organic compounds\(\def\hfill{\hskip 5em}\def\hfil{\hskip 3em}\def\eqno#1{\hfil {#1}}\)

Journal logoCRYSTALLOGRAPHIC
COMMUNICATIONS
ISSN: 2056-9890

4-Amino­pyridinium azide 4-amino­pyridine solvate

aCollege of Sciences, Nanjing University of Technology, Nanjing 210009, People's Republic of China, and bState Key Laboratory of Coordination Chemistry, Nanjing National Laboratory of Microstructures, School of Chemistry and Chemical Engineering, Nanjing University, Nanjing 210093, People's Republic of China
*Correspondence e-mail: whuang@nju.edu.cn,

(Received 29 October 2010; accepted 2 November 2010; online 6 November 2010)

In the title compound, C5H7N2+·N3·C5H6N2, all N atoms of the azide anion are situated on a twofold rotational axis, so the 4-amino­pyridinium cation and 4-amino­pyridine mol­ecule, being related by symmetry, occupy one position in the asymmetric unit. Inter­molecular N—H⋯N hydrogen bonds generate a three-dimensional hydrogen-bonding network which consolidates the crystal packing.

Related literature

For a related compound, see: Teulon et al. (1985[Teulon, P., Delaplane, R. G., Olovsson, I. & Rozière, J. (1985). Acta Cryst. C41, 479-483.]).

[Scheme 1]

Experimental

Crystal data
  • C5H7N2+·N3·C5H6N2

  • Mr = 231.27

  • Monoclinic, C 2/c

  • a = 7.507 (3) Å

  • b = 12.247 (5) Å

  • c = 13.634 (5) Å

  • β = 99.278 (5)°

  • V = 1237.0 (8) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.08 mm−1

  • T = 291 K

  • 0.14 × 0.11 × 0.10 mm

Data collection
  • Bruker SMART 1K CCD area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2000[Bruker (2000). SMART, SAINT and SADABS. Bruker AXS Inc., Madison, Wisconsin, USA.]) Tmin = 0.988, Tmax = 0.992

  • 3027 measured reflections

  • 1096 independent reflections

  • 852 reflections with I > 2σ(I)

  • Rint = 0.072

Refinement
  • R[F2 > 2σ(F2)] = 0.036

  • wR(F2) = 0.105

  • S = 1.08

  • 1096 reflections

  • 80 parameters

  • 1 restraint

  • H-atom parameters constrained

  • Δρmax = 0.11 e Å−3

  • Δρmin = −0.11 e Å−3

Table 1
Hydrogen-bond geometry (Å, °)

D—H⋯A D—H H⋯A DA D—H⋯A
N1—H1A⋯N5i 0.86 2.15 3.008 (2) 174
N1—H1B⋯N3ii 0.86 2.14 2.9942 (18) 172
N2—H2A⋯N2iii 0.86 1.84 2.689 (3) 169
Symmetry codes: (i) [-x+{\script{1\over 2}}, -y+{\script{1\over 2}}, -z+1]; (ii) -x+1, -y, -z+1; (iii) [-x, y, -z-{\script{1\over 2}}].

Data collection: SMART (Bruker, 2000[Bruker (2000). SMART, SAINT and SADABS. Bruker AXS Inc., Madison, Wisconsin, USA.]); cell refinement: SAINT (Bruker, 2000[Bruker (2000). SMART, SAINT and SADABS. Bruker AXS Inc., Madison, Wisconsin, USA.]); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.

Supporting information


Comment top

The crystal structure of 4-aminopyridine hemiperchlorate, has been previously reported (Teulon et al., 1985). In this paper, we report the X-ray single-crystal structure of 4-aminopyridinium azide 4-aminopyridine (I).

The molecular structure of (I) is illustrated in Fig. 1. All N atoms of the azide anions are situated on a twofold rotational axis, so 4-aminopyridinium cation and 4-aminopyridine molecule being related by symmetry occupy one position in the asymmetric unit. Intermolecular N—H···N hydrogen bonds (Table 1) generate a three-dimensional hydrogen-bonding network which consolidate the crystal packing.

Related literature top

For a related compound, see: Teulon et al. (1985).

Experimental top

The title compound (I) was prepared by the treatment of 4-aminopyridine (0.5 mmol, 0.041 g) and excess sodium azide (NaN3) in 20 ml methanol with a few drops of acetate acid (HOAc). Colourless single crystals suitable for X-ray diffraction measurement were grown from its methanol solution after five days' slow evaporation at room temperature in air. Anal. Calcd. for C10H13N7: C, 51.94; H, 5.66; N, 42.40%. Found: C, 51.85; H, 5.81; N, 42.29%. FT–IR (KBr pellets, cm-1): 3447 (vs), 2057 (s), 1645 (s), 1463 (m), 1202 (w), 1202 (w), 840 (w), and 590 (w).

Refinement top

One restraint (DELU 0.001 C1 C2) was used to reduce the components of the anisotropic displacement parameters along chemical C—C bond. The H atoms were placed in geometrically idealized positions and refined as riding, with C—H = 0.93 Å and N—H = 0.86 Å, Uiso(H) = 1.2Ueq(C) and Uiso(H) = 1.2Ueq(N).

Structure description top

The crystal structure of 4-aminopyridine hemiperchlorate, has been previously reported (Teulon et al., 1985). In this paper, we report the X-ray single-crystal structure of 4-aminopyridinium azide 4-aminopyridine (I).

The molecular structure of (I) is illustrated in Fig. 1. All N atoms of the azide anions are situated on a twofold rotational axis, so 4-aminopyridinium cation and 4-aminopyridine molecule being related by symmetry occupy one position in the asymmetric unit. Intermolecular N—H···N hydrogen bonds (Table 1) generate a three-dimensional hydrogen-bonding network which consolidate the crystal packing.

For a related compound, see: Teulon et al. (1985).

Computing details top

Data collection: SMART (Bruker, 2000); cell refinement: SAINT (Bruker, 2000); data reduction: SAINT (Bruker, 2000); program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).

Figures top
[Figure 1] Fig. 1. Molecular structure of the title compound with the atom-numbering scheme. Displacement ellipsoids are drawn at the 30% probability level.
4-Aminopyridinium azide 4-aminopyridine solvate top
Crystal data top
C5H7N2+·N3·C5H6N2F(000) = 488
Mr = 231.27Dx = 1.242 Mg m3
Monoclinic, C2/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -C 2ycCell parameters from 1359 reflections
a = 7.507 (3) Åθ = 3.0–25.4°
b = 12.247 (5) ŵ = 0.08 mm1
c = 13.634 (5) ÅT = 291 K
β = 99.278 (5)°Block, colourless
V = 1237.0 (8) Å30.14 × 0.11 × 0.10 mm
Z = 4
Data collection top
Bruker SMART 1K CCD area-detector
diffractometer
1096 independent reflections
Radiation source: fine-focus sealed tube852 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.072
φ and ω scansθmax = 25.0°, θmin = 3.0°
Absorption correction: multi-scan
(SADABS; Bruker, 2000)
h = 88
Tmin = 0.988, Tmax = 0.992k = 1214
3027 measured reflectionsl = 1615
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.036H-atom parameters constrained
wR(F2) = 0.105 w = 1/[σ2(Fo2) + (0.0493P)2 + 0.0478P]
where P = (Fo2 + 2Fc2)/3
S = 1.08(Δ/σ)max < 0.001
1096 reflectionsΔρmax = 0.11 e Å3
80 parametersΔρmin = 0.11 e Å3
1 restraintExtinction correction: SHELXTL (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.042 (5)
Crystal data top
C5H7N2+·N3·C5H6N2V = 1237.0 (8) Å3
Mr = 231.27Z = 4
Monoclinic, C2/cMo Kα radiation
a = 7.507 (3) ŵ = 0.08 mm1
b = 12.247 (5) ÅT = 291 K
c = 13.634 (5) Å0.14 × 0.11 × 0.10 mm
β = 99.278 (5)°
Data collection top
Bruker SMART 1K CCD area-detector
diffractometer
1096 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 2000)
852 reflections with I > 2σ(I)
Tmin = 0.988, Tmax = 0.992Rint = 0.072
3027 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0361 restraint
wR(F2) = 0.105H-atom parameters constrained
S = 1.08Δρmax = 0.11 e Å3
1096 reflectionsΔρmin = 0.11 e Å3
80 parameters
Special details top

Experimental. The structure was solved by direct methods (Bruker, 2000) and successive difference Fourier syntheses.

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) top
xyzUiso*/UeqOcc. (<1)
C10.1721 (2)0.05406 (12)0.09812 (12)0.0879 (5)
H10.23210.00330.13160.106*
C20.22248 (18)0.06466 (10)0.00146 (11)0.0780 (4)
H20.31450.02140.03500.094*
C30.13523 (16)0.14103 (10)0.05345 (9)0.0699 (4)
C40.00162 (18)0.20282 (11)0.00180 (11)0.0791 (4)
H40.06350.25470.02940.095*
C50.0439 (2)0.18672 (13)0.10131 (12)0.0932 (5)
H50.13550.22860.13710.112*
N10.18164 (16)0.15416 (9)0.15211 (9)0.0858 (4)
H1A0.12650.20160.18280.103*
H1B0.26650.11510.18460.103*
N20.04055 (19)0.11306 (11)0.15027 (9)0.0948 (4)
H2A0.01080.10420.21340.114*0.50
N30.50000.02503 (17)0.75000.1009 (6)
N40.50000.07152 (17)0.75000.0760 (5)
N50.50000.16656 (17)0.75000.1062 (6)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0948 (10)0.0867 (9)0.0891 (8)0.0181 (8)0.0353 (8)0.0118 (8)
C20.0744 (8)0.0752 (8)0.0879 (8)0.0108 (6)0.0231 (6)0.0057 (6)
C30.0681 (7)0.0682 (7)0.0762 (9)0.0163 (6)0.0206 (6)0.0037 (6)
C40.0765 (8)0.0799 (8)0.0834 (9)0.0071 (6)0.0205 (7)0.0009 (7)
C50.0938 (10)0.1000 (11)0.0854 (11)0.0100 (8)0.0132 (8)0.0090 (8)
N10.0900 (8)0.0873 (8)0.0803 (8)0.0016 (5)0.0144 (6)0.0086 (6)
N20.1105 (10)0.1050 (9)0.0714 (8)0.0251 (7)0.0223 (7)0.0032 (7)
N30.0964 (13)0.0868 (12)0.1185 (15)0.0000.0141 (10)0.000
N40.0626 (9)0.0993 (13)0.0671 (9)0.0000.0139 (6)0.000
N50.1123 (14)0.0918 (14)0.1242 (16)0.0000.0488 (12)0.000
Geometric parameters (Å, º) top
C1—N21.333 (2)C4—H40.9300
C1—C21.356 (2)C5—N21.341 (2)
C1—H10.9300C5—H50.9300
C2—C31.3985 (18)N1—H1A0.8600
C2—H20.9300N1—H1B0.8600
C3—N11.3437 (17)N2—H2A0.8600
C3—C41.395 (2)N3—N41.182 (3)
C4—C51.357 (2)N4—N51.164 (2)
N2—C1—C2123.06 (14)C3—C4—H4120.2
N2—C1—H1118.5N2—C5—C4122.83 (15)
C2—C1—H1118.5N2—C5—H5118.6
C1—C2—C3119.58 (14)C4—C5—H5118.6
C1—C2—H2120.2C3—N1—H1A120.0
C3—C2—H2120.2C3—N1—H1B120.0
N1—C3—C4121.68 (12)H1A—N1—H1B120.0
N1—C3—C2121.36 (13)C1—N2—C5117.93 (13)
C4—C3—C2116.97 (13)C1—N2—H2A121.0
C5—C4—C3119.63 (14)C5—N2—H2A121.0
C5—C4—H4120.2N5—N4—N3180.000 (1)
N2—C1—C2—C30.5 (2)C2—C3—C4—C50.10 (18)
C1—C2—C3—N1179.81 (11)C3—C4—C5—N20.0 (2)
C1—C2—C3—C40.11 (17)C2—C1—N2—C50.6 (2)
N1—C3—C4—C5179.98 (11)C4—C5—N2—C10.3 (2)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1A···N5i0.862.153.008 (2)174
N1—H1B···N3ii0.862.142.9942 (18)172
N2—H2A···N2iii0.861.842.689 (3)169
Symmetry codes: (i) x+1/2, y+1/2, z+1; (ii) x+1, y, z+1; (iii) x, y, z1/2.

Experimental details

Crystal data
Chemical formulaC5H7N2+·N3·C5H6N2
Mr231.27
Crystal system, space groupMonoclinic, C2/c
Temperature (K)291
a, b, c (Å)7.507 (3), 12.247 (5), 13.634 (5)
β (°) 99.278 (5)
V3)1237.0 (8)
Z4
Radiation typeMo Kα
µ (mm1)0.08
Crystal size (mm)0.14 × 0.11 × 0.10
Data collection
DiffractometerBruker SMART 1K CCD area-detector
Absorption correctionMulti-scan
(SADABS; Bruker, 2000)
Tmin, Tmax0.988, 0.992
No. of measured, independent and
observed [I > 2σ(I)] reflections
3027, 1096, 852
Rint0.072
(sin θ/λ)max1)0.595
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.036, 0.105, 1.08
No. of reflections1096
No. of parameters80
No. of restraints1
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.11, 0.11

Computer programs: SMART (Bruker, 2000), SAINT (Bruker, 2000), SHELXTL (Sheldrick, 2008).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1A···N5i0.862.153.008 (2)173.8
N1—H1B···N3ii0.862.142.9942 (18)171.9
N2—H2A···N2iii0.861.842.689 (3)168.9
Symmetry codes: (i) x+1/2, y+1/2, z+1; (ii) x+1, y, z+1; (iii) x, y, z1/2.
 

Acknowledgements

WH acknowledges the National Natural Science Foundation of China (grant No. 20871065) and the Jiangsu Province Department of Science and Technology (grant No. BK2009226) for financial support.

References

First citationBruker (2000). SMART, SAINT and SADABS. Bruker AXS Inc., Madison, Wisconsin, USA.  Google Scholar
First citationSheldrick, G. M. (2008). Acta Cryst. A64, 112–122.  Web of Science CrossRef CAS IUCr Journals Google Scholar
First citationTeulon, P., Delaplane, R. G., Olovsson, I. & Rozière, J. (1985). Acta Cryst. C41, 479–483.  CSD CrossRef CAS Web of Science IUCr Journals Google Scholar

This is an open-access article distributed under the terms of the Creative Commons Attribution (CC-BY) Licence, which permits unrestricted use, distribution, and reproduction in any medium, provided the original authors and source are cited.

Journal logoCRYSTALLOGRAPHIC
COMMUNICATIONS
ISSN: 2056-9890
Follow Acta Cryst. E
Sign up for e-alerts
Follow Acta Cryst. on Twitter
Follow us on facebook
Sign up for RSS feeds