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In the title compound, C12H11BrN5+·Cl, the cation exists as the N3-protonated N7 tautomer. The crystal structure is stabilized by N—H...Cl hydrogen bonds, which connect cations and anions into linear chains along the [010] direction. There are also some additional π–π stacking inter­actions and weak inter­atomic contacts of the types C...Cl and C...Br.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536806042176/sg2070sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536806042176/sg2070Isup2.hkl
Contains datablock I

CCDC reference: 628391

Key indicators

  • Single-crystal X-ray study
  • T = 100 K
  • Mean [sigma](C-C)= 0.005 Å
  • R factor = 0.043
  • wR factor = 0.106
  • Data-to-parameter ratio = 13.5

checkCIF/PLATON results

No syntax errors found


No errors found in this datablock

Computing details top

Data collection: CrysAlis CCD (Oxford Diffraction, 2002); cell refinement: CrysAlis RED (Oxford Diffraction, 2002); data reduction: CrysAlis RED; program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: DIAMOND (Brandenburg, 2006); software used to prepare material for publication: SHELXL97 and DIAMOND (Brandenburg, 2006).

6-(3-Bromobenzylamino)purin-3-ium chloride top
Crystal data top
C12H11BrN5+·ClF(000) = 680
Mr = 340.62Dx = 1.719 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 2295 reflections
a = 18.823 (2) Åθ = 3.2–28.8°
b = 8.8276 (11) ŵ = 3.32 mm1
c = 7.9658 (11) ÅT = 100 K
β = 96.244 (10)°Prism, colourless
V = 1315.8 (3) Å30.35 × 0.25 × 0.20 mm
Z = 4
Data collection top
Oxford Xcalibur2
diffractometer
2316 independent reflections
Radiation source: fine-focus sealed tube2100 reflections with I > 2σ(I)
Enhance (Oxford Diffraction) monochromatorRint = 0.058
Detector resolution: 16.3 pixels mm-1θmax = 25.0°, θmin = 3.5°
rotation method, ω scansh = 2222
Absorption correction: empirical (using intensity measurements)
(Blessing, 1995)
k = 1010
Tmin = 0.360, Tmax = 0.515l = 69
6666 measured reflections
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) = 0.106H-atom parameters constrained
S = 1.04 w = 1/[σ2(Fo2) + (0.0587P)2 + 1.865P]
where P = (Fo2 + 2Fc2)/3
2316 reflections(Δ/σ)max < 0.001
172 parametersΔρmax = 0.90 e Å3
0 restraintsΔρmin = 0.67 e Å3
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
Br10.124482 (19)0.37458 (5)0.03153 (5)0.03533 (17)
N10.29147 (14)0.8093 (3)0.5937 (3)0.0163 (5)
Cl10.36705 (4)0.29997 (8)0.36066 (9)0.0185 (2)
C20.31436 (17)0.9452 (4)0.5629 (4)0.0169 (6)
H2A0.28691.02840.59550.020*
N30.37315 (13)0.9770 (3)0.4892 (3)0.0168 (6)
H3A0.38671.07110.47520.020*
C40.41108 (17)0.8590 (3)0.4369 (4)0.0152 (6)
C50.38913 (16)0.7129 (3)0.4637 (4)0.0136 (6)
N60.30568 (14)0.5500 (3)0.5842 (3)0.0167 (5)
H6A0.33290.47130.56890.020*
C60.32843 (16)0.6869 (3)0.5467 (4)0.0146 (6)
N70.43783 (14)0.6233 (3)0.3938 (3)0.0151 (6)
H7A0.43860.52370.39080.018*
C80.48413 (17)0.7183 (4)0.3308 (4)0.0179 (6)
H8A0.52320.68460.27460.022*
N90.47003 (15)0.8637 (3)0.3547 (3)0.0171 (6)
C90.23722 (17)0.5254 (4)0.6497 (4)0.0206 (7)
H9A0.23150.60070.73930.025*
H9B0.23710.42340.70130.025*
C100.17512 (17)0.5381 (3)0.5154 (4)0.0176 (6)
C110.17802 (17)0.4658 (4)0.3601 (4)0.0194 (7)
H11A0.21950.41180.33720.023*
C120.11931 (19)0.4747 (4)0.2411 (4)0.0237 (7)
C130.05811 (18)0.5522 (4)0.2679 (5)0.0281 (8)
H13A0.01830.55590.18370.034*
C140.0564 (2)0.6243 (4)0.4209 (5)0.0336 (9)
H14A0.01490.67890.44280.040*
C150.11461 (19)0.6177 (4)0.5431 (4)0.0249 (8)
H15A0.11270.66880.64750.030*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Br10.0239 (2)0.0528 (3)0.0279 (2)0.00378 (16)0.00354 (16)0.01291 (16)
N10.0172 (13)0.0159 (13)0.0148 (13)0.0013 (11)0.0029 (10)0.0028 (10)
Cl10.0249 (4)0.0110 (3)0.0199 (4)0.0019 (3)0.0031 (3)0.0019 (3)
C20.0193 (16)0.0167 (15)0.0137 (14)0.0035 (13)0.0019 (12)0.0022 (12)
N30.0226 (14)0.0102 (12)0.0165 (13)0.0001 (10)0.0026 (11)0.0013 (10)
C40.0176 (16)0.0144 (15)0.0120 (14)0.0000 (12)0.0059 (12)0.0003 (11)
C50.0146 (15)0.0123 (14)0.0126 (15)0.0004 (12)0.0044 (11)0.0006 (11)
N60.0188 (13)0.0136 (12)0.0174 (13)0.0017 (11)0.0004 (10)0.0006 (10)
C60.0187 (16)0.0150 (14)0.0090 (14)0.0004 (13)0.0042 (11)0.0011 (11)
N70.0176 (14)0.0116 (12)0.0155 (13)0.0008 (10)0.0013 (10)0.0000 (9)
C80.0155 (15)0.0196 (15)0.0178 (15)0.0009 (13)0.0022 (12)0.0011 (12)
N90.0182 (14)0.0150 (13)0.0173 (13)0.0019 (10)0.0017 (11)0.0008 (10)
C90.0244 (17)0.0196 (16)0.0181 (16)0.0047 (14)0.0037 (13)0.0002 (13)
C100.0178 (16)0.0153 (14)0.0207 (16)0.0045 (13)0.0064 (12)0.0028 (12)
C110.0153 (16)0.0182 (15)0.0252 (17)0.0007 (13)0.0046 (13)0.0011 (13)
C120.0234 (17)0.0216 (16)0.0254 (17)0.0034 (14)0.0000 (13)0.0008 (14)
C130.0173 (17)0.0321 (19)0.0340 (19)0.0006 (15)0.0011 (14)0.0055 (16)
C140.023 (2)0.032 (2)0.047 (2)0.0087 (15)0.0086 (17)0.0001 (17)
C150.0253 (19)0.0218 (17)0.0286 (19)0.0016 (14)0.0076 (15)0.0048 (13)
Geometric parameters (Å, º) top
Br1—C121.901 (3)C8—N91.329 (4)
N1—C21.307 (4)C8—H8A0.9500
N1—C61.360 (4)C9—C101.501 (4)
C2—N31.337 (4)C9—H9A0.9900
C2—H2A0.9500C9—H9B0.9900
N3—C41.354 (4)C10—C151.376 (5)
N3—H3A0.8800C10—C111.398 (5)
C4—N91.349 (4)C11—C121.378 (5)
C4—C51.377 (4)C11—H11A0.9500
C5—N71.374 (4)C12—C131.376 (5)
C5—C61.400 (4)C13—C141.378 (6)
N6—C61.327 (4)C13—H13A0.9500
N6—C91.458 (4)C14—C151.386 (5)
N6—H6A0.8800C14—H14A0.9500
N7—C81.345 (4)C15—H15A0.9500
N7—H7A0.8800
C2—N1—C6119.3 (3)C8—N9—C4103.1 (3)
N1—C2—N3125.5 (3)N6—C9—C10112.6 (2)
N1—C2—H2A117.3N6—C9—H9A109.1
N3—C2—H2A117.3C10—C9—H9A109.1
C2—N3—C4117.6 (3)N6—C9—H9B109.1
C2—N3—H3A121.2C10—C9—H9B109.1
C4—N3—H3A121.2H9A—C9—H9B107.8
N3—C4—N9127.9 (3)C15—C10—C11119.2 (3)
N3—C4—C5119.7 (3)C15—C10—C9121.2 (3)
N9—C4—C5112.4 (3)C11—C10—C9119.6 (3)
N7—C5—C4104.6 (3)C12—C11—C10118.5 (3)
N7—C5—C6135.4 (3)C12—C11—H11A120.7
C4—C5—C6120.0 (3)C10—C11—H11A120.7
C6—N6—C9122.4 (3)C11—C12—C13122.9 (3)
C6—N6—H6A118.8C11—C12—Br1117.7 (3)
C9—N6—H6A118.8C13—C12—Br1119.4 (3)
N6—C6—N1118.3 (3)C14—C13—C12117.9 (3)
N6—C6—C5123.7 (3)C14—C13—H13A121.1
N1—C6—C5117.9 (3)C12—C13—H13A121.1
C8—N7—C5106.3 (2)C13—C14—C15120.6 (3)
C8—N7—H7A126.9C13—C14—H14A119.7
C5—N7—H7A126.9C15—C14—H14A119.7
N9—C8—N7113.7 (3)C10—C15—C14120.9 (3)
N9—C8—H8A123.2C10—C15—H15A119.5
N7—C8—H8A123.2C14—C15—H15A119.5
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N3—H3A···Cl1i0.882.233.028 (3)150
N6—H6A···Cl10.882.383.134 (3)143
N7—H7A···Cl10.882.393.149 (3)145
Symmetry code: (i) x, y+1, z.
 

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