organic compounds
Redetermination of phenylhydrazinium chloride
aDepartamento de Quimica, UFMG, Campus - Pampulha, 31270-901 Belo Horizonte, Minas Gerais, Brazil, and bDepartment of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland
*Correspondence e-mail: w.harrison@abdn.ac.uk
In the redetermined structure [Koo (1965). Bull. Chem. Soc. Jpn, 38, 286] of the title compound, C6H9N2+·Cl−, the H atoms have been located and the hydrogen-bonding scheme established. A series of N—H⋯Cl and N—H⋯N hydrogen bonds leads to a layered network parallel to the (010) plane.
Related literature
For the earlier ). For a related structure, see: Hammerl et al. (2001). For reference structural data, see: Allen et al. (1987).
see: Koo (1965Experimental
Crystal data
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Refinement
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Data collection: COLLECT (Nonius, 1998); cell SCALEPACK (Otwinowski & Minor, 1997); data reduction: DENZO (Otwinowski & Minor, 1997), SCALEPACK and SORTAV (Blessing, 1995); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 (Farrugia, 1997); software used to prepare material for publication: SHELXL97.
Supporting information
https://doi.org/10.1107/S1600536807066974/bt2663sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S1600536807066974/bt2663Isup2.hkl
The title compound was prepared by dropwise addition of concentrated hydrochloric acid (1 equivalent) to an ethanolic solution of phenylhydrazine. The product, which appreared on standing, was collected and colourless blades of (I) were recrystallized from EtOH, m.p 525–528 K (decomp).
The N-bound H atoms were located in a difference map and their positions were freely refined with the constraint Uiso(H) = 1.2Ueq(N). The C-bound H atoms were placed in calculated positions (C—H = 0.93 Å) and refined as riding with Uiso(H) = 1.2Ueq(C).
The structure of the title compound, (I), was established by Koo (1965), but no hydrogen atoms were located. The hydrogen bonding pattern in the crystal of (I) cannot be established based on geometrical placement of the H atoms because roatation of the terminal –NH3+ group leads to different plausible arrangements for the hydrogen bonds. Here, the redetermined structure of (I), including the H atom positions is presented (Fig. 1), and the hydrogen bonding scheme is definitively established.
In (I), atoms N1 and N2 deviate from the C1—C6 ring plane by -0.098 (4)Å and 0.418 (4) Å, respectively. The bond-angle sum for N1 is 331°, indicative of sp3
for this atom. Otherwise, the geometrical paramaters for (I) may be regarded as normal (Allen et al., 1987).The crystal packing for (I) is influenced by cation-to-cation N—H···N and cation-to-anion N—H···Cl hydrogen bonds (Table 1). The former of these leads to [100] chains in the crystal. One of the H···Cl separations is unusually short, with H···Cl = 2.04 (6) Å, which possibly correlates with the its long N—H separation of 1.04 (6) Å. Together, the hydrogen bonds lead to sheets parallel to the (010) plane (Fig. 2).
Only one other
containing the phenylhydrazinium cation has been determined (Hammerl et al., 2001), which has similar geometrical paramaters to those in (I).For the previous structure, see: Koo (1965). For a related structure, see: Hammerl et al. (2001). For reference structural data, see: Allen et al. (1987).
Data collection: COLLECT (Nonius, 1998); cell
SCALEPACK (Otwinowski & Minor, 1997); data reduction: DENZO and SCALEPACK (Otwinowski & Minor, 1997), and SORTAV (Blessing, 1995); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 (Farrugia, 1997); software used to prepare material for publication: SHELXL97 (Sheldrick, 1997).Fig. 1. View of the molecular structure of (I) showing 50% displacement ellipsoids. The H atoms are drawn as spheres of arbitrary radius and the hydrogen bond is shown as a double-dashed line. |
C6H9N2+·Cl− | F(000) = 304 |
Mr = 144.60 | Dx = 1.396 Mg m−3 |
Monoclinic, P21/n | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2yn | Cell parameters from 1173 reflections |
a = 3.8223 (5) Å | θ = 2.9–27.5° |
b = 30.461 (5) Å | µ = 0.46 mm−1 |
c = 6.0121 (10) Å | T = 120 K |
β = 100.686 (6)° | Blade, colourless |
V = 687.86 (18) Å3 | 0.30 × 0.07 × 0.01 mm |
Z = 4 |
Nonius KappaCCD diffractometer | 1288 independent reflections |
Radiation source: fine-focus sealed tube | 1073 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.053 |
ω and φ scans | θmax = 26.0°, θmin = 3.5° |
Absorption correction: multi-scan (SADABS; Bruker, 2003) | h = −4→4 |
Tmin = 0.874, Tmax = 0.995 | k = −35→37 |
3891 measured reflections | l = −6→7 |
Refinement on F2 | Primary atom site location: structure-invariant direct methods |
Least-squares matrix: full | Secondary atom site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.072 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.212 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.12 | w = 1/[σ2(Fo2) + (0.0789P)2 + 3.5247P] where P = (Fo2 + 2Fc2)/3 |
1288 reflections | (Δ/σ)max = 0.001 |
94 parameters | Δρmax = 0.57 e Å−3 |
0 restraints | Δρmin = −0.62 e Å−3 |
C6H9N2+·Cl− | V = 687.86 (18) Å3 |
Mr = 144.60 | Z = 4 |
Monoclinic, P21/n | Mo Kα radiation |
a = 3.8223 (5) Å | µ = 0.46 mm−1 |
b = 30.461 (5) Å | T = 120 K |
c = 6.0121 (10) Å | 0.30 × 0.07 × 0.01 mm |
β = 100.686 (6)° |
Nonius KappaCCD diffractometer | 1288 independent reflections |
Absorption correction: multi-scan (SADABS; Bruker, 2003) | 1073 reflections with I > 2σ(I) |
Tmin = 0.874, Tmax = 0.995 | Rint = 0.053 |
3891 measured reflections |
R[F2 > 2σ(F2)] = 0.072 | 0 restraints |
wR(F2) = 0.212 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.12 | Δρmax = 0.57 e Å−3 |
1288 reflections | Δρmin = −0.62 e Å−3 |
94 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 | ||
C1 | 0.2381 (11) | 0.12905 (16) | 0.7787 (9) | 0.0198 (11) | |
C2 | 0.1470 (12) | 0.10308 (16) | 0.9478 (9) | 0.0230 (11) | |
H2A | 0.0795 | 0.1161 | 1.0771 | 0.028* | |
C3 | 0.1557 (13) | 0.05785 (17) | 0.9259 (9) | 0.0244 (11) | |
H3A | 0.0939 | 0.0398 | 1.0416 | 0.029* | |
C4 | 0.2530 (13) | 0.03857 (17) | 0.7383 (9) | 0.0268 (12) | |
H4A | 0.2574 | 0.0075 | 0.7245 | 0.032* | |
C5 | 0.3432 (13) | 0.06488 (17) | 0.5721 (9) | 0.0253 (12) | |
H5 | 0.4120 | 0.0519 | 0.4432 | 0.030* | |
C6 | 0.3349 (12) | 0.11030 (16) | 0.5904 (9) | 0.0212 (11) | |
H6 | 0.3955 | 0.1283 | 0.4741 | 0.025* | |
N1 | 0.1991 (10) | 0.17567 (13) | 0.8023 (7) | 0.0195 (9) | |
H1 | 0.262 (15) | 0.1852 (18) | 0.947 (11) | 0.023* | |
N2 | 0.4198 (11) | 0.20052 (14) | 0.6761 (8) | 0.0204 (10) | |
H2 | 0.384 (15) | 0.234 (2) | 0.707 (10) | 0.031* | |
H3 | 0.303 (17) | 0.1992 (18) | 0.532 (12) | 0.031* | |
H4 | 0.652 (17) | 0.190 (2) | 0.712 (10) | 0.031* | |
Cl1 | −0.2104 (3) | 0.20115 (4) | 0.2468 (2) | 0.0192 (4) |
U11 | U22 | U33 | U12 | U13 | U23 | |
C1 | 0.013 (2) | 0.021 (2) | 0.023 (3) | 0.0028 (17) | −0.0015 (19) | 0.0009 (19) |
C2 | 0.017 (2) | 0.024 (3) | 0.026 (3) | −0.0009 (18) | −0.002 (2) | 0.002 (2) |
C3 | 0.024 (3) | 0.025 (3) | 0.024 (3) | −0.0042 (19) | 0.003 (2) | 0.007 (2) |
C4 | 0.026 (3) | 0.021 (3) | 0.034 (3) | 0.003 (2) | 0.006 (2) | 0.001 (2) |
C5 | 0.021 (3) | 0.025 (3) | 0.030 (3) | −0.001 (2) | 0.003 (2) | −0.002 (2) |
C6 | 0.014 (2) | 0.024 (2) | 0.025 (3) | 0.0012 (18) | 0.0011 (19) | 0.000 (2) |
N1 | 0.018 (2) | 0.022 (2) | 0.017 (2) | −0.0013 (15) | 0.0005 (17) | −0.0011 (17) |
N2 | 0.013 (2) | 0.022 (2) | 0.025 (3) | 0.0040 (16) | −0.0003 (17) | 0.0046 (18) |
Cl1 | 0.0187 (6) | 0.0199 (6) | 0.0182 (7) | −0.0015 (4) | 0.0015 (4) | −0.0010 (4) |
C1—C6 | 1.378 (7) | C5—C6 | 1.389 (7) |
C1—C2 | 1.383 (7) | C5—H5 | 0.9500 |
C1—N1 | 1.438 (6) | C6—H6 | 0.9500 |
C2—C3 | 1.385 (7) | N1—N2 | 1.449 (6) |
C2—H2A | 0.9500 | N1—H1 | 0.90 (6) |
C3—C4 | 1.382 (8) | N2—H2 | 1.04 (6) |
C3—H3A | 0.9500 | N2—H3 | 0.90 (7) |
C4—C5 | 1.374 (8) | N2—H4 | 0.93 (6) |
C4—H4A | 0.9500 | ||
C6—C1—C2 | 120.6 (5) | C6—C5—H5 | 119.6 |
C6—C1—N1 | 122.6 (4) | C1—C6—C5 | 119.4 (5) |
C2—C1—N1 | 116.6 (4) | C1—C6—H6 | 120.3 |
C1—C2—C3 | 119.0 (5) | C5—C6—H6 | 120.3 |
C1—C2—H2A | 120.5 | C1—N1—N2 | 112.5 (4) |
C3—C2—H2A | 120.5 | C1—N1—H1 | 113 (4) |
C4—C3—C2 | 121.0 (5) | N2—N1—H1 | 105 (4) |
C4—C3—H3A | 119.5 | N1—N2—H2 | 108 (3) |
C2—C3—H3A | 119.5 | N1—N2—H3 | 104 (4) |
C5—C4—C3 | 119.2 (5) | H2—N2—H3 | 99 (5) |
C5—C4—H4A | 120.4 | N1—N2—H4 | 109 (4) |
C3—C4—H4A | 120.4 | H2—N2—H4 | 116 (5) |
C4—C5—C6 | 120.7 (5) | H3—N2—H4 | 120 (6) |
C4—C5—H5 | 119.6 | ||
C6—C1—C2—C3 | 0.2 (7) | C2—C1—C6—C5 | −0.5 (7) |
N1—C1—C2—C3 | 175.6 (4) | N1—C1—C6—C5 | −175.5 (4) |
C1—C2—C3—C4 | −0.1 (7) | C4—C5—C6—C1 | 0.6 (7) |
C2—C3—C4—C5 | 0.2 (7) | C6—C1—N1—N2 | −27.3 (6) |
C3—C4—C5—C6 | −0.5 (7) | C2—C1—N1—N2 | 157.5 (4) |
D—H···A | D—H | H···A | D···A | D—H···A |
N2—H4···N1i | 0.93 (6) | 2.11 (6) | 3.031 (6) | 173 (5) |
N1—H1···Cl1ii | 0.90 (6) | 2.49 (6) | 3.256 (4) | 142 (5) |
N2—H2···Cl1iii | 1.04 (6) | 2.04 (6) | 3.079 (4) | 176 (5) |
N2—H3···Cl1 | 0.90 (7) | 2.35 (7) | 3.187 (5) | 154 (6) |
Symmetry codes: (i) x+1, y, z; (ii) x+1, y, z+1; (iii) x+1/2, −y+1/2, z+1/2. |
Experimental details
Crystal data | |
Chemical formula | C6H9N2+·Cl− |
Mr | 144.60 |
Crystal system, space group | Monoclinic, P21/n |
Temperature (K) | 120 |
a, b, c (Å) | 3.8223 (5), 30.461 (5), 6.0121 (10) |
β (°) | 100.686 (6) |
V (Å3) | 687.86 (18) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 0.46 |
Crystal size (mm) | 0.30 × 0.07 × 0.01 |
Data collection | |
Diffractometer | Nonius KappaCCD |
Absorption correction | Multi-scan (SADABS; Bruker, 2003) |
Tmin, Tmax | 0.874, 0.995 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 3891, 1288, 1073 |
Rint | 0.053 |
(sin θ/λ)max (Å−1) | 0.617 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.072, 0.212, 1.12 |
No. of reflections | 1288 |
No. of parameters | 94 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.57, −0.62 |
Computer programs: COLLECT (Nonius, 1998), DENZO and SCALEPACK (Otwinowski & Minor, 1997), and SORTAV (Blessing, 1995), SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), ORTEP-3 (Farrugia, 1997).
D—H···A | D—H | H···A | D···A | D—H···A |
N2—H4···N1i | 0.93 (6) | 2.11 (6) | 3.031 (6) | 173 (5) |
N1—H1···Cl1ii | 0.90 (6) | 2.49 (6) | 3.256 (4) | 142 (5) |
N2—H2···Cl1iii | 1.04 (6) | 2.04 (6) | 3.079 (4) | 176 (5) |
N2—H3···Cl1 | 0.90 (7) | 2.35 (7) | 3.187 (5) | 154 (6) |
Symmetry codes: (i) x+1, y, z; (ii) x+1, y, z+1; (iii) x+1/2, −y+1/2, z+1/2. |
Acknowledgements
The authors thank the EPSRC UK National Crystallography Service (University of Southampton) for the data collection.
References
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The structure of the title compound, (I), was established by Koo (1965), but no hydrogen atoms were located. The hydrogen bonding pattern in the crystal of (I) cannot be established based on geometrical placement of the H atoms because roatation of the terminal –NH3+ group leads to different plausible arrangements for the hydrogen bonds. Here, the redetermined structure of (I), including the H atom positions is presented (Fig. 1), and the hydrogen bonding scheme is definitively established.
In (I), atoms N1 and N2 deviate from the C1—C6 ring plane by -0.098 (4)Å and 0.418 (4) Å, respectively. The bond-angle sum for N1 is 331°, indicative of sp3 hybridization for this atom. Otherwise, the geometrical paramaters for (I) may be regarded as normal (Allen et al., 1987).
The crystal packing for (I) is influenced by cation-to-cation N—H···N and cation-to-anion N—H···Cl hydrogen bonds (Table 1). The former of these leads to [100] chains in the crystal. One of the H···Cl separations is unusually short, with H···Cl = 2.04 (6) Å, which possibly correlates with the its long N—H separation of 1.04 (6) Å. Together, the hydrogen bonds lead to sheets parallel to the (010) plane (Fig. 2).
Only one other crystal structure containing the phenylhydrazinium cation has been determined (Hammerl et al., 2001), which has similar geometrical paramaters to those in (I).