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The positions of the cyano­methyl and 4-bromo­phenyl substituents in the title compound, C17H13BrN4O2, have been confirmed by single-crystal X-ray structure determination. The crystal packing shows weak hydrogen-bonding and aromatic π–π interactions.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536801004986/bt6027sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536801004986/bt6027Isup2.hkl
Contains datablock I

CCDC reference: 165649

Key indicators

  • Single-crystal X-ray study
  • T = 296 K
  • Mean [sigma](C-C) = 0.007 Å
  • R factor = 0.043
  • wR factor = 0.120
  • Data-to-parameter ratio = 16.5

checkCIF results

No syntax errors found

ADDSYM reports no extra symmetry


Yellow Alert Alert Level C:
ABSTM_02 Alert C The ratio of expected to reported Tmax/Tmin(RR) is > 1.10 Tmin and Tmax reported: 0.509 0.769 Tmin and Tmax expected: 0.398 0.769 RR = 1.277 Please check that your absorption correction is appropriate.
0 Alert Level A = Potentially serious problem
0 Alert Level B = Potential problem
1 Alert Level C = Please check

Comment top

The therapeutic importance (Furuya & Ohataki, 1994a,b; Heber et al., 1993; Piper et al., 1989) of suitably functionalized pyrido[2,3-d]pyrimidine ring systems enthused us to develop an innovative synthesis in which different substituents could be arranged in a pharmacophoric pattern to display diverse pharmacological activities of higher order. The title compound, (I), was prepared (Srivastava et al., 2000) by ring-transformation reactions of 6-aryl-3-cyano-4-methylthio-2H-pyran-2-one and 6-amino-1,3-dimethyluracil. The present X-ray crystallography study has been undertaken to confirm the structure of (I).

The conformation of (I) along with the atom-numbering scheme is shown in Fig. 1. The molecule contains one fused-ring system (A/B) to which a bromophenyl ring (C) is attached at the 7 position. All the rings are planar [deviations of the atoms from their least-squares planes are within the range -0.015 (3)–0.011 (3) Å]. The bromophenyl ring is coplanar with the A/B ring system [torsion angle N8—C7—C71—C72 - 179.0 (4)°]. The cyano group is twisted out of the A/B plane. The crystal structure analysis reveals the presence of weak hydrogen-bonding interactions, such as C—H···N, C—H···Br and C—H···O (Fig. 2 and Table 1). Moreover, the crystal packing (Fig. 3) also shows intermolecular stacking as a result of ππ interactions between rings B and C (Hunter & Sanders, 1990). The overlapping rings (B and C) are in a `parallel-displaced orientation'; the average distance of separation between their mean planes is 3.480 (6) Å, the angle between them being 1.0 (3)°. The different intermolecular interactions seen in the crystal structure of (I) might well be a reflection of the possible interactions in the molecular recognition process in view of the diverse pharmacological properties associated with the suitably functionalized pyrido[2,3-d]pyrimidines.

Experimental top

The synthesis of (I) was carried out by reaction of 6-amino-1,3-dimethyluracil with 6-(4-bromophenyl)-3-cyano-4-methylthio-2H-pyran-2-one (Srivastava et al., 2000). Diffraction-quality crystals were grown by slow evaporation from a solution in a dichloromethane–ethyl acetate mixture at room temperature.

Refinement top

All the H atoms were placed in geometrically idealized positions and allowed to ride on their parent atoms, to which each was bonded for the final cycles of refinement.

Computing details top

Data collection: Rigaku/AFC Diffractometer Control Software (Rigaku, 1995); cell refinement: Rigaku/AFC Diffractometer Control Software; data reduction: TEXSAN (Molecular Structure Corporation/Rigaku Corporation, 1998); program(s) used to solve structure: SHELXS86 (Sheldrick, 1990); program(s) used to refine structure: SHELXL93 (Sheldrick, 1993); molecular graphics: NRCVAX (Gabe et al.,, 1989); software used to prepare material for publication: SHELXL93.

Figures top
[Figure 1] Fig. 1. ORTEP (Johnson, 1965) diagram showing the molecular structure of (I) with labelling for non-H atoms and displacement ellipsoids at 50% probability.
[Figure 2] Fig. 2. PLUTO (Motherwell & Clegg, 1978) crystal-packing diagram showing the C—H···O hydrogen bonds as dotted lines and the C—H···Br hydrogen bonds as dashed lines.
[Figure 3] Fig. 3. The crystal packing (perpendicular view to the plane through atoms C6, C7 and N8 of ring B) showing the partial overlapping (as indicated by black shed) of rings B and C owing to intermolecular stacking.
7-(4-bromophenyl)-5-cyanomethyl-1,3-dimethyl-2,4-dioxypyrido[2,3-d]pyrimidine top
Crystal data top
C17H13BrN4O2F(000) = 388
Mr = 385.22Dx = 1.628 Mg m3
Triclinic, P1Melting point = 220–230 K
a = 8.728 (3) ÅMo Kα radiation, λ = 0.71073 Å
b = 12.087 (4) ÅCell parameters from 24 reflections
c = 8.672 (3) Åθ = 14.7–15.0°
α = 108.22 (3)°µ = 2.63 mm1
β = 113.43 (2)°T = 296 K
γ = 91.24 (3)°Block, colourless
V = 786.1 (5) Å30.4 × 0.3 × 0.1 mm
Z = 2
Data collection top
Rigaku AFC-5R
diffractometer
2254 reflections with I > 2σ(I)
Radiation source: rotating anodeRint = 0.000
Graphite monochromatorθmax = 27.5°, θmin = 2.6°
ω–2θ scansh = 1111
Absorption correction: empirical (using intensity measurements)
(TEXSAN; Molecular Structure Corporation/Rigaku Corporation, 1998)
k = 150
Tmin = 0.509, Tmax = 0.769l = 1011
3619 measured reflections3 standard reflections every 150 reflections
3619 independent reflections intensity decay: <0.2%
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.043Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.120H-atom parameters constrained
S = 1.03 w = 1/[σ2(Fo2) + (0.0669P)2 + 0.8316P]
where P = (Fo2 + 2Fc2)/3
3616 reflections(Δ/σ)max < 0.001
219 parametersΔρmax = 0.48 e Å3
0 restraintsΔρmin = 0.43 e Å3
Crystal data top
C17H13BrN4O2γ = 91.24 (3)°
Mr = 385.22V = 786.1 (5) Å3
Triclinic, P1Z = 2
a = 8.728 (3) ÅMo Kα radiation
b = 12.087 (4) ŵ = 2.63 mm1
c = 8.672 (3) ÅT = 296 K
α = 108.22 (3)°0.4 × 0.3 × 0.1 mm
β = 113.43 (2)°
Data collection top
Rigaku AFC-5R
diffractometer
2254 reflections with I > 2σ(I)
Absorption correction: empirical (using intensity measurements)
(TEXSAN; Molecular Structure Corporation/Rigaku Corporation, 1998)
Rint = 0.000
Tmin = 0.509, Tmax = 0.7693 standard reflections every 150 reflections
3619 measured reflections intensity decay: <0.2%
3619 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0430 restraints
wR(F2) = 0.120H-atom parameters constrained
S = 1.03Δρmax = 0.48 e Å3
3616 reflectionsΔρmin = 0.43 e Å3
219 parameters
Special details top

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 on F2 for ALL reflections except for 3 with very negative F2 or flagged by the user for potential systematic errors. Weighted R-factors wR and all goodnesses 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*/Ueq
Br0.08388 (7)0.28864 (4)0.14885 (8)0.0565 (2)
C1A0.5035 (5)0.3069 (3)0.0501 (6)0.0348 (8)
N10.4360 (4)0.3982 (3)0.2164 (5)0.0402 (8)
C110.2806 (6)0.3883 (4)0.3600 (6)0.0558 (13)
H11A0.29390.31300.37260.084*
H11B0.18680.39520.33030.084*
H11C0.25950.45020.47090.084*
C20.5054 (6)0.4975 (4)0.2526 (6)0.0418 (9)
O210.4402 (5)0.5786 (3)0.3964 (5)0.0631 (10)
N30.6523 (5)0.5053 (3)0.1141 (5)0.0422 (8)
C310.7350 (7)0.6072 (4)0.1563 (7)0.0540 (12)
H31A0.66680.65990.27640.081*
H31B0.74830.64780.07370.081*
H31C0.84430.58090.14630.081*
C40.7317 (5)0.4211 (4)0.0569 (6)0.0411 (9)
O410.8613 (4)0.4372 (3)0.1683 (5)0.0575 (9)
C4A0.6496 (5)0.3176 (3)0.0898 (6)0.0357 (8)
C50.7086 (5)0.2240 (4)0.2554 (6)0.0387 (9)
C510.8651 (6)0.2219 (5)0.4198 (6)0.0502 (11)
H51A0.85990.16900.52730.060*
H51B0.86680.30040.42680.060*
C521.0196 (7)0.1826 (5)0.4111 (7)0.0556 (12)
N531.1398 (6)0.1492 (5)0.4054 (8)0.084 (2)
C60.6231 (5)0.1299 (4)0.2705 (6)0.0397 (9)
H60.65960.06830.38010.048*
C70.4812 (5)0.1261 (3)0.1220 (6)0.0352 (8)
C710.3874 (5)0.0253 (3)0.1297 (6)0.0353 (8)
C720.4376 (6)0.0728 (4)0.2855 (6)0.0444 (10)
H720.53180.07540.38790.053*
C730.3483 (6)0.1675 (4)0.2903 (6)0.0467 (10)
H730.38380.23330.39470.056*
C740.2074 (6)0.1626 (4)0.1392 (6)0.0412 (9)
C750.1566 (6)0.0668 (4)0.0179 (6)0.0449 (10)
H750.06230.06440.11990.054*
C760.2483 (6)0.0266 (4)0.0221 (6)0.0444 (10)
H760.21550.09060.12840.053*
N80.4227 (4)0.2154 (3)0.0368 (5)0.0354 (7)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Br0.0632 (3)0.0492 (3)0.0733 (4)0.0251 (2)0.0380 (3)0.0292 (2)
C1A0.038 (2)0.031 (2)0.037 (2)0.004 (2)0.017 (2)0.012 (2)
N10.041 (2)0.035 (2)0.037 (2)0.0084 (15)0.013 (2)0.0072 (15)
C110.058 (3)0.052 (3)0.036 (2)0.015 (2)0.008 (2)0.003 (2)
C20.047 (2)0.036 (2)0.046 (3)0.011 (2)0.024 (2)0.014 (2)
O210.072 (2)0.042 (2)0.056 (2)0.013 (2)0.021 (2)0.001 (2)
N30.043 (2)0.035 (2)0.054 (2)0.011 (2)0.026 (2)0.016 (2)
C310.060 (3)0.042 (2)0.070 (3)0.023 (2)0.035 (3)0.022 (2)
C40.038 (2)0.044 (2)0.050 (3)0.009 (2)0.022 (2)0.022 (2)
O410.051 (2)0.060 (2)0.063 (2)0.024 (2)0.019 (2)0.029 (2)
C4A0.034 (2)0.037 (2)0.040 (2)0.009 (2)0.018 (2)0.017 (2)
C50.038 (2)0.044 (2)0.037 (2)0.008 (2)0.016 (2)0.018 (2)
C510.049 (3)0.057 (3)0.038 (2)0.010 (2)0.012 (2)0.017 (2)
C520.044 (3)0.061 (3)0.041 (3)0.009 (2)0.003 (2)0.011 (2)
N530.041 (3)0.102 (4)0.085 (4)0.001 (3)0.012 (3)0.025 (3)
C60.040 (2)0.038 (2)0.035 (2)0.005 (2)0.015 (2)0.006 (2)
C70.034 (2)0.034 (2)0.039 (2)0.005 (2)0.018 (2)0.011 (2)
C710.034 (2)0.034 (2)0.038 (2)0.006 (2)0.016 (2)0.011 (2)
C720.041 (2)0.041 (2)0.039 (2)0.006 (2)0.013 (2)0.004 (2)
C730.052 (3)0.037 (2)0.045 (3)0.007 (2)0.021 (2)0.005 (2)
C740.045 (2)0.039 (2)0.050 (3)0.009 (2)0.027 (2)0.020 (2)
C750.042 (2)0.048 (2)0.040 (2)0.007 (2)0.012 (2)0.016 (2)
C760.048 (2)0.042 (2)0.038 (2)0.005 (2)0.016 (2)0.010 (2)
N80.034 (2)0.034 (2)0.035 (2)0.0064 (14)0.0137 (15)0.0104 (14)
Geometric parameters (Å, º) top
Br—C741.885 (4)C5—C61.374 (6)
C1A—N81.323 (5)C5—C511.525 (6)
C1A—N11.395 (5)C51—C521.458 (7)
C1A—C4A1.411 (6)C52—N531.140 (7)
N1—C21.361 (5)C6—C71.402 (6)
N1—C111.470 (6)C7—N81.345 (5)
C2—O211.220 (5)C7—C711.481 (5)
C2—N31.395 (6)C71—C761.387 (6)
N3—C41.387 (6)C71—C721.388 (6)
N3—C311.463 (5)C72—C731.398 (6)
C4—O411.228 (5)C73—C741.379 (7)
C4—C4A1.462 (6)C74—C751.380 (6)
C4A—C51.406 (6)C75—C761.397 (6)
N8—C1A—N1116.1 (4)C6—C5—C51118.3 (4)
N8—C1A—C4A124.9 (4)C4A—C5—C51122.7 (4)
N1—C1A—C4A119.0 (4)C52—C51—C5111.0 (4)
C2—N1—C1A123.3 (4)N53—C52—C51178.4 (6)
C2—N1—C11117.9 (3)C5—C6—C7120.5 (4)
C1A—N1—C11118.8 (3)N8—C7—C6121.0 (4)
O21—C2—N1122.3 (4)N8—C7—C71116.3 (4)
O21—C2—N3120.7 (4)C6—C7—C71122.7 (4)
N1—C2—N3116.9 (4)C76—C71—C72118.6 (4)
C4—N3—C2125.4 (4)C76—C71—C7119.9 (4)
C4—N3—C31117.3 (4)C72—C71—C7121.5 (4)
C2—N3—C31117.2 (4)C71—C72—C73120.7 (4)
O41—C4—N3119.8 (4)C74—C73—C72119.6 (4)
O41—C4—C4A124.8 (4)C73—C74—C75120.7 (4)
N3—C4—C4A115.4 (4)C73—C74—Br119.3 (3)
C5—C4A—C1A116.1 (4)C75—C74—Br120.1 (3)
C5—C4A—C4123.9 (4)C74—C75—C76119.3 (4)
C1A—C4A—C4119.9 (4)C71—C76—C75121.0 (4)
C6—C5—C4A119.1 (4)C1A—N8—C7118.3 (3)
N8—C1A—N1—C2179.0 (4)C4—C4A—C5—C510.8 (6)
C4A—C1A—N1—C21.0 (6)C6—C5—C51—C5298.7 (5)
N8—C1A—N1—C111.9 (6)C4A—C5—C51—C5281.0 (5)
C4A—C1A—N1—C11178.0 (4)C4A—C5—C6—C71.4 (6)
C1A—N1—C2—O21176.7 (4)C51—C5—C6—C7178.3 (4)
C11—N1—C2—O212.4 (7)C5—C6—C7—N81.9 (6)
C1A—N1—C2—N30.6 (6)C5—C6—C7—C71178.3 (4)
C11—N1—C2—N3179.7 (4)N8—C7—C71—C760.4 (6)
O21—C2—N3—C4176.6 (4)C6—C7—C71—C76179.8 (4)
N1—C2—N3—C40.7 (6)N8—C7—C71—C72179.0 (4)
O21—C2—N3—C317.4 (6)C6—C7—C71—C721.2 (6)
N1—C2—N3—C31175.3 (4)C76—C71—C72—C731.0 (7)
C2—N3—C4—O41179.7 (4)C7—C71—C72—C73179.6 (4)
C31—N3—C4—O413.7 (6)C71—C72—C73—C740.9 (7)
C2—N3—C4—C4A0.7 (6)C72—C73—C74—C751.8 (7)
C31—N3—C4—C4A176.7 (4)C72—C73—C74—Br178.1 (3)
N8—C1A—C4A—C51.5 (6)C73—C74—C75—C760.8 (7)
N1—C1A—C4A—C5178.4 (4)Br—C74—C75—C76179.2 (3)
N8—C1A—C4A—C4177.6 (4)C72—C71—C76—C752.0 (7)
N1—C1A—C4A—C42.5 (6)C7—C71—C76—C75179.4 (4)
O41—C4—C4A—C50.8 (7)C74—C75—C76—C711.1 (7)
N3—C4—C4A—C5178.7 (4)N1—C1A—N8—C7178.8 (3)
O41—C4—C4A—C1A178.1 (4)C4A—C1A—N8—C71.1 (6)
N3—C4—C4A—C1A2.3 (6)C6—C7—N8—C1A0.6 (6)
C1A—C4A—C5—C60.2 (6)C71—C7—N8—C1A179.5 (3)
C4—C4A—C5—C6178.8 (4)C52—N53—H75i—C75i36
C1A—C4A—C5—C51179.8 (4)
Symmetry code: (i) x+1, y, z.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C31—H31B···Brii0.963.073.701 (5)125
C31—H31B···N8iii0.962.813.639 (6)145
C31—H31C···O41iv0.962.663.600 (6)166
C6—H6···N53v0.932.763.565 (7)146
C72—H72···N53v0.932.653.476 (7)148
C73—H73···O21vi0.932.323.223 (6)165
Symmetry codes: (ii) x+1, y1, z; (iii) x+1, y1, z; (iv) x+2, y1, z; (v) x+2, y, z+1; (vi) x, y+1, z+1.

Experimental details

Crystal data
Chemical formulaC17H13BrN4O2
Mr385.22
Crystal system, space groupTriclinic, P1
Temperature (K)296
a, b, c (Å)8.728 (3), 12.087 (4), 8.672 (3)
α, β, γ (°)108.22 (3), 113.43 (2), 91.24 (3)
V3)786.1 (5)
Z2
Radiation typeMo Kα
µ (mm1)2.63
Crystal size (mm)0.4 × 0.3 × 0.1
Data collection
DiffractometerRigaku AFC-5R
diffractometer
Absorption correctionEmpirical (using intensity measurements)
(TEXSAN; Molecular Structure Corporation/Rigaku Corporation, 1998)
Tmin, Tmax0.509, 0.769
No. of measured, independent and
observed [I > 2σ(I)] reflections
3619, 3619, 2254
Rint0.000
(sin θ/λ)max1)0.649
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.043, 0.120, 1.03
No. of reflections3616
No. of parameters219
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.48, 0.43

Computer programs: Rigaku/AFC Diffractometer Control Software (Rigaku, 1995), Rigaku/AFC Diffractometer Control Software, TEXSAN (Molecular Structure Corporation/Rigaku Corporation, 1998), SHELXS86 (Sheldrick, 1990), SHELXL93 (Sheldrick, 1993), NRCVAX (Gabe et al.,, 1989), SHELXL93.

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C31—H31B···Bri0.963.073.701 (5)125
C31—H31B···N8ii0.962.813.639 (6)145
C31—H31C···O41iii0.962.663.600 (6)166
C6—H6···N53iv0.932.763.565 (7)146
C72—H72···N53iv0.932.653.476 (7)148
C73—H73···O21v0.932.323.223 (6)165
Symmetry codes: (i) x+1, y1, z; (ii) x+1, y1, z; (iii) x+2, y1, z; (iv) x+2, y, z+1; (v) x, y+1, z+1.
 

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