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The non-H atoms of the title mol­ecule, C10H8BrNO, are essentially coplanar. In the crystal structure, mol­ecules are linked by weak inter­molecular C—H...π(arene) inter­actions, forming one-dimensional chains along the a axis.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536808014591/pv2082sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536808014591/pv2082Isup2.hkl
Contains datablock I

CCDC reference: 690990

Key indicators

  • Single-crystal X-ray study
  • T = 150 K
  • Mean [sigma](C-C) = 0.004 Å
  • R factor = 0.028
  • wR factor = 0.060
  • Data-to-parameter ratio = 16.9

checkCIF/PLATON results

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Alert level G REFLT03_ALERT_4_G Please check that the estimate of the number of Friedel pairs is correct. If it is not, please give the correct count in the _publ_section_exptl_refinement section of the submitted CIF. From the CIF: _diffrn_reflns_theta_max 27.46 From the CIF: _reflns_number_total 2026 Count of symmetry unique reflns 1217 Completeness (_total/calc) 166.47% TEST3: Check Friedels for noncentro structure Estimate of Friedel pairs measured 809 Fraction of Friedel pairs measured 0.665 Are heavy atom types Z>Si present yes
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 0 ALERT level C = Check and explain 1 ALERT level G = General alerts; check 0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 0 ALERT type 2 Indicator that the structure model may be wrong or deficient 0 ALERT type 3 Indicator that the structure quality may be low 1 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check

Comment top

Quinoline derivatatives are established chelating agents and also have applications as precursors for pesticides and pharmaceuticals (Michael, 2008). Our laboratories are pursuing the development of radiohalogenated 8-hydroxyquinoline derivatives for positron emission tomography (PET) and single photon emission computed tomography (SPECT), specifically to image extracellular glial deposition of amyloid plaque protein in Alzheimer's disease and matrix metalloproteinases in tumours (Kulkarni et al., 2006). 4-Bromo-8-methoxyquinoline, first reported by Irving & Pinnington (1957) may be used as a precursor for radiohalogenation reactions to prepare labelled 8-hydroxyquinoline-based PET or SPECT radiopharmaceuticals. To our surprise, neutral compounds bearing a 4-halogen substituted, 8-phenoxyquinoline core have not yet been studied by single-crystal X-ray crystallography. In the present study we report the crystal structure of the title compound at 150 K.

The non-hydrogen atoms of title molecule (Fig. 1), C10H8BrNO, are essentially co-planar (r.m.s. deviation of all non-H atoms = 0.0242 Å). In the crystal structure, molecules are linked by weak intermolecuar C—H···π(arene) interactions to form one-dimensional chains along the a axis (Fig. 2). There are no other hydrogen bonds or π···π stacking interactions.

Related literature top

For related literature, see: Michael (2008); Kulkarni et al. (2006); Irving & Pinnington (1957). Cg is the centroid of the C4–C9 ring.

Experimental top

X-ray quality crystals were obtained by evaporation of a solution of the title compound (ECA International Corporation, Palatine, Illinois, USA) in chloroform.

Refinement top

H atoms were placed in calculated positions with C—H = 0.95Å (aryl) and 0.98Å (methyl) and were included in the refinement in the riding-model approximation with Uiso(H) = 1.2Ueq(C) or Uiso(H) = 1.5Ueq(C) for methyl H atoms.

Computing details top

Data collection: COLLECT (Nonius, 2002); cell refinement: DENZO-SMN (Otwinowski & Minor, 1997); data reduction: DENZO-SMN (Otwinowski & Minor, 1997); program(s) used to solve structure: SIR92 (Altomare et al., 1994); program(s) used to refine structure: SHELXTL (Sheldrick, 2008); molecular graphics: PLATON (Spek, 2003) and SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).

Figures top
[Figure 1] Fig. 1. Molecular structure showing 30% probability displacement ellipsoids (arbitrary spheres for H atoms).
[Figure 2] Fig. 2. Part of the crystal structure showing weak C—H···π(arene) interactions as dashed lines.
4-Bromo-8-methoxyquinoline top
Crystal data top
C10H8BrNOF(000) = 472
Mr = 238.08Dx = 1.773 Mg m3
Orthorhombic, P212121Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2ac 2abCell parameters from 6134 reflections
a = 5.1615 (1) Åθ = 2.9–27.5°
b = 12.1337 (6) ŵ = 4.56 mm1
c = 14.2436 (7) ÅT = 150 K
V = 892.05 (6) Å3Needle, colourless
Z = 40.30 × 0.12 × 0.11 mm
Data collection top
Nonius KappaCCD
diffractometer
2026 independent reflections
Radiation source: fine-focus sealed tube1872 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.036
Detector resolution: 9 pixels mm-1θmax = 27.5°, θmin = 2.9°
ϕ scans and ω scans with κ offsetsh = 56
Absorption correction: multi-scan
(SORTAV; Blessing 1995)
k = 1415
Tmin = 0.545, Tmax = 0.607l = 1818
6134 measured reflections
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.028 w = 1/[σ2(Fo2) + (0.0306P)2 + 0.0333P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.059(Δ/σ)max = 0.001
S = 1.01Δρmax = 0.38 e Å3
2026 reflectionsΔρmin = 0.40 e Å3
120 parametersExtinction correction: SHELXTL (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraintsExtinction coefficient: 0.0062 (8)
Primary atom site location: structure-invariant direct methodsAbsolute structure: Flack (1983), 815 Friedel pairs
Secondary atom site location: difference Fourier mapAbsolute structure parameter: 0.017 (11)
Crystal data top
C10H8BrNOV = 892.05 (6) Å3
Mr = 238.08Z = 4
Orthorhombic, P212121Mo Kα radiation
a = 5.1615 (1) ŵ = 4.56 mm1
b = 12.1337 (6) ÅT = 150 K
c = 14.2436 (7) Å0.30 × 0.12 × 0.11 mm
Data collection top
Nonius KappaCCD
diffractometer
2026 independent reflections
Absorption correction: multi-scan
(SORTAV; Blessing 1995)
1872 reflections with I > 2σ(I)
Tmin = 0.545, Tmax = 0.607Rint = 0.036
6134 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.028H-atom parameters constrained
wR(F2) = 0.059Δρmax = 0.38 e Å3
S = 1.01Δρmin = 0.40 e Å3
2026 reflectionsAbsolute structure: Flack (1983), 815 Friedel pairs
120 parametersAbsolute structure parameter: 0.017 (11)
0 restraints
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 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*/Ueq
Br11.02034 (5)0.36147 (2)0.509948 (18)0.02940 (11)
O10.1007 (3)0.62674 (16)0.72708 (14)0.0259 (4)
N10.4260 (4)0.64140 (17)0.58326 (14)0.0233 (4)
C10.5884 (5)0.6481 (2)0.51287 (18)0.0278 (6)
H1A0.58190.71260.47520.033*
C20.7717 (5)0.5671 (2)0.48878 (19)0.0268 (6)
H2A0.88420.57680.43660.032*
C30.7833 (5)0.4746 (2)0.54217 (19)0.0239 (6)
C40.6190 (5)0.4611 (2)0.62176 (17)0.0188 (5)
C50.6239 (5)0.3694 (2)0.68244 (18)0.0232 (6)
H5A0.74290.31090.67180.028*
C60.4556 (5)0.3650 (2)0.75705 (17)0.0243 (6)
H6A0.46240.30380.79860.029*
C70.2739 (5)0.4487 (2)0.77325 (18)0.0235 (6)
H7A0.15580.44240.82410.028*
C80.2656 (5)0.5400 (2)0.71586 (17)0.0195 (5)
C90.4408 (5)0.54916 (19)0.63810 (16)0.0199 (5)
C100.0731 (5)0.6201 (2)0.80535 (18)0.0271 (7)
H10C0.17840.68720.80830.041*
H10D0.02690.61260.86350.041*
H10A0.18650.55590.79780.041*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Br10.02472 (15)0.03108 (16)0.03239 (16)0.00303 (10)0.00306 (11)0.00756 (11)
O10.0264 (10)0.0255 (11)0.0259 (10)0.0030 (8)0.0047 (7)0.0004 (8)
N10.0281 (10)0.0212 (11)0.0206 (11)0.0009 (9)0.0021 (8)0.0001 (10)
C10.0339 (13)0.0259 (14)0.0237 (14)0.0019 (10)0.0030 (10)0.0087 (14)
C20.0265 (12)0.0299 (14)0.0240 (14)0.0065 (10)0.0049 (12)0.0001 (13)
C30.0215 (13)0.0257 (14)0.0246 (15)0.0015 (10)0.0025 (10)0.0078 (12)
C40.0210 (13)0.0184 (13)0.0169 (13)0.0037 (9)0.0018 (9)0.0016 (11)
C50.0224 (12)0.0215 (14)0.0257 (14)0.0016 (11)0.0064 (10)0.0019 (12)
C60.0328 (15)0.0176 (13)0.0225 (13)0.0037 (13)0.0074 (11)0.0035 (11)
C70.0257 (14)0.0258 (15)0.0191 (14)0.0088 (11)0.0018 (11)0.0010 (11)
C80.0208 (13)0.0185 (13)0.0193 (13)0.0003 (10)0.0021 (10)0.0014 (11)
C90.0207 (12)0.0204 (13)0.0186 (12)0.0042 (10)0.0046 (10)0.0010 (10)
C100.0240 (14)0.0314 (17)0.0258 (15)0.0015 (12)0.0047 (11)0.0028 (12)
Geometric parameters (Å, º) top
Br1—C31.895 (2)C4—C91.429 (3)
O1—C81.362 (3)C5—C61.374 (4)
O1—C101.433 (3)C5—H5A0.9500
N1—C11.309 (3)C6—C71.402 (4)
N1—C91.367 (3)C6—H6A0.9500
C1—C21.407 (4)C7—C81.378 (4)
C1—H1A0.9500C7—H7A0.9500
C2—C31.357 (3)C8—C91.434 (3)
C2—H2A0.9500C10—H10C0.9800
C3—C41.425 (3)C10—H10D0.9800
C4—C51.409 (4)C10—H10A0.9800
C8—O1—C10116.0 (2)C5—C6—H6A119.3
C1—N1—C9116.9 (2)C7—C6—H6A119.3
N1—C1—C2125.0 (2)C8—C7—C6120.4 (2)
N1—C1—H1A117.5C8—C7—H7A119.8
C2—C1—H1A117.5C6—C7—H7A119.8
C3—C2—C1118.1 (2)O1—C8—C7124.8 (2)
C3—C2—H2A121.0O1—C8—C9115.1 (2)
C1—C2—H2A121.0C7—C8—C9120.0 (2)
C2—C3—C4121.0 (2)N1—C9—C4123.7 (2)
C2—C3—Br1119.4 (2)N1—C9—C8118.0 (2)
C4—C3—Br1119.58 (19)C4—C9—C8118.3 (2)
C5—C4—C3124.6 (2)O1—C10—H10C109.5
C5—C4—C9120.1 (2)O1—C10—H10D109.5
C3—C4—C9115.3 (2)H10C—C10—H10D109.5
C6—C5—C4119.6 (3)O1—C10—H10A109.5
C6—C5—H5A120.2H10C—C10—H10A109.5
C4—C5—H5A120.2H10D—C10—H10A109.5
C5—C6—C7121.5 (2)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C10—H10A···Cgi0.982.663.531 (3)148
Symmetry code: (i) x1, y, z.

Experimental details

Crystal data
Chemical formulaC10H8BrNO
Mr238.08
Crystal system, space groupOrthorhombic, P212121
Temperature (K)150
a, b, c (Å)5.1615 (1), 12.1337 (6), 14.2436 (7)
V3)892.05 (6)
Z4
Radiation typeMo Kα
µ (mm1)4.56
Crystal size (mm)0.30 × 0.12 × 0.11
Data collection
DiffractometerNonius KappaCCD
diffractometer
Absorption correctionMulti-scan
(SORTAV; Blessing 1995)
Tmin, Tmax0.545, 0.607
No. of measured, independent and
observed [I > 2σ(I)] reflections
6134, 2026, 1872
Rint0.036
(sin θ/λ)max1)0.649
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.028, 0.059, 1.01
No. of reflections2026
No. of parameters120
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.38, 0.40
Absolute structureFlack (1983), 815 Friedel pairs
Absolute structure parameter0.017 (11)

Computer programs: COLLECT (Nonius, 2002), DENZO-SMN (Otwinowski & Minor, 1997), SIR92 (Altomare et al., 1994), PLATON (Spek, 2003) and SHELXTL (Sheldrick, 2008).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C10—H10A···Cgi0.982.663.531 (3)148
Symmetry code: (i) x1, y, z.
 

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