organic compounds
A new polymorph of sulfanilic acid monohydrate
aSchool of Chemistry, Cardiff University, Cardiff CF10 3AT, Wales
*Correspondence e-mail: acsbd@yahoo.com
An orthorhombic polymorph of sulfanilic acid monohydrate, C6H7NO3S·H2O, is described in which there are significant hydrogen-bonding interactions between the components of the structure.
Comment
The P21/n) of sulfanilic acid monohydrate, (II), has been described (Rae & Maslen, 1962). Here, the structure of an orthorhombic form, (I) (P212121), obtained by recrystallization from a methanol solution of the compound, is described (Fig. 1 and Table 1).
of a monoclinic form (The C—S and C—N bond lengths in (I) (Table 1) are close to the corresponding distances in (II) and O3SC6H4NH–CH–N(CH3)2·H2O (Hempel et al., 1999). The S—O bond distances in (I) are similar to those found in (II) (Rae & Maslen, 1962), in metanilic acid (Hall & Maslen, 1965), and in 2,5-dichlorobenzenesulfonic acid and 2,5-dibromobenzenesulfonic acid (Lundgren & Lundin, 1972). The C—S—O and O—S—O angles deviate from 109.5° in the expected manner.
The is stabilized by intermolecular N—H⋯O and O—H⋯O hydrogen bonds (Table 2), which result in the formation of a hydrogen-bonded network (Fig. 2). The water molecule is hydrogen bonded to the amine group (N1/H1B). The distance between the two parallel structures, with symmetry (1 + x, y, z), in the packing diagram (Fig. 2) is 6.163 (3) Å.
of (I)Experimental
Sulfanilic acid (1.732 g, 1 mmol) was dissolved in methanol (20 ml) and stirred for 1 h. After filtration, the clear solution was left for crystallization, and after two weeks, pale-yellow crystals were obtained.
Crystal data
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Data collection
Refinement
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In the absence of significant Uiso(H) = 1.2Ueq(C). H atoms attached to N and O(water) were located from an fixed in these positions and assigned individual isotropic displacement parameters; see Table 2 for bond distances.
Friedel pairs were merged before the final C-bound H atoms were included in the riding model approximation with C—H = 0.95 Å, and withData collection: CAD-4 EXPRESS (Enraf–Nonius, 1992); cell CAD-4 EXPRESS; data reduction: CAD-4 Processing Program (Hursthouse, 1976); program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: WinGX (Farrugia, 1999).
Supporting information
https://doi.org/10.1107/S1600536806016060/tk2027sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S1600536806016060/tk2027Isup2.hkl
Data collection: CAD-4 EXPRESS (Enraf–Nonius, 1992); cell
CAD-4 EXPRESS; data reduction: CAD-4 Processing Program (Hursthouse, 1976); program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: WinGX (Farrugia, 1999).C6H7NO3S·H2O | F(000) = 400 |
Mr = 191.20 | Dx = 1.616 Mg m−3 |
Orthorhombic, P212121 | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: P 2ac 2ab | Cell parameters from 957 reflections |
a = 6.1630 (6) Å | θ = 2.9–26.3° |
b = 6.9607 (5) Å | µ = 0.39 mm−1 |
c = 18.3251 (10) Å | T = 150 K |
V = 786.12 (10) Å3 | Block, pale yellow |
Z = 4 | 0.25 × 0.22 × 0.20 mm |
Enraf–Nonius CAD-4 diffractometer | 793 reflections with I > 2σ(I) |
Radiation source: fine-focus sealed tube | Rint = 0.024 |
Graphite monochromator | θmax = 26.3°, θmin = 2.2° |
ω/θ scans | h = −7→0 |
Absorption correction: part of the (Walker & Stuart, 1983) | model (ΔF) k = −8→2 |
Tmin = 0.910, Tmax = 0.927 | l = −22→22 |
3 measured reflections | 1534 standard reflections every 134 reflections |
957 independent reflections | intensity decay: none |
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.035 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.092 | w = 1/[σ2(Fo2) + (0.0544P)2 + 0.1313P] where P = (Fo2 + 2Fc2)/3 |
S = 1.04 | (Δ/σ)max = 0.001 |
957 reflections | Δρmax = 0.31 e Å−3 |
114 parameters | Δρmin = −0.29 e Å−3 |
5 restraints | Absolute structure: Flack (1983) |
Primary atom site location: structure-invariant direct methods |
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 | ||
S1 | −0.01053 (14) | 0.48483 (12) | 0.63841 (4) | 0.0291 (2) | |
O1 | 0.2228 (4) | 0.5066 (5) | 0.63447 (13) | 0.0463 (7) | |
O2 | −0.1130 (5) | 0.6505 (4) | 0.67294 (13) | 0.0386 (7) | |
O3 | −0.0795 (5) | 0.3055 (4) | 0.67078 (13) | 0.0428 (7) | |
O4 | 0.0515 (4) | 0.6429 (5) | 0.25576 (15) | 0.0663 (11) | |
N1 | −0.3138 (4) | 0.5290 (4) | 0.32896 (13) | 0.0307 (7) | |
C1 | −0.1055 (5) | 0.4873 (4) | 0.54710 (15) | 0.0252 (7) | |
C2 | −0.3124 (6) | 0.5482 (5) | 0.53154 (17) | 0.0303 (8) | |
H2 | −0.4084 | 0.5827 | 0.5699 | 0.036* | |
C3 | −0.3807 (6) | 0.5591 (5) | 0.45936 (17) | 0.0307 (8) | |
H3 | −0.5234 | 0.6011 | 0.4480 | 0.037* | |
C4 | −0.2392 (5) | 0.5081 (5) | 0.40465 (16) | 0.0273 (7) | |
C5 | −0.0359 (6) | 0.4401 (5) | 0.41925 (16) | 0.0304 (8) | |
H5 | 0.0554 | 0.4006 | 0.3803 | 0.036* | |
C6 | 0.0381 (4) | 0.4282 (4) | 0.49055 (13) | 0.0299 (8) | |
H6 | 0.1797 | 0.3823 | 0.5013 | 0.036* | |
H1A | −0.3781 | 0.4113 | 0.3158 | 0.053 (13)* | |
H1B | −0.1976 | 0.5436 | 0.2970 | 0.041 (11)* | |
H1C | −0.4142 | 0.6317 | 0.3197 | 0.059 (14)* | |
H4A | 0.1434 | 0.6163 | 0.2156 | 0.12 (2)* | |
H4B | 0.1615 | 0.7184 | 0.2777 | 0.15 (3)* |
U11 | U22 | U33 | U12 | U13 | U23 | |
S1 | 0.0329 (4) | 0.0347 (4) | 0.0195 (3) | 0.0022 (5) | −0.0003 (3) | 0.0014 (4) |
O1 | 0.0293 (13) | 0.079 (2) | 0.0311 (12) | −0.0029 (16) | −0.0032 (10) | 0.0047 (17) |
O2 | 0.0500 (18) | 0.0387 (13) | 0.0270 (12) | 0.0017 (14) | 0.0012 (14) | −0.0070 (11) |
O3 | 0.0549 (19) | 0.0419 (14) | 0.0315 (13) | 0.0020 (14) | 0.0023 (15) | 0.0098 (11) |
O4 | 0.052 (2) | 0.096 (3) | 0.0513 (16) | −0.025 (2) | 0.0144 (17) | −0.0228 (18) |
N1 | 0.0376 (16) | 0.0327 (16) | 0.0217 (12) | −0.0033 (15) | −0.0041 (13) | 0.0000 (12) |
C1 | 0.0299 (16) | 0.0241 (15) | 0.0216 (13) | −0.0018 (18) | 0.0004 (12) | 0.0007 (13) |
C2 | 0.0306 (18) | 0.0334 (18) | 0.0268 (16) | 0.0028 (16) | 0.0057 (14) | −0.0008 (14) |
C3 | 0.0296 (19) | 0.0331 (17) | 0.0294 (16) | 0.0016 (16) | −0.0019 (14) | −0.0002 (14) |
C4 | 0.0353 (17) | 0.0254 (16) | 0.0212 (15) | 0.0001 (17) | −0.0030 (12) | −0.0001 (15) |
C5 | 0.0321 (19) | 0.0353 (17) | 0.0237 (14) | 0.0036 (15) | 0.0054 (15) | −0.0067 (13) |
C6 | 0.031 (2) | 0.0305 (16) | 0.0284 (15) | 0.0041 (15) | 0.0018 (15) | −0.0026 (13) |
S1—O1 | 1.448 (3) | C1—C2 | 1.374 (5) |
S1—O2 | 1.459 (3) | C1—C6 | 1.424 (4) |
S1—O3 | 1.446 (3) | C2—C3 | 1.390 (4) |
S1—C1 | 1.773 (3) | C2—H2 | 0.9500 |
O4—H4A | 0.9476 | C3—C4 | 1.376 (5) |
O4—H4B | 0.9474 | C3—H3 | 0.9500 |
N1—C4 | 1.468 (4) | C4—C5 | 1.366 (5) |
N1—H1A | 0.9415 | C5—C6 | 1.386 (4) |
N1—H1B | 0.9315 | C5—H5 | 0.9500 |
N1—H1C | 0.9606 | C6—H6 | 0.9500 |
O1—S1—O2 | 111.64 (19) | C1—C2—C3 | 119.7 (3) |
O1—S1—O3 | 113.77 (19) | C1—C2—H2 | 120.2 |
O1—S1—C1 | 106.26 (15) | C3—C2—H2 | 120.2 |
O2—S1—O3 | 112.15 (15) | C4—C3—C2 | 119.2 (3) |
O2—S1—C1 | 105.00 (15) | C4—C3—H3 | 120.4 |
O3—S1—C1 | 107.36 (15) | C2—C3—H3 | 120.4 |
H4A—O4—H4B | 90.5 | C5—C4—C3 | 121.9 (3) |
C4—N1—H1A | 106.8 | C5—C4—N1 | 120.4 (3) |
C4—N1—H1B | 111.4 | C3—C4—N1 | 117.7 (3) |
H1A—N1—H1B | 104.9 | C4—C5—C6 | 120.5 (3) |
C4—N1—H1C | 116.3 | C4—C5—H5 | 119.8 |
H1A—N1—H1C | 109.3 | C6—C5—H5 | 119.8 |
H1B—N1—H1C | 107.6 | C5—C6—C1 | 117.7 (3) |
C2—C1—C6 | 121.0 (3) | C5—C6—H6 | 121.2 |
C2—C1—S1 | 120.4 (2) | C1—C6—H6 | 121.2 |
C6—C1—S1 | 118.6 (2) |
D—H···A | D—H | H···A | D···A | D—H···A |
O4—H4a···O1i | 0.95 | 1.90 | 2.821 (3) | 163 |
O4—H4b···O2ii | 0.95 | 1.89 | 2.838 (4) | 175 |
N1—H1a···O3iii | 0.94 | 1.97 | 2.846 (4) | 154 |
N1—H1b···O4 | 0.93 | 1.84 | 2.738 (3) | 160 |
N1—H1c···O2iv | 0.96 | 1.95 | 2.895 (4) | 166 |
Symmetry codes: (i) −x+1/2, −y+1, z−1/2; (ii) x+1/2, −y+3/2, −z+1; (iii) x−1/2, −y+1/2, −z+1; (iv) x−1/2, −y+3/2, −z+1. |
Acknowledgements
GMGH acknowledges the Ministry of Science and Technology, The People's Republic of Bangladesh, for the award of a Bangabandhu Fellowship.
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