Buy article online - an online subscription or single-article purchase is required to access this article.
Download citation
Download citation
link to html
The title compound, C9H8BrN3O2, crystallizes with two almost identical mol­ecules in the asymmetric unit. The crystal packing is stabilized by N—H...N hydrogen bonds and π–π stacking inter­actions.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536806035689/sg2054sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536806035689/sg2054Isup2.hkl
Contains datablock I

CCDC reference: 624974

Key indicators

  • Single-crystal X-ray study
  • T = 173 K
  • Mean [sigma](C-C) = 0.010 Å
  • R factor = 0.073
  • wR factor = 0.220
  • Data-to-parameter ratio = 13.3

checkCIF/PLATON results

No syntax errors found



Alert level C PLAT220_ALERT_2_C Large Non-Solvent C Ueq(max)/Ueq(min) ... 3.37 Ratio PLAT222_ALERT_3_C Large Non-Solvent H Ueq(max)/Ueq(min) ... 3.48 Ratio PLAT341_ALERT_3_C Low Bond Precision on C-C bonds (x 1000) Ang ... 10 PLAT431_ALERT_2_C Short Inter HL..A Contact Br1A .. Br1A .. 3.54 Ang. PLAT432_ALERT_2_C Short Inter X...Y Contact C2A .. C14A .. 3.17 Ang. PLAT720_ALERT_4_C Number of Unusual/Non-Standard Label(s) ........ 2
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 6 ALERT level C = Check and explain 0 ALERT level G = General alerts; check 0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 3 ALERT type 2 Indicator that the structure model may be wrong or deficient 2 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

Computing details top

Data collection: X-AREA (Stoe & Cie, 2001); cell refinement: X-AREA; data reduction: X-AREA; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: XP in SHELXTL-Plus (Sheldrick, 1991); software used to prepare material for publication: SHELXL97.

5-(2-Bromo-5-methoxyphenyl)-1,3,4-oxadiazol-2-amine top
Crystal data top
C9H8BrN3O2F(000) = 1072
Mr = 270.09Dx = 1.729 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 9913 reflections
a = 18.1501 (19) Åθ = 3.6–25.2°
b = 10.3513 (7) ŵ = 3.94 mm1
c = 11.0955 (10) ÅT = 173 K
β = 95.298 (8)°Plate, colourless
V = 2075.7 (3) Å30.47 × 0.36 × 0.21 mm
Z = 8
Data collection top
Stoe IPDS II two-circle
diffractometer
3644 independent reflections
Radiation source: fine-focus sealed tube2876 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.079
ω scansθmax = 25.0°, θmin = 3.6°
Absorption correction: multi-scan
(MULABS; Spek, 2003; Blessing, 1995)
h = 1821
Tmin = 0.215, Tmax = 0.441k = 1212
10488 measured reflectionsl = 1313
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.073H-atom parameters constrained
wR(F2) = 0.220 w = 1/[σ2(Fo2) + (0.1458P)2 + 1.2938P]
where P = (Fo2 + 2Fc2)/3
S = 1.05(Δ/σ)max < 0.001
3644 reflectionsΔρmax = 1.77 e Å3
274 parametersΔρmin = 1.42 e Å3
0 restraintsExtinction correction: SHELXL97 (Sheldrick, 1997), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.021 (2)
Special details top

Experimental. Analysis for C9H8BrN3O2, found (calculated): C 40 (40.04), H 2.89 (2.99), N 15.36 (15.56)%. Spectroscopic analysis: 1H NMR (300 MHz, CDCl3, δ, p.p.m.): 3.84 (s, 3H, –OCH3), 5.16 (s, 2H, –NH2), 6.88 (dd, J = 6.7 Hz, 1H, ArH), 7.36 (d, J = 2.28 Hz, 1H, ArH), 7.59 (d, J = 6.7 Hz, 1H, ArH); FAB-MS: m/z 270 (100%, M+), m/z 271 (50%, M+1), m/z 272 (98%, M+2).

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
Br10.51499 (5)0.47549 (8)0.17728 (7)0.0398 (4)
C10.5573 (4)0.6682 (6)0.4087 (5)0.0205 (14)
O10.5742 (3)0.7368 (4)0.5157 (4)0.0204 (10)
C20.6471 (5)0.7659 (7)0.5122 (6)0.0267 (16)
N10.6142 (4)0.6600 (6)0.3468 (5)0.0255 (13)
N20.6739 (3)0.7235 (6)0.4141 (5)0.0254 (13)
N30.6819 (4)0.8321 (7)0.6037 (5)0.0321 (15)
H3A0.72890.85240.60230.039*
H3B0.65780.85550.66540.039*
C110.4818 (4)0.6210 (6)0.3897 (5)0.0203 (14)
C120.4303 (4)0.6621 (6)0.4717 (6)0.0215 (14)
H120.44600.72180.53390.026*
C130.3597 (4)0.6183 (6)0.4632 (6)0.0263 (15)
C140.3343 (5)0.5289 (7)0.3730 (7)0.0297 (16)
H140.28490.49710.36750.036*
C150.3838 (5)0.4888 (6)0.2927 (7)0.0284 (16)
H150.36780.42740.23220.034*
C160.4551 (4)0.5343 (6)0.2972 (6)0.0223 (14)
O170.3070 (3)0.6564 (5)0.5375 (5)0.0357 (13)
C170.3289 (5)0.7586 (8)0.6231 (7)0.041 (2)
H17A0.36860.72730.68170.062*
H17B0.28630.78420.66590.062*
H17C0.34660.83320.57960.062*
Br1A0.99274 (5)0.49736 (7)0.65777 (6)0.0360 (4)
C1A1.0400 (4)0.3329 (6)0.9065 (5)0.0226 (15)
O1A1.0575 (3)0.2699 (4)1.0167 (4)0.0203 (10)
C2A1.1293 (4)0.2357 (6)1.0099 (5)0.0200 (14)
N1A1.0954 (4)0.3361 (5)0.8424 (5)0.0244 (13)
N2A1.1549 (3)0.2720 (5)0.9092 (5)0.0228 (12)
N3A1.1640 (4)0.1696 (6)1.1024 (5)0.0270 (13)
H3A11.21030.14521.09940.032*
H3A21.14060.15071.16610.032*
C11A0.9651 (5)0.3856 (6)0.8901 (6)0.0260 (16)
C12A0.9172 (4)0.3643 (6)0.9829 (6)0.0239 (15)
H12A0.93360.31111.04980.029*
C13A0.8485 (4)0.4180 (7)0.9782 (6)0.0282 (16)
C14A0.8216 (5)0.4928 (7)0.8771 (7)0.0295 (16)
H14A0.77340.52940.87270.035*
C15A0.8662 (5)0.5116 (6)0.7854 (6)0.0274 (17)
H15A0.84830.56130.71690.033*
C16A0.9366 (4)0.4601 (6)0.7902 (6)0.0236 (15)
O17A0.7997 (3)0.4066 (6)1.0652 (5)0.0391 (14)
C17A0.8242 (6)0.3319 (13)1.1703 (9)0.068 (3)
H17D0.83300.24251.14630.101*
H17E0.78610.33341.22750.101*
H17F0.87020.36881.20900.101*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Br10.0523 (7)0.0372 (5)0.0319 (5)0.0113 (4)0.0139 (4)0.0169 (3)
C10.028 (4)0.017 (3)0.018 (3)0.002 (3)0.004 (3)0.002 (2)
O10.024 (3)0.024 (2)0.015 (2)0.001 (2)0.0046 (17)0.0004 (16)
C20.038 (5)0.026 (3)0.017 (3)0.000 (3)0.007 (3)0.005 (3)
N10.028 (4)0.031 (3)0.018 (3)0.000 (3)0.006 (2)0.001 (2)
N20.023 (3)0.035 (3)0.018 (3)0.005 (3)0.005 (2)0.002 (2)
N30.021 (3)0.050 (4)0.027 (3)0.016 (3)0.008 (2)0.013 (3)
C110.025 (4)0.019 (3)0.018 (3)0.001 (3)0.005 (3)0.003 (2)
C120.020 (4)0.020 (3)0.024 (3)0.003 (3)0.002 (3)0.003 (2)
C130.026 (4)0.022 (3)0.032 (3)0.001 (3)0.010 (3)0.001 (3)
C140.032 (5)0.022 (3)0.034 (4)0.005 (3)0.002 (3)0.008 (3)
C150.032 (5)0.019 (3)0.032 (4)0.005 (3)0.006 (3)0.002 (3)
C160.030 (4)0.017 (3)0.020 (3)0.001 (3)0.005 (3)0.002 (2)
O170.021 (3)0.039 (3)0.048 (3)0.001 (2)0.009 (2)0.008 (2)
C170.047 (6)0.038 (4)0.041 (4)0.002 (4)0.014 (4)0.014 (3)
Br1A0.0476 (6)0.0419 (5)0.0202 (4)0.0179 (4)0.0126 (3)0.0108 (3)
C1A0.039 (4)0.016 (3)0.012 (3)0.001 (3)0.002 (3)0.001 (2)
O1A0.023 (3)0.022 (2)0.017 (2)0.002 (2)0.0069 (17)0.0016 (17)
C2A0.029 (4)0.017 (3)0.015 (3)0.001 (3)0.004 (2)0.002 (2)
N1A0.033 (4)0.025 (3)0.017 (3)0.001 (3)0.011 (2)0.002 (2)
N2A0.023 (3)0.026 (3)0.020 (3)0.003 (2)0.006 (2)0.002 (2)
N3A0.029 (4)0.032 (3)0.020 (3)0.006 (3)0.007 (2)0.005 (2)
C11A0.046 (5)0.014 (3)0.019 (3)0.005 (3)0.009 (3)0.003 (2)
C12A0.020 (4)0.023 (3)0.029 (3)0.001 (3)0.003 (3)0.007 (3)
C13A0.024 (4)0.029 (4)0.032 (4)0.003 (3)0.006 (3)0.005 (3)
C14A0.027 (4)0.024 (3)0.037 (4)0.001 (3)0.002 (3)0.001 (3)
C15A0.043 (5)0.016 (3)0.023 (3)0.000 (3)0.001 (3)0.003 (2)
C16A0.033 (4)0.019 (3)0.020 (3)0.006 (3)0.008 (3)0.002 (2)
O17A0.024 (3)0.052 (3)0.043 (3)0.008 (3)0.014 (2)0.021 (3)
C17A0.048 (6)0.106 (9)0.053 (6)0.013 (6)0.026 (5)0.043 (6)
Geometric parameters (Å, º) top
Br1—C161.895 (7)Br1A—C16A1.903 (7)
C1—N11.295 (9)C1A—N1A1.283 (9)
C1—O11.393 (7)C1A—O1A1.396 (7)
C1—C111.452 (10)C1A—C11A1.460 (11)
O1—C21.361 (9)O1A—C2A1.359 (8)
C2—N21.308 (9)C2A—N2A1.304 (8)
C2—N31.334 (9)C2A—N3A1.342 (8)
N1—N21.420 (9)N1A—N2A1.418 (8)
N3—H3A0.8800N3A—H3A10.8800
N3—H3B0.8800N3A—H3A20.8800
C11—C161.414 (9)C11A—C16A1.408 (9)
C11—C121.429 (9)C11A—C12A1.425 (10)
C12—C131.354 (10)C12A—C13A1.362 (11)
C12—H120.9500C12A—H12A0.9500
C13—O171.376 (9)C13A—O17A1.375 (9)
C13—C141.409 (10)C13A—C14A1.413 (10)
C14—C151.386 (12)C14A—C15A1.371 (11)
C14—H140.9500C14A—H14A0.9500
C15—C161.374 (11)C15A—C16A1.382 (11)
C15—H150.9500C15A—H15A0.9500
O17—C171.453 (9)O17A—C17A1.436 (10)
C17—H17A0.9800C17A—H17D0.9800
C17—H17B0.9800C17A—H17E0.9800
C17—H17C0.9800C17A—H17F0.9800
N1—C1—O1111.2 (6)N1A—C1A—O1A111.8 (6)
N1—C1—C11133.5 (6)N1A—C1A—C11A133.5 (6)
O1—C1—C11115.3 (6)O1A—C1A—C11A114.7 (6)
C2—O1—C1103.1 (5)C2A—O1A—C1A102.4 (5)
N2—C2—N3128.3 (7)N2A—C2A—N3A128.5 (7)
N2—C2—O1112.8 (6)N2A—C2A—O1A113.1 (6)
N3—C2—O1119.0 (6)N3A—C2A—O1A118.4 (6)
C1—N1—N2107.4 (5)C1A—N1A—N2A107.3 (5)
C2—N2—N1105.6 (6)C2A—N2A—N1A105.5 (6)
C2—N3—H3A120.0C2A—N3A—H3A1120.0
C2—N3—H3B120.0C2A—N3A—H3A2120.0
H3A—N3—H3B120.0H3A1—N3A—H3A2120.0
C16—C11—C12116.8 (7)C16A—C11A—C12A116.7 (7)
C16—C11—C1125.1 (6)C16A—C11A—C1A124.9 (6)
C12—C11—C1118.1 (6)C12A—C11A—C1A118.4 (6)
C13—C12—C11121.8 (6)C13A—C12A—C11A121.8 (6)
C13—C12—H12119.1C13A—C12A—H12A119.1
C11—C12—H12119.1C11A—C12A—H12A119.1
C12—C13—O17124.6 (6)C12A—C13A—O17A125.8 (6)
C12—C13—C14121.0 (7)C12A—C13A—C14A120.2 (7)
O17—C13—C14114.4 (7)O17A—C13A—C14A114.0 (7)
C15—C14—C13117.6 (8)C15A—C14A—C13A118.8 (8)
C15—C14—H14121.2C15A—C14A—H14A120.6
C13—C14—H14121.2C13A—C14A—H14A120.6
C16—C15—C14122.6 (7)C14A—C15A—C16A121.6 (7)
C16—C15—H15118.7C14A—C15A—H15A119.2
C14—C15—H15118.7C16A—C15A—H15A119.2
C15—C16—C11120.2 (7)C15A—C16A—C11A120.9 (7)
C15—C16—Br1117.6 (5)C15A—C16A—Br1A116.8 (5)
C11—C16—Br1122.2 (6)C11A—C16A—Br1A122.3 (6)
C13—O17—C17115.9 (6)C13A—O17A—C17A116.4 (7)
O17—C17—H17A109.5O17A—C17A—H17D109.5
O17—C17—H17B109.5O17A—C17A—H17E109.5
H17A—C17—H17B109.5H17D—C17A—H17E109.5
O17—C17—H17C109.5O17A—C17A—H17F109.5
H17A—C17—H17C109.5H17D—C17A—H17F109.5
H17B—C17—H17C109.5H17E—C17A—H17F109.5
N1—C1—O1—C21.2 (7)N1A—C1A—O1A—C2A0.4 (7)
C11—C1—O1—C2178.4 (5)C11A—C1A—O1A—C2A177.9 (5)
C1—O1—C2—N21.1 (7)C1A—O1A—C2A—N2A0.2 (7)
C1—O1—C2—N3179.6 (6)C1A—O1A—C2A—N3A178.8 (6)
O1—C1—N1—N21.0 (7)O1A—C1A—N1A—N2A0.4 (7)
C11—C1—N1—N2178.6 (6)C11A—C1A—N1A—N2A177.2 (7)
N3—C2—N2—N1179.8 (7)N3A—C2A—N2A—N1A178.9 (6)
O1—C2—N2—N10.5 (7)O1A—C2A—N2A—N1A0.0 (7)
C1—N1—N2—C20.3 (7)C1A—N1A—N2A—C2A0.2 (7)
N1—C1—C11—C168.9 (11)N1A—C1A—C11A—C16A1.1 (12)
O1—C1—C11—C16170.6 (6)O1A—C1A—C11A—C16A175.7 (6)
N1—C1—C11—C12172.5 (7)N1A—C1A—C11A—C12A179.2 (7)
O1—C1—C11—C127.9 (8)O1A—C1A—C11A—C12A2.4 (8)
C16—C11—C12—C131.4 (9)C16A—C11A—C12A—C13A3.0 (10)
C1—C11—C12—C13177.2 (6)C1A—C11A—C12A—C13A175.3 (6)
C11—C12—C13—O17178.4 (6)C11A—C12A—C13A—O17A177.6 (7)
C11—C12—C13—C140.6 (10)C11A—C12A—C13A—C14A2.8 (11)
C12—C13—C14—C150.8 (10)C12A—C13A—C14A—C15A1.0 (11)
O17—C13—C14—C15178.3 (6)O17A—C13A—C14A—C15A179.3 (6)
C13—C14—C15—C161.0 (10)C13A—C14A—C15A—C16A0.4 (11)
C14—C15—C16—C113.1 (10)C14A—C15A—C16A—C11A0.2 (10)
C14—C15—C16—Br1177.6 (5)C14A—C15A—C16A—Br1A178.7 (5)
C12—C11—C16—C153.1 (9)C12A—C11A—C16A—C15A1.5 (10)
C1—C11—C16—C15175.4 (6)C1A—C11A—C16A—C15A176.6 (6)
C12—C11—C16—Br1177.6 (5)C12A—C11A—C16A—Br1A179.7 (5)
C1—C11—C16—Br13.9 (9)C1A—C11A—C16A—Br1A2.2 (9)
C12—C13—O17—C175.3 (10)C12A—C13A—O17A—C17A0.5 (12)
C14—C13—O17—C17173.7 (6)C14A—C13A—O17A—C17A179.8 (8)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N3—H3A···N2Ai0.882.283.043 (9)145
N3—H3B···N1ii0.882.243.067 (8)158
N3A—H3A1···N2iii0.882.273.015 (9)142
N3A—H3A2···N1Aiv0.882.193.043 (8)162
Symmetry codes: (i) x+2, y+1/2, z+3/2; (ii) x, y+3/2, z+1/2; (iii) x+2, y1/2, z+3/2; (iv) x, y+1/2, z+1/2.
 

Subscribe to Acta Crystallographica Section E: Crystallographic Communications

The full text of this article is available to subscribers to the journal.

If you have already registered and are using a computer listed in your registration details, please email support@iucr.org for assistance.

Buy online

You may purchase this article in PDF and/or HTML formats. For purchasers in the European Community who do not have a VAT number, VAT will be added at the local rate. Payments to the IUCr are handled by WorldPay, who will accept payment by credit card in several currencies. To purchase the article, please complete the form below (fields marked * are required), and then click on `Continue'.
E-mail address* 
Repeat e-mail address* 
(for error checking) 

Format*   PDF (US $40)
   HTML (US $40)
   PDF+HTML (US $50)
In order for VAT to be shown for your country javascript needs to be enabled.

VAT number 
(non-UK EC countries only) 
Country* 
 

Terms and conditions of use
Contact us

Follow Acta Cryst. E
Sign up for e-alerts
Follow Acta Cryst. on Twitter
Follow us on facebook
Sign up for RSS feeds