organic compounds
N-(2-Chloropyrimidin-4-yl)-N,2-dimethyl-2H-indazol-6-amine
aMaterials Science and Engineering, Tianjin Polytechnic University, Tianjin 300160, People's Republic of China, and bTianjin Institute of Pharmaceutical Research, Tianjin 300193, People's Republic of China
*Correspondence e-mail: lbn_1111@yahoo.com.cn
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).
Experimental
Crystal data
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Refinement
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Data collection: CrystalClear (Rigaku/MSC, 2005); cell 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.
Supporting information
https://doi.org/10.1107/S1600536810042753/cv2775sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S1600536810042753/cv2775Isup2.hkl
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.
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).
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
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 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].
TheFor 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).
Data collection: CrystalClear (Rigaku/MSC, 2005); cell
CrystalClear (Rigaku/MSC, 2005); data reduction: CrystalClear (Rigaku/MSC, 2005); 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 (Sheldrick, 2008).Fig. 1. The molecular structure of (I). Displacement ellipsoids are drawn at the 50% probability level. |
C13H12ClN5 | F(000) = 1136 |
Mr = 273.73 | Dx = 1.375 Mg m−3 |
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 mm−1 |
β = 90.25 (3)° | T = 113 K |
V = 2644.1 (9) Å3 | Block, white |
Z = 8 | 0.20 × 0.18 × 0.12 mm |
Rigaku Saturn CCD area-detector diffractometer | 2323 independent reflections |
Radiation source: rotating anode | 1982 reflections with I > 2σ(I) |
Confocal monochromator | 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 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 Å−3 |
175 parameters | Δρmin = −0.25 e Å−3 |
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) |
C13H12ClN5 | V = 2644.1 (9) Å3 |
Mr = 273.73 | Z = 8 |
Monoclinic, C2/c | Mo Kα radiation |
a = 21.432 (4) Å | µ = 0.28 mm−1 |
b = 9.836 (2) Å | T = 113 K |
c = 12.542 (3) Å | 0.20 × 0.18 × 0.12 mm |
β = 90.25 (3)° |
Rigaku Saturn CCD area-detector diffractometer | 2323 independent reflections |
Absorption correction: multi-scan (CrystalClear; Rigaku/MSC, 2005) | 1982 reflections with I > 2σ(I) |
Tmin = 0.946, Tmax = 0.967 | Rint = 0.043 |
10576 measured reflections |
R[F2 > 2σ(F2)] = 0.036 | 0 restraints |
wR(F2) = 0.100 | H-atom parameters constrained |
S = 1.01 | Δρmax = 0.21 e Å−3 |
2323 reflections | Δρmin = −0.25 e Å−3 |
175 parameters |
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. |
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* |
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) |
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 code: (i) −x, y, −z+3/2. |
D—H···A | D—H | H···A | D···A | D—H···A |
C13—H13B···N2ii | 0.98 | 2.56 | 3.517 (2) | 166 |
Symmetry code: (ii) −x, −y+1, −z+2. |
Experimental details
Crystal data | |
Chemical formula | C13H12ClN5 |
Mr | 273.73 |
Crystal system, space group | Monoclinic, C2/c |
Temperature (K) | 113 |
a, b, c (Å) | 21.432 (4), 9.836 (2), 12.542 (3) |
β (°) | 90.25 (3) |
V (Å3) | 2644.1 (9) |
Z | 8 |
Radiation type | Mo Kα |
µ (mm−1) | 0.28 |
Crystal size (mm) | 0.20 × 0.18 × 0.12 |
Data collection | |
Diffractometer | Rigaku Saturn CCD area-detector |
Absorption correction | Multi-scan (CrystalClear; Rigaku/MSC, 2005) |
Tmin, Tmax | 0.946, 0.967 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 10576, 2323, 1982 |
Rint | 0.043 |
(sin θ/λ)max (Å−1) | 0.595 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.036, 0.100, 1.01 |
No. of reflections | 2323 |
No. of parameters | 175 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.21, −0.25 |
Computer programs: CrystalClear (Rigaku/MSC, 2005), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008).
D—H···A | D—H | H···A | D···A | D—H···A |
C13—H13B···N2i | 0.98 | 2.56 | 3.517 (2) | 165.7 |
Symmetry code: (i) −x, −y+1, −z+2. |
Acknowledgements
The authors thank Mr Hai-Bin Song of Nankai University and Mr Shuai Mu of Tianjin University for their helpful suggestions.
References
Limvorasak, S. & Posadas, E. M. (2009). Expert Opin. Pharmacother. 10, 3091–3102. Web of Science CrossRef PubMed CAS Google Scholar
Rigaku/MSC (2005). CrystalClear. Rigaku/MSC Inc., The Woodlands, Texas, USA. Google Scholar
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. Web of Science CrossRef CAS IUCr Journals Google Scholar
Sloan, B. & Scheinfeld, N. S. (2008). Curr. Opin. Investig. Drugs, 9, 1324–1335. Web of Science PubMed CAS Google Scholar
Sonpavde, G. M. D., Hutson, T. E. D. O. & Pharm, D. (2007). Curr. Oncol. Rep. 9, 115–119. CrossRef PubMed CAS Google Scholar
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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].