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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2010 Oct 30;66(Pt 11):o2955. doi: 10.1107/S1600536810042753

N-(2-Chloro­pyrimidin-4-yl)-N,2-di­methyl-2H-indazol-6-amine

Hao-Fei Qi a, Bing-Ni Liu b,*, Mo Liu b, Deng-Ke Liu b
PMCID: PMC3009102  PMID: 21589123

Abstract

In the title compound, C13H12ClN5, which is a derivative of the anti­tumor agent pazopanib {systematic name: 5-[[4-[(2,3-di­methyl-2H-indazol-6-yl)methylamino]-2-pyrimidinyl]amino]-2-methylbenzolsulfonamide}, the indazole and pyrim­idine fragments form a dihedral angle of 62.63 (5)°. In the crystal, pairs of mol­ecules related by twofold rotational symmetry are linked into dimers through π–π inter­actions between the indazole ring systems [centroid–centroid distance = 3.720 (2) Å]. Weak inter­molecular C—H⋯N hydrogen bonds further assemble these dimers into columns propagated in [001].

Related literature

For background to the pharmacokinetics and clinical studies of the anti­tumor agent pazopanib, see: Limvorasak & Posadas (2009); Sloan & Scheinfeld 2008; Sonpavde et al. (2007). For the synthesis of pazopanib, see: Sorbera et al. (2006).graphic file with name e-66-o2955-scheme1.jpg

Experimental

Crystal data

  • C13H12ClN5

  • M r = 273.73

  • Monoclinic, Inline graphic

  • a = 21.432 (4) Å

  • b = 9.836 (2) Å

  • c = 12.542 (3) Å

  • β = 90.25 (3)°

  • V = 2644.1 (9) Å3

  • Z = 8

  • Mo Kα radiation

  • μ = 0.28 mm−1

  • T = 113 K

  • 0.20 × 0.18 × 0.12 mm

Data collection

  • Rigaku Saturn CCD area-detector diffractometer

  • Absorption correction: multi-scan (CrystalClear; Rigaku/MSC, 2005) T min = 0.946, T max = 0.967

  • 10576 measured reflections

  • 2323 independent reflections

  • 1982 reflections with I > 2σ(I)

  • R int = 0.043

Refinement

  • R[F 2 > 2σ(F 2)] = 0.036

  • wR(F 2) = 0.100

  • S = 1.01

  • 2323 reflections

  • 175 parameters

  • H-atom parameters constrained

  • Δρmax = 0.21 e Å−3

  • Δρmin = −0.25 e Å−3

Data collection: CrystalClear (Rigaku/MSC, 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: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL.

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536810042753/cv2775sup1.cif

e-66-o2955-sup1.cif (18.1KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810042753/cv2775Isup2.hkl

e-66-o2955-Isup2.hkl (114.3KB, hkl)

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
C13—H13B⋯N2i 0.98 2.56 3.517 (2) 166

Symmetry code: (i) Inline graphic.

Acknowledgments

The authors thank Mr Hai-Bin Song of Nankai University and Mr Shuai Mu of Tianjin University for their helpful suggestions.

supplementary crystallographic information

Comment

Pazopanib is an oral, second-generation multi-targeted tyrosine kinase inhibitor that targets VEGFR, platelet-derived growth factor receptor and c-kit, key proteins responsible for tumor growth and survival (Limvorasak et al., 2009; Sloan et al., 2008; Sonpavde et al., 2007). The crystal structure of the title compound (I), a derivative of pazopanib, synthesized through the transformation of pazopanib (Sorbera et al., 2006), is reported here.

In (I) (Fig. 1), the indazole and pyrimidine fragments form a dihedral angle of 62.63 (5)°. In the crystal structure, The π–π contacts between the indazole systems from the adjacent molecules (Table 1) link them into dimers. Weak intermolecular C—H···N hydrogen bonds (Table 2) link further the dimers into columns propagated in direction [001].

Experimental

To a stirred solution of the N-(2-chloropyrimidin-4-yl)-2 -methyl-2H-indazol-6-amine 5 g (0.02 mol) in DMF (30 ml) was added Cs2CO3 9.8 g (0.03 mol) and iodomethane 2.5 ml (5.7 g, 0.04 mol) at room temperature. The mixture was stirred for 5 h. The reaction mixture was then poured into an ice-water bath, and the precipitate was collected via filtration and washed with water. The precipitate was air-dried to get off-white solid as crude product. The solid was dissolved in ethyl acetate 30 ml at 278 k, then white crystals were generated slowly.

Refinement

C-bound H atoms were geometrically positioned (C—H 0.95–0.98 Å), and refined as riding with Uiso = 1.2-1.5 Ueq(C).

Figures

Fig. 1.

Fig. 1.

The molecular structure of (I). Displacement ellipsoids are drawn at the 50% probability level.

Crystal data

C13H12ClN5 F(000) = 1136
Mr = 273.73 Dx = 1.375 Mg m3
Monoclinic, C2/c Mo Kα radiation, λ = 0.71073 Å
a = 21.432 (4) Å Cell parameters from 4286 reflections
b = 9.836 (2) Å θ = 1.9–27.9°
c = 12.542 (3) Å µ = 0.28 mm1
β = 90.25 (3)° T = 113 K
V = 2644.1 (9) Å3 Block, white
Z = 8 0.20 × 0.18 × 0.12 mm

Data collection

Rigaku Saturn CCD area-detector diffractometer 2323 independent reflections
Radiation source: rotating anode 1982 reflections with I > 2σ(I)
confocal Rint = 0.043
Detector resolution: 7.31 pixels mm-1 θmax = 25.0°, θmin = 1.9°
ω and φ scans h = −25→25
Absorption correction: multi-scan (CrystalClear; Rigaku/MSC, 2005) k = −11→11
Tmin = 0.946, Tmax = 0.967 l = −14→14
10576 measured reflections

Refinement

Refinement on F2 Secondary atom site location: difference Fourier map
Least-squares matrix: full Hydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.036 H-atom parameters constrained
wR(F2) = 0.100 w = 1/[σ2(Fo2) + (0.070P)2] where P = (Fo2 + 2Fc2)/3
S = 1.01 (Δ/σ)max = 0.001
2323 reflections Δρmax = 0.21 e Å3
175 parameters Δρmin = −0.25 e Å3
0 restraints Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methods Extinction coefficient: 0.0191 (14)

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
Cl1 0.227613 (19) 0.06867 (4) 0.79285 (3) 0.0308 (2)
N1 0.13815 (6) 0.18363 (13) 0.68576 (10) 0.0268 (4)
N2 0.18239 (6) 0.30697 (12) 0.83256 (10) 0.0206 (3)
N3 0.14793 (6) 0.52060 (13) 0.88097 (10) 0.0206 (3)
N4 −0.06548 (6) 0.69175 (13) 0.92048 (10) 0.0223 (3)
N5 −0.08472 (6) 0.82333 (13) 0.91397 (10) 0.0218 (3)
C1 0.17633 (7) 0.20335 (15) 0.76669 (12) 0.0211 (4)
C2 0.10043 (8) 0.29266 (17) 0.66821 (13) 0.0284 (4)
H2 0.0720 0.2880 0.6101 0.034*
C3 0.10066 (8) 0.40761 (16) 0.72803 (12) 0.0235 (4)
H3 0.0736 0.4815 0.7124 0.028*
C4 0.14298 (7) 0.41252 (15) 0.81461 (12) 0.0189 (4)
C5 0.19380 (7) 0.52028 (18) 0.96815 (13) 0.0295 (4)
H5A 0.1776 0.4671 1.0280 0.044*
H5B 0.2016 0.6139 0.9915 0.044*
H5C 0.2329 0.4797 0.9432 0.044*
C6 0.10170 (7) 0.62570 (16) 0.88222 (11) 0.0194 (4)
C7 0.12160 (7) 0.76193 (16) 0.86613 (13) 0.0252 (4)
H7 0.1644 0.7801 0.8529 0.030*
C8 0.07992 (7) 0.86753 (17) 0.86940 (13) 0.0267 (4)
H8 0.0935 0.9585 0.8592 0.032*
C9 0.01641 (7) 0.83811 (15) 0.88831 (12) 0.0209 (4)
C10 −0.00297 (7) 0.70070 (15) 0.90426 (11) 0.0188 (4)
C11 0.04067 (7) 0.59365 (15) 0.90219 (12) 0.0195 (4)
H11 0.0282 0.5023 0.9142 0.023*
C12 −0.03903 (7) 0.91238 (17) 0.89500 (12) 0.0246 (4)
H12 −0.0434 1.0080 0.8875 0.030*
C13 −0.15098 (7) 0.85326 (18) 0.92276 (13) 0.0286 (4)
H13A −0.1573 0.9519 0.9201 0.043*
H13B −0.1667 0.8179 0.9906 0.043*
H13C −0.1735 0.8102 0.8636 0.043*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Cl1 0.0287 (3) 0.0271 (3) 0.0365 (3) 0.00976 (17) −0.00266 (19) −0.00407 (17)
N1 0.0329 (8) 0.0226 (8) 0.0250 (8) 0.0042 (6) −0.0049 (6) −0.0020 (6)
N2 0.0177 (7) 0.0222 (8) 0.0220 (7) 0.0014 (6) 0.0025 (5) 0.0001 (6)
N3 0.0176 (7) 0.0228 (7) 0.0214 (7) 0.0028 (6) −0.0009 (5) −0.0045 (6)
N4 0.0207 (7) 0.0194 (8) 0.0267 (8) 0.0035 (6) 0.0006 (6) 0.0018 (5)
N5 0.0223 (7) 0.0204 (7) 0.0226 (7) 0.0049 (6) −0.0011 (5) 0.0004 (6)
C1 0.0205 (8) 0.0200 (9) 0.0228 (9) 0.0009 (7) 0.0050 (7) 0.0024 (7)
C2 0.0344 (9) 0.0284 (10) 0.0225 (9) 0.0018 (8) −0.0080 (7) 0.0005 (7)
C3 0.0274 (9) 0.0220 (9) 0.0210 (8) 0.0041 (7) −0.0025 (7) 0.0036 (7)
C4 0.0181 (8) 0.0203 (9) 0.0184 (8) −0.0010 (6) 0.0052 (6) 0.0028 (6)
C5 0.0229 (9) 0.0349 (10) 0.0307 (10) 0.0057 (8) −0.0078 (7) −0.0107 (8)
C6 0.0206 (8) 0.0214 (9) 0.0163 (8) 0.0019 (7) −0.0011 (6) −0.0024 (6)
C7 0.0212 (8) 0.0254 (9) 0.0290 (9) −0.0040 (7) 0.0022 (7) −0.0015 (7)
C8 0.0278 (9) 0.0194 (9) 0.0328 (10) −0.0036 (7) 0.0007 (7) 0.0011 (7)
C9 0.0239 (8) 0.0188 (8) 0.0200 (8) −0.0002 (7) −0.0013 (6) 0.0001 (6)
C10 0.0201 (8) 0.0199 (8) 0.0164 (8) −0.0004 (6) −0.0025 (6) −0.0002 (6)
C11 0.0225 (8) 0.0176 (8) 0.0185 (8) −0.0005 (6) −0.0001 (6) −0.0003 (6)
C12 0.0303 (10) 0.0180 (8) 0.0255 (9) 0.0009 (7) −0.0013 (7) 0.0003 (7)
C13 0.0223 (9) 0.0308 (10) 0.0328 (10) 0.0082 (7) 0.0023 (7) 0.0053 (7)

Geometric parameters (Å, °)

Cl1—C1 1.7515 (16) C5—H5B 0.9800
N1—C1 1.315 (2) C5—H5C 0.9800
N1—C2 1.360 (2) C6—C11 1.370 (2)
N2—C1 1.3182 (19) C6—C7 1.421 (2)
N2—C4 1.3564 (19) C7—C8 1.371 (2)
N3—C4 1.3540 (19) C7—H7 0.9500
N3—C6 1.4321 (19) C8—C9 1.413 (2)
N3—C5 1.467 (2) C8—H8 0.9500
N4—C10 1.3586 (19) C9—C12 1.398 (2)
N4—N5 1.3607 (17) C9—C10 1.428 (2)
N5—C12 1.336 (2) C10—C11 1.409 (2)
N5—C13 1.4551 (19) C11—H11 0.9500
C2—C3 1.357 (2) C12—H12 0.9500
C2—H2 0.9500 C13—H13A 0.9800
C3—C4 1.413 (2) C13—H13B 0.9800
C3—H3 0.9500 C13—H13C 0.9800
C5—H5A 0.9800
Cg1···Cg2i 3.720 (2)
C1—N1—C2 112.08 (13) C11—C6—C7 122.04 (14)
C1—N2—C4 115.36 (12) C11—C6—N3 119.81 (14)
C4—N3—C6 121.42 (12) C7—C6—N3 118.11 (13)
C4—N3—C5 120.45 (13) C8—C7—C6 120.96 (15)
C6—N3—C5 117.04 (12) C8—C7—H7 119.5
C10—N4—N5 103.19 (12) C6—C7—H7 119.5
C12—N5—N4 114.34 (13) C7—C8—C9 118.58 (15)
C12—N5—C13 126.67 (14) C7—C8—H8 120.7
N4—N5—C13 118.92 (13) C9—C8—H8 120.7
N1—C1—N2 131.07 (14) C12—C9—C8 136.31 (15)
N1—C1—Cl1 114.88 (12) C12—C9—C10 103.78 (14)
N2—C1—Cl1 114.05 (11) C8—C9—C10 119.90 (14)
C3—C2—N1 124.52 (14) N4—C10—C11 127.55 (14)
C3—C2—H2 117.7 N4—C10—C9 111.71 (13)
N1—C2—H2 117.7 C11—C10—C9 120.74 (14)
C2—C3—C4 117.01 (15) C6—C11—C10 117.78 (14)
C2—C3—H3 121.5 C6—C11—H11 121.1
C4—C3—H3 121.5 C10—C11—H11 121.1
N3—C4—N2 116.87 (13) N5—C12—C9 106.98 (14)
N3—C4—C3 123.20 (14) N5—C12—H12 126.5
N2—C4—C3 119.91 (14) C9—C12—H12 126.5
N3—C5—H5A 109.5 N5—C13—H13A 109.5
N3—C5—H5B 109.5 N5—C13—H13B 109.5
H5A—C5—H5B 109.5 H13A—C13—H13B 109.5
N3—C5—H5C 109.5 N5—C13—H13C 109.5
H5A—C5—H5C 109.5 H13A—C13—H13C 109.5
H5B—C5—H5C 109.5 H13B—C13—H13C 109.5
C10—N4—N5—C12 0.03 (17) C11—C6—C7—C8 −0.4 (2)
C10—N4—N5—C13 177.21 (12) N3—C6—C7—C8 −178.15 (13)
C2—N1—C1—N2 1.9 (2) C6—C7—C8—C9 −0.5 (2)
C2—N1—C1—Cl1 −178.80 (12) C7—C8—C9—C12 −178.16 (16)
C4—N2—C1—N1 −0.3 (2) C7—C8—C9—C10 0.4 (2)
C4—N2—C1—Cl1 −179.62 (10) N5—N4—C10—C11 −179.72 (13)
C1—N1—C2—C3 −1.4 (2) N5—N4—C10—C9 0.32 (16)
N1—C2—C3—C4 −0.4 (3) C12—C9—C10—N4 −0.53 (17)
C6—N3—C4—N2 −168.27 (13) C8—C9—C10—N4 −179.54 (12)
C5—N3—C4—N2 −0.5 (2) C12—C9—C10—C11 179.50 (13)
C6—N3—C4—C3 13.5 (2) C8—C9—C10—C11 0.5 (2)
C5—N3—C4—C3 −178.74 (15) C7—C6—C11—C10 1.3 (2)
C1—N2—C4—N3 179.92 (13) N3—C6—C11—C10 179.02 (12)
C1—N2—C4—C3 −1.8 (2) N4—C10—C11—C6 178.69 (14)
C2—C3—C4—N3 −179.73 (15) C9—C10—C11—C6 −1.3 (2)
C2—C3—C4—N2 2.1 (2) N4—N5—C12—C9 −0.37 (18)
C4—N3—C6—C11 57.33 (19) C13—N5—C12—C9 −177.29 (13)
C5—N3—C6—C11 −110.80 (17) C8—C9—C12—N5 179.28 (16)
C4—N3—C6—C7 −124.86 (16) C10—C9—C12—N5 0.52 (16)
C5—N3—C6—C7 67.01 (18)

Symmetry codes: (i) −x, y, −z+3/2.

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
C13—H13B···N2ii 0.98 2.56 3.517 (2) 166

Symmetry codes: (ii) −x, −y+1, −z+2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: CV2775).

References

  1. Limvorasak, S. & Posadas, E. M. (2009). Expert Opin. Pharmacother.10, 3091–3102. [DOI] [PubMed]
  2. Rigaku/MSC (2005). CrystalClear Rigaku/MSC Inc., The Woodlands, Texas, USA.
  3. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  4. Sloan, B. & Scheinfeld, N. S. (2008). Curr. Opin. Investig. Drugs, 9, 1324–1335. [PubMed]
  5. Sonpavde, G. M. D., Hutson, T. E. D. O. & Pharm, D. (2007). Curr. Oncol. Rep.9, 115–119. [DOI] [PubMed]
  6. Sorbera, L. A., Bolos, J. & Serradell, N. (2006). Drugs. Fut.31, 585–589.

Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536810042753/cv2775sup1.cif

e-66-o2955-sup1.cif (18.1KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810042753/cv2775Isup2.hkl

e-66-o2955-Isup2.hkl (114.3KB, hkl)

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


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