Buy article online - an online subscription or single-article purchase is required to access this article.
Download citation
Download citation
link to html
In the title com­pounds, 3-(di­hydroxy­bor­yl)anilinium bis­ulfate monohydrate, C6H9BNO2+·HSO4·H2O (I), and 3-(di­hydroxy­bor­yl)anilinium methyl sulfate, C6H9BNO2+·CH3SO4 (II), the almost planar boronic acid mol­ecules are linked by pairs of O—H...O hydro­gen bonds, forming centrosymmetric motifs that can be described by the graph-set R22(8) motif. In both crystals, the B(OH)2 group acquires a synanti conformation (with respect to the H atoms). The presence of the hydro­gen-bonding functional groups B(OH)2, NH3+, HSO4, CH3SO4 and H2O generates three-dimensional hydro­gen-bonded networks, in which the bis­ulfate (HSO4) and methyl sulfate (CH3SO4) counter-ions act as the central building blocks within the crystal structures. Furthermore, in both structures, the packing is stabilized by weak boron–π inter­actions, as shown by noncovalent inter­actions (NCI) index calculations.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2053229623005065/vp3028sup1.cif
Contains datablocks I, II, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229623005065/vp3028Isup2.hkl
Contains datablock I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229623005065/vp3028IIsup3.hkl
Contains datablock II

cml

Chemical Markup Language (CML) file https://doi.org/10.1107/S2053229623005065/vp3028Isup4.cml
Supplementary material

cml

Chemical Markup Language (CML) file https://doi.org/10.1107/S2053229623005065/vp3028IIsup5.cml
Supplementary material

CCDC references: 2268110; 2268109

Computing details top

For both structures, data collection: CrysAlis PRO (Agilent, 2014); cell refinement: CrysAlis PRO (Agilent, 2014); data reduction: CrysAlis PRO (Agilent, 2014); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL2018 (Sheldrick, 2015); molecular graphics: OLEX2 (Dolomanov et al., 2009); software used to prepare material for publication: OLEX2 (Dolomanov et al., 2009).

3-(Dihydroxyboryl)anilinium hydrogen sulfate monohydrate (I) top
Crystal data top
C6H9BNO2+·HSO4·H2ODx = 1.582 Mg m3
Mr = 253.04Cu Kα radiation, λ = 1.54184 Å
Orthorhombic, PbcaCell parameters from 2687 reflections
a = 14.1807 (6) Åθ = 4.3–72.3°
b = 7.4675 (3) ŵ = 2.96 mm1
c = 20.0702 (8) ÅT = 293 K
V = 2125.32 (15) Å3Block, clear yellowish yellow
Z = 80.34 × 0.2 × 0.16 mm
F(000) = 1056
Data collection top
Agilent SuperNova Dual Source
diffractometer with an Eos detector
1914 reflections with I > 2σ(I)
Detector resolution: 8.0769 pixels mm-1Rint = 0.040
ω scansθmax = 72.7°, θmin = 4.4°
Absorption correction: multi-scan
(CrysAlis PRO; Agilent, 2014)
h = 179
Tmin = 0.589, Tmax = 1.000k = 97
4648 measured reflectionsl = 2324
2071 independent reflections
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullHydrogen site location: mixed
R[F2 > 2σ(F2)] = 0.051H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.138 w = 1/[σ2(Fo2) + (0.0922P)2 + 0.8783P]
where P = (Fo2 + 2Fc2)/3
S = 1.08(Δ/σ)max = 0.001
2071 reflectionsΔρmax = 0.74 e Å3
177 parametersΔρmin = 0.82 e Å3
8 restraints
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
C10.39986 (14)0.5777 (3)0.55191 (9)0.0136 (4)
C20.40815 (14)0.5262 (3)0.61859 (9)0.0134 (4)
H20.4352190.6039480.6493070.016*
C30.37619 (14)0.3597 (3)0.63916 (9)0.0130 (4)
C40.33477 (16)0.2402 (3)0.59484 (11)0.0165 (4)
H40.3135010.1289600.6092840.020*
C50.32584 (16)0.2906 (3)0.52852 (10)0.0180 (4)
H50.2982590.2125510.4981000.022*
C60.35800 (14)0.4573 (3)0.50738 (10)0.0153 (4)
H60.3515470.4892580.4628260.018*
B10.43950 (17)0.7658 (3)0.53047 (12)0.0142 (5)
N10.38825 (13)0.3073 (2)0.70905 (8)0.0136 (4)
H1D0.4285 (14)0.222 (2)0.7134 (13)0.019 (7)*
H1B0.3392 (11)0.264 (3)0.7284 (12)0.015 (6)*
H1C0.405 (2)0.394 (2)0.7347 (12)0.032 (8)*
O10.49180 (11)0.8560 (2)0.57635 (7)0.0180 (4)
H1A0.509 (3)0.953 (2)0.5618 (15)0.055 (11)*
O20.42498 (11)0.8431 (2)0.46978 (7)0.0180 (4)
H2A0.3939 (17)0.791 (3)0.4412 (10)0.026 (7)*
O30.31753 (11)0.7391 (2)0.36457 (7)0.0165 (4)
O40.43779 (11)0.8888 (2)0.29739 (7)0.0179 (4)
O50.28937 (11)0.8106 (2)0.24853 (7)0.0205 (4)
O60.40248 (11)0.5799 (2)0.27829 (8)0.0214 (4)
H6A0.390 (3)0.510 (4)0.3084 (12)0.073 (14)*
O70.37303 (11)0.3040 (2)0.34654 (8)0.0182 (4)
H7A0.4087 (18)0.257 (4)0.3736 (12)0.036 (9)*
H7B0.3234 (12)0.270 (4)0.3633 (15)0.045 (11)*
S10.35902 (4)0.76286 (7)0.29823 (2)0.0129 (2)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0127 (10)0.0194 (10)0.0086 (9)0.0008 (7)0.0001 (6)0.0002 (7)
C20.0118 (9)0.0203 (10)0.0080 (9)0.0004 (7)0.0001 (6)0.0019 (7)
C30.0106 (9)0.0208 (10)0.0077 (9)0.0008 (7)0.0011 (7)0.0021 (7)
C40.0163 (10)0.0198 (10)0.0135 (10)0.0030 (7)0.0006 (9)0.0006 (7)
C50.0196 (11)0.0233 (10)0.0110 (9)0.0048 (9)0.0008 (8)0.0032 (8)
C60.0171 (10)0.0218 (10)0.0072 (9)0.0004 (7)0.0008 (7)0.0001 (7)
B10.0132 (11)0.0203 (11)0.0092 (10)0.0000 (8)0.0011 (9)0.0005 (8)
N10.0129 (8)0.0198 (9)0.0081 (8)0.0009 (7)0.0007 (6)0.0022 (6)
O10.0233 (8)0.0199 (7)0.0109 (7)0.0057 (6)0.0053 (6)0.0033 (5)
O20.0225 (8)0.0220 (8)0.0095 (7)0.0063 (6)0.0054 (6)0.0021 (6)
O30.0158 (8)0.0265 (8)0.0072 (7)0.0007 (6)0.0006 (5)0.0002 (5)
O40.0135 (8)0.0196 (8)0.0207 (8)0.0028 (6)0.0018 (5)0.0021 (5)
O50.0147 (7)0.0357 (9)0.0111 (7)0.0034 (7)0.0028 (6)0.0049 (6)
O60.0243 (8)0.0210 (8)0.0187 (8)0.0005 (6)0.0081 (6)0.0007 (6)
O70.0173 (8)0.0243 (8)0.0130 (7)0.0006 (6)0.0021 (6)0.0031 (6)
S10.0114 (3)0.0192 (3)0.0083 (3)0.00132 (17)0.00057 (15)0.00027 (16)
Geometric parameters (Å, º) top
C1—C21.397 (3)B1—O21.364 (3)
C1—C61.400 (3)N1—H1D0.8600 (10)
C1—B11.573 (3)N1—H1B0.8600 (11)
C2—H20.9300N1—H1C0.8601 (11)
C2—C31.386 (3)O1—H1A0.8200 (11)
C3—C41.390 (3)O2—H2A0.8200 (11)
C3—N11.466 (2)O3—S11.4665 (15)
C4—H40.9300O4—S11.4604 (16)
C4—C51.389 (3)O5—S11.4482 (15)
C5—H50.9300O6—H6A0.8200 (10)
C5—C61.392 (3)O6—S11.5510 (16)
C6—H60.9300O7—H7A0.8200 (10)
B1—O11.361 (3)O7—H7B0.8200 (11)
C2—C1—C6118.06 (19)O1—B1—O2118.48 (19)
C2—C1—B1118.54 (18)O2—B1—C1124.66 (19)
C6—C1—B1123.39 (18)C3—N1—H1D111.9 (18)
C1—C2—H2119.9C3—N1—H1B116.0 (18)
C3—C2—C1120.30 (18)C3—N1—H1C113.9 (19)
C3—C2—H2119.9H1D—N1—H1B102 (2)
C2—C3—C4121.55 (18)H1D—N1—H1C108 (3)
C2—C3—N1119.06 (18)H1B—N1—H1C104 (3)
C4—C3—N1119.38 (19)B1—O1—H1A111 (2)
C3—C4—H4120.7B1—O2—H2A120 (2)
C5—C4—C3118.55 (19)S1—O6—H6A107 (3)
C5—C4—H4120.7H7A—O7—H7B97 (3)
C4—C5—H5119.9O3—S1—O6106.70 (9)
C4—C5—C6120.29 (19)O4—S1—O3113.27 (9)
C6—C5—H5119.9O4—S1—O6105.09 (9)
C1—C6—H6119.4O5—S1—O3112.42 (9)
C5—C6—C1121.24 (18)O5—S1—O4110.81 (9)
C5—C6—H6119.4O5—S1—O6108.05 (10)
O1—B1—C1116.85 (18)
C1—C2—C3—C40.4 (3)C4—C5—C6—C10.0 (3)
C1—C2—C3—N1178.29 (18)C6—C1—C2—C30.5 (3)
C2—C1—C6—C50.3 (3)C6—C1—B1—O1169.55 (19)
C2—C1—B1—O19.3 (3)C6—C1—B1—O210.5 (3)
C2—C1—B1—O2170.6 (2)B1—C1—C2—C3178.42 (18)
C2—C3—C4—C50.1 (3)B1—C1—C6—C5178.56 (19)
C3—C4—C5—C60.1 (3)N1—C3—C4—C5178.59 (19)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1D···O4i0.86 (2)2.08 (1)2.872 (2)153 (1)
N1—H1B···O5ii0.86 (2)1.95 (1)2.783 (2)163 (2)
N1—H1B···O7iii0.86 (2)2.47 (2)2.89 (2)111 (1)
N1—H1C···O4iv0.86 (2)2.11 (1)2.964 (2)177 (3)
O1—H1A···O2v0.82 (2)1.90 (3)2.702 (2)168 (4)
O2—H2A···O30.82 (2)1.92 (2)2.717 (2)163 (2)
O6—H6A···O70.82 (3)1.74 (3)2.509 (2)157 (3)
O7—H7A···O1i0.82 (3)1.93 (3)2.738 (2)170 (2)
O7—H7B···O3vi0.82 (2)2.01 (1)2.769 (2)153 (3)
C2—H2···O10.932.522.862 (3)102
Symmetry codes: (i) x+1, y+1, z+1; (ii) x+1/2, y+1, z+1/2; (iii) x, y+1/2, z+1/2; (iv) x, y+3/2, z+1/2; (v) x+1, y+2, z+1; (vi) x+1/2, y1/2, z.
3-(Dihydroxyboryl)anilinium methyl sulfate (II) top
Crystal data top
C6H9BNO2+·CH3SO4F(000) = 520
Mr = 249.05Dx = 1.582 Mg m3
Monoclinic, P21/nCu Kα radiation, λ = 1.54184 Å
a = 10.97561 (18) ÅCell parameters from 2836 reflections
b = 7.22452 (11) Åθ = 5.9–72.5°
c = 13.5494 (2) ŵ = 2.93 mm1
β = 103.3430 (15)°T = 293 K
V = 1045.38 (3) Å3Plate, clear yellowish yellow
Z = 40.34 × 0.3 × 0.14 mm
Data collection top
Agilent SuperNova Dual Source
diffractometer with an Eos detector
1965 reflections with I > 2σ(I)
Detector resolution: 8.0769 pixels mm-1Rint = 0.014
ω scansθmax = 72.8°, θmin = 4.7°
Absorption correction: multi-scan
(CrysAlis PRO; Agilent, 2014)
h = 1213
Tmin = 0.726, Tmax = 1.000k = 86
3631 measured reflectionsl = 1615
2017 independent reflections
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullHydrogen site location: mixed
R[F2 > 2σ(F2)] = 0.030H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.079 w = 1/[σ2(Fo2) + (0.0367P)2 + 0.659P]
where P = (Fo2 + 2Fc2)/3
S = 1.11(Δ/σ)max = 0.001
2017 reflectionsΔρmax = 0.35 e Å3
166 parametersΔρmin = 0.40 e Å3
5 restraints
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
C10.96725 (14)0.5585 (2)0.36273 (11)0.0132 (3)
C21.05927 (14)0.5033 (2)0.31245 (11)0.0131 (3)
H21.1279960.5792410.3136740.016*
C31.04875 (14)0.3366 (2)0.26100 (11)0.0129 (3)
C40.94961 (15)0.2183 (2)0.25800 (12)0.0173 (3)
H40.9441150.1065010.2232170.021*
C50.85795 (16)0.2701 (2)0.30822 (13)0.0214 (4)
H50.7904760.1918370.3075510.026*
C60.86641 (15)0.4380 (2)0.35948 (12)0.0174 (3)
H60.8039090.4709840.3922390.021*
C70.39900 (15)0.8002 (2)0.57398 (13)0.0190 (3)
H7A0.4179830.9242140.5980600.029*
H7B0.4098330.7172560.6307170.029*
H7C0.3139110.7943390.5354440.029*
B10.98218 (17)0.7522 (2)0.41861 (13)0.0143 (3)
N11.14551 (13)0.28718 (19)0.20638 (10)0.0142 (3)
H1B1.149 (2)0.368 (2)0.1603 (11)0.028 (6)*
H1C1.131 (2)0.1802 (13)0.1782 (14)0.026 (5)*
H1D1.2181 (10)0.287 (3)0.2475 (14)0.038 (7)*
O11.08772 (11)0.84897 (16)0.41822 (9)0.0179 (3)
H1A1.092 (2)0.9469 (15)0.4495 (14)0.034 (6)*
O20.89447 (11)0.82604 (16)0.46424 (9)0.0174 (2)
H2A0.8312 (12)0.766 (3)0.4643 (18)0.034 (6)*
O30.67631 (11)0.64619 (17)0.48249 (8)0.0202 (3)
O40.67689 (11)0.89182 (16)0.60384 (9)0.0202 (3)
O50.62808 (11)0.58524 (16)0.64640 (8)0.0191 (3)
O60.48264 (10)0.74674 (17)0.51004 (8)0.0185 (3)
S10.62503 (3)0.71551 (5)0.56395 (3)0.01183 (12)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0159 (7)0.0125 (7)0.0108 (6)0.0009 (6)0.0021 (5)0.0005 (6)
C20.0150 (7)0.0116 (7)0.0127 (7)0.0015 (6)0.0032 (5)0.0004 (6)
C30.0158 (7)0.0136 (7)0.0094 (6)0.0026 (6)0.0029 (5)0.0008 (6)
C40.0228 (8)0.0125 (8)0.0170 (8)0.0018 (6)0.0053 (6)0.0051 (6)
C50.0216 (8)0.0177 (8)0.0269 (9)0.0075 (7)0.0099 (7)0.0067 (7)
C60.0176 (8)0.0173 (8)0.0191 (8)0.0010 (6)0.0078 (6)0.0044 (6)
C70.0157 (8)0.0224 (9)0.0197 (8)0.0019 (6)0.0059 (6)0.0016 (7)
B10.0174 (8)0.0120 (8)0.0134 (8)0.0006 (7)0.0037 (6)0.0004 (7)
N10.0166 (7)0.0137 (7)0.0122 (6)0.0015 (5)0.0032 (5)0.0026 (5)
O10.0199 (6)0.0125 (6)0.0234 (6)0.0033 (5)0.0090 (5)0.0074 (5)
O20.0179 (6)0.0137 (6)0.0226 (6)0.0035 (5)0.0092 (5)0.0067 (5)
O30.0203 (6)0.0254 (6)0.0176 (5)0.0027 (5)0.0098 (4)0.0072 (5)
O40.0198 (6)0.0157 (6)0.0261 (6)0.0034 (5)0.0076 (5)0.0057 (5)
O50.0222 (6)0.0168 (6)0.0196 (6)0.0031 (5)0.0075 (5)0.0073 (5)
O60.0147 (6)0.0271 (6)0.0133 (5)0.0012 (5)0.0025 (4)0.0006 (5)
S10.01295 (19)0.0115 (2)0.01144 (19)0.00018 (13)0.00369 (13)0.00016 (13)
Geometric parameters (Å, º) top
C1—C21.400 (2)C7—H7C0.9600
C1—C61.401 (2)C7—O61.4524 (19)
C1—B11.581 (2)B1—O11.354 (2)
C2—H20.9300B1—O21.367 (2)
C2—C31.383 (2)N1—H1B0.8601 (10)
C3—C41.377 (2)N1—H1C0.8601 (10)
C3—N11.4716 (19)N1—H1D0.8600 (10)
C4—H40.9300O1—H1A0.8200 (10)
C4—C51.390 (2)O2—H2A0.8199 (11)
C5—H50.9300O3—S11.4396 (11)
C5—C61.390 (2)O4—S11.4480 (12)
C6—H60.9300O5—S11.4552 (11)
C7—H7A0.9600O6—S11.5811 (11)
C7—H7B0.9600
C2—C1—C6117.43 (14)O6—C7—H7A109.5
C2—C1—B1118.59 (14)O6—C7—H7B109.5
C6—C1—B1123.98 (14)O6—C7—H7C109.5
C1—C2—H2119.7O1—B1—C1116.69 (14)
C3—C2—C1120.53 (14)O1—B1—O2119.53 (14)
C3—C2—H2119.7O2—B1—C1123.77 (14)
C2—C3—N1118.60 (14)C3—N1—H1B110.9 (14)
C4—C3—C2121.93 (14)C3—N1—H1C111.2 (15)
C4—C3—N1119.46 (14)C3—N1—H1D110.0 (16)
C3—C4—H4120.8H1B—N1—H1C108.6 (19)
C3—C4—C5118.36 (15)H1B—N1—H1D106 (2)
C5—C4—H4120.8H1C—N1—H1D110 (2)
C4—C5—H5119.8B1—O1—H1A113.1 (16)
C4—C5—C6120.47 (15)B1—O2—H2A118.6 (16)
C6—C5—H5119.8C7—O6—S1117.11 (10)
C1—C6—H6119.4O3—S1—O4113.74 (7)
C5—C6—C1121.29 (14)O3—S1—O5114.82 (7)
C5—C6—H6119.4O3—S1—O6102.42 (6)
H7A—C7—H7B109.5O4—S1—O5110.18 (7)
H7A—C7—H7C109.5O4—S1—O6107.96 (7)
H7B—C7—H7C109.5O5—S1—O6106.98 (7)
C1—C2—C3—C40.8 (2)C6—C1—B1—O1177.38 (15)
C1—C2—C3—N1177.95 (13)C6—C1—B1—O24.0 (2)
C2—C1—C6—C50.1 (2)C7—O6—S1—O3174.01 (12)
C2—C1—B1—O13.2 (2)C7—O6—S1—O465.67 (13)
C2—C1—B1—O2175.46 (15)C7—O6—S1—O552.90 (13)
C2—C3—C4—C50.2 (2)B1—C1—C2—C3178.78 (13)
C3—C4—C5—C60.4 (3)B1—C1—C6—C5179.39 (15)
C4—C5—C6—C10.5 (3)N1—C3—C4—C5178.53 (15)
C6—C1—C2—C30.7 (2)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1B···O6i0.86 (1)2.58 (1)2.959 (2)108 (1)
N1—H1B···O4ii0.86 (1)1.95 (1)2.765 (2)158 (1)
N1—H1C···O5iii0.86 (1)1.96 (1)2.804 (2)165 (1)
N1—H1D···O4iv0.86 (1)2.45 (1)3.126 (2)136 (1)
N1—H1D···O5iv0.86 (1)2.16 (1)2.952 (2)154 (1)
O1—H1A···O2v0.82 (1)2.00 (1)2.818 (2)176 (1)
O2—H2A···O30.82 (2)1.97 (1)2.785 (2)171 (2)
C2—H2···O10.932.512.860 (2)103
C6—H6···O30.932.423.316 (2)162
C7—H7B···O50.962.542.925 (2)104
Symmetry codes: (i) x+3/2, y1/2, z+1/2; (ii) x+1/2, y+3/2, z1/2; (iii) x+1/2, y+1/2, z1/2; (iv) x+2, y+1, z+1; (v) x+2, y+2, z+1.
 

Subscribe to Acta Crystallographica Section C: Structural Chemistry

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