloro-pyrimidin-1-ium) naphthalene-1,5-di-sulfonate.

Authors:  Robert Swinton Darious; Packianathan Thomas Muthiah; Franc Perdih
Journal:  Acta Crystallogr E Crystallogr Commun       Date:  2018-01-26

2.  2,6-Di-amino-4-chloro-pyrimidinium 4-carb-oxy-butano-ate.

Authors:  Bellarmin Edison; Kasthuri Balasubramani; Kaliyaperumal Thanigaimani; Nuridayanti Che Khalib; Suhana Arshad; Ibrahim Abdul Razak
Journal:  Acta Crystallogr Sect E Struct Rep Online       Date:  2014-07-05
  2 in total

北京卡尤迪生物科技股份有限公司 © 2022-2023.