Literature DB >> 21580991

Bis[(m-phenyl-enedimethyl-ene)-diammonium] tetra-deca-borate.

Xiao Jiang1, Shu-Li Wu, Zhi-Dong Shao, Yun-Xiao Liang.   

Abstract

The title compound 2C(8)H(14)N(2) (2+)·[B(14)O(20)(OH)(6)](4-), contains diprotonated C(8)H(14)N(2) (2+) cations and centrosymmetric tetra-deca-borate anions. The crystal structure is stabilized by O-H⋯O and N-H⋯O hydrogen bonds.

Entities:  

Year:  2008        PMID: 21580991      PMCID: PMC2959632          DOI: 10.1107/S1600536808033333

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

For background on the importance of borate compounds, see: Chen et al. (1995 ▶); Grice et al. (1999 ▶). For previous work on boron oxoanions, see: Liu et al. (2006 ▶); Pan et al. (2007 ▶); Grice et al. (1999 ▶); Schubert et al. (2000 ▶); Touboul et al. (2003 ▶); Burns (1995 ▶).

Experimental

Crystal data

2C8H14N2 2+·B14H6O26 4− M = 849.81 Triclinic, a = 9.1025 (18) Å b = 10.293 (2) Å c = 10.942 (2) Å α = 109.68 (3)° β = 108.24 (3)° γ = 102.19 (3)° V = 857.4 (5) Å3 Z = 1 Mo Kα radiation μ = 0.14 mm−1 T = 295 (2) K 0.34 × 0.26 × 0.18 mm

Data collection

Rigaku R-AXIS RAPID diffractometer Absorption correction: multi-scan (ABSCOR; Higashi, 1995 ▶) T min = 0.964, T max = 0.973 6803 measured reflections 3009 independent reflections 2002 reflections with I > 2σ(I) R int = 0.023

Refinement

R[F 2 > 2σ(F 2)] = 0.035 wR(F 2) = 0.128 S = 1.24 3009 reflections 272 parameters H-atom parameters constrained Δρmax = 0.42 e Å−3 Δρmin = −0.46 e Å−3 Data collection: RAPID-AUTO (Rigaku, 1998 ▶); cell refinement: RAPID-AUTO; data reduction: CrystalStructure (Rigaku/MSC, 2002 ▶); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEPII (Johnson, 1976 ▶); software used to prepare material for publication: SHELXL97. Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536808033333/bt2801sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536808033333/bt2801Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
2C8H14N22+·B14H6O264Z = 1
Mr = 849.81F(000) = 436
Triclinic, P1Dx = 1.646 Mg m3
Hall symbol: -P1Mo Kα radiation, λ = 0.71073 Å
a = 9.1025 (18) ÅCell parameters from 4940 reflections
b = 10.293 (2) Åθ = 6.7–54.9°
c = 10.942 (2) ŵ = 0.14 mm1
α = 109.68 (3)°T = 295 K
β = 108.24 (3)°Block, colourless
γ = 102.19 (3)°0.34 × 0.26 × 0.18 mm
V = 857.4 (5) Å3
Rigaku R-AXIS RAPID diffractometer3009 independent reflections
Radiation source: fine-focus sealed tube2002 reflections with I > 2σ(I)
graphiteRint = 0.023
ω scansθmax = 25.0°, θmin = 3.4°
Absorption correction: multi-scan (ABSCOR; Higashi, 1995)h = −10→10
Tmin = 0.964, Tmax = 0.973k = −12→12
6803 measured reflectionsl = −12→12
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.035H-atom parameters constrained
wR(F2) = 0.128w = 1/[σ2(Fo2) + (0.0299P)2 + 1.2547P] where P = (Fo2 + 2Fc2)/3
S = 1.24(Δ/σ)max < 0.001
3009 reflectionsΔρmax = 0.42 e Å3
272 parametersΔρmin = −0.46 e Å3
0 restraintsExtinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.012 (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.
xyzUiso*/Ueq
B10.6460 (5)0.4668 (4)0.7888 (4)0.0240 (8)
B20.7413 (4)0.3345 (4)0.6060 (4)0.0222 (8)
B30.5338 (4)0.1936 (4)0.6602 (4)0.0247 (8)
B40.6535 (4)0.6248 (4)1.0187 (4)0.0209 (7)
B50.4617 (5)0.6104 (4)0.8040 (4)0.0233 (8)
B60.7437 (4)0.3478 (4)0.3829 (4)0.0225 (8)
B70.9709 (5)0.3173 (4)0.5343 (4)0.0252 (8)
O10.7649 (3)0.4597 (2)0.7304 (2)0.0238 (5)
O20.6220 (3)0.1961 (2)0.5811 (2)0.0279 (5)
O30.5410 (3)0.3195 (2)0.7601 (2)0.0266 (5)
O40.7324 (3)0.5555 (2)0.9474 (2)0.0231 (5)
O50.5160 (3)0.6519 (2)0.9489 (2)0.0259 (5)
O60.5330 (3)0.5377 (2)0.7283 (2)0.0248 (5)
O70.6718 (3)0.3576 (2)0.4736 (2)0.0263 (5)
O80.8946 (3)0.3301 (3)0.4095 (2)0.0297 (6)
O90.9009 (3)0.3166 (2)0.6244 (2)0.0260 (5)
O100.4275 (3)0.0652 (3)0.6413 (3)0.0447 (7)
H10A0.4225−0.00420.57330.067*
O110.7074 (3)0.6690 (2)1.1630 (2)0.0269 (5)
H11A0.62970.67221.18520.040*
O120.3292 (3)0.6490 (3)0.7475 (2)0.0284 (5)
O131.1239 (3)0.3064 (3)0.5617 (2)0.0374 (6)
H13A1.16590.31470.64330.056*
N10.3291 (3)0.3057 (3)0.4112 (3)0.0329 (7)
H1A0.43530.32870.46540.049*
H1B0.27470.32280.46620.049*
H1C0.32030.36050.36330.049*
N2−0.1153 (3)0.4082 (3)0.0950 (3)0.0320 (7)
H2A−0.13720.46670.05310.048*
H2B−0.00780.44270.15130.048*
H2C−0.17300.40600.14710.048*
C10.0788 (4)0.1079 (4)0.2176 (4)0.0316 (8)
C20.0378 (4)0.1765 (4)0.1291 (4)0.0313 (8)
H2D0.12140.23500.11850.038*
C3−0.1245 (4)0.1600 (4)0.0564 (4)0.0310 (8)
C4−0.2492 (4)0.0650 (4)0.0667 (4)0.0380 (9)
H4A−0.35930.05050.01650.046*
C5−0.2107 (5)−0.0074 (4)0.1508 (4)0.0452 (10)
H5A−0.2949−0.07130.15630.054*
C6−0.0475 (5)0.0143 (4)0.2272 (4)0.0387 (9)
H6A−0.0220−0.03370.28500.046*
C70.2573 (5)0.1467 (4)0.3083 (4)0.0413 (9)
H7A0.26810.08650.36000.050*
H7B0.31660.12740.24830.050*
C8−0.1624 (5)0.2555 (4)−0.0168 (4)0.0373 (9)
H8A−0.27940.2172−0.07890.045*
H8B−0.10060.2570−0.07440.045*
U11U22U33U12U13U23
B10.0293 (19)0.027 (2)0.0191 (19)0.0131 (16)0.0134 (16)0.0092 (16)
B20.0212 (18)0.025 (2)0.0231 (19)0.0095 (15)0.0124 (16)0.0104 (16)
B30.0267 (19)0.024 (2)0.024 (2)0.0084 (16)0.0132 (16)0.0098 (17)
B40.0219 (18)0.0198 (18)0.0207 (19)0.0057 (14)0.0104 (15)0.0081 (15)
B50.0287 (19)0.0248 (19)0.0197 (19)0.0128 (16)0.0115 (16)0.0101 (16)
B60.0245 (19)0.0242 (19)0.0179 (18)0.0128 (15)0.0081 (15)0.0060 (15)
B70.0265 (19)0.032 (2)0.0162 (18)0.0142 (17)0.0085 (16)0.0072 (16)
O10.0236 (11)0.0247 (12)0.0230 (12)0.0071 (9)0.0145 (10)0.0067 (10)
O20.0325 (12)0.0254 (12)0.0273 (13)0.0089 (10)0.0197 (11)0.0073 (10)
O30.0327 (13)0.0219 (12)0.0295 (13)0.0083 (10)0.0211 (11)0.0095 (10)
O40.0253 (11)0.0272 (12)0.0160 (11)0.0119 (9)0.0086 (9)0.0071 (10)
O50.0291 (12)0.0354 (13)0.0188 (12)0.0186 (10)0.0117 (10)0.0119 (10)
O60.0292 (12)0.0320 (13)0.0190 (11)0.0182 (10)0.0119 (10)0.0113 (10)
O70.0251 (12)0.0394 (14)0.0243 (12)0.0182 (10)0.0145 (10)0.0168 (11)
O80.0280 (12)0.0458 (15)0.0253 (13)0.0196 (11)0.0161 (10)0.0183 (11)
O90.0248 (12)0.0392 (14)0.0237 (12)0.0175 (10)0.0153 (10)0.0157 (11)
O100.0624 (17)0.0251 (14)0.0473 (16)0.0051 (12)0.0399 (15)0.0069 (12)
O110.0280 (12)0.0377 (14)0.0196 (12)0.0158 (10)0.0130 (10)0.0123 (10)
O120.0315 (13)0.0418 (14)0.0240 (12)0.0234 (11)0.0155 (10)0.0178 (11)
O130.0271 (13)0.0688 (18)0.0272 (13)0.0275 (13)0.0146 (11)0.0238 (13)
N10.0276 (15)0.0430 (18)0.0291 (16)0.0123 (13)0.0137 (13)0.0152 (14)
N20.0338 (16)0.0351 (17)0.0316 (16)0.0160 (13)0.0139 (13)0.0170 (14)
C10.0338 (19)0.0238 (18)0.0276 (19)0.0091 (15)0.0082 (15)0.0054 (15)
C20.0323 (19)0.0286 (19)0.0274 (19)0.0091 (15)0.0107 (16)0.0085 (15)
C30.0325 (19)0.0279 (19)0.0270 (19)0.0117 (15)0.0102 (16)0.0072 (15)
C40.0290 (19)0.029 (2)0.045 (2)0.0075 (16)0.0120 (17)0.0087 (18)
C50.044 (2)0.033 (2)0.054 (3)0.0065 (18)0.024 (2)0.014 (2)
C60.050 (2)0.028 (2)0.043 (2)0.0132 (17)0.0213 (19)0.0194 (18)
C70.041 (2)0.037 (2)0.038 (2)0.0188 (18)0.0109 (18)0.0096 (18)
C80.041 (2)0.038 (2)0.0250 (19)0.0164 (17)0.0063 (16)0.0113 (17)
B1—O11.421 (4)O13—H13A0.8200
B1—O31.480 (4)N1—C71.489 (5)
B1—O41.496 (4)N1—H1A0.8900
B1—O61.499 (4)N1—H1B0.8900
B2—O11.442 (4)N1—H1C0.8900
B2—O91.463 (4)N2—C81.497 (4)
B2—O21.477 (4)N2—H2A0.8900
B2—O71.509 (4)N2—H2B0.8900
B3—O21.354 (4)N2—H2C0.8900
B3—O31.358 (4)C1—C21.385 (5)
B3—O101.370 (4)C1—C61.391 (5)
B4—O41.351 (4)C1—C71.495 (5)
B4—O111.370 (4)C2—C31.383 (5)
B4—O51.386 (4)C2—H2D0.9300
B5—O61.338 (4)C3—C41.394 (5)
B5—O121.377 (4)C3—C81.492 (5)
B5—O51.380 (4)C4—C51.377 (6)
B6—O71.338 (4)C4—H4A0.9300
B6—O81.377 (4)C5—C61.383 (5)
B6—O12i1.388 (4)C5—H5A0.9300
B7—O91.332 (4)C6—H6A0.9300
B7—O131.368 (4)C7—H7A0.9700
B7—O81.388 (4)C7—H7B0.9700
O10—H10A0.8200C8—H8A0.9700
O11—H11A0.8200C8—H8B0.9700
O12—B6i1.388 (4)
O1—B1—O3112.6 (3)C7—N1—H1B109.5
O1—B1—O4109.6 (3)H1A—N1—H1B109.5
O3—B1—O4107.5 (2)C7—N1—H1C109.5
O1—B1—O6111.1 (3)H1A—N1—H1C109.5
O3—B1—O6107.2 (3)H1B—N1—H1C109.5
O4—B1—O6108.6 (2)C8—N2—H2A109.5
O1—B2—O9108.6 (3)C8—N2—H2B109.5
O1—B2—O2112.9 (2)H2A—N2—H2B109.5
O9—B2—O2109.0 (3)C8—N2—H2C109.5
O1—B2—O7110.2 (3)H2A—N2—H2C109.5
O9—B2—O7110.1 (2)H2B—N2—H2C109.5
O2—B2—O7105.9 (3)C2—C1—C6118.9 (3)
O2—B3—O3121.8 (3)C2—C1—C7118.6 (3)
O2—B3—O10122.5 (3)C6—C1—C7122.2 (3)
O3—B3—O10115.7 (3)C3—C2—C1121.5 (3)
O4—B4—O11120.4 (3)C3—C2—H2D119.2
O4—B4—O5121.5 (3)C1—C2—H2D119.2
O11—B4—O5118.1 (3)C2—C3—C4118.6 (3)
O6—B5—O12124.5 (3)C2—C3—C8120.2 (3)
O6—B5—O5121.6 (3)C4—C3—C8120.9 (3)
O12—B5—O5113.8 (3)C5—C4—C3120.5 (3)
O7—B6—O8122.9 (3)C5—C4—H4A119.8
O7—B6—O12i122.9 (3)C3—C4—H4A119.8
O8—B6—O12i114.2 (3)C4—C5—C6120.3 (4)
O9—B7—O13120.9 (3)C4—C5—H5A119.8
O9—B7—O8122.5 (3)C6—C5—H5A119.8
O13—B7—O8116.6 (3)C5—C6—C1120.1 (3)
B1—O1—B2123.5 (3)C5—C6—H6A120.0
B3—O2—B2122.1 (3)C1—C6—H6A120.0
B3—O3—B1121.8 (2)N1—C7—C1109.5 (3)
B4—O4—B1119.7 (3)N1—C7—H7A109.8
B5—O5—B4118.9 (2)C1—C7—H7A109.8
B5—O6—B1120.7 (2)N1—C7—H7B109.8
B6—O7—B2122.4 (2)C1—C7—H7B109.8
B6—O8—B7117.6 (3)H7A—C7—H7B108.2
B7—O9—B2124.2 (3)C3—C8—N2108.3 (3)
B3—O10—H10A109.5C3—C8—H8A110.0
B4—O11—H11A109.5N2—C8—H8A110.0
B5—O12—B6i132.5 (3)C3—C8—H8B110.0
B7—O13—H13A109.5N2—C8—H8B110.0
C7—N1—H1A109.5H8A—C8—H8B108.4
D—H···AD—HH···AD···AD—H···A
O10—H10A···O2ii0.821.982.784 (2)168
O11—H11A···O3iii0.821.842.659 (2)179
O13—H13A···O11iv0.822.002.815 (2)173
N1—H1A···O70.892.082.863 (2)146
N1—H1B···O13v0.891.982.850 (2)166
N1—H1C···O6i0.892.202.916 (2)137
N1—H1C···O1i0.892.543.394 (2)161
N2—H2A···O4vi0.891.972.822 (2)159
N2—H2B···O1i0.891.992.877 (2)173
N2—H2B···O9i0.892.553.052 (2)116
N2—H2C···O12vii0.892.193.067 (2)168
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯AD—HH⋯ADAD—H⋯A
O10—H10A⋯O2i0.821.982.784 (2)168
O11—H11A⋯O3ii0.821.842.659 (2)179
O13—H13A⋯O11iii0.822.002.815 (2)173
N1—H1A⋯O70.892.082.863 (2)146
N1—H1B⋯O13iv0.891.982.850 (2)166
N1—H1C⋯O6v0.892.202.916 (2)137
N1—H1C⋯O1v0.892.543.394 (2)161
N2—H2A⋯O4vi0.891.972.822 (2)159
N2—H2B⋯O1v0.891.992.877 (2)173
N2—H2B⋯O9v0.892.553.052 (2)116
N2—H2C⋯O12vii0.892.193.067 (2)168

Symmetry codes: (i) ; (ii) ; (iii) ; (iv) ; (v) ; (vi) ; (vii) .

  3 in total

1.  A short history of SHELX.

Authors:  George M Sheldrick
Journal:  Acta Crystallogr A       Date:  2007-12-21       Impact factor: 2.290

2.  Two new borates containing the first examples of large isolated polyborate anions: chain [B7O9(OH)5]2- and ring [B14O20(OH)6]4-.

Authors:  Zhi-Hong Liu; Lian-Qing Li; Wen-Juan Zhang
Journal:  Inorg Chem       Date:  2006-02-20       Impact factor: 5.165

3.  Guanidinium and imidazolium borates containing the first examples of an isolated nonaborate oxoanion: [B9O12(OH)6]3-.

Authors:  D M Schubert; M Z Visi; C B Knobler
Journal:  Inorg Chem       Date:  2000-05-29       Impact factor: 5.165

  3 in total

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