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In the crystal structure, the title compound, C25H52BNO3Si, a vinyl­ic α-carbamoyl­oxyborane, forms the five-membered ring of an alkyl­idene oxoniaboratadi­hydro­furan as a result of the bonding interaction of the carbonyl group with the boron atom. The ring is almost planar, with the boron atom in a tetrahedral configuration. The mol­ecule exhibits a carbenoid-type bonding arrangement.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536802003215/cv6092sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536802003215/cv6092Isup2.hkl
Contains datablock I

CCDC reference: 182641

Key indicators

  • Single-crystal X-ray study
  • T = 193 K
  • Mean [sigma](C-C) = 0.007 Å
  • R factor = 0.059
  • wR factor = 0.169
  • Data-to-parameter ratio = 10.6

checkCIF results

No syntax errors found

ADDSYM reports no extra symmetry


Red Alert Alert Level A:
THETM_01 Alert A The value of sine(theta_max)/wavelength is less than 0.550 Calculated sin(theta_max)/wavelength = 0.5327 General Notes
ABSTM_02 When printed, the submitted absorption T values will be replaced by the scaled T values. Since the ratio of scaled T's is identical to the ratio of reported T values, the scaling does not imply a change to the absorption corrections used in the study. Ratio of Tmax expected/reported 1.372 Tmax scaled 0.919 Tmin scaled 0.686
1 Alert Level A = Potentially serious problem
0 Alert Level B = Potential problem
0 Alert Level C = Please check

Comment top

Nucleophilic substitution at cyclopropane and especially vinyl-type carbon atoms occurs only if the respective carbon bears both a metal and a leaving group (carbenoid) (Boche & Lohrenz, 2001; Kocieński & Barber, 1990), or if a metallate rearrangement is involved. The latter requires a leaving group and an -ate complex of Al, B, Cu, Ni, Zn or Zr at the same carbon atom (Nelson & Matthews, 1994; Harada et al., 1993; Sidduri et al., 1993). Here we describe the solid-state structure of the vinylic α-carbamoyloxy boran, (I), which was formed from the corresponding lithium borate and acetic acid (Birkinshaw & Kocieński, 1991).

Owing to the bonding contact of the carbonyl group to boron, the structure has to be described as an oxoniaborata dihydrofuran. A comparable situation can be found in the crystal structure of 2,2-Diethyl-3,4-dimethoxy-5-((1-phenylethyl)amino)1-oxonia-2-borata -1(5),3-cyclopentadiene (Barua et al., 1987).

Most remarkably, the C1—O1 bond is lengthened to 1.460 (4) Å. In six non-metallated carbamoyloxy-substituted vinylic compounds, the mean Csp2O(carbamoyloxy) value is 1.396 Å (Boche et al. 1992). It thus turns out that a boron substituent together with a leaving group leads also to a carbenoid-type bonding situation, as is the case with lithium (Boche & Lohrenz, 2001; Boche et al., 1992).

Experimental top

Please give some details of the preparation of the title compound.

Refinement top

The disorder of the isopropyl group bonded to C5 was refined using restraints for distances and temperature factores.

Computing details top

Data collection: CAD-4 EXPRESS (Enraf-Nonius, 1994); cell refinement: CAD-4 EXPRESS; data reduction: XCAD4 (Harms, 1997); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: DIAMOND (Brandenburg, 2001); software used to prepare material for publication: SHELXTL (Sheldrick, 1996).

Figures top
[Figure 1] Fig. 1. DIAMOND (Brandenburg, 2001) drawing of the title compound, showing the atomic numbering and disorder of the isopropyl group bonded to C5. Displacement ellipsoids are drawn here at the 30% probability level. Methyl and methylene H atoms are not shown.
3,3-diethyl-5-diisopropylamino-2- (2,4-dimethyl-3-(tert-butyl-dimethylsilyloxy)-pentyliden)- 4-oxonia-3-borata-2,3-dihydrofuran top
Crystal data top
C25H52BNO3SiF(000) = 1008
Mr = 453.58Dx = 0.995 Mg m3
Monoclinic, P21/nCu Kα radiation, λ = 1.54178 Å
a = 14.684 (6) ÅCell parameters from 25 reflections
b = 9.355 (1) Åθ = 35–50°
c = 22.515 (9) ŵ = 0.84 mm1
β = 101.68 (2)°T = 193 K
V = 3028.8 (18) Å3Needle, colorless
Z = 40.4 × 0.2 × 0.1 mm
Data collection top
Enraf Nonius CAD-4
diffractometer
2882 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.046
Graphite monochromatorθmax = 55.2°, θmin = 4.0°
ω scansh = 015
Absorption correction: part of the refinement model (ΔF)
(DIFABS; Walker & Stuart, 1983)
k = 09
Tmin = 0.50, Tmax = 0.67l = 2323
3959 measured reflections2 standard reflections every 60 min
3786 independent reflections intensity decay: none
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.059Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.169H atoms treated by a mixture of independent and constrained refinement
S = 1.04 w = 1/[σ2(Fo2) + (0.0818P)2 + 2.3718P]
where P = (Fo2 + 2Fc2)/3
3786 reflections(Δ/σ)max < 0.001
356 parametersΔρmax = 0.55 e Å3
25 restraintsΔρmin = 0.18 e Å3
Crystal data top
C25H52BNO3SiV = 3028.8 (18) Å3
Mr = 453.58Z = 4
Monoclinic, P21/nCu Kα radiation
a = 14.684 (6) ŵ = 0.84 mm1
b = 9.355 (1) ÅT = 193 K
c = 22.515 (9) Å0.4 × 0.2 × 0.1 mm
β = 101.68 (2)°
Data collection top
Enraf Nonius CAD-4
diffractometer
2882 reflections with I > 2σ(I)
Absorption correction: part of the refinement model (ΔF)
(DIFABS; Walker & Stuart, 1983)
Rint = 0.046
Tmin = 0.50, Tmax = 0.67θmax = 55.2°
3959 measured reflections2 standard reflections every 60 min
3786 independent reflections intensity decay: none
Refinement top
R[F2 > 2σ(F2)] = 0.05925 restraints
wR(F2) = 0.169H atoms treated by a mixture of independent and constrained refinement
S = 1.04Δρmax = 0.55 e Å3
3786 reflectionsΔρmin = 0.18 e Å3
356 parameters
Special details top

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) top
xyzUiso*/UeqOcc. (<1)
B10.0863 (3)0.3880 (4)0.63219 (18)0.0489 (10)
O10.05233 (16)0.6150 (2)0.68841 (10)0.0547 (6)
O20.11881 (15)0.5355 (2)0.59696 (10)0.0521 (6)
C10.0441 (2)0.4605 (4)0.69673 (16)0.0548 (9)
C20.0079 (3)0.4197 (5)0.75204 (19)0.0740 (13)
H20.005 (3)0.325 (5)0.7562 (18)0.085 (14)*
C30.0219 (4)0.5076 (5)0.8088 (2)0.0938 (17)
H30.037 (3)0.605 (5)0.796 (2)0.103 (15)*
C50.1097 (3)0.4618 (5)0.84798 (19)0.0837 (13)
H5B0.11660.51490.88720.100*0.548 (18)
H5A0.11840.51610.88700.100*0.452 (18)
O30.10279 (16)0.3106 (3)0.86086 (10)0.0606 (7)
Si10.13984 (6)0.22269 (11)0.92340 (4)0.0539 (3)
C90.0881 (3)0.2950 (5)0.98653 (17)0.0801 (12)
H9A0.10910.23761.02310.120*
H9B0.02010.29100.97500.120*
H9C0.10780.39440.99460.120*
C100.2679 (3)0.2308 (5)0.9465 (2)0.0824 (13)
H10A0.28850.16810.98150.124*
H10B0.28710.32920.95750.124*
H10C0.29600.19930.91280.124*
C110.1014 (3)0.0354 (5)0.90311 (18)0.0721 (11)
C120.1355 (5)0.0655 (6)0.9554 (2)0.120 (2)
H12A0.11190.03400.99100.181*
H12B0.20360.06550.96500.181*
H12C0.11290.16230.94410.181*
C130.1393 (4)0.0128 (5)0.8480 (2)0.0933 (14)
H13A0.11670.05180.81390.140*
H13B0.11800.11030.83680.140*
H13C0.20740.01080.85780.140*
C140.0064 (3)0.0318 (6)0.8857 (3)0.1135 (18)
H14A0.03240.06190.92050.170*
H14B0.02720.06560.87390.170*
H14C0.02780.09700.85160.170*
C150.1772 (3)0.2943 (4)0.6325 (2)0.0608 (10)
H15A0.200 (2)0.252 (4)0.5930 (18)0.069 (11)*
H15B0.158 (3)0.214 (5)0.6611 (18)0.082 (12)*
C160.2568 (3)0.3723 (5)0.6520 (2)0.0913 (14)
H16A0.30770.30510.65290.137*
H16B0.27890.44930.62320.137*
H16C0.23530.41290.69260.137*
C170.0115 (3)0.3166 (4)0.5991 (2)0.0629 (10)
H17A0.012 (3)0.240 (4)0.6222 (17)0.077 (13)*
H17B0.045 (3)0.281 (4)0.5574 (18)0.076 (12)*
C180.0688 (3)0.4131 (5)0.5903 (2)0.0814 (13)
H18A0.11490.35630.57480.122*
H18B0.09780.45600.62920.122*
H18C0.04490.48890.56120.122*
C190.0951 (2)0.6402 (4)0.63183 (15)0.0471 (8)
N10.10997 (19)0.7748 (3)0.61510 (12)0.0511 (7)
C200.1566 (3)0.8062 (4)0.55203 (16)0.0622 (10)
H200.166 (2)0.717 (4)0.5315 (13)0.045 (9)*
C210.2498 (3)0.8737 (5)0.5495 (2)0.0946 (15)
H21A0.28180.88410.50710.142*
H21B0.24160.96800.56880.142*
H21C0.28690.81300.57100.142*
C220.0932 (4)0.8947 (5)0.52033 (19)0.0931 (15)
H22A0.12180.90410.47720.140*
H22B0.03290.84700.52450.140*
H22C0.08440.98970.53890.140*
C230.0802 (3)0.8962 (4)0.65749 (18)0.0663 (11)
H230.102 (2)0.975 (4)0.6307 (16)0.067 (11)*
C240.1303 (4)0.8964 (5)0.71037 (19)0.0964 (16)
H24A0.12060.98860.73140.145*
H24B0.10550.81960.73860.145*
H24C0.19690.88120.69520.145*
C250.0239 (3)0.9069 (5)0.6762 (2)0.0925 (15)
H25A0.04770.82530.70200.139*
H25B0.04050.99590.69880.139*
H25C0.05150.90660.64010.139*
C40.0586 (4)0.5000 (7)0.8490 (2)0.123 (2)
H4A0.07210.39980.85650.185*
H4B0.11510.54660.82680.185*
H4C0.03690.54890.88770.185*
C60.1766 (10)0.526 (2)0.8083 (5)0.080 (4)0.452 (18)
H6A0.14370.59730.77860.096*0.452 (18)
C70.2545 (10)0.594 (3)0.8533 (8)0.119 (7)0.452 (18)
H7A0.28090.52440.88450.179*0.452 (18)
H7B0.23030.67610.87240.179*0.452 (18)
H7C0.30300.62670.83220.179*0.452 (18)
C80.218 (2)0.408 (4)0.7768 (16)0.175 (14)0.452 (18)
H8A0.26800.44720.75880.262*0.452 (18)
H8B0.16950.36740.74480.262*0.452 (18)
H8C0.24270.33370.80620.262*0.452 (18)
C6A0.2064 (7)0.4703 (13)0.8266 (6)0.077 (4)0.548 (18)
H6AA0.25750.43610.85990.092*0.548 (18)
C7A0.2273 (15)0.6199 (18)0.8083 (13)0.169 (10)0.548 (18)
H7A10.29120.62430.80190.254*0.548 (18)
H7A20.22000.68680.84050.254*0.548 (18)
H7A30.18410.64580.77070.254*0.548 (18)
C8A0.2056 (12)0.384 (2)0.7704 (6)0.103 (5)0.548 (18)
H8A10.19030.28460.77770.155*0.548 (18)
H8A20.26710.38850.75980.155*0.548 (18)
H8A30.15890.42320.73700.155*0.548 (18)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
B10.049 (2)0.034 (2)0.062 (2)0.0032 (18)0.0075 (19)0.0079 (18)
O10.0689 (16)0.0378 (13)0.0550 (14)0.0025 (11)0.0068 (12)0.0021 (11)
O20.0589 (14)0.0396 (13)0.0560 (13)0.0006 (11)0.0071 (11)0.0015 (11)
C10.060 (2)0.037 (2)0.065 (2)0.0001 (17)0.0058 (18)0.0066 (17)
C20.104 (3)0.040 (2)0.068 (3)0.001 (2)0.008 (2)0.006 (2)
C30.142 (5)0.054 (3)0.069 (3)0.008 (3)0.018 (3)0.002 (2)
C50.102 (4)0.082 (3)0.065 (3)0.008 (3)0.012 (2)0.005 (2)
O30.0621 (15)0.0678 (17)0.0513 (13)0.0156 (13)0.0102 (11)0.0004 (12)
Si10.0439 (5)0.0689 (7)0.0486 (5)0.0029 (5)0.0092 (4)0.0005 (5)
C90.077 (3)0.102 (3)0.064 (2)0.000 (3)0.023 (2)0.011 (2)
C100.055 (2)0.105 (4)0.082 (3)0.000 (2)0.003 (2)0.009 (3)
C110.075 (3)0.075 (3)0.068 (2)0.008 (2)0.020 (2)0.003 (2)
C120.177 (6)0.087 (4)0.098 (4)0.005 (4)0.029 (4)0.017 (3)
C130.108 (4)0.083 (3)0.092 (3)0.003 (3)0.029 (3)0.021 (3)
C140.081 (3)0.124 (5)0.139 (5)0.036 (3)0.031 (3)0.027 (4)
C150.060 (2)0.055 (2)0.067 (2)0.004 (2)0.0119 (19)0.000 (2)
C160.062 (3)0.100 (4)0.120 (4)0.001 (3)0.036 (3)0.002 (3)
C170.051 (2)0.058 (3)0.079 (3)0.005 (2)0.011 (2)0.002 (2)
C180.061 (3)0.096 (3)0.092 (3)0.005 (2)0.027 (2)0.007 (3)
C190.0448 (19)0.046 (2)0.052 (2)0.0050 (16)0.0129 (16)0.0012 (18)
N10.0632 (18)0.0371 (17)0.0536 (17)0.0079 (14)0.0128 (14)0.0013 (13)
C200.085 (3)0.044 (2)0.055 (2)0.011 (2)0.0075 (19)0.0003 (18)
C210.093 (3)0.083 (3)0.096 (3)0.030 (3)0.007 (3)0.002 (3)
C220.146 (5)0.073 (3)0.068 (3)0.001 (3)0.040 (3)0.010 (2)
C230.095 (3)0.039 (2)0.063 (2)0.008 (2)0.011 (2)0.0024 (19)
C240.157 (5)0.069 (3)0.068 (3)0.028 (3)0.033 (3)0.005 (2)
C250.102 (4)0.059 (3)0.103 (3)0.016 (2)0.010 (3)0.003 (2)
C40.095 (4)0.203 (7)0.075 (3)0.033 (4)0.025 (3)0.036 (4)
C60.088 (9)0.077 (11)0.078 (8)0.015 (8)0.027 (7)0.045 (6)
C70.088 (10)0.123 (15)0.158 (14)0.059 (10)0.052 (10)0.014 (11)
C80.11 (2)0.25 (3)0.15 (2)0.08 (2)0.001 (15)0.04 (2)
C6A0.084 (7)0.068 (7)0.084 (8)0.012 (6)0.027 (6)0.027 (6)
C7A0.156 (15)0.102 (10)0.26 (3)0.001 (10)0.075 (17)0.078 (15)
C8A0.047 (6)0.204 (15)0.069 (8)0.000 (9)0.035 (6)0.014 (9)
Geometric parameters (Å, º) top
B1—C171.594 (6)C17—H17A0.91 (4)
B1—C151.599 (5)C17—H17B1.02 (4)
B1—C11.609 (5)C18—H18A0.9800
B1—O21.614 (4)C18—H18B0.9800
O1—C191.322 (4)C18—H18C0.9800
O1—C11.460 (4)C19—N11.320 (4)
O2—C191.259 (4)N1—C201.476 (4)
C1—C21.308 (5)N1—C231.491 (4)
C2—C31.508 (6)C20—C211.498 (6)
C2—H20.89 (4)C20—C221.526 (6)
C3—C51.471 (6)C20—H200.95 (3)
C3—C41.629 (7)C21—H21A0.9800
C3—H31.00 (5)C21—H21B0.9800
C5—O31.452 (5)C21—H21C0.9800
C5—C61.573 (9)C22—H22A0.9800
C5—C6A1.591 (8)C22—H22B0.9800
C5—H5B1.0000C22—H22C0.9800
C5—H5A1.0000C23—C251.505 (6)
O3—Si11.626 (2)C23—C241.520 (6)
Si1—C101.848 (4)C23—H230.96 (4)
Si1—C91.869 (4)C24—H24A0.9800
Si1—C111.869 (4)C24—H24B0.9800
C9—H9A0.9800C24—H24C0.9800
C9—H9B0.9800C25—H25A0.9800
C9—H9C0.9800C25—H25B0.9800
C10—H10A0.9800C25—H25C0.9800
C10—H10B0.9800C4—H4A0.9800
C10—H10C0.9800C4—H4B0.9800
C11—C121.513 (6)C4—H4C0.9800
C11—C131.527 (6)C6—C81.499 (10)
C11—C141.553 (6)C6—C71.510 (10)
C12—H12A0.9800C6—H6A1.0000
C12—H12B0.9800C7—H7A0.9800
C12—H12C0.9800C7—H7B0.9800
C13—H13A0.9800C7—H7C0.9800
C13—H13B0.9800C8—H8A0.9800
C13—H13C0.9800C8—H8B0.9800
C14—H14A0.9800C8—H8C0.9800
C14—H14B0.9800C6A—C8A1.497 (10)
C14—H14C0.9800C6A—C7A1.507 (9)
C15—C161.516 (6)C6A—H6AA1.0000
C15—H15A0.97 (4)C7A—H7A10.9800
C15—H15B0.99 (4)C7A—H7A20.9800
C16—H16A0.9800C7A—H7A30.9800
C16—H16B0.9800C8A—H8A10.9800
C16—H16C0.9800C8A—H8A20.9800
C17—C181.529 (5)C8A—H8A30.9800
C17—B1—C15115.3 (3)C15—C16—H16C109.5
C17—B1—C1115.1 (3)H16A—C16—H16C109.5
C15—B1—C1113.3 (3)H16B—C16—H16C109.5
C17—B1—O2106.9 (3)C18—C17—B1115.8 (3)
C15—B1—O2107.9 (3)C18—C17—H17A109 (2)
C1—B1—O296.0 (2)B1—C17—H17A106 (3)
C19—O1—C1108.1 (3)C18—C17—H17B108 (2)
C19—O2—B1110.0 (2)B1—C17—H17B108 (2)
C2—C1—O1114.7 (3)H17A—C17—H17B109 (3)
C2—C1—B1138.1 (3)C17—C18—H18A109.5
O1—C1—B1107.1 (3)C17—C18—H18B109.5
C1—C2—C3129.8 (4)H18A—C18—H18B109.5
C1—C2—H2113 (3)C17—C18—H18C109.5
C3—C2—H2117 (3)H18A—C18—H18C109.5
C5—C3—C2114.8 (4)H18B—C18—H18C109.5
C5—C3—C4107.5 (4)O2—C19—N1123.7 (3)
C2—C3—C4109.1 (4)O2—C19—O1118.6 (3)
C5—C3—H3103 (3)N1—C19—O1117.6 (3)
C2—C3—H3107 (3)C19—N1—C20118.8 (3)
C4—C3—H3116 (3)C19—N1—C23122.3 (3)
O3—C5—C3108.4 (4)C20—N1—C23118.9 (3)
O3—C5—C6124.0 (9)N1—C20—C21111.2 (3)
C3—C5—C696.9 (7)N1—C20—C22110.5 (3)
O3—C5—C6A102.2 (6)C21—C20—C22113.1 (4)
C3—C5—C6A122.1 (7)N1—C20—H20106.7 (18)
C6—C5—C6A27.2 (5)C21—C20—H20108.2 (19)
O3—C5—H5B107.8C22—C20—H20106.8 (19)
C3—C5—H5B107.8C20—C21—H21A109.5
C6—C5—H5B110.5C20—C21—H21B109.5
C6A—C5—H5B107.8H21A—C21—H21B109.5
O3—C5—H5A108.7C20—C21—H21C109.5
C3—C5—H5A108.7H21A—C21—H21C109.5
C6—C5—H5A108.9H21B—C21—H21C109.5
C6A—C5—H5A106.1C20—C22—H22A109.5
H5B—C5—H5A1.7C20—C22—H22B109.5
C5—O3—Si1129.9 (2)H22A—C22—H22B109.5
O3—Si1—C10111.47 (18)C20—C22—H22C109.5
O3—Si1—C9111.05 (17)H22A—C22—H22C109.5
C10—Si1—C9108.6 (2)H22B—C22—H22C109.5
O3—Si1—C11103.34 (16)N1—C23—C25112.3 (3)
C10—Si1—C11110.3 (2)N1—C23—C24112.1 (4)
C9—Si1—C11112.1 (2)C25—C23—C24113.9 (4)
Si1—C9—H9A109.5N1—C23—H2399 (2)
Si1—C9—H9B109.5C25—C23—H23108 (2)
H9A—C9—H9B109.5C24—C23—H23110 (2)
Si1—C9—H9C109.5C23—C24—H24A109.5
H9A—C9—H9C109.5C23—C24—H24B109.5
H9B—C9—H9C109.5H24A—C24—H24B109.5
Si1—C10—H10A109.5C23—C24—H24C109.5
Si1—C10—H10B109.5H24A—C24—H24C109.5
H10A—C10—H10B109.5H24B—C24—H24C109.5
Si1—C10—H10C109.5C23—C25—H25A109.5
H10A—C10—H10C109.5C23—C25—H25B109.5
H10B—C10—H10C109.5H25A—C25—H25B109.5
C12—C11—C13109.4 (4)C23—C25—H25C109.5
C12—C11—C14110.0 (4)H25A—C25—H25C109.5
C13—C11—C14108.0 (4)H25B—C25—H25C109.5
C12—C11—Si1111.0 (3)C3—C4—H4A109.5
C13—C11—Si1109.5 (3)C3—C4—H4B109.5
C14—C11—Si1108.9 (3)H4A—C4—H4B109.5
C11—C12—H12A109.5C3—C4—H4C109.5
C11—C12—H12B109.5H4A—C4—H4C109.5
H12A—C12—H12B109.5H4B—C4—H4C109.5
C11—C12—H12C109.5C8—C6—C7108 (2)
H12A—C12—H12C109.5C8—C6—C5110.5 (18)
H12B—C12—H12C109.5C7—C6—C5104.9 (10)
C11—C13—H13A109.5C8—C6—H6A111.2
C11—C13—H13B109.5C7—C6—H6A111.2
H13A—C13—H13B109.5C5—C6—H6A111.2
C11—C13—H13C109.5C8A—C6A—C7A103.7 (19)
H13A—C13—H13C109.5C8A—C6A—C5112.0 (9)
H13B—C13—H13C109.5C7A—C6A—C5111.8 (11)
C11—C14—H14A109.5C8A—C6A—H6AA109.7
C11—C14—H14B109.5C7A—C6A—H6AA109.7
H14A—C14—H14B109.5C5—C6A—H6AA109.7
C11—C14—H14C109.5C6A—C7A—H7A1109.5
H14A—C14—H14C109.5C6A—C7A—H7A2109.5
H14B—C14—H14C109.5H7A1—C7A—H7A2109.5
C16—C15—B1115.5 (4)C6A—C7A—H7A3109.5
C16—C15—H15A109 (2)H7A1—C7A—H7A3109.5
B1—C15—H15A110 (2)H7A2—C7A—H7A3109.5
C16—C15—H15B108 (2)C6A—C8A—H8A1109.5
B1—C15—H15B107 (2)C6A—C8A—H8A2109.5
H15A—C15—H15B107 (3)H8A1—C8A—H8A2109.5
C15—C16—H16A109.5C6A—C8A—H8A3109.5
C15—C16—H16B109.5H8A1—C8A—H8A3109.5
H16A—C16—H16B109.5H8A2—C8A—H8A3109.5
C17—B1—O2—C19115.6 (3)C9—Si1—C11—C1457.4 (4)
C15—B1—O2—C19119.8 (3)C17—B1—C15—C16167.9 (4)
C1—B1—O2—C192.9 (3)C1—B1—C15—C1656.6 (5)
C19—O1—C1—C2176.1 (4)O2—B1—C15—C1648.5 (5)
C19—O1—C1—B12.8 (4)C15—B1—C17—C18171.4 (4)
C17—B1—C1—C272.9 (6)C1—B1—C17—C1853.8 (5)
C15—B1—C1—C262.8 (6)O2—B1—C17—C1851.5 (4)
O2—B1—C1—C2175.2 (5)B1—O2—C19—N1178.0 (3)
C17—B1—C1—O1108.7 (3)B1—O2—C19—O11.6 (4)
C15—B1—C1—O1115.7 (3)C1—O1—C19—O20.8 (4)
O2—B1—C1—O13.2 (3)C1—O1—C19—N1179.6 (3)
O1—C1—C2—C33.5 (7)O2—C19—N1—C200.3 (5)
B1—C1—C2—C3174.9 (5)O1—C19—N1—C20179.3 (3)
C1—C2—C3—C5139.0 (5)O2—C19—N1—C23179.5 (3)
C1—C2—C3—C4100.4 (6)O1—C19—N1—C230.1 (5)
C2—C3—C5—O353.3 (6)C19—N1—C20—C21114.2 (4)
C4—C3—C5—O368.2 (5)C23—N1—C20—C2166.5 (5)
C2—C3—C5—C676.1 (9)C19—N1—C20—C22119.3 (4)
C4—C3—C5—C6162.4 (8)C23—N1—C20—C2260.0 (4)
C2—C3—C5—C6A64.8 (7)C19—N1—C23—C2565.9 (5)
C4—C3—C5—C6A173.7 (6)C20—N1—C23—C25113.3 (4)
C3—C5—O3—Si1140.7 (3)C19—N1—C23—C2463.9 (5)
C6—C5—O3—Si1107.1 (7)C20—N1—C23—C24117.0 (4)
C6A—C5—O3—Si189.2 (6)O3—C5—C6—C811 (2)
C5—O3—Si1—C1062.8 (4)C3—C5—C6—C8107.2 (18)
C5—O3—Si1—C958.4 (4)C6A—C5—C6—C852 (2)
C5—O3—Si1—C11178.7 (3)O3—C5—C6—C7105.3 (18)
O3—Si1—C11—C12176.4 (3)C3—C5—C6—C7137.0 (18)
C10—Si1—C11—C1257.2 (4)C6A—C5—C6—C764.3 (18)
C9—Si1—C11—C1263.9 (4)O3—C5—C6A—C8A62.2 (14)
O3—Si1—C11—C1355.6 (3)C3—C5—C6A—C8A58.9 (14)
C10—Si1—C11—C1363.7 (4)C6—C5—C6A—C8A84 (3)
C9—Si1—C11—C13175.2 (3)O3—C5—C6A—C7A178.0 (17)
O3—Si1—C11—C1462.3 (3)C3—C5—C6A—C7A56.9 (18)
C10—Si1—C11—C14178.4 (3)C6—C5—C6A—C7A31.8 (16)

Experimental details

Crystal data
Chemical formulaC25H52BNO3Si
Mr453.58
Crystal system, space groupMonoclinic, P21/n
Temperature (K)193
a, b, c (Å)14.684 (6), 9.355 (1), 22.515 (9)
β (°) 101.68 (2)
V3)3028.8 (18)
Z4
Radiation typeCu Kα
µ (mm1)0.84
Crystal size (mm)0.4 × 0.2 × 0.1
Data collection
DiffractometerEnraf Nonius CAD-4
diffractometer
Absorption correctionPart of the refinement model (ΔF)
(DIFABS; Walker & Stuart, 1983)
Tmin, Tmax0.50, 0.67
No. of measured, independent and
observed [I > 2σ(I)] reflections
3959, 3786, 2882
Rint0.046
θmax (°)55.2
(sin θ/λ)max1)0.533
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.059, 0.169, 1.04
No. of reflections3786
No. of parameters356
No. of restraints25
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.55, 0.18

Computer programs: CAD-4 EXPRESS (Enraf-Nonius, 1994), CAD-4 EXPRESS, XCAD4 (Harms, 1997), SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), DIAMOND (Brandenburg, 2001), SHELXTL (Sheldrick, 1996).

Selected geometric parameters (Å, º) top
B1—C171.594 (6)O1—C191.322 (4)
B1—C151.599 (5)O1—C11.460 (4)
B1—C11.609 (5)O2—C191.259 (4)
B1—O21.614 (4)C1—C21.308 (5)
C17—B1—C15115.3 (3)C19—O1—C1108.1 (3)
C17—B1—C1115.1 (3)C19—O2—B1110.0 (2)
C15—B1—C1113.3 (3)C2—C1—O1114.7 (3)
C17—B1—O2106.9 (3)C2—C1—B1138.1 (3)
C15—B1—O2107.9 (3)O1—C1—B1107.1 (3)
C1—B1—O296.0 (2)
C1—B1—O2—C192.9 (3)O2—B1—C1—O13.2 (3)
C19—O1—C1—C2176.1 (4)O1—C1—C2—C33.5 (7)
C19—O1—C1—B12.8 (4)B1—O2—C19—O11.6 (4)
O2—B1—C1—C2175.2 (5)C1—O1—C19—O20.8 (4)
 

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