Abstract
In the crystal structure of the title compound, C9H14BNO4, the boronic acid group and carbamate groups are nearly co-planar with the pyrrole ring, making dihedral angles of 0.1 (2) and 2.2 (2)°, respectively. Intramolecular and intermolecular O—H⋯O hydrogen bonds help to stabilize the structure, the latter interaction leading to inversion dimers..
Related literature
For general background, see: Hall (2005 ▶); Kelly & Fuchs (1993 ▶).
Experimental
Crystal data
C9H14BNO4
M r = 211.02
Orthorhombic,
a = 13.014 (3) Å
b = 9.940 (2) Å
c = 17.417 (4) Å
V = 2252.9 (9) Å3
Z = 8
Mo Kα radiation
μ = 0.10 mm−1
T = 293 K
0.25 × 0.12 × 0.10 mm
Data collection
Bruker SMART 1000 CCD area-detector diffractometer
Absorption correction: none
9542 measured reflections
2213 independent reflections
1208 reflections with I > 2σ(I)
R int = 0.065
Refinement
R[F 2 > 2σ(F 2)] = 0.042
wR(F 2) = 0.106
S = 0.85
2213 reflections
192 parameters
All H-atom parameters refined
Δρmax = 0.12 e Å−3
Δρmin = −0.21 e Å−3
Data collection: SMART (Bruker, 2001 ▶); cell refinement: SAINT (Bruker, 2001 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.
Supplementary Material
Crystal structure: contains datablocks I, New_Global_Publ_Block. DOI: 10.1107/S1600536809007375/xu2484sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536809007375/xu2484Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| O3—H3A⋯O2 | 0.87 (2) | 1.73 (2) | 2.5819 (18) | 164.7 (18) |
| O4—H4⋯O3i | 0.89 (3) | 1.88 (3) | 2.769 (3) | 173 (3) |
Symmetry code: (i)
.
Acknowledgments
We thank Professor Lin-Hong Weng, Fudan University, for the X-ray analysis.
supplementary crystallographic information
Comment
Boronic acids are versatile compounds widely used in the synthesis of biaryls, as therapeutical agents, and as chemical sensors (Hall, 2005). The title compound is the key intermediate for the synthesis of (+)-pinanediol-L-boroproline (Kelly & Fuchs, 1993).
In the molecular structure of the title compound (Fig. 1), the pyrrole ring, the boronic acid group and the carboxyl groups are almost co-planar. The carbonyl links with the adjacent boronic acid group via O3—H3···O2 hydrogen bonding. Intermolecular hydrogen bond is also observed in the crystal structure (Table 1).
Experimental
All chemical reagents are commercial and used as received. Under -78°C and argon atmosphere, lithium diisopropylamide (1.0 M in THF, 5.0 ml, 5.0 mmol) was added dropwise to a solution of tert-butyl 1H-pyrrole-1-carboxylate (835 mg, 5.0 mmol) in dry THF (15 ml), and the solution was stirred at this temperature for 30 min. Trimethylborate (1.7 ml, 15 mmol) was added dropwise, and the mixture was allowed to warm to room temperature over 2 h and stirred overnight. After aqueous workup, the crude product was crystallized from hexanes. Single crystals suitable for X-ray analysis were obtained by recrystallization from a mixed solvent of ethyl acetate and hexane at ambient temperature (20–25°C).
Refinement
H atoms were located in a difference Fourier map and refined isotropically.
Figures
Fig. 1.
The molecular structure of the title compound with displacement ellipsoids drawn at the 50% probability level. H atoms are drawn as spheres of arbitrary radii.
Crystal data
| C9H14BNO4 | F(000) = 896 |
| Mr = 211.02 | Dx = 1.244 Mg m−3 |
| Orthorhombic, Pbca | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2ac 2ab | Cell parameters from 810 reflections |
| a = 13.014 (3) Å | θ = 2.3–22.4° |
| b = 9.940 (2) Å | µ = 0.10 mm−1 |
| c = 17.417 (4) Å | T = 293 K |
| V = 2252.9 (9) Å3 | Prism, colorless |
| Z = 8 | 0.25 × 0.12 × 0.10 mm |
Data collection
| Bruker SMART 1000 CCD area-detector diffractometer | 1208 reflections with I > 2σ(I) |
| Radiation source: fine-focus sealed tube | Rint = 0.065 |
| graphite | θmax = 26.0°, θmin = 2.3° |
| φ and ω scans | h = −16→13 |
| 9542 measured reflections | k = −12→12 |
| 2213 independent reflections | l = −21→19 |
Refinement
| 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)] = 0.042 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.106 | All H-atom parameters refined |
| S = 0.85 | w = 1/[σ2(Fo2) + (0.0588P)2] where P = (Fo2 + 2Fc2)/3 |
| 2213 reflections | (Δ/σ)max < 0.001 |
| 192 parameters | Δρmax = 0.12 e Å−3 |
| 0 restraints | Δρmin = −0.20 e Å−3 |
Special details
| 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. |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)
| x | y | z | Uiso*/Ueq | ||
| B1 | 1.03949 (15) | 0.6990 (2) | 0.51802 (11) | 0.0727 (6) | |
| C1 | 1.09811 (14) | 1.0494 (2) | 0.59196 (12) | 0.0767 (5) | |
| C2 | 1.17519 (16) | 1.0274 (3) | 0.54329 (13) | 0.0893 (7) | |
| C3 | 1.16298 (14) | 0.8995 (3) | 0.51194 (12) | 0.0821 (6) | |
| C4 | 1.07732 (12) | 0.83956 (18) | 0.54116 (8) | 0.0644 (5) | |
| C5 | 0.94986 (12) | 0.92187 (19) | 0.63777 (9) | 0.0635 (4) | |
| C6 | 0.85439 (15) | 1.03344 (19) | 0.74024 (10) | 0.0771 (5) | |
| C7 | 0.75166 (18) | 1.0282 (3) | 0.70204 (16) | 0.0955 (7) | |
| C8 | 0.8711 (3) | 0.9215 (3) | 0.79700 (14) | 0.1000 (7) | |
| C9 | 0.8746 (3) | 1.1693 (3) | 0.7756 (2) | 0.1119 (9) | |
| N1 | 1.03646 (9) | 0.93560 (14) | 0.59221 (7) | 0.0631 (4) | |
| O1 | 0.93714 (8) | 1.02801 (13) | 0.68119 (7) | 0.0754 (4) | |
| O2 | 0.89519 (9) | 0.82427 (13) | 0.63724 (7) | 0.0776 (4) | |
| O3 | 0.95566 (10) | 0.63485 (15) | 0.54641 (8) | 0.0921 (5) | |
| O4 | 1.09809 (10) | 0.6338 (2) | 0.46635 (8) | 0.0960 (5) | |
| H3 | 1.2044 (14) | 0.8510 (17) | 0.4741 (10) | 0.083 (5)* | |
| H7A | 0.7006 (17) | 1.040 (2) | 0.7397 (13) | 0.104 (7)* | |
| H7B | 0.7430 (18) | 1.106 (3) | 0.6664 (14) | 0.131 (10)* | |
| H8A | 0.8247 (16) | 0.934 (2) | 0.8403 (14) | 0.109 (7)* | |
| H1 | 1.0760 (14) | 1.126 (2) | 0.6241 (11) | 0.089 (6)* | |
| H9A | 0.8259 (16) | 1.184 (2) | 0.8132 (14) | 0.122 (8)* | |
| H9B | 0.8706 (15) | 1.236 (2) | 0.7359 (14) | 0.109 (9)* | |
| H7C | 0.7384 (15) | 0.942 (2) | 0.6764 (13) | 0.104 (7)* | |
| H2 | 1.2262 (17) | 1.090 (2) | 0.5323 (11) | 0.104 (7)* | |
| H8B | 0.941 (2) | 0.928 (2) | 0.8167 (14) | 0.130 (9)* | |
| H9C | 0.949 (2) | 1.169 (3) | 0.7937 (16) | 0.169 (12)* | |
| H8C | 0.8565 (17) | 0.826 (3) | 0.7735 (14) | 0.135 (9)* | |
| H3A | 0.9265 (14) | 0.6888 (19) | 0.5791 (11) | 0.087 (6)* | |
| H4 | 1.080 (2) | 0.548 (3) | 0.4581 (16) | 0.145 (12)* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| B1 | 0.0572 (11) | 0.1046 (17) | 0.0563 (11) | 0.0146 (11) | −0.0040 (9) | −0.0053 (11) |
| C1 | 0.0616 (11) | 0.0916 (15) | 0.0767 (12) | −0.0077 (11) | −0.0134 (10) | 0.0135 (12) |
| C2 | 0.0590 (12) | 0.120 (2) | 0.0888 (15) | −0.0117 (12) | −0.0074 (11) | 0.0335 (14) |
| C3 | 0.0565 (11) | 0.1260 (19) | 0.0638 (11) | 0.0091 (12) | 0.0003 (9) | 0.0161 (13) |
| C4 | 0.0524 (9) | 0.0915 (13) | 0.0492 (8) | 0.0113 (9) | −0.0034 (7) | 0.0069 (9) |
| C5 | 0.0586 (10) | 0.0744 (12) | 0.0576 (9) | 0.0032 (9) | −0.0030 (8) | 0.0004 (9) |
| C6 | 0.0834 (13) | 0.0832 (13) | 0.0647 (11) | 0.0110 (10) | 0.0065 (9) | −0.0149 (10) |
| C7 | 0.0793 (15) | 0.116 (2) | 0.0913 (17) | 0.0166 (14) | 0.0054 (13) | −0.0170 (17) |
| C8 | 0.119 (2) | 0.115 (2) | 0.0655 (13) | 0.0172 (16) | 0.0126 (14) | 0.0019 (14) |
| C9 | 0.129 (2) | 0.103 (2) | 0.103 (2) | 0.0076 (16) | 0.0117 (18) | −0.0376 (18) |
| N1 | 0.0494 (7) | 0.0814 (10) | 0.0585 (8) | −0.0007 (7) | −0.0031 (6) | 0.0075 (7) |
| O1 | 0.0787 (8) | 0.0766 (8) | 0.0708 (7) | −0.0010 (6) | 0.0069 (6) | −0.0128 (7) |
| O2 | 0.0698 (7) | 0.0786 (9) | 0.0844 (8) | −0.0067 (6) | 0.0214 (6) | −0.0166 (7) |
| O3 | 0.0730 (8) | 0.1037 (11) | 0.0996 (10) | −0.0004 (7) | 0.0200 (7) | −0.0384 (8) |
| O4 | 0.0799 (9) | 0.1217 (14) | 0.0863 (9) | 0.0147 (8) | 0.0190 (7) | −0.0238 (9) |
Geometric parameters (Å, °)
| B1—O4 | 1.346 (2) | C6—C7 | 1.494 (3) |
| B1—O3 | 1.357 (2) | C6—C8 | 1.504 (3) |
| B1—C4 | 1.535 (3) | C6—C9 | 1.507 (3) |
| C1—C2 | 1.331 (3) | C7—H7A | 0.94 (2) |
| C1—N1 | 1.387 (2) | C7—H7B | 0.99 (3) |
| C1—H1 | 0.99 (2) | C7—H7C | 0.98 (2) |
| C2—C3 | 1.393 (3) | C8—H8A | 0.97 (2) |
| C2—H2 | 0.93 (2) | C8—H8B | 0.98 (3) |
| C3—C4 | 1.363 (3) | C8—H8C | 1.05 (3) |
| C3—H3 | 0.978 (18) | C9—H9A | 0.92 (2) |
| C4—N1 | 1.409 (2) | C9—H9B | 0.96 (2) |
| C5—O2 | 1.2030 (19) | C9—H9C | 1.02 (3) |
| C5—O1 | 1.309 (2) | O3—H3A | 0.87 (2) |
| C5—N1 | 1.385 (2) | O4—H4 | 0.89 (3) |
| C6—O1 | 1.490 (2) | ||
| O4—B1—O3 | 118.2 (2) | C6—C7—H7A | 108.5 (13) |
| O4—B1—C4 | 115.60 (19) | C6—C7—H7B | 110.6 (14) |
| O3—B1—C4 | 126.14 (17) | H7A—C7—H7B | 105.0 (18) |
| C2—C1—N1 | 107.7 (2) | C6—C7—H7C | 112.9 (12) |
| C2—C1—H1 | 135.0 (12) | H7A—C7—H7C | 107.4 (18) |
| N1—C1—H1 | 117.2 (11) | H7B—C7—H7C | 112 (2) |
| C1—C2—C3 | 108.3 (2) | C6—C8—H8A | 109.2 (12) |
| C1—C2—H2 | 123.9 (13) | C6—C8—H8B | 108.4 (15) |
| C3—C2—H2 | 127.8 (13) | H8A—C8—H8B | 107 (2) |
| C4—C3—C2 | 110.3 (2) | C6—C8—H8C | 112.7 (13) |
| C4—C3—H3 | 119.1 (11) | H8A—C8—H8C | 107.5 (18) |
| C2—C3—H3 | 130.7 (10) | H8B—C8—H8C | 111 (2) |
| C3—C4—N1 | 104.36 (18) | C6—C9—H9A | 107.9 (16) |
| C3—C4—B1 | 124.22 (18) | C6—C9—H9B | 108.3 (13) |
| N1—C4—B1 | 131.40 (15) | H9A—C9—H9B | 112 (2) |
| O2—C5—O1 | 125.44 (15) | C6—C9—H9C | 107.0 (17) |
| O2—C5—N1 | 123.79 (16) | H9A—C9—H9C | 116 (2) |
| O1—C5—N1 | 110.77 (15) | H9B—C9—H9C | 106 (2) |
| O1—C6—C7 | 109.75 (16) | C5—N1—C1 | 123.57 (16) |
| O1—C6—C8 | 108.80 (16) | C5—N1—C4 | 127.01 (15) |
| C7—C6—C8 | 113.4 (2) | C1—N1—C4 | 109.41 (16) |
| O1—C6—C9 | 100.86 (18) | C5—O1—C6 | 121.30 (13) |
| C7—C6—C9 | 111.6 (2) | B1—O3—H3A | 107.4 (12) |
| C8—C6—C9 | 111.6 (2) | B1—O4—H4 | 114.5 (18) |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| O4—H4···O3i | 0.89 (3) | 1.88 (3) | 2.769 (3) | 173 (3) |
| O3—H3A···O2 | 0.87 (2) | 1.73 (2) | 2.5819 (18) | 164.7 (18) |
Symmetry codes: (i) −x+2, −y+1, −z+1.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: XU2484).
References
Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablocks I, New_Global_Publ_Block. DOI: 10.1107/S1600536809007375/xu2484sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536809007375/xu2484Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report

