
Acta Cryst. (2012). E68, o3070 [ doi:10.1107/S1600536812040974 ]
B)-4-Methyl-3-pyridyl[N-methyliminodiacetate-O,O',N]boraneThe title compound, C11H13BN2O4, has a rigid bicyclic structure due to an intramolecular nitrogen-boron dative bond. The B atom is in a distorted tetrahedron environment with a B-N bond length of 1.640 (2) Å, which is in good comparison with the values in analogues compounds. In the crystal, the molecules are linked by weak C-H
O and C-H
N interactions, forming a three-dimensional network.
The title compound was received from Aldrich. Single crystals suitable for X-ray diffraction analysis were grown by cooling a solution of the ester (0.2 g) in diethyl ether (10 ml) and dimethyl sulfoxide (5 ml).
All H atoms were placed in calculated positions with C—H distances of 0.95 Å (phenyl), 0.98 Å (methyl) and 0.99 Å (methylene). They were located in difference maps and were included in the refinement in riding approximation with Uiso(phenyl and methylene H) = 1.2Ueq(C) and Uiso(methyl H) = 1.5Ueq(C).
Data collection: CrysAlis PRO (Agilent, 2011); cell refinement: CrysAlis PRO (Agilent, 2011); data reduction: CrysAlis PRO (Agilent, 2011); program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg, 2005); software used to prepare material for publication: SHELXTL (Sheldrick, 2008) and PLATON (Spek, 2009).
| C11H13BN2O4 | F(000) = 520 |
| Mr = 248.04 | Dx = 1.423 Mg m−3 |
| Monoclinic, P21/n | Mo Kα radiation, λ = 0.7107 Å |
| Hall symbol: -P 2yn | Cell parameters from 9561 reflections |
| a = 7.306 (3) Å | θ = 1.9–32.2° |
| b = 14.7425 (4) Å | µ = 0.11 mm−1 |
| c = 10.8281 (19) Å | T = 100 K |
| β = 96.91 (4)° | Unshaped, colourless |
| V = 1157.8 (5) Å3 | 0.16 × 0.12 × 0.10 mm |
| Z = 4 |
| Agilent Xcalibur Opal diffractometer | 3993 independent reflections |
| Radiation source: Enhance (Mo) X-ray Source | 3148 reflections with I > 2σ(I) |
| Graphite monochromator | Rint = 0.075 |
| Detector resolution: 8.4441 pixels mm-1 | θmax = 32.3°, θmin = 2.3° |
| ω scan | h = −10→10 |
| Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2011) | k = −21→21 |
| Tmin = 0.910, Tmax = 0.989 | l = −16→16 |
| 26273 measured reflections |
| 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)] = 0.052 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.147 | H-atom parameters constrained |
| S = 1.07 | w = 1/[σ2(Fo2) + (0.0715P)2 + 0.4349P] where P = (Fo2 + 2Fc2)/3 |
| 3993 reflections | (Δ/σ)max < 0.001 |
| 163 parameters | Δρmax = 0.47 e Å−3 |
| 0 restraints | Δρmin = −0.43 e Å−3 |
| C11H13BN2O4 | V = 1157.8 (5) Å3 |
| Mr = 248.04 | Z = 4 |
| Monoclinic, P21/n | Mo Kα radiation |
| a = 7.306 (3) Å | µ = 0.11 mm−1 |
| b = 14.7425 (4) Å | T = 100 K |
| c = 10.8281 (19) Å | 0.16 × 0.12 × 0.10 mm |
| β = 96.91 (4)° |
| Agilent Xcalibur Opal diffractometer | 3993 independent reflections |
| Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2011) | 3148 reflections with I > 2σ(I) |
| Tmin = 0.910, Tmax = 0.989 | Rint = 0.075 |
| 26273 measured reflections | θmax = 32.3° |
| R[F2 > 2σ(F2)] = 0.052 | H-atom parameters constrained |
| wR(F2) = 0.147 | Δρmax = 0.47 e Å−3 |
| S = 1.07 | Δρmin = −0.43 e Å−3 |
| 3993 reflections | Absolute structure: ? |
| 163 parameters | Flack parameter: ? |
| 0 restraints | Rogers parameter: ? |
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 | ||
| C11 | −0.2305 (2) | 0.29350 (10) | 0.44416 (12) | 0.0241 (3) | |
| H12A | −0.1311 | 0.3273 | 0.4117 | 0.036* | |
| H12B | −0.2901 | 0.3322 | 0.5011 | 0.036* | |
| H12C | −0.3216 | 0.2748 | 0.3750 | 0.036* | |
| O1 | 0.10475 (13) | 0.14926 (6) | 0.64076 (9) | 0.0195 (2) | |
| O2 | −0.13312 (13) | 0.22847 (6) | 0.73583 (8) | 0.0196 (2) | |
| N2 | −0.15248 (15) | 0.21153 (7) | 0.51222 (9) | 0.0157 (2) | |
| C2 | 0.11011 (17) | 0.32272 (8) | 0.63785 (11) | 0.0167 (2) | |
| O3 | 0.20124 (15) | 0.04826 (7) | 0.50831 (11) | 0.0275 (2) | |
| O4 | −0.41001 (16) | 0.17271 (7) | 0.76432 (11) | 0.0305 (3) | |
| C8 | −0.04008 (19) | 0.15473 (9) | 0.43621 (12) | 0.0198 (3) | |
| H10A | 0.0208 | 0.1927 | 0.3777 | 0.024* | |
| H10B | −0.1177 | 0.1087 | 0.3882 | 0.024* | |
| C3 | 0.06232 (18) | 0.40943 (9) | 0.67863 (12) | 0.0188 (2) | |
| C9 | −0.29166 (19) | 0.18660 (8) | 0.69872 (12) | 0.0199 (3) | |
| B1 | −0.01072 (19) | 0.23263 (9) | 0.63818 (12) | 0.0157 (2) | |
| C10 | −0.30028 (19) | 0.15837 (9) | 0.56364 (13) | 0.0213 (3) | |
| H8A | −0.2776 | 0.0925 | 0.5570 | 0.026* | |
| H8B | −0.4226 | 0.1727 | 0.5181 | 0.026* | |
| C4 | 0.1896 (2) | 0.47963 (9) | 0.67544 (13) | 0.0228 (3) | |
| H4 | 0.1618 | 0.5384 | 0.7041 | 0.027* | |
| C7 | 0.10090 (18) | 0.11005 (8) | 0.53041 (12) | 0.0189 (2) | |
| C1 | 0.28286 (19) | 0.31591 (10) | 0.59509 (14) | 0.0246 (3) | |
| H1 | 0.3165 | 0.2579 | 0.5669 | 0.029* | |
| N1 | 0.40557 (18) | 0.38297 (9) | 0.58999 (14) | 0.0305 (3) | |
| C6 | −0.1176 (2) | 0.43051 (10) | 0.72727 (17) | 0.0310 (3) | |
| H6A | −0.1941 | 0.3757 | 0.7236 | 0.046* | |
| H6B | −0.1825 | 0.4781 | 0.6762 | 0.046* | |
| H6C | −0.0934 | 0.4514 | 0.8136 | 0.046* | |
| C5 | 0.3558 (2) | 0.46393 (10) | 0.63083 (15) | 0.0274 (3) | |
| H5 | 0.4393 | 0.5132 | 0.6290 | 0.033* |
| U11 | U22 | U33 | U12 | U13 | U23 | |
| C11 | 0.0284 (7) | 0.0246 (6) | 0.0183 (6) | 0.0100 (5) | −0.0018 (5) | 0.0020 (5) |
| O1 | 0.0217 (5) | 0.0160 (4) | 0.0201 (4) | 0.0042 (3) | −0.0009 (3) | 0.0005 (3) |
| O2 | 0.0235 (5) | 0.0203 (4) | 0.0153 (4) | −0.0028 (3) | 0.0043 (3) | −0.0011 (3) |
| N2 | 0.0161 (5) | 0.0157 (4) | 0.0153 (4) | 0.0022 (4) | 0.0014 (4) | −0.0016 (3) |
| C2 | 0.0160 (5) | 0.0167 (5) | 0.0173 (5) | 0.0009 (4) | 0.0016 (4) | −0.0001 (4) |
| O3 | 0.0270 (5) | 0.0197 (5) | 0.0372 (6) | 0.0076 (4) | 0.0092 (4) | −0.0022 (4) |
| O4 | 0.0326 (6) | 0.0271 (5) | 0.0355 (6) | −0.0047 (4) | 0.0198 (5) | −0.0006 (4) |
| C8 | 0.0228 (6) | 0.0207 (6) | 0.0164 (5) | 0.0042 (5) | 0.0043 (4) | −0.0027 (4) |
| C3 | 0.0192 (6) | 0.0171 (5) | 0.0201 (5) | 0.0006 (4) | 0.0030 (4) | −0.0009 (4) |
| C9 | 0.0227 (6) | 0.0147 (5) | 0.0234 (6) | 0.0006 (4) | 0.0080 (5) | −0.0012 (4) |
| B1 | 0.0172 (6) | 0.0152 (6) | 0.0144 (5) | 0.0016 (5) | 0.0010 (5) | −0.0007 (4) |
| C10 | 0.0186 (6) | 0.0204 (6) | 0.0257 (6) | −0.0026 (5) | 0.0052 (5) | −0.0057 (5) |
| C4 | 0.0261 (7) | 0.0155 (5) | 0.0268 (6) | −0.0019 (5) | 0.0030 (5) | 0.0003 (5) |
| C7 | 0.0195 (6) | 0.0148 (5) | 0.0231 (6) | 0.0007 (4) | 0.0053 (5) | 0.0001 (4) |
| C1 | 0.0192 (6) | 0.0231 (6) | 0.0325 (7) | −0.0002 (5) | 0.0079 (5) | −0.0049 (5) |
| N1 | 0.0219 (6) | 0.0286 (6) | 0.0431 (7) | −0.0049 (5) | 0.0120 (5) | −0.0048 (5) |
| C6 | 0.0267 (7) | 0.0213 (6) | 0.0475 (9) | 0.0007 (5) | 0.0155 (7) | −0.0108 (6) |
| C5 | 0.0254 (7) | 0.0232 (6) | 0.0344 (7) | −0.0073 (5) | 0.0062 (6) | 0.0010 (5) |
| C11—N2 | 1.4924 (17) | C8—H10A | 0.9900 |
| C11—H12A | 0.9800 | C8—H10B | 0.9900 |
| C11—H12B | 0.9800 | C3—C4 | 1.3947 (18) |
| C11—H12C | 0.9800 | C3—C6 | 1.506 (2) |
| O1—C7 | 1.3246 (16) | C9—C10 | 1.5147 (19) |
| O1—B1 | 1.4891 (16) | C10—H8A | 0.9900 |
| O2—C9 | 1.3313 (17) | C10—H8B | 0.9900 |
| O2—B1 | 1.4660 (17) | C4—C5 | 1.379 (2) |
| N2—C8 | 1.4884 (16) | C4—H4 | 0.9500 |
| N2—C10 | 1.4950 (18) | C1—N1 | 1.3403 (19) |
| N2—B1 | 1.6400 (19) | C1—H1 | 0.9500 |
| C2—C1 | 1.3993 (19) | N1—C5 | 1.338 (2) |
| C2—C3 | 1.4101 (17) | C6—H6A | 0.9800 |
| C2—B1 | 1.5950 (19) | C6—H6B | 0.9800 |
| O3—C7 | 1.2111 (16) | C6—H6C | 0.9800 |
| O4—C9 | 1.2009 (17) | C5—H5 | 0.9500 |
| C8—C7 | 1.511 (2) | ||
| N2—C11—H12A | 109.5 | O2—B1—C2 | 114.98 (10) |
| N2—C11—H12B | 109.5 | O1—B1—C2 | 112.01 (11) |
| H12A—C11—H12B | 109.5 | O2—B1—N2 | 102.29 (10) |
| N2—C11—H12C | 109.5 | O1—B1—N2 | 99.13 (9) |
| H12A—C11—H12C | 109.5 | C2—B1—N2 | 116.77 (10) |
| H12B—C11—H12C | 109.5 | N2—C10—C9 | 105.53 (10) |
| C7—O1—B1 | 113.13 (10) | N2—C10—H8A | 110.6 |
| C9—O2—B1 | 112.70 (10) | C9—C10—H8A | 110.6 |
| C8—N2—C11 | 112.70 (10) | N2—C10—H8B | 110.6 |
| C8—N2—C10 | 112.48 (10) | C9—C10—H8B | 110.6 |
| C11—N2—C10 | 110.99 (11) | H8A—C10—H8B | 108.8 |
| C8—N2—B1 | 103.37 (10) | C5—C4—C3 | 120.13 (13) |
| C11—N2—B1 | 115.00 (10) | C5—C4—H4 | 119.9 |
| C10—N2—B1 | 101.65 (9) | C3—C4—H4 | 119.9 |
| C1—C2—C3 | 115.84 (12) | O3—C7—O1 | 123.98 (13) |
| C1—C2—B1 | 117.55 (11) | O3—C7—C8 | 125.05 (12) |
| C3—C2—B1 | 126.60 (11) | O1—C7—C8 | 110.94 (11) |
| N2—C8—C7 | 104.40 (10) | N1—C1—C2 | 126.53 (13) |
| N2—C8—H10A | 110.9 | N1—C1—H1 | 116.7 |
| C7—C8—H10A | 110.9 | C2—C1—H1 | 116.7 |
| N2—C8—H10B | 110.9 | C5—N1—C1 | 115.76 (13) |
| C7—C8—H10B | 110.9 | C3—C6—H6A | 109.5 |
| H10A—C8—H10B | 108.9 | C3—C6—H6B | 109.5 |
| C4—C3—C2 | 118.29 (12) | H6A—C6—H6B | 109.5 |
| C4—C3—C6 | 117.93 (12) | C3—C6—H6C | 109.5 |
| C2—C3—C6 | 123.78 (12) | H6A—C6—H6C | 109.5 |
| O4—C9—O2 | 124.26 (13) | H6B—C6—H6C | 109.5 |
| O4—C9—C10 | 125.11 (13) | N1—C5—C4 | 123.44 (13) |
| O2—C9—C10 | 110.63 (11) | N1—C5—H5 | 118.3 |
| O2—B1—O1 | 110.20 (10) | C4—C5—H5 | 118.3 |
| C11—N2—C8—C7 | 150.72 (11) | C10—N2—B1—O2 | −25.44 (11) |
| C10—N2—C8—C7 | −82.89 (13) | C8—N2—B1—O1 | −29.06 (11) |
| B1—N2—C8—C7 | 25.95 (12) | C11—N2—B1—O1 | −152.32 (10) |
| C1—C2—C3—C4 | −1.18 (19) | C10—N2—B1—O1 | 87.71 (11) |
| B1—C2—C3—C4 | 177.63 (12) | C8—N2—B1—C2 | 91.36 (12) |
| C1—C2—C3—C6 | 179.70 (14) | C11—N2—B1—C2 | −31.90 (15) |
| B1—C2—C3—C6 | −1.5 (2) | C10—N2—B1—C2 | −151.87 (11) |
| B1—O2—C9—O4 | 177.44 (13) | C8—N2—C10—C9 | 134.54 (11) |
| B1—O2—C9—C10 | −1.95 (15) | C11—N2—C10—C9 | −98.15 (12) |
| C9—O2—B1—O1 | −87.36 (13) | B1—N2—C10—C9 | 24.61 (12) |
| C9—O2—B1—C2 | 144.91 (11) | O4—C9—C10—N2 | 164.50 (13) |
| C9—O2—B1—N2 | 17.32 (13) | O2—C9—C10—N2 | −16.11 (14) |
| C7—O1—B1—O2 | 129.43 (11) | C2—C3—C4—C5 | 1.3 (2) |
| C7—O1—B1—C2 | −101.22 (12) | C6—C3—C4—C5 | −179.51 (14) |
| C7—O1—B1—N2 | 22.64 (13) | B1—O1—C7—O3 | 170.72 (12) |
| C1—C2—B1—O2 | 149.59 (12) | B1—O1—C7—C8 | −7.42 (15) |
| C3—C2—B1—O2 | −29.19 (18) | N2—C8—C7—O3 | 168.47 (12) |
| C1—C2—B1—O1 | 22.78 (16) | N2—C8—C7—O1 | −13.41 (14) |
| C3—C2—B1—O1 | −156.01 (12) | C3—C2—C1—N1 | 0.4 (2) |
| C1—C2—B1—N2 | −90.54 (14) | B1—C2—C1—N1 | −178.55 (14) |
| C3—C2—B1—N2 | 90.67 (15) | C2—C1—N1—C5 | 0.4 (2) |
| C8—N2—B1—O2 | −142.20 (10) | C1—N1—C5—C4 | −0.2 (2) |
| C11—N2—B1—O2 | 94.54 (12) | C3—C4—C5—N1 | −0.6 (2) |
| D—H···A | D—H | H···A | D···A | D—H···A |
| C8—H10A···O4i | 0.99 | 2.42 | 3.356 (1) | 158 |
| C11—H12B···N1ii | 0.98 | 2.64 | 3.509 (1) | 149 |
| C11—H12A···O4i | 0.98 | 2.40 | 3.259 (1) | 146 |
| C10—H8A···O3iii | 0.99 | 2.28 | 3.247 (1) | 165 |
| C11—H12C···O2iv | 0.98 | 2.57 | 3.500 (1) | 158 |
| Symmetry codes: (i) x+1/2, −y+1/2, z−1/2; (ii) x−1, y, z; (iii) −x, −y, −z+1; (iv) x−1/2, −y+1/2, z−1/2. |
| D—H···A | D—H | H···A | D···A | D—H···A |
| C8—H10A···O4i | 0.99 | 2.418 | 3.356 (1) | 158 |
| C11—H12B···N1ii | 0.98 | 2.635 | 3.509 (1) | 149 |
| C11—H12A···O4i | 0.98 | 2.403 | 3.259 (1) | 146 |
| C10—H8A···O3iii | 0.99 | 2.283 | 3.247 (1) | 165 |
| C11—H12C···O2iv | 0.98 | 2.574 | 3.500 (1) | 158 |
| Symmetry codes: (i) x+1/2, −y+1/2, z−1/2; (ii) x−1, y, z; (iii) −x, −y, −z+1; (iv) x−1/2, −y+1/2, z−1/2. |
The X-ray measurements were undertaken in the Crystallographic Unit of the Physical Chemistry Laboratory at the Chemistry Department of the University of Warsaw. This work was supported by the Aldrich Chemical Co. through donation of chemicals and equipment and by the Warsaw University of Technology.
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Boron heterocycles derived from amino acids have received considerable attention due to their utilization in organic synthesis and medicine. Boronic acids that are susceptible to degradations are protected with N-methyliminodiacetic acid (MIDA) ligand. The MIDA boronates are compatible with a wide range of common synthetic reagents, allowing them to be functionalized to create complex boronic acid derivatives (Mancilla et al., 1997, 2005; Gillis et al., 2008; Knapp et al., 2009; Percino et al., 2009). Our interest has focused on the MIDA esters of pyridineboronic acids and their structural behavior.
In the title compound, the boron atom has a tetrahedral geometry with bond angles at the B atom ranging from 99.1 (2) to 116.8 (1)°. The B—O [1.466 (2) and 1.489 (2) Å] and B—C [1.595 (2) Å] bond lengths are in the normal ranges for such compounds. The B—N bond length is equal to 1.640 (2) Å and is similar to the values found in the other structures of MIDA boronate esters. As indicated by the C1—B1—N2—C11 and C2—C2—B1—O1 torsion angles, the bicycle ring is significantly distorted and the aryl unit is twisted along C—B bond. The crystal structure is dominated by weak C—H···O and C—H···N hydrogen interactions (Table 1).