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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 May 20;67(Pt 6):o1481. doi: 10.1107/S1600536811018642

N 6-(4-Fluoro­benz­yl)-3-nitro­pyridine-2,6-diamine

Ji-long Ge a,*, Xiao-min Qian b
PMCID: PMC3120364  PMID: 21754850

Abstract

In the title compound, C12H11FN4O2, the pyridine ring is connected to a benzene ring by a –CH2—NH2- chain. The nitro group is twisted out of the pyridine ring plane [torsion angle O—N—C—C = 10.41 (10)°]. An intramolecular N—H⋯O hydrogen bond occurs. The fluoro­benzene ring is disordered over two positions [occupancy ratio = 0.59 (3):0.41 (3)]. Inter­molecular N—H⋯O and N—H⋯N hydrogen bonds stabilize the crystal structure.

Related literature

The title compound is an inter­mediate in the synthesis of analgesic drugs. For the analgesic properties of flupirtine (systematic name eth­yl{2-amino-6-[(4-fluoro­benz­yl)amino]­pyridin-3-yl}carbamate), see: Klawe & Maschke (2009). For synthetic procedures, see: Gerhard & Ilia (2010). For a related structure, see: Wang (2009).graphic file with name e-67-o1481-scheme1.jpg

Experimental

Crystal data

  • C12H11FN4O2

  • M r = 262.25

  • Monoclinic, Inline graphic

  • a = 14.8187 (14) Å

  • b = 5.9972 (6) Å

  • c = 14.8840 (15) Å

  • β = 109.827 (1)°

  • V = 1244.3 (2) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.11 mm−1

  • T = 298 K

  • 0.38 × 0.15 × 0.11 mm

Data collection

  • Rigaku SCXmini CCD diffractometer

  • Absorption correction: multi-scan (CrystalClear; Rigaku, 2005) T min = 0.960, T max = 0.988

  • 5923 measured reflections

  • 2184 independent reflections

  • 1169 reflections with I > 2σ(I)

  • R int = 0.056

Refinement

  • R[F 2 > 2σ(F 2)] = 0.052

  • wR(F 2) = 0.140

  • S = 1.03

  • 2184 reflections

  • 227 parameters

  • H-atom parameters constrained

  • Δρmax = 0.21 e Å−3

  • Δρmin = −0.22 e Å−3

Data collection: CrystalClear (Rigaku, 2005); cell refinement: CrystalClear; data reduction: CrystalClear; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997) and PLATON (Spek, 2009); software used to prepare material for publication: SHELXL97.

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536811018642/pv2411sup1.cif

e-67-o1481-sup1.cif (19.3KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811018642/pv2411Isup2.hkl

e-67-o1481-Isup2.hkl (107.4KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536811018642/pv2411Isup3.cml

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

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
N3—H3B⋯O1 0.86 2.03 2.651 (3) 129
N3—H3A⋯N1i 0.86 2.17 3.028 (3) 174
N2—H2⋯O1ii 0.86 2.35 3.060 (3) 141

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

supplementary crystallographic information

Comment

Flupirtine, ethyl{2-amino-6-[(4-fluorobenzyl)amino]pyridin-3-yl}carbamate, is of great importance owing to its analgesic properties (Klawe & Maschke, 2009). In this article, we report the crystal structure of the title compound which is one of the key intermediates in the synthsis of analgesia drugs (Gerhard & Ilia, 2010).

In the title molecule (Fig. 1), a pyridine ring is connected with a benzene ring by –CH2—NH2- chain and the nitro group is twisted out of the pyridine ring plane [torsion angle O1—N4—C4—C5 = 10.41 (10)°]. The crystal structure is stabilized by intermolecular N—H···O and N—H···N hydrogen bonds (Figure 2 and Table 1).

Experimental

To a solution of 2-amino-3-nitro-6-chloropyridine (7.8 g, 45 mmol) in 2-propanol (50 ml) were added 4-fluorobenzylamine (5.63 g, 45 mmol) and triethylamine (6.45 g,64 mmol) (Gerhard & Ilia, 2010). Then another 30 ml 2-propanol was add to the above solution. The mixture was heated to backflow and stirred for 3 h. Then 100 ml water was add to the mixture to obtain the title compound which was recrystallized from ethanol by slow evaporation (yield 10.2 g, 91%).

Refinement

H atoms bonded to C atoms were placed geometrically and treated as riding, with C—H = 0.93 (benzene ring) or 0.97 Å (methylene) and N—H = 0.86 Å with Uiso(H) = 1.2Ueq(C or N) or Uiso(H) = 1.5Ueq(methylene). The fluoro benzene ring was disordered over two positions with site occupancy factors 0.59 (3) and 0.41 (3).

Figures

Fig. 1.

Fig. 1.

An ORTEP (Farrugia, 1997) view of the title compound with the atom-numbering scheme. Displacement ellipsoids are drawn at the 30% probability level. Smaller fraction of the fluorobenzene ring has been plotted with hollow bonds.

Fig. 2.

Fig. 2.

A packing diagram of the title compound showing hydrogen bonds. Smaller fraction of the fluorobenzene ring has been excluded.

Crystal data

C12H11FN4O2 F(000) = 544
Mr = 262.25 Dx = 1.400 Mg m3
Monoclinic, P21/n Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2yn Cell parameters from 1144 reflections
a = 14.8187 (14) Å θ = 2.4–26.9°
b = 5.9972 (6) Å µ = 0.11 mm1
c = 14.8840 (15) Å T = 298 K
β = 109.827 (1)° Prism, yellow
V = 1244.3 (2) Å3 0.38 × 0.15 × 0.11 mm
Z = 4

Data collection

Rigaku SCXmini CCD diffractometer 2184 independent reflections
Radiation source: fine-focus sealed tube 1169 reflections with I > 2σ(I)
graphite Rint = 0.056
Detector resolution: 8.192 pixels mm-1 θmax = 25.0°, θmin = 2.4°
φ and ω scans h = −14→17
Absorption correction: multi-scan (CrystalClear; Rigaku, 2005) k = −5→7
Tmin = 0.960, Tmax = 0.988 l = −17→17
5923 measured reflections

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)] = 0.052 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.140 H-atom parameters constrained
S = 1.02 w = 1/[σ2(Fo2) + (0.0585P)2] where P = (Fo2 + 2Fc2)/3
2184 reflections (Δ/σ)max = 0.001
227 parameters Δρmax = 0.21 e Å3
0 restraints Δρmin = −0.22 e Å3

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 Occ. (<1)
F1 0.6846 (16) 0.5113 (18) 0.0036 (13) 0.121 (4) 0.59 (3)
F1' 0.7330 (17) 0.538 (2) 0.050 (2) 0.105 (5) 0.41 (3)
N1 0.55771 (13) 0.2584 (4) 0.46588 (14) 0.0474 (6)
N2 0.49151 (15) 0.4615 (4) 0.33021 (15) 0.0608 (7)
H2 0.4453 0.3666 0.3173 0.073*
N3 0.61662 (15) 0.0425 (4) 0.59818 (14) 0.0597 (7)
H3A 0.5670 −0.0413 0.5754 0.072*
H3B 0.6593 0.0109 0.6523 0.072*
N4 0.78769 (16) 0.3201 (4) 0.66405 (17) 0.0611 (7)
O1 0.78379 (14) 0.1726 (4) 0.72145 (14) 0.0792 (7)
O2 0.86264 (15) 0.4308 (4) 0.68041 (15) 0.0852 (7)
C1 0.56363 (18) 0.4356 (5) 0.41323 (18) 0.0487 (7)
C2 0.6413 (2) 0.5883 (5) 0.4429 (2) 0.0604 (8)
H2A 0.6429 0.7126 0.4061 0.072*
C3 0.71288 (19) 0.5481 (5) 0.5260 (2) 0.0581 (8)
H3 0.7649 0.6448 0.5463 0.070*
C4 0.70977 (17) 0.3639 (4) 0.58174 (18) 0.0488 (7)
C5 0.62743 (17) 0.2205 (4) 0.54982 (17) 0.0454 (6)
C6 0.4844 (2) 0.6355 (5) 0.2601 (2) 0.0666 (8)
H6A 0.5020 0.7765 0.2934 0.080*
H6B 0.4180 0.6470 0.2188 0.080*
C7 0.5459 (2) 0.6006 (5) 0.1989 (2) 0.0611 (8)
C8 0.6128 (14) 0.425 (4) 0.2145 (16) 0.067 (4) 0.59 (3)
H8 0.6195 0.3224 0.2632 0.081* 0.59 (3)
C9 0.669 (3) 0.407 (6) 0.156 (3) 0.097 (7) 0.59 (3)
H9 0.7225 0.3149 0.1712 0.116* 0.59 (3)
C10 0.6390 (18) 0.540 (6) 0.071 (2) 0.087 (6) 0.59 (3)
C11 0.5858 (15) 0.726 (3) 0.0609 (13) 0.082 (4) 0.59 (3)
H11 0.5823 0.8329 0.0145 0.099* 0.59 (3)
C12 0.5373 (18) 0.747 (4) 0.1241 (16) 0.072 (4) 0.59 (3)
H12 0.4958 0.8669 0.1164 0.086* 0.59 (3)
C8' 0.581 (2) 0.398 (6) 0.186 (2) 0.081 (6) 0.41 (3)
H8' 0.5631 0.2733 0.2137 0.097* 0.41 (3)
C9' 0.641 (3) 0.369 (8) 0.134 (3) 0.086 (8) 0.41 (3)
H9' 0.6603 0.2268 0.1225 0.103* 0.41 (3)
C10' 0.673 (3) 0.559 (7) 0.098 (3) 0.078 (7) 0.41 (3)
C11' 0.626 (2) 0.753 (4) 0.099 (2) 0.082 (6) 0.41 (3)
H11' 0.6350 0.8719 0.0630 0.099* 0.41 (3)
C12' 0.566 (2) 0.782 (7) 0.152 (3) 0.080 (7) 0.41 (3)
H12' 0.5393 0.9213 0.1550 0.096* 0.41 (3)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
F1 0.158 (10) 0.109 (4) 0.135 (8) 0.014 (5) 0.100 (7) 0.009 (5)
F1' 0.124 (10) 0.090 (5) 0.141 (11) 0.018 (6) 0.097 (9) 0.018 (6)
N1 0.0386 (12) 0.0553 (15) 0.0437 (12) −0.0061 (10) 0.0080 (10) 0.0023 (11)
N2 0.0504 (14) 0.0698 (17) 0.0557 (14) −0.0039 (11) 0.0096 (12) 0.0163 (12)
N3 0.0514 (13) 0.0679 (17) 0.0481 (12) −0.0160 (12) 0.0016 (11) 0.0080 (12)
N4 0.0469 (15) 0.0722 (18) 0.0548 (15) −0.0129 (13) 0.0050 (13) −0.0155 (14)
O1 0.0631 (13) 0.0991 (18) 0.0574 (12) −0.0146 (12) −0.0030 (10) 0.0125 (12)
O2 0.0537 (13) 0.0941 (18) 0.0881 (15) −0.0231 (12) −0.0015 (11) −0.0111 (13)
C1 0.0441 (15) 0.0529 (18) 0.0504 (15) −0.0001 (13) 0.0180 (13) 0.0025 (14)
C2 0.0638 (18) 0.0505 (19) 0.0666 (19) −0.0090 (15) 0.0218 (16) 0.0059 (14)
C3 0.0485 (16) 0.0545 (19) 0.0687 (18) −0.0170 (14) 0.0165 (15) −0.0079 (16)
C4 0.0418 (15) 0.0527 (18) 0.0478 (15) −0.0069 (12) 0.0100 (13) −0.0068 (13)
C5 0.0399 (14) 0.0534 (18) 0.0417 (14) −0.0054 (13) 0.0121 (12) −0.0031 (13)
C6 0.0653 (19) 0.071 (2) 0.0636 (18) 0.0142 (16) 0.0224 (16) 0.0190 (16)
C7 0.0670 (19) 0.054 (2) 0.0666 (19) 0.0078 (16) 0.0278 (16) 0.0107 (16)
C8 0.078 (9) 0.056 (7) 0.074 (8) 0.010 (6) 0.034 (7) 0.010 (6)
C9 0.108 (15) 0.074 (14) 0.122 (15) 0.017 (10) 0.056 (12) 0.005 (9)
C10 0.101 (14) 0.081 (11) 0.102 (13) 0.014 (11) 0.063 (10) 0.009 (9)
C11 0.101 (10) 0.073 (7) 0.083 (8) 0.011 (7) 0.044 (7) 0.024 (6)
C12 0.082 (11) 0.064 (9) 0.079 (10) 0.015 (7) 0.039 (8) 0.019 (7)
C8' 0.101 (18) 0.060 (9) 0.090 (16) −0.004 (11) 0.045 (12) 0.012 (10)
C9' 0.11 (2) 0.057 (12) 0.111 (19) 0.010 (13) 0.069 (16) 0.007 (13)
C10' 0.096 (18) 0.057 (10) 0.11 (2) −0.003 (13) 0.066 (14) 0.010 (12)
C11' 0.098 (14) 0.067 (9) 0.098 (14) −0.004 (9) 0.054 (11) 0.019 (10)
C12' 0.091 (17) 0.062 (10) 0.097 (19) 0.003 (11) 0.044 (13) 0.010 (11)

Geometric parameters (Å, °)

F1—C10 1.39 (3) C6—H6B 0.9700
F1'—C10' 1.32 (4) C7—C8' 1.36 (3)
N1—C1 1.341 (3) C7—C12' 1.38 (4)
N1—C5 1.343 (3) C7—C12 1.39 (3)
N2—C1 1.341 (3) C7—C8 1.41 (2)
N2—C6 1.454 (3) C8—C9 1.40 (4)
N2—H2 0.8600 C8—H8 0.9300
N3—C5 1.327 (3) C9—C10 1.43 (5)
N3—H3A 0.8600 C9—H9 0.9300
N3—H3B 0.8600 C10—C11 1.35 (4)
N4—O1 1.245 (3) C11—C12 1.37 (3)
N4—O2 1.245 (3) C11—H11 0.9300
N4—C4 1.394 (3) C12—H12 0.9300
C1—C2 1.419 (4) C8'—C9' 1.38 (6)
C2—C3 1.350 (4) C8'—H8' 0.9300
C2—H2A 0.9300 C9'—C10' 1.41 (7)
C3—C4 1.392 (4) C9'—H9' 0.9300
C3—H3 0.9300 C10'—C11' 1.36 (5)
C4—C5 1.436 (3) C11'—C12' 1.38 (4)
C6—C7 1.506 (4) C11'—H11' 0.9300
C6—H6A 0.9700 C12'—H12' 0.9300
C1—N1—C5 119.7 (2) C12—C7—C8 118.1 (15)
C1—N2—C6 125.8 (2) C8'—C7—C6 123.0 (15)
C1—N2—H2 117.1 C12'—C7—C6 118.4 (18)
C6—N2—H2 117.1 C12—C7—C6 119.2 (12)
C5—N3—H3A 120.0 C8—C7—C6 122.6 (10)
C5—N3—H3B 120.0 C9—C8—C7 119 (2)
H3A—N3—H3B 120.0 C9—C8—H8 120.4
O1—N4—O2 119.4 (2) C7—C8—H8 120.4
O1—N4—C4 121.3 (2) C8—C9—C10 116 (3)
O2—N4—C4 119.3 (3) C8—C9—H9 122.0
N2—C1—N1 116.1 (2) C10—C9—H9 122.0
N2—C1—C2 121.4 (3) C11—C10—F1 116 (2)
N1—C1—C2 122.5 (2) C11—C10—C9 123 (3)
C3—C2—C1 118.1 (3) F1—C10—C9 119 (3)
C3—C2—H2A 120.9 C10—C11—C12 115 (2)
C1—C2—H2A 120.9 C10—C11—H11 122.5
C2—C3—C4 120.9 (3) C12—C11—H11 122.5
C2—C3—H3 119.6 C11—C12—C7 125 (2)
C4—C3—H3 119.6 C11—C12—H12 117.7
C3—C4—N4 119.2 (2) C7—C12—H12 117.7
C3—C4—C5 118.3 (2) C7—C8'—C9' 123 (3)
N4—C4—C5 122.4 (2) C7—C8'—H8' 118.7
N3—C5—N1 116.4 (2) C9'—C8'—H8' 118.7
N3—C5—C4 123.2 (2) C8'—C9'—C10' 119 (4)
N1—C5—C4 120.4 (2) C8'—C9'—H9' 120.7
N2—C6—C7 115.0 (2) C10'—C9'—H9' 120.7
N2—C6—H6A 108.5 F1'—C10'—C11' 122 (3)
C7—C6—H6A 108.5 F1'—C10'—C9' 120 (4)
N2—C6—H6B 108.5 C11'—C10'—C9' 116 (4)
C7—C6—H6B 108.5 C10'—C11'—C12' 123 (3)
H6A—C6—H6B 107.5 C10'—C11'—H11' 118.3
C8'—C7—C12' 119 (2) C12'—C11'—H11' 118.3
C8'—C7—C12 112.9 (17) C7—C12'—C11' 119 (3)
C12'—C7—C12 21.8 (14) C7—C12'—H12' 120.7
C8'—C7—C8 22.5 (12) C11'—C12'—H12' 120.7
C12'—C7—C8 114.4 (19)
C6—N2—C1—N1 −177.6 (2) C12—C7—C8—C9 1.3 (19)
C6—N2—C1—C2 2.4 (4) C6—C7—C8—C9 −178.4 (13)
C5—N1—C1—N2 179.7 (2) C7—C8—C9—C10 −14 (3)
C5—N1—C1—C2 −0.3 (4) C8—C9—C10—C11 24 (3)
N2—C1—C2—C3 −178.1 (2) C8—C9—C10—F1 −172.7 (18)
N1—C1—C2—C3 2.0 (4) F1—C10—C11—C12 176.8 (13)
C1—C2—C3—C4 −0.9 (4) C9—C10—C11—C12 −19 (3)
C2—C3—C4—N4 176.0 (2) C10—C11—C12—C7 5(2)
C2—C3—C4—C5 −1.5 (4) C8'—C7—C12—C11 −21 (2)
O1—N4—C4—C3 171.9 (3) C12'—C7—C12—C11 89 (8)
O2—N4—C4—C3 −8.0 (4) C8—C7—C12—C11 3.6 (19)
O1—N4—C4—C5 −10.7 (4) C6—C7—C12—C11 −176.7 (11)
O2—N4—C4—C5 169.3 (2) C12'—C7—C8'—C9' 5(3)
C1—N1—C5—N3 179.8 (2) C12—C7—C8'—C9' 29 (3)
C1—N1—C5—C4 −2.3 (3) C8—C7—C8'—C9' −80 (6)
C3—C4—C5—N3 −179.0 (2) C6—C7—C8'—C9' −177 (2)
N4—C4—C5—N3 3.6 (4) C7—C8'—C9'—C10' 5(4)
C3—C4—C5—N1 3.2 (4) C8'—C9'—C10'—F1' 178 (3)
N4—C4—C5—N1 −174.2 (2) C8'—C9'—C10'—C11' −14 (5)
C1—N2—C6—C7 77.2 (3) F1'—C10'—C11'—C12' −177.8 (19)
N2—C6—C7—C8' 20.6 (16) C9'—C10'—C11'—C12' 15 (4)
N2—C6—C7—C12' −161.0 (15) C8'—C7—C12'—C11' −5(2)
N2—C6—C7—C12 174.1 (10) C12—C7—C12'—C11' −85 (8)
N2—C6—C7—C8 −6.3 (10) C8—C7—C12'—C11' 20 (2)
C8'—C7—C8—C9 83 (6) C6—C7—C12'—C11' 176.8 (13)
C12'—C7—C8—C9 −23 (2) C10'—C11'—C12'—C7 −6(3)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N3—H3B···O1 0.86 2.03 2.651 (3) 129
N3—H3A···N1i 0.86 2.17 3.028 (3) 174
N2—H2···O1ii 0.86 2.35 3.060 (3) 141

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: PV2411).

References

  1. Farrugia, L. J. (1997). J. Appl. Cryst. 30, 565.
  2. Gerhard. J & Ilia, F. (2010). Patent WO 2010/136113 A1, 2 December 2010.
  3. Klawe, C. & Maschke, M. (2009). Expert Opin. Pharmacother. 10, 1495–1500. [DOI] [PubMed]
  4. Rigaku (2005). CrystalClear Rigaku Corporation, Tokyo, Japan.
  5. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  6. Spek, A. L. (2009). Acta Cryst. D65, 148–155. [DOI] [PMC free article] [PubMed]
  7. Wang, B. (2009). Acta Cryst. E65, m861. [DOI] [PMC free article] [PubMed]

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/S1600536811018642/pv2411sup1.cif

e-67-o1481-sup1.cif (19.3KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811018642/pv2411Isup2.hkl

e-67-o1481-Isup2.hkl (107.4KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536811018642/pv2411Isup3.cml

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


Articles from Acta Crystallographica Section E: Structure Reports Online are provided here courtesy of International Union of Crystallography

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