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Recently lithium bis(oxalato)borate, LiB(C2O4)2, has been proposed as an alternative lithium salt for the electrolyte in rechargeable batteries that do not contain explosive perchlorate, reactive fluoride or toxic arsenic. This lithium salt crystallizes in the form of solvates from such solvents as water, acetonitrile, acetone, dimethoxyethane, 1,3-dioxolane and ethylene carbonate. Their crystal structures were determined in order to explore the crystal chemistry of this lithium salt. It was found that most of the solvents consist of a lithium bis(oxalato)borate dimer in which the ligand acts as both a chelating and a bridging agent. Lithium has octahedral coordination that typically includes one or, less commonly, two solvent molecules. An exception to this rule is the ethylene carbonate solvate where the lithium is tetrahedrally surrounded exclusively by the solvent and bis(oxalato)borate plays the role of counter-ion only. The ethylene carbonate solvates were also studied for LiPF6 and LiAsF6 salts and they have similar structures to the bis(oxalato)borate tetrahedral complexes.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108768104022153/ta5011sup1.cif
Contains datablocks I, II, III, IV, V, VI

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768104022153/ta5011Isup2.hkl
Contains datablock I

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Structure factor file (CIF format) https://doi.org/10.1107/S0108768104022153/ta5011IIsup3.hkl
Contains datablock II

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Structure factor file (CIF format) https://doi.org/10.1107/S0108768104022153/ta5011IIIsup4.hkl
Contains datablock III

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Structure factor file (CIF format) https://doi.org/10.1107/S0108768104022153/ta5011IVsup5.hkl
Contains datablock IV

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Structure factor file (CIF format) https://doi.org/10.1107/S0108768104022153/ta5011Vsup6.hkl
Contains datablock V

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Structure factor file (CIF format) https://doi.org/10.1107/S0108768104022153/ta5011VIsup7.hkl
Contains datablock VI

CCDC references: 257791; 257792; 257793; 257794; 257795; 257796

Computing details top

For all compounds, data collection: SMART (Bruker, 1999); cell refinement: SAINT (Bruker, 1999); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997). Molecular graphics: Materials Studio (2001) for (I), (II), (III), (IV), (V); Materials Studio (2001), ATOMS (Dowty,1999) for (VI). For all compounds, software used to prepare material for publication: SHELXL97.

Figures top
[Figure 1]
[Figure 2]
(I) Lithium bis(oxalato)borate hydrate top
Crystal data top
C4H2BLiO9F(000) = 848
Mr = 211.81Dx = 1.968 Mg m3
Orthorhombic, PbcaMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ac 2abCell parameters from 3095 reflections
a = 16.075 (3) Åθ = 2.5–30.5°
b = 15.880 (3) ŵ = 0.20 mm1
c = 5.6008 (9) ÅT = 294 K
V = 1429.7 (4) Å3Plate, colorless
Z = 80.38 × 0.09 × 0.02 mm
Data collection top
Three-circle
diffractometer
1440 independent reflections
Radiation source: fine-focus sealed tube1044 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.082
Detector resolution: 8.33 pixels mm-1θmax = 26.4°, θmin = 2.5°
ω scansh = 1920
Absorption correction: multi-scan
XPREP (Sheldrick, 1997)
k = 1919
Tmin = 0.873, Tmax = 0.996l = 76
9124 measured reflections
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)] = 0.060Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.089H-atom parameters constrained
S = 1.00 w = 1/[σ2(Fo2) + (0.001P)2 + 2.51P], P = (max(Fo2,0) + 2Fc2)/3
1440 reflections(Δ/σ)max < 0.001
144 parametersΔρmax = 0.23 e Å3
0 restraintsΔρmin = 0.30 e Å3
Crystal data top
C4H2BLiO9V = 1429.7 (4) Å3
Mr = 211.81Z = 8
Orthorhombic, PbcaMo Kα radiation
a = 16.075 (3) ŵ = 0.20 mm1
b = 15.880 (3) ÅT = 294 K
c = 5.6008 (9) Å0.38 × 0.09 × 0.02 mm
Data collection top
Three-circle
diffractometer
1440 independent reflections
Absorption correction: multi-scan
XPREP (Sheldrick, 1997)
1044 reflections with I > 2σ(I)
Tmin = 0.873, Tmax = 0.996Rint = 0.082
9124 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0600 restraints
wR(F2) = 0.089H-atom parameters constrained
S = 1.00Δρmax = 0.23 e Å3
1440 reflectionsΔρmin = 0.30 e Å3
144 parameters
Special details top

Experimental. XPREP absorption correction for lamina with cut-off angle 8 °.

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.

Least-squares planes (x,y,z in crystal coordinates) and deviations from them (* indicates atom used to define plane)

13.4467 (0.0090) x + 2.8591 (0.0148) y + 2.8986 (0.0043) z = 9.1102 (0.0074)

* 0.0008 (0.0025) C3 * 0.0046 (0.0026) C4 * −0.0074 (0.0015) O5 * 0.0045 (0.0015) O6 * 0.0050 (0.0015) O7 * −0.0075 (0.0015) O8 − 0.0636 (0.0046) B1 Rms deviation of fitted atoms = 0.0054

4.7314 (0.0130) x + 9.7343 (0.0128) y − 4.1065 (0.0036) z = 3.0814 (0.0080)

Angle to previous plane (with approximate e.s.d.) = 88.69 (0.07)

* 0.0127 (0.0027) C1 * 0.0149 (0.0026) C2 * −0.0182 (0.0016) O1 * 0.0023 (0.0015) O2 * 0.0062 (0.0015) O3 * −0.0179 (0.0016) O4 − 0.0400 (0.0047) B1 Rms deviation of fitted atoms = 0.0134

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*/Ueq
Li10.6555 (3)0.2483 (4)0.8774 (12)0.0306 (13)
B10.4103 (2)0.4425 (2)0.7811 (7)0.0223 (9)
C10.50447 (19)0.34586 (19)0.6476 (6)0.0222 (8)
C20.4211 (2)0.33274 (19)0.5199 (6)0.0211 (7)
C30.36667 (18)0.57436 (19)0.8757 (6)0.0209 (7)
C40.33841 (19)0.51274 (19)1.0689 (6)0.0209 (7)
O70.36703 (13)0.43764 (12)1.0103 (4)0.0241 (5)
O20.56587 (13)0.30409 (13)0.6219 (5)0.0275 (6)
O60.35228 (13)0.64869 (12)0.8704 (4)0.0261 (6)
O10.49551 (12)0.40936 (13)0.7953 (4)0.0240 (6)
O40.40447 (14)0.27839 (13)0.3799 (4)0.0305 (6)
O80.29696 (14)0.53018 (14)1.2398 (4)0.0283 (6)
O50.40957 (14)0.53234 (12)0.7153 (4)0.0247 (6)
O30.36915 (12)0.39059 (13)0.5993 (4)0.0238 (5)
O1w0.73558 (15)0.20418 (16)1.1266 (5)0.0278 (6)
H10.786 (3)0.224 (3)1.135 (8)0.072 (15)*
H20.740 (2)0.153 (2)1.161 (7)0.049 (13)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Li10.035 (3)0.034 (3)0.023 (3)0.001 (3)0.003 (3)0.001 (3)
B10.0203 (19)0.0183 (18)0.028 (2)0.0007 (15)0.0013 (18)0.0028 (17)
C10.0241 (17)0.0195 (17)0.023 (2)0.0014 (14)0.0053 (16)0.0032 (15)
C20.0252 (18)0.0187 (16)0.0193 (19)0.0003 (14)0.0011 (15)0.0057 (15)
C30.0185 (16)0.0218 (16)0.0223 (18)0.0013 (13)0.0072 (15)0.0003 (15)
C40.0201 (16)0.0226 (17)0.020 (2)0.0028 (14)0.0033 (15)0.0033 (14)
O70.0299 (13)0.0163 (11)0.0261 (14)0.0036 (9)0.0055 (11)0.0002 (10)
O20.0227 (12)0.0257 (12)0.0341 (15)0.0073 (10)0.0050 (12)0.0003 (11)
O60.0339 (13)0.0143 (11)0.0301 (14)0.0023 (10)0.0008 (12)0.0005 (10)
O10.0203 (11)0.0242 (12)0.0275 (15)0.0003 (10)0.0021 (10)0.0092 (10)
O40.0357 (13)0.0276 (12)0.0281 (14)0.0022 (11)0.0037 (12)0.0085 (12)
O80.0317 (13)0.0289 (12)0.0242 (14)0.0045 (11)0.0067 (12)0.0026 (11)
O50.0322 (13)0.0185 (11)0.0234 (14)0.0023 (10)0.0068 (11)0.0004 (10)
O30.0206 (11)0.0237 (11)0.0270 (14)0.0056 (10)0.0016 (11)0.0039 (10)
O1w0.0242 (13)0.0235 (14)0.0358 (16)0.0039 (11)0.0020 (12)0.0053 (12)
Geometric parameters (Å, º) top
Li1—O1w2.024 (6)C1—O21.198 (3)
Li1—O1wi2.050 (6)C1—O11.312 (4)
Li1—O6ii2.108 (7)C1—C21.534 (4)
Li1—O2iii2.154 (6)C2—O41.196 (4)
Li1—O6iv2.165 (7)C2—O31.319 (4)
Li1—O22.216 (7)C3—O61.203 (3)
Li1—Li1iii2.801 (5)C3—O51.314 (4)
Li1—Li1i2.801 (5)C3—C41.528 (4)
B1—O71.463 (4)C4—O81.199 (4)
B1—O31.468 (4)C4—O71.320 (3)
B1—O11.469 (4)O1w—H10.87 (4)
B1—O51.473 (4)O1w—H20.84 (4)
O1w—Li1—O1wi101.5 (3)O4—C2—O3125.6 (3)
O1w—Li1—O6ii103.4 (3)O4—C2—C1126.8 (3)
O1wi—Li1—O6ii82.1 (2)O3—C2—C1107.5 (3)
O1w—Li1—O2iii81.6 (2)O6—C3—O5125.6 (3)
O1wi—Li1—O2iii176.2 (4)O6—C3—C4126.1 (3)
O6ii—Li1—O2iii95.1 (2)O5—C3—C4108.3 (3)
O1w—Li1—O6iv81.3 (2)O8—C4—O7126.9 (3)
O1wi—Li1—O6iv101.8 (3)O8—C4—C3125.6 (3)
O6ii—Li1—O6iv173.3 (3)O7—C4—C3107.4 (3)
O2iii—Li1—O6iv80.7 (2)C4—O7—B1109.6 (2)
O1w—Li1—O2176.0 (3)C1—O2—Li1i147.3 (3)
O1wi—Li1—O279.5 (2)C1—O2—Li1132.8 (3)
O6ii—Li1—O280.6 (2)Li1i—O2—Li179.72 (18)
O2iii—Li1—O297.5 (2)C3—O6—Li1v139.8 (3)
O6iv—Li1—O294.7 (2)C3—O6—Li1iv137.4 (3)
Li1iii—Li1—Li1i177.8 (5)Li1v—O6—Li1iv81.91 (7)
O7—B1—O3111.4 (3)C1—O1—B1110.1 (3)
O7—B1—O1112.1 (3)C3—O5—B1109.0 (3)
O3—B1—O1104.9 (3)C2—O3—B1109.9 (2)
O7—B1—O5105.5 (3)Li1—O1w—Li1iii86.9 (2)
O3—B1—O5111.5 (3)Li1—O1w—H1120 (3)
O1—B1—O5111.6 (3)Li1iii—O1w—H1114 (3)
O2—C1—O1126.3 (3)Li1—O1w—H2123 (3)
O2—C1—C2126.1 (3)Li1iii—O1w—H2105 (3)
O1—C1—C2107.6 (3)H1—O1w—H2105 (4)
O2—C1—C2—O41.5 (6)O6iv—Li1—O2—Li1i140.7 (3)
O1—C1—C2—O4176.6 (3)O5—C3—O6—Li1v23.2 (6)
O2—C1—C2—O3179.0 (3)C4—C3—O6—Li1v156.8 (3)
O1—C1—C2—O31.0 (3)O5—C3—O6—Li1iv141.6 (3)
O6—C3—C4—O81.1 (5)C4—C3—O6—Li1iv38.4 (5)
O5—C3—C4—O8178.9 (3)O2—C1—O1—B1178.0 (3)
O6—C3—C4—O7179.7 (3)C2—C1—O1—B10.1 (4)
O5—C3—C4—O70.3 (3)O7—B1—O1—C1120.1 (3)
O8—C4—O7—B1176.4 (3)O3—B1—O1—C11.0 (4)
C3—C4—O7—B12.7 (3)O5—B1—O1—C1121.9 (3)
O3—B1—O7—C4117.2 (3)O6—C3—O5—B1177.8 (3)
O1—B1—O7—C4125.7 (3)C4—C3—O5—B12.2 (3)
O5—B1—O7—C44.0 (3)O7—B1—O5—C33.8 (3)
O1—C1—O2—Li1i128.8 (5)O3—B1—O5—C3117.3 (3)
C2—C1—O2—Li1i53.5 (6)O1—B1—O5—C3125.8 (3)
O1—C1—O2—Li143.3 (5)O4—C2—O3—B1176.0 (3)
C2—C1—O2—Li1134.4 (4)C1—C2—O3—B11.6 (3)
O1wi—Li1—O2—C1136.1 (3)O7—B1—O3—C2119.9 (3)
O6ii—Li1—O2—C1140.3 (3)O1—B1—O3—C21.6 (3)
O2iii—Li1—O2—C146.3 (4)O5—B1—O3—C2122.6 (3)
O6iv—Li1—O2—C134.9 (4)O1wi—Li1—O1w—Li1iii139.1 (4)
O1wi—Li1—O2—Li1i39.57 (14)O6ii—Li1—O1w—Li1iii136.4 (3)
O6ii—Li1—O2—Li1i44.0 (2)O2iii—Li1—O1w—Li1iii43.08 (13)
O2iii—Li1—O2—Li1i138.0 (3)O6iv—Li1—O1w—Li1iii38.7 (2)
Symmetry codes: (i) x, y+1/2, z1/2; (ii) x+1, y1/2, z+3/2; (iii) x, y+1/2, z+1/2; (iv) x+1, y+1, z+2; (v) x+1, y+1/2, z+3/2.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1w—H2···O3vi0.84 (4)2.57 (4)3.039 (3)117 (3)
O1w—H2···O8vii0.84 (4)2.11 (4)2.910 (3)159 (4)
O1w—H1···O4viii0.87 (4)2.09 (4)2.960 (3)174 (4)
Symmetry codes: (vi) x+1/2, y+1/2, z+2; (vii) x+1, y1/2, z+5/2; (viii) x+1/2, y, z+3/2.
(II) Lithium bis(oxalato)borate acetonitrile top
Crystal data top
C12H6B2Li2N2O16·3(C2H3N)F(000) = 1208
Mr = 592.85Dx = 1.527 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 2595 reflections
a = 7.6346 (8) Åθ = 3.0–28.1°
b = 22.631 (2) ŵ = 0.13 mm1
c = 14.9338 (16) ÅT = 110 K
β = 91.879 (2)°Prism, colorless
V = 2578.9 (5) Å30.48 × 0.36 × 0.30 mm
Z = 4
Data collection top
Three-circle
diffractometer
4542 independent reflections
Radiation source: fine-focus sealed tube3039 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.039
Detector resolution: 8.33 pixels mm-1θmax = 25.0°, θmin = 1.6°
ω scansh = 89
Absorption correction: multi-scan
XPREP (Sheldrick, 1997)
k = 2526
Tmin = 0.873, Tmax = 0.961l = 1717
14456 measured reflections
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)] = 0.042Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.090H-atom parameters constrained
S = 1.00 w = 1/[σ2(Fo2) + (0.0299P)2], P = (max(Fo2,0) + 2Fc2)/3
4542 reflections(Δ/σ)max = 0.001
393 parametersΔρmax = 0.21 e Å3
0 restraintsΔρmin = 0.26 e Å3
Crystal data top
C12H6B2Li2N2O16·3(C2H3N)V = 2578.9 (5) Å3
Mr = 592.85Z = 4
Monoclinic, P21/nMo Kα radiation
a = 7.6346 (8) ŵ = 0.13 mm1
b = 22.631 (2) ÅT = 110 K
c = 14.9338 (16) Å0.48 × 0.36 × 0.30 mm
β = 91.879 (2)°
Data collection top
Three-circle
diffractometer
4542 independent reflections
Absorption correction: multi-scan
XPREP (Sheldrick, 1997)
3039 reflections with I > 2σ(I)
Tmin = 0.873, Tmax = 0.961Rint = 0.039
14456 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0420 restraints
wR(F2) = 0.090H-atom parameters constrained
S = 1.00Δρmax = 0.21 e Å3
4542 reflectionsΔρmin = 0.26 e Å3
393 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*/Ueq
Li10.5269 (6)0.18159 (19)0.7873 (3)0.0334 (11)
Li20.4930 (6)0.32406 (19)0.7433 (3)0.0354 (11)
B11.0175 (3)0.32099 (12)0.96650 (17)0.0193 (6)
C11.0338 (3)0.35140 (10)1.11137 (15)0.0190 (5)
C21.0179 (3)0.28490 (10)1.10787 (15)0.0182 (5)
O11.03503 (18)0.37135 (6)1.02875 (9)0.0201 (4)
O21.00830 (19)0.26797 (7)1.02395 (9)0.0198 (4)
O31.04189 (19)0.37985 (7)1.17977 (10)0.0230 (4)
O41.01478 (19)0.25428 (7)1.17424 (10)0.0214 (4)
C30.5208 (3)0.28880 (10)0.92046 (15)0.0189 (5)
C40.5060 (3)0.35533 (10)0.92363 (15)0.0197 (5)
O50.53100 (18)0.26836 (6)1.00289 (9)0.0195 (4)
O60.50574 (18)0.37175 (6)1.00851 (9)0.0194 (4)
O70.52210 (19)0.26085 (7)0.85195 (10)0.0214 (4)
O80.49627 (19)0.38634 (7)0.85840 (10)0.0238 (4)
B20.5219 (3)0.31891 (12)1.06549 (17)0.0195 (6)
C51.1072 (3)0.32066 (10)0.82119 (15)0.0205 (5)
C60.9071 (3)0.32700 (10)0.82206 (15)0.0192 (5)
O91.16448 (18)0.31646 (6)0.90618 (9)0.0198 (4)
O100.86137 (18)0.32661 (7)0.90749 (9)0.0207 (4)
O111.19590 (19)0.31860 (7)0.75675 (10)0.0243 (4)
O120.80822 (19)0.33108 (7)0.75829 (10)0.0248 (4)
C70.4322 (3)0.31248 (10)1.20998 (15)0.0209 (5)
C80.6329 (3)0.31866 (10)1.20997 (15)0.0207 (5)
O130.37498 (18)0.31193 (7)1.12504 (9)0.0201 (4)
O140.67897 (18)0.32111 (7)1.12514 (9)0.0204 (4)
O150.3435 (2)0.30791 (7)1.27424 (10)0.0258 (4)
O160.73046 (19)0.31975 (7)1.27476 (10)0.0245 (4)
N110.5279 (3)0.13306 (9)0.90490 (14)0.0309 (5)
C110.5012 (3)0.13301 (11)0.97909 (17)0.0271 (6)
C120.4634 (4)0.13395 (12)1.07412 (15)0.0414 (7)
H110.40510.09711.09030.062*
H120.38660.16751.08650.062*
H130.57320.13791.10950.062*
N210.4772 (3)0.37373 (9)0.62578 (14)0.0313 (5)
C210.4812 (3)0.37551 (11)0.54945 (17)0.0271 (6)
C220.4861 (3)0.37588 (12)0.45255 (14)0.0336 (7)
H210.60520.36690.43410.050*
H220.45130.41500.43000.050*
H230.40490.34600.42800.050*
N310.5786 (3)0.05329 (10)0.34944 (14)0.0370 (6)
C310.6552 (3)0.02783 (11)0.40301 (18)0.0289 (6)
C320.7526 (3)0.00375 (11)0.47338 (17)0.0397 (7)
H31N0.84620.02690.44690.060*
H32N0.67330.03030.50440.060*
H33N0.80380.02470.51630.060*
N411.0028 (3)0.06373 (11)0.69941 (15)0.0463 (7)
C410.9059 (3)0.03063 (12)0.72521 (17)0.0297 (6)
C420.7835 (3)0.01151 (12)0.75907 (18)0.0477 (8)
H410.82890.05160.75090.071*
H420.67070.00740.72650.071*
H430.76760.00420.82300.071*
N510.7552 (3)0.49660 (10)0.51037 (17)0.0514 (7)
C510.7828 (4)0.49651 (12)0.4361 (2)0.0392 (7)
C520.8194 (4)0.49573 (14)0.34188 (17)0.0556 (9)
H510.76960.53110.31310.083*
H520.76690.46040.31410.083*
H530.94640.49510.33450.083*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Li10.055 (3)0.029 (3)0.016 (2)0.001 (2)0.003 (2)0.0013 (19)
Li20.059 (3)0.030 (3)0.016 (2)0.007 (2)0.001 (2)0.002 (2)
B10.0174 (14)0.0250 (16)0.0153 (14)0.0002 (12)0.0024 (12)0.0008 (12)
C10.0116 (12)0.0305 (15)0.0148 (14)0.0010 (10)0.0002 (10)0.0015 (11)
C20.0104 (12)0.0286 (15)0.0157 (14)0.0013 (10)0.0002 (10)0.0006 (11)
O10.0191 (9)0.0257 (10)0.0155 (9)0.0005 (7)0.0007 (7)0.0024 (7)
O20.0212 (9)0.0266 (9)0.0116 (9)0.0002 (7)0.0009 (7)0.0013 (7)
O30.0229 (9)0.0295 (10)0.0165 (9)0.0013 (7)0.0008 (7)0.0047 (8)
O40.0198 (9)0.0291 (10)0.0153 (9)0.0005 (7)0.0004 (7)0.0030 (8)
C30.0121 (12)0.0297 (15)0.0150 (14)0.0001 (10)0.0014 (10)0.0016 (12)
C40.0083 (12)0.0304 (15)0.0205 (14)0.0011 (10)0.0022 (10)0.0011 (12)
O50.0219 (9)0.0246 (9)0.0120 (9)0.0001 (7)0.0012 (7)0.0000 (7)
O60.0206 (8)0.0239 (9)0.0137 (9)0.0001 (7)0.0002 (7)0.0013 (7)
O70.0202 (9)0.0296 (10)0.0142 (9)0.0002 (7)0.0005 (7)0.0033 (8)
O80.0215 (9)0.0320 (10)0.0179 (9)0.0009 (7)0.0010 (7)0.0067 (8)
B20.0159 (14)0.0253 (16)0.0175 (15)0.0025 (12)0.0010 (12)0.0003 (13)
C50.0253 (14)0.0217 (14)0.0145 (13)0.0007 (11)0.0012 (11)0.0022 (11)
C60.0221 (13)0.0215 (14)0.0140 (13)0.0020 (10)0.0018 (11)0.0003 (10)
O90.0177 (8)0.0289 (9)0.0128 (8)0.0015 (7)0.0010 (7)0.0018 (7)
O100.0169 (8)0.0321 (10)0.0129 (9)0.0009 (7)0.0016 (7)0.0013 (7)
O110.0247 (9)0.0353 (10)0.0129 (9)0.0050 (8)0.0031 (7)0.0014 (8)
O120.0228 (9)0.0348 (11)0.0164 (9)0.0011 (7)0.0046 (8)0.0016 (8)
C70.0230 (13)0.0235 (14)0.0162 (14)0.0018 (10)0.0003 (11)0.0030 (11)
C80.0219 (13)0.0219 (13)0.0183 (14)0.0026 (10)0.0011 (11)0.0022 (11)
O130.0178 (8)0.0308 (10)0.0117 (8)0.0022 (7)0.0014 (7)0.0008 (7)
O140.0171 (8)0.0323 (10)0.0118 (9)0.0005 (7)0.0005 (7)0.0021 (7)
O150.0269 (10)0.0368 (11)0.0139 (9)0.0057 (8)0.0024 (8)0.0012 (8)
O160.0245 (9)0.0338 (10)0.0151 (9)0.0022 (7)0.0040 (8)0.0018 (8)
N110.0358 (13)0.0349 (14)0.0218 (13)0.0016 (10)0.0021 (10)0.0039 (10)
C110.0302 (15)0.0292 (15)0.0216 (15)0.0028 (11)0.0049 (12)0.0000 (12)
C120.0510 (19)0.0504 (19)0.0229 (15)0.0161 (14)0.0051 (14)0.0012 (13)
N210.0372 (13)0.0343 (13)0.0222 (13)0.0023 (10)0.0011 (10)0.0049 (10)
C210.0238 (14)0.0273 (15)0.0299 (16)0.0002 (11)0.0024 (12)0.0022 (12)
C220.0397 (16)0.0453 (18)0.0158 (14)0.0012 (13)0.0005 (12)0.0005 (12)
N310.0403 (14)0.0366 (14)0.0339 (14)0.0008 (11)0.0033 (12)0.0057 (11)
C310.0270 (14)0.0281 (15)0.0321 (16)0.0040 (12)0.0072 (13)0.0095 (13)
C320.0317 (15)0.0398 (17)0.0474 (18)0.0012 (13)0.0006 (14)0.0054 (14)
N410.0529 (17)0.0400 (16)0.0461 (16)0.0025 (12)0.0035 (13)0.0080 (12)
C410.0315 (15)0.0309 (16)0.0266 (15)0.0042 (13)0.0011 (13)0.0007 (12)
C420.0393 (17)0.055 (2)0.0485 (19)0.0088 (15)0.0021 (15)0.0002 (16)
N510.0638 (18)0.0436 (16)0.0469 (16)0.0055 (13)0.0047 (14)0.0003 (14)
C510.0372 (17)0.0399 (18)0.0402 (19)0.0008 (13)0.0030 (15)0.0031 (15)
C520.050 (2)0.081 (3)0.0354 (19)0.0081 (17)0.0018 (16)0.0045 (17)
Geometric parameters (Å, º) top
Li1—O72.038 (4)C5—C61.535 (3)
Li1—N112.072 (4)C6—O121.199 (2)
Li1—O3i2.130 (4)C6—O101.334 (2)
Li1—O4i2.225 (4)C7—O151.197 (2)
Li1—O16i2.265 (5)C7—O131.328 (2)
Li1—O15ii2.443 (5)C7—C81.538 (3)
Li1—Li23.299 (6)C8—O161.202 (2)
Li2—O4i2.061 (4)C8—O141.327 (3)
Li2—N212.085 (4)N11—C111.133 (3)
Li2—O72.169 (4)C11—C121.458 (3)
Li2—O82.222 (4)C12—H110.9800
Li2—O11iii2.287 (5)C12—H120.9800
Li2—O122.415 (5)C12—H130.9800
B1—O101.465 (3)N21—C211.142 (3)
B1—O91.465 (3)C21—C221.449 (3)
B1—O11.474 (3)C22—H210.9800
B1—O21.478 (3)C22—H220.9800
C1—O31.207 (2)C22—H230.9800
C1—O11.314 (2)N31—C311.133 (3)
C1—C21.511 (3)C31—C321.455 (3)
C2—O41.210 (2)C32—H31N0.9800
C2—O21.310 (2)C32—H32N0.9800
C3—O71.203 (2)C32—H33N0.9800
C3—O51.315 (2)N41—C411.129 (3)
C3—C41.511 (3)C41—C421.439 (4)
C4—O81.201 (2)C42—H410.9800
C4—O61.321 (3)C42—H420.9800
O5—B21.480 (3)C42—H430.9800
O6—B21.470 (3)N51—C511.136 (3)
B2—O131.462 (3)C51—C521.443 (4)
B2—O141.471 (3)C52—H510.9800
C5—O111.195 (2)C52—H520.9800
C5—O91.332 (2)C52—H530.9800
O7—Li1—N1193.68 (17)O6—B2—O14111.96 (19)
O7—Li1—O3i159.1 (2)O13—B2—O5110.69 (18)
N11—Li1—O3i107.1 (2)O6—B2—O5105.54 (18)
O7—Li1—O4i77.56 (15)O14—B2—O5110.74 (19)
N11—Li1—O4i171.0 (2)O11—C5—O9126.0 (2)
O3i—Li1—O4i81.73 (14)O11—C5—C6126.9 (2)
O7—Li1—O16i90.99 (18)O9—C5—C6107.11 (19)
N11—Li1—O16i92.22 (18)O12—C6—O10125.6 (2)
O3i—Li1—O16i90.42 (16)O12—C6—C5127.0 (2)
O4i—Li1—O16i85.96 (15)O10—C6—C5107.43 (18)
O7—Li1—O15ii89.16 (17)C5—O9—B1110.30 (17)
N11—Li1—O15ii98.21 (17)C6—O10—B1110.02 (18)
O3i—Li1—O15ii85.75 (16)C5—O11—Li2v131.13 (17)
O4i—Li1—O15ii83.85 (15)C6—O12—Li2131.91 (17)
O16i—Li1—O15ii169.5 (2)O15—C7—O13126.0 (2)
O4i—Li2—N2192.61 (17)O15—C7—C8126.7 (2)
O4i—Li2—O778.41 (16)O13—C7—C8107.30 (19)
N21—Li2—O7170.8 (2)O16—C8—O14126.2 (2)
O4i—Li2—O8159.1 (2)O16—C8—C7126.3 (2)
N21—Li2—O8107.94 (19)O14—C8—C7107.40 (19)
O7—Li2—O880.90 (15)C7—O13—B2110.17 (17)
O4i—Li2—O11iii95.39 (18)C8—O14—B2109.89 (18)
N21—Li2—O11iii94.16 (17)C7—O15—Li1vi130.00 (17)
O7—Li2—O11iii88.65 (17)C8—O16—Li1iv131.09 (18)
O8—Li2—O11iii87.28 (16)C11—N11—Li1146.5 (2)
O4i—Li2—O1290.37 (17)N11—C11—C12178.7 (3)
N21—Li2—O1294.15 (18)C11—C12—H11109.5
O7—Li2—O1284.08 (15)C11—C12—H12109.5
O8—Li2—O1284.32 (15)H11—C12—H12109.5
O11iii—Li2—O12169.7 (2)C11—C12—H13109.5
O10—B1—O9105.12 (18)H11—C12—H13109.5
O10—B1—O1111.56 (19)H12—C12—H13109.5
O9—B1—O1112.74 (18)C21—N21—Li2149.0 (2)
O10—B1—O2111.48 (19)N21—C21—C22178.3 (3)
O9—B1—O2110.62 (18)C21—C22—H21109.5
O1—B1—O2105.46 (18)C21—C22—H22109.5
O3—C1—O1127.5 (2)H21—C22—H22109.5
O3—C1—C2124.2 (2)C21—C22—H23109.5
O1—C1—C2108.23 (19)H21—C22—H23109.5
O4—C2—O2127.9 (2)H22—C22—H23109.5
O4—C2—C1123.1 (2)N31—C31—C32178.6 (3)
O2—C2—C1109.05 (19)C31—C32—H31N109.5
C1—O1—B1108.86 (18)C31—C32—H32N109.5
C2—O2—B1108.40 (18)H31N—C32—H32N109.5
C1—O3—Li1iv106.67 (19)C31—C32—H33N109.5
C2—O4—Li2iv155.05 (19)H31N—C32—H33N109.5
C2—O4—Li1iv104.26 (18)H32N—C32—H33N109.5
Li2iv—O4—Li1iv100.57 (17)N41—C41—C42179.3 (3)
O7—C3—O5127.5 (2)C41—C42—H41109.5
O7—C3—C4123.6 (2)C41—C42—H42109.5
O5—C3—C4108.9 (2)H41—C42—H42109.5
O8—C4—O6127.7 (2)C41—C42—H43109.5
O8—C4—C3124.0 (2)H41—C42—H43109.5
O6—C4—C3108.24 (19)H42—C42—H43109.5
C3—O5—B2108.46 (18)N51—C51—C52179.2 (3)
C4—O6—B2108.89 (18)C51—C52—H51109.5
C3—O7—Li1150.05 (19)C51—C52—H52109.5
C3—O7—Li2106.61 (19)H51—C52—H52109.5
Li1—O7—Li2103.24 (17)C51—C52—H53109.5
C4—O8—Li2104.80 (19)H51—C52—H53109.5
O13—B2—O6112.86 (19)H52—C52—H53109.5
O13—B2—O14105.17 (18)
O3—C1—C2—O41.2 (3)O11iii—Li2—O8—C486.71 (17)
O1—C1—C2—O4179.41 (19)O12—Li2—O8—C487.26 (17)
O3—C1—C2—O2178.6 (2)C4—O6—B2—O13121.26 (19)
O1—C1—C2—O20.7 (2)C4—O6—B2—O14120.3 (2)
O3—C1—O1—B1178.4 (2)C4—O6—B2—O50.3 (2)
C2—C1—O1—B10.9 (2)C3—O5—B2—O13122.15 (19)
O10—B1—O1—C1120.4 (2)C3—O5—B2—O60.3 (2)
O9—B1—O1—C1121.62 (19)C3—O5—B2—O14121.6 (2)
O2—B1—O1—C10.8 (2)O11—C5—C6—O120.2 (4)
O4—C2—O2—B1180.0 (2)O9—C5—C6—O12178.9 (2)
C1—C2—O2—B10.2 (2)O11—C5—C6—O10179.1 (2)
O10—B1—O2—C2120.9 (2)O9—C5—C6—O100.5 (2)
O9—B1—O2—C2122.52 (19)O11—C5—O9—B1179.9 (2)
O1—B1—O2—C20.3 (2)C6—C5—O9—B11.4 (2)
O1—C1—O3—Li1iv178.7 (2)O10—B1—O9—C51.8 (2)
C2—C1—O3—Li1iv0.5 (3)O1—B1—O9—C5120.0 (2)
O2—C2—O4—Li2iv3.6 (6)O2—B1—O9—C5122.24 (19)
C1—C2—O4—Li2iv176.2 (4)O12—C6—O10—B1180.0 (2)
O2—C2—O4—Li1iv177.8 (2)C5—C6—O10—B10.6 (2)
C1—C2—O4—Li1iv2.0 (3)O9—B1—O10—C61.4 (2)
O7—C3—C4—O80.9 (3)O1—B1—O10—C6121.1 (2)
O5—C3—C4—O8179.2 (2)O2—B1—O10—C6121.3 (2)
O7—C3—C4—O6179.1 (2)O9—C5—O11—Li2v12.8 (4)
O5—C3—C4—O60.8 (2)C6—C5—O11—Li2v168.9 (2)
O7—C3—C4—Li21.1 (2)O10—C6—O12—Li211.8 (4)
O5—C3—C4—Li2178.74 (19)C5—C6—O12—Li2167.5 (2)
O7—C3—O5—B2179.2 (2)O4i—Li2—O12—C6111.1 (2)
C4—C3—O5—B20.6 (2)N21—Li2—O12—C6156.2 (2)
O8—C4—O6—B2179.4 (2)O7—Li2—O12—C632.8 (3)
C3—C4—O6—B20.6 (2)O8—Li2—O12—C648.6 (3)
O5—C3—O7—Li13.5 (5)O11iii—Li2—O12—C612.8 (13)
C4—C3—O7—Li1176.4 (3)O15—C7—C8—O160.1 (4)
O5—C3—O7—Li2178.4 (2)O13—C7—C8—O16178.7 (2)
C4—C3—O7—Li21.5 (3)O15—C7—C8—O14178.6 (2)
N11—Li1—O7—C30.7 (5)O13—C7—C8—O140.2 (2)
O3i—Li1—O7—C3173.3 (5)O15—C7—O13—B2179.7 (2)
O4i—Li1—O7—C3178.6 (3)C8—C7—O13—B21.5 (2)
O16i—Li1—O7—C393.0 (4)O6—B2—O13—C7119.8 (2)
O15ii—Li1—O7—C397.5 (4)O14—B2—O13—C72.5 (2)
N11—Li1—O7—Li2174.36 (17)O5—B2—O13—C7122.18 (19)
O3i—Li1—O7—Li211.7 (7)O16—C8—O14—B2179.7 (2)
O4i—Li1—O7—Li23.58 (19)C7—C8—O14—B21.8 (2)
O16i—Li1—O7—Li282.07 (18)O13—B2—O14—C82.6 (2)
O15ii—Li1—O7—Li287.47 (17)O6—B2—O14—C8120.3 (2)
O4i—Li2—O7—C3178.74 (16)O5—B2—O14—C8122.3 (2)
O8—Li2—O7—C32.0 (2)O13—C7—O15—Li1vi15.9 (4)
O11iii—Li2—O7—C385.48 (18)C8—C7—O15—Li1vi165.6 (2)
O12—Li2—O7—C387.15 (17)O14—C8—O16—Li1iv5.9 (4)
O4i—Li2—O7—Li13.8 (2)C7—C8—O16—Li1iv172.4 (2)
O8—Li2—O7—Li1179.39 (16)O7—Li1—N11—C1118.4 (5)
O11iii—Li2—O7—Li191.93 (18)O3i—Li1—N11—C11163.9 (4)
O12—Li2—O7—Li195.44 (17)O16i—Li1—N11—C1172.7 (4)
O6—C4—O8—Li2177.4 (2)O15ii—Li1—N11—C11108.1 (4)
C3—C4—O8—Li22.5 (3)O4i—Li2—N21—C214.1 (5)
O4i—Li2—O8—C411.3 (7)O8—Li2—N21—C21171.9 (4)
N21—Li2—O8—C4179.8 (2)O11iii—Li2—N21—C2199.7 (4)
O7—Li2—O8—C42.36 (19)O12—Li2—N21—C2186.5 (5)
Symmetry codes: (i) x1/2, y+1/2, z1/2; (ii) x+1/2, y+1/2, z1/2; (iii) x1, y, z; (iv) x+1/2, y+1/2, z+1/2; (v) x+1, y, z; (vi) x1/2, y+1/2, z+1/2.
(III) Lithium bis(oxalato)borate acetone top
Crystal data top
C7H6BLiO9·0.33(C3H6O)F(000) = 555
Mr = 271.21Dx = 1.531 Mg m3
Monoclinic, C2/mMo Kα radiation, λ = 0.71073 Å
Hall symbol: -C 2yCell parameters from 2604 reflections
a = 16.3987 (16) Åθ = 2.6–31.1°
b = 7.6308 (7) ŵ = 0.14 mm1
c = 10.9904 (11) ÅT = 110 K
β = 121.201 (2)°Needle, colorless
V = 1176.4 (2) Å30.50 × 0.16 × 0.11 mm
Z = 4
Data collection top
Three-circle
diffractometer
1437 independent reflections
Radiation source: fine-focus sealed tube1116 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.041
Detector resolution: 8.33 pixels mm-1θmax = 27.5°, θmin = 2.2°
ω scansh = 2019
Absorption correction: multi-scan
XPREP (Sheldrick, 1997)
k = 99
Tmin = 0.914, Tmax = 0.985l = 1414
4923 measured reflections
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)] = 0.047Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.129H-atom parameters constrained
S = 1.00 w = 1/[σ2(Fo2) + (0.07P)2 + 0.94P], P = (max(Fo2,0) + 2Fc2)/3
1437 reflections(Δ/σ)max < 0.001
134 parametersΔρmax = 0.40 e Å3
38 restraintsΔρmin = 0.32 e Å3
Crystal data top
C7H6BLiO9·0.33(C3H6O)V = 1176.4 (2) Å3
Mr = 271.21Z = 4
Monoclinic, C2/mMo Kα radiation
a = 16.3987 (16) ŵ = 0.14 mm1
b = 7.6308 (7) ÅT = 110 K
c = 10.9904 (11) Å0.50 × 0.16 × 0.11 mm
β = 121.201 (2)°
Data collection top
Three-circle
diffractometer
1437 independent reflections
Absorption correction: multi-scan
XPREP (Sheldrick, 1997)
1116 reflections with I > 2σ(I)
Tmin = 0.914, Tmax = 0.985Rint = 0.041
4923 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.04738 restraints
wR(F2) = 0.129H-atom parameters constrained
S = 1.00Δρmax = 0.40 e Å3
1437 reflectionsΔρmin = 0.32 e Å3
134 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)
Li10.4553 (3)0.50000.3184 (5)0.0353 (12)
B10.1970 (2)0.50000.4670 (3)0.0199 (6)
C10.04544 (12)0.3988 (3)0.38430 (18)0.0213 (4)
O10.13486 (8)0.34723 (16)0.43429 (13)0.0229 (3)
O20.02221 (9)0.30551 (19)0.34642 (14)0.0284 (4)
C20.33668 (17)0.50000.4698 (3)0.0175 (5)
O30.24415 (12)0.50000.38254 (17)0.0184 (4)
O40.39806 (12)0.50000.44008 (19)0.0211 (4)
C30.35768 (18)0.50000.6224 (3)0.0205 (6)
O50.27568 (12)0.50000.61686 (18)0.0236 (5)
O60.43586 (13)0.50000.72712 (19)0.0255 (5)
O70.34606 (14)0.50000.1240 (2)0.0383 (6)
C40.3209 (3)0.4491 (5)0.0033 (4)0.0378 (12)0.50
C50.2275 (3)0.5302 (12)0.1198 (5)0.059 (2)0.50
H5A0.18130.54420.08930.088*0.50
H5B0.20080.45270.20280.088*0.50
H5C0.24140.64500.14490.088*0.50
C60.3752 (4)0.3209 (7)0.0274 (5)0.0482 (13)0.50
H6A0.40650.38110.07100.072*0.50
H6B0.33170.23150.09290.072*0.50
H6C0.42350.26500.06140.072*0.50
O80.4733 (4)0.00000.1384 (6)0.0348 (18)0.334 (4)
C70.4232 (6)0.00000.0894 (7)0.053 (3)0.334 (4)
C80.3905 (7)0.1639 (13)0.0577 (9)0.069 (3)0.334 (4)
H8A0.39210.25870.11660.104*0.334 (4)
H8B0.43250.19340.04310.104*0.334 (4)
H8C0.32520.14880.07830.104*0.334 (4)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Li10.016 (2)0.065 (4)0.025 (2)0.0000.0100 (19)0.000
B10.0147 (15)0.0199 (14)0.0261 (14)0.0000.0114 (12)0.000
C10.0138 (9)0.0270 (10)0.0235 (9)0.0005 (7)0.0099 (7)0.0030 (7)
O10.0119 (7)0.0209 (7)0.0356 (7)0.0007 (5)0.0121 (5)0.0044 (6)
O20.0145 (7)0.0313 (8)0.0370 (8)0.0039 (6)0.0117 (6)0.0061 (6)
C20.0137 (13)0.0116 (11)0.0260 (12)0.0000.0094 (10)0.000
O30.0118 (9)0.0206 (9)0.0230 (9)0.0000.0091 (7)0.000
O40.0172 (10)0.0172 (9)0.0351 (10)0.0000.0179 (8)0.000
C30.0146 (13)0.0198 (13)0.0275 (13)0.0000.0111 (11)0.000
O50.0140 (10)0.0338 (11)0.0254 (9)0.0000.0119 (8)0.000
O60.0139 (10)0.0321 (11)0.0253 (9)0.0000.0064 (8)0.000
O70.0217 (11)0.0629 (16)0.0254 (11)0.0000.0087 (9)0.000
C40.029 (2)0.051 (3)0.0341 (19)0.0023 (17)0.0171 (16)0.0042 (16)
C50.049 (2)0.075 (5)0.041 (2)0.022 (3)0.0151 (18)0.002 (3)
C60.054 (3)0.052 (3)0.039 (2)0.002 (2)0.025 (2)0.001 (2)
O80.035 (4)0.039 (4)0.029 (3)0.0000.015 (3)0.000
C70.077 (7)0.046 (6)0.043 (5)0.0000.036 (5)0.000
C80.089 (6)0.057 (5)0.069 (5)0.002 (5)0.047 (5)0.006 (4)
Geometric parameters (Å, º) top
Li1—O71.951 (5)C3—O61.200 (3)
Li1—O41.993 (5)C3—O51.314 (3)
Li1—O6i2.087 (5)O7—C41.230 (4)
Li1—O2ii2.3554 (17)C4—C61.475 (7)
Li1—O2iii2.3554 (17)C4—C51.553 (7)
Li1—O4i2.493 (5)C5—H5A0.9800
Li1—Li1i3.468 (9)C5—H5B0.9800
B1—O11.465 (2)C5—H5C0.9800
B1—O1iv1.465 (2)C6—H6A0.9800
B1—O51.475 (3)C6—H6B0.9800
B1—O31.485 (3)C6—H6C0.9800
C1—O21.197 (2)O8—C71.193 (13)
C1—O11.331 (2)C7—C81.472 (11)
C1—C1iv1.544 (4)C7—C8v1.472 (11)
C2—O41.208 (3)C8—H8A0.9800
C2—O31.309 (3)C8—H8B0.9800
C2—C31.527 (4)C8—H8C0.9800
O7—Li1—O4104.5 (2)Li1—O4—Li1i100.66 (17)
O7—Li1—O6i98.8 (2)O6—C3—O5127.1 (2)
O4—Li1—O6i156.8 (3)O6—C3—C2125.1 (2)
O7—Li1—O2ii97.81 (12)O5—C3—C2107.8 (2)
O4—Li1—O2ii90.47 (12)C3—O5—B1109.54 (19)
O6i—Li1—O2ii86.35 (12)C3—O6—Li1i113.0 (2)
O7—Li1—O2iii97.81 (12)C4—O7—Li1141.7 (3)
O4—Li1—O2iii90.47 (12)O7—C4—C6123.4 (4)
O6i—Li1—O2iii86.35 (12)O7—C4—C5116.2 (4)
O2ii—Li1—O2iii163.6 (2)C6—C4—C5120.3 (4)
O7—Li1—O4i176.2 (3)C4—C5—H5A109.5
O4—Li1—O4i79.34 (17)C4—C5—H5B109.5
O6i—Li1—O4i77.45 (16)H5A—C5—H5B109.5
O2ii—Li1—O4i82.04 (12)C4—C5—H5C109.5
O2iii—Li1—O4i82.04 (12)H5A—C5—H5C109.5
O1—B1—O1iv105.5 (2)H5B—C5—H5C109.5
O1—B1—O5111.68 (14)C4—C6—H6A109.5
O1iv—B1—O5111.68 (14)C4—C6—H6B109.5
O1—B1—O3111.55 (14)H6A—C6—H6B109.5
O1iv—B1—O3111.55 (14)C4—C6—H6C109.5
O5—B1—O3105.1 (2)H6A—C6—H6C109.5
O2—C1—O1126.29 (18)H6B—C6—H6C109.5
O2—C1—C1iv126.51 (11)O8—C7—C8121.8 (6)
O1—C1—C1iv107.20 (10)O8—C7—C8v121.8 (6)
C1—O1—B1110.06 (15)C8—C7—C8v116.4 (11)
C1—O2—Li1vi133.49 (17)C7—C8—H8A109.5
O4—C2—O3127.8 (2)C7—C8—H8B109.5
O4—C2—C3123.5 (2)H8A—C8—H8B109.5
O3—C2—C3108.7 (2)C7—C8—H8C109.5
C2—O3—B1108.87 (19)H8A—C8—H8C109.5
C2—O4—Li1158.3 (2)H8B—C8—H8C109.5
C2—O4—Li1i101.00 (19)
O2—C1—O1—B1179.07 (19)O2ii—Li1—O4—Li1i81.81 (12)
C1iv—C1—O1—B10.88 (16)O2iii—Li1—O4—Li1i81.81 (12)
O1iv—B1—O1—C11.4 (3)O4i—Li1—O4—Li1i0.000 (1)
O5—B1—O1—C1122.88 (17)C3i—Li1—O4—Li1i0.000 (1)
O3—B1—O1—C1119.87 (17)O4—C2—C3—O60.0
O1—C1—O2—Li1vi5.6 (3)O3—C2—C3—O6180.0
C1iv—C1—O2—Li1vi174.36 (17)O4—C2—C3—O5180.0
O4—C2—O3—B1180.0O3—C2—C3—O50.0
C3—C2—O3—B10.0O4—C2—C3—Li1i0.0
O1—B1—O3—C2121.17 (15)O3—C2—C3—Li1i180.0
O1iv—B1—O3—C2121.17 (15)O6—C3—O5—B1180.000 (1)
O5—B1—O3—C20.0C2—C3—O5—B10.0
O3—C2—O4—Li10.000 (2)O1—B1—O5—C3121.09 (15)
C3—C2—O4—Li1180.000 (1)O1iv—B1—O5—C3121.09 (15)
O3—C2—O4—Li1i180.0O3—B1—O5—C30.0
C3—C2—O4—Li1i0.0O5—C3—O6—Li1i180.0
O7—Li1—O4—C20.000 (1)C2—C3—O6—Li1i0.0
O6i—Li1—O4—C2180.000 (2)O4—Li1—O7—C4149.3 (3)
O2ii—Li1—O4—C298.19 (12)O6i—Li1—O7—C430.7 (3)
O2iii—Li1—O4—C298.19 (12)O2ii—Li1—O7—C4118.1 (2)
O4i—Li1—O4—C2180.000 (1)O2iii—Li1—O7—C456.8 (3)
C3i—Li1—O4—C2180.000 (1)Li1—O7—C4—C613.2 (4)
O7—Li1—O4—Li1i180.0Li1—O7—C4—C5165.7 (4)
O6i—Li1—O4—Li1i0.000 (2)
Symmetry codes: (i) x+1, y+1, z+1; (ii) x+1/2, y+1/2, z; (iii) x+1/2, y+1/2, z; (iv) x, y+1, z; (v) x, y, z; (vi) x1/2, y1/2, z.
(IV) Lithium bis(oxalato)borate dimethoxyethylene top
Crystal data top
C8H10BLiO10Z = 2
Mr = 283.91F(000) = 292
Triclinic, P1Dx = 1.545 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 8.6690 (7) ÅCell parameters from 2770 reflections
b = 8.8519 (7) Åθ = 2.7–31.1°
c = 9.3328 (8) ŵ = 0.14 mm1
α = 114.159 (2)°T = 110 K
β = 94.764 (2)°Prism, colorless
γ = 106.412 (2)°0.51 × 0.36 × 0.26 mm
V = 610.45 (9) Å3
Data collection top
Three-circle
diffractometer
3509 independent reflections
Radiation source: fine-focus sealed tube3051 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.021
Detector resolution: 8.33 pixels mm-1θmax = 30.0°, θmin = 2.5°
ω scansh = 1212
Absorption correction: multi-scan
XPREP (Sheldrick, 1997)
k = 1212
Tmin = 0.841, Tmax = 0.964l = 1313
7526 measured reflections
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)] = 0.035Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.096H-atom parameters constrained
S = 1.00 w = 1/[σ2(Fo2) + (0.0661P)2], P = (max(Fo2,0) + 2Fc2)/3
3509 reflections(Δ/σ)max < 0.001
221 parametersΔρmax = 0.53 e Å3
0 restraintsΔρmin = 0.22 e Å3
Crystal data top
C8H10BLiO10γ = 106.412 (2)°
Mr = 283.91V = 610.45 (9) Å3
Triclinic, P1Z = 2
a = 8.6690 (7) ÅMo Kα radiation
b = 8.8519 (7) ŵ = 0.14 mm1
c = 9.3328 (8) ÅT = 110 K
α = 114.159 (2)°0.51 × 0.36 × 0.26 mm
β = 94.764 (2)°
Data collection top
Three-circle
diffractometer
3509 independent reflections
Absorption correction: multi-scan
XPREP (Sheldrick, 1997)
3051 reflections with I > 2σ(I)
Tmin = 0.841, Tmax = 0.964Rint = 0.021
7526 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0350 restraints
wR(F2) = 0.096H-atom parameters constrained
S = 1.00Δρmax = 0.53 e Å3
3509 reflectionsΔρmin = 0.22 e Å3
221 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*/Ueq
Li10.9908 (2)0.4673 (2)0.66495 (19)0.0229 (3)
B10.40189 (12)0.22735 (12)0.35914 (12)0.01674 (19)
C10.64402 (10)0.21424 (11)0.46098 (10)0.01740 (17)
C20.52292 (10)0.02575 (11)0.34779 (10)0.01819 (17)
O10.57021 (7)0.32714 (8)0.46203 (8)0.01825 (14)
O20.78055 (8)0.25042 (9)0.53412 (8)0.02201 (15)
O30.38654 (7)0.04142 (8)0.28830 (8)0.01931 (14)
O40.54796 (9)0.10880 (9)0.31981 (9)0.02514 (16)
C30.24817 (10)0.34638 (12)0.25628 (10)0.01801 (17)
C40.19216 (10)0.33526 (11)0.40392 (10)0.01550 (16)
O50.37064 (8)0.28348 (9)0.23412 (8)0.01965 (14)
O60.18617 (8)0.40082 (10)0.17704 (8)0.02549 (16)
O70.27791 (7)0.26145 (8)0.45761 (7)0.01679 (14)
O80.08443 (7)0.38691 (8)0.45699 (8)0.01888 (14)
C51.20340 (14)0.86761 (13)0.88249 (13)0.0280 (2)
H511.1326 (16)0.8849 (17)0.9588 (16)0.032 (3)*
H521.1604 (16)0.8882 (17)0.7965 (16)0.030 (3)*
H531.3164 (17)0.9499 (18)0.9335 (16)0.031 (3)*
O91.20013 (8)0.69028 (8)0.81689 (7)0.02184 (15)
C61.26904 (12)0.65323 (13)0.93876 (11)0.0250 (2)
H611.2022 (15)0.6723 (16)1.0206 (15)0.029 (3)*
H621.3850 (17)0.7268 (18)0.9867 (16)0.035 (3)*
C71.25813 (11)0.46405 (13)0.85966 (11)0.02255 (19)
H711.3247 (14)0.4436 (15)0.7803 (14)0.019 (3)*
H721.2981 (15)0.4322 (16)0.9414 (15)0.024 (3)*
O101.08761 (8)0.35962 (9)0.78452 (8)0.02237 (15)
C81.05617 (14)0.17565 (13)0.73139 (14)0.0273 (2)
H811.0806 (17)0.1551 (18)0.8241 (17)0.037 (3)*
H821.1243 (16)0.1343 (18)0.6584 (17)0.034 (3)*
H830.9404 (18)0.1152 (19)0.6741 (17)0.038 (3)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Li10.0208 (7)0.0228 (8)0.0251 (8)0.0083 (6)0.0034 (6)0.0107 (7)
B10.0144 (4)0.0164 (4)0.0178 (4)0.0060 (3)0.0034 (3)0.0059 (4)
C10.0154 (4)0.0183 (4)0.0197 (4)0.0070 (3)0.0054 (3)0.0087 (3)
C20.0162 (4)0.0188 (4)0.0190 (4)0.0074 (3)0.0043 (3)0.0071 (3)
O10.0139 (3)0.0160 (3)0.0228 (3)0.0057 (2)0.0020 (2)0.0070 (2)
O20.0142 (3)0.0243 (3)0.0268 (3)0.0061 (3)0.0022 (2)0.0118 (3)
O30.0157 (3)0.0159 (3)0.0213 (3)0.0060 (2)0.0007 (2)0.0040 (2)
O40.0255 (3)0.0193 (3)0.0298 (4)0.0111 (3)0.0048 (3)0.0085 (3)
C30.0159 (4)0.0190 (4)0.0171 (4)0.0055 (3)0.0029 (3)0.0069 (3)
C40.0132 (4)0.0142 (4)0.0157 (4)0.0031 (3)0.0009 (3)0.0052 (3)
O50.0191 (3)0.0243 (3)0.0188 (3)0.0108 (3)0.0068 (2)0.0103 (3)
O60.0258 (4)0.0321 (4)0.0244 (3)0.0130 (3)0.0041 (3)0.0167 (3)
O70.0152 (3)0.0184 (3)0.0187 (3)0.0077 (2)0.0048 (2)0.0088 (2)
O80.0147 (3)0.0199 (3)0.0212 (3)0.0075 (2)0.0047 (2)0.0075 (2)
C50.0311 (5)0.0184 (5)0.0265 (5)0.0051 (4)0.0038 (4)0.0054 (4)
O90.0236 (3)0.0193 (3)0.0177 (3)0.0062 (3)0.0002 (2)0.0053 (3)
C60.0240 (5)0.0284 (5)0.0165 (4)0.0062 (4)0.0006 (3)0.0074 (4)
C70.0189 (4)0.0286 (5)0.0201 (4)0.0082 (4)0.0008 (3)0.0117 (4)
O100.0191 (3)0.0217 (3)0.0262 (3)0.0064 (3)0.0013 (3)0.0120 (3)
C80.0293 (5)0.0232 (5)0.0333 (5)0.0104 (4)0.0065 (4)0.0159 (4)
Geometric parameters (Å, º) top
Li1—O102.0059 (17)C3—C41.5294 (12)
Li1—O22.0574 (17)C4—O81.2081 (10)
Li1—O8i2.0949 (17)C4—O71.3081 (10)
Li1—O92.1112 (17)C5—O91.4231 (11)
Li1—O8ii2.2229 (17)C5—H510.972 (13)
Li1—O6ii2.4232 (18)C5—H520.962 (13)
Li1—Li1iii3.366 (3)C5—H530.976 (14)
B1—O31.4611 (11)O9—C61.4356 (11)
B1—O11.4751 (11)C6—C71.4984 (14)
B1—O51.4765 (11)C6—H610.986 (13)
B1—O71.4870 (11)C6—H620.976 (14)
C1—O21.2009 (10)C7—O101.4340 (11)
C1—O11.3277 (10)C7—H710.967 (12)
C1—C21.5444 (12)C7—H720.984 (12)
C2—O41.1978 (10)O10—C81.4276 (12)
C2—O31.3311 (10)C8—H810.973 (14)
C3—O61.2001 (11)C8—H820.965 (14)
C3—O51.3252 (10)C8—H830.976 (15)
O10—Li1—O296.17 (7)O8—C4—O7127.70 (8)
O10—Li1—O8i100.87 (7)O8—C4—C3123.38 (8)
O2—Li1—O8i86.83 (7)O7—C4—C3108.92 (7)
O10—Li1—O981.46 (6)C3—O5—B1109.10 (7)
O2—Li1—O9175.18 (9)C3—O6—Li1ii104.28 (7)
O8i—Li1—O997.73 (7)C4—O7—B1108.76 (6)
O10—Li1—O8ii172.64 (9)C4—O8—Li1iv142.70 (7)
O2—Li1—O8ii90.94 (6)C4—O8—Li1ii110.73 (7)
O8i—Li1—O8ii77.61 (6)Li1iv—O8—Li1ii102.39 (6)
O9—Li1—O8ii91.57 (7)O9—C5—H51109.6 (7)
O10—Li1—O6ii106.28 (7)O9—C5—H52108.7 (8)
O2—Li1—O6ii86.16 (6)H51—C5—H52108.1 (10)
O8i—Li1—O6ii152.52 (8)O9—C5—H53110.4 (8)
O9—Li1—O6ii90.46 (6)H51—C5—H53111.2 (11)
O8ii—Li1—O6ii75.98 (5)H52—C5—H53108.9 (11)
O10—Li1—Li1iii140.56 (10)C5—O9—C6111.40 (7)
O2—Li1—Li1iii88.65 (7)C5—O9—Li1124.38 (7)
O8i—Li1—Li1iii40.17 (4)C6—O9—Li1107.55 (7)
O9—Li1—Li1iii95.84 (8)O9—C6—C7107.67 (7)
O8ii—Li1—Li1iii37.44 (4)O9—C6—H61107.5 (7)
O6ii—Li1—Li1iii113.09 (8)C7—C6—H61110.4 (7)
O3—B1—O1106.01 (6)O9—C6—H62111.8 (8)
O3—B1—O5111.68 (7)C7—C6—H62108.1 (8)
O1—B1—O5112.24 (7)H61—C6—H62111.3 (11)
O3—B1—O7111.55 (7)O10—C7—C6106.92 (7)
O1—B1—O7110.05 (7)O10—C7—H71110.3 (7)
O5—B1—O7105.41 (7)C6—C7—H71111.5 (7)
O2—C1—O1126.66 (8)O10—C7—H72110.4 (7)
O2—C1—C2125.50 (8)C6—C7—H72109.7 (7)
O1—C1—C2107.83 (7)H71—C7—H72108.0 (9)
O4—C2—O3126.78 (8)C8—O10—C7112.18 (7)
O4—C2—C1126.00 (8)C8—O10—Li1126.24 (8)
O3—C2—C1107.22 (7)C7—O10—Li1110.05 (7)
C1—O1—B1109.08 (7)O10—C8—H81109.4 (8)
C1—O2—Li1139.52 (8)O10—C8—H82111.2 (8)
C2—O3—B1109.71 (7)H81—C8—H82108.4 (11)
O6—C3—O5128.35 (8)O10—C8—H83106.2 (8)
O6—C3—C4123.92 (8)H81—C8—H83112.7 (12)
O5—C3—C4107.72 (7)H82—C8—H83109.0 (12)
O2—C1—C2—O41.14 (14)O8—C4—O7—B1177.41 (9)
O1—C1—C2—O4178.99 (8)C3—C4—O7—B13.18 (9)
O2—C1—C2—O3179.05 (8)O3—B1—O7—C4124.26 (7)
O1—C1—C2—O30.82 (9)O1—B1—O7—C4118.36 (7)
O2—C1—O1—B1178.51 (8)O5—B1—O7—C42.88 (9)
C2—C1—O1—B11.62 (9)O7—C4—O8—Li1iv21.13 (17)
O3—B1—O1—C13.32 (9)C3—C4—O8—Li1iv159.55 (10)
O5—B1—O1—C1125.50 (7)O7—C4—O8—Li1ii172.26 (8)
O7—B1—O1—C1117.44 (7)C3—C4—O8—Li1ii8.41 (11)
O1—C1—O2—Li111.63 (17)O10—Li1—O9—C5145.33 (8)
C2—C1—O2—Li1168.21 (9)O8i—Li1—O9—C5114.76 (8)
O10—Li1—O2—C1159.67 (10)O8ii—Li1—O9—C537.06 (10)
O8i—Li1—O2—C199.73 (11)O6ii—Li1—O9—C538.94 (10)
O8ii—Li1—O2—C122.20 (13)O10—Li1—O9—C612.48 (8)
O6ii—Li1—O2—C153.68 (12)O8i—Li1—O9—C6112.38 (7)
O4—C2—O3—B1176.89 (9)O8ii—Li1—O9—C6169.91 (6)
C1—C2—O3—B12.92 (9)O6ii—Li1—O9—C693.92 (7)
O1—B1—O3—C23.89 (9)C5—O9—C6—C7179.15 (8)
O5—B1—O3—C2126.43 (7)Li1—O9—C6—C739.68 (9)
O7—B1—O3—C2115.90 (8)O9—C6—C7—O1056.72 (10)
O6—C3—C4—O82.95 (14)C6—C7—O10—C8168.80 (8)
O5—C3—C4—O8178.17 (8)C6—C7—O10—Li145.27 (9)
O6—C3—C4—O7176.49 (8)O2—Li1—O10—C825.70 (11)
O5—C3—C4—O72.39 (9)O8i—Li1—O10—C862.25 (11)
O6—C3—O5—B1178.34 (9)O9—Li1—O10—C8158.54 (8)
C4—C3—O5—B10.48 (9)O6ii—Li1—O10—C8113.48 (9)
O3—B1—O5—C3122.62 (7)O2—Li1—O10—C7165.67 (7)
O1—B1—O5—C3118.47 (8)O8i—Li1—O10—C777.72 (8)
O7—B1—O5—C31.32 (9)O9—Li1—O10—C718.57 (8)
O5—C3—O6—Li1ii170.36 (9)O6ii—Li1—O10—C7106.55 (8)
C4—C3—O6—Li1ii10.99 (11)
Symmetry codes: (i) x+1, y, z; (ii) x+1, y+1, z+1; (iii) x+2, y+1, z+1; (iv) x1, y, z.
(V) Lithium bis(oxalato)borate 1,3-dioxolane hydrate top
Crystal data top
C17H20B2Li2O23Z = 2
Mr = 627.83F(000) = 644
Triclinic, P1Dx = 1.735 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 9.1327 (14) ÅCell parameters from 2243 reflections
b = 9.6378 (15) Åθ = 2.5–27.5°
c = 14.812 (2) ŵ = 0.16 mm1
α = 80.640 (3)°T = 110 K
β = 79.414 (3)°Prism, colorles
γ = 70.642 (3)°0.27 × 0.14 × 0.08 mm
V = 1201.8 (3) Å3
Data collection top
Three-circle
diffractometer
4074 independent reflections
Radiation source: fine-focus sealed tube2144 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.098
Detector resolution: 8.33 pixels mm-1θmax = 24.7°, θmin = 1.4°
ω scansh = 1010
Absorption correction: multi-scan
XPREP (Sheldrick, 1997)
k = 1111
Tmin = 0.881, Tmax = 0.987l = 1717
9591 measured reflections
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.058H-atom parameters constrained
wR(F2) = 0.110 w = 1/[σ2(Fo2) + (0.005P)2], P = (max(Fo2,0) + 2Fc2)/3
S = 0.89(Δ/σ)max < 0.001
4074 reflectionsΔρmax = 0.38 e Å3
398 parametersΔρmin = 0.36 e Å3
282 restraintsExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0130 (17)
Crystal data top
C17H20B2Li2O23γ = 70.642 (3)°
Mr = 627.83V = 1201.8 (3) Å3
Triclinic, P1Z = 2
a = 9.1327 (14) ÅMo Kα radiation
b = 9.6378 (15) ŵ = 0.16 mm1
c = 14.812 (2) ÅT = 110 K
α = 80.640 (3)°0.27 × 0.14 × 0.08 mm
β = 79.414 (3)°
Data collection top
Three-circle
diffractometer
4074 independent reflections
Absorption correction: multi-scan
XPREP (Sheldrick, 1997)
2144 reflections with I > 2σ(I)
Tmin = 0.881, Tmax = 0.987Rint = 0.098
9591 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.058282 restraints
wR(F2) = 0.110H-atom parameters constrained
S = 0.89Δρmax = 0.38 e Å3
4074 reflectionsΔρmin = 0.36 e Å3
398 parameters
Special details top

Experimental. Crystal was split and only major part was integrated.

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*/Ueq
Li11.1028 (10)0.8227 (9)0.0353 (6)0.027 (2)
Li20.3957 (10)0.4003 (8)0.5058 (5)0.022 (2)
B10.5272 (6)0.8893 (6)0.1303 (4)0.0165 (13)
C10.7596 (6)0.9301 (5)0.0783 (3)0.0162 (11)
C20.6465 (5)1.0653 (5)0.1213 (3)0.0159 (11)
C30.3905 (5)0.7319 (5)0.2027 (3)0.0131 (11)
C40.3296 (6)0.8048 (5)0.1118 (3)0.0149 (11)
O10.6915 (3)0.8301 (3)0.08320 (19)0.0166 (8)
O20.8944 (4)0.9228 (3)0.0445 (2)0.0198 (8)
O30.5134 (3)1.0338 (3)0.15269 (19)0.0167 (8)
O40.6728 (4)1.1783 (3)0.1245 (2)0.0184 (8)
O50.5005 (3)0.7875 (3)0.21389 (19)0.0151 (8)
O60.3480 (4)0.6410 (3)0.2576 (2)0.0192 (8)
O70.4129 (4)0.8932 (3)0.0722 (2)0.0167 (8)
O80.2263 (4)0.7830 (3)0.0820 (2)0.0176 (8)
B20.0924 (6)0.9593 (6)0.3683 (4)0.0123 (12)
C50.1887 (6)0.7379 (5)0.4518 (3)0.0161 (11)
C60.2941 (6)0.8323 (5)0.4497 (3)0.0166 (11)
C70.0118 (5)1.0917 (5)0.2326 (3)0.0167 (11)
C80.1001 (6)1.1625 (5)0.3159 (3)0.0174 (11)
O90.0727 (3)0.8176 (3)0.40509 (19)0.0167 (8)
O100.2077 (4)0.6138 (3)0.4880 (2)0.0185 (8)
O110.2304 (3)0.9639 (3)0.40495 (19)0.0162 (8)
O120.4151 (4)0.7968 (3)0.4821 (2)0.0188 (8)
O130.1232 (3)0.9779 (3)0.26550 (19)0.0168 (8)
O140.0019 (4)1.1346 (3)0.1526 (2)0.0212 (8)
O150.0493 (3)1.0832 (3)0.39216 (19)0.0162 (8)
O160.2143 (4)1.2697 (3)0.3116 (2)0.0216 (8)
O1W0.5365 (3)0.4941 (3)0.40200 (19)0.0165 (8)
H1W0.47610.56480.35560.025*
H2W0.62600.41880.37110.025*
C90.1557 (6)0.3283 (5)0.4152 (3)0.0240 (13)
H9A0.08590.42520.43400.029*
H9B0.13160.24940.46130.029*
C100.3967 (5)0.2434 (5)0.3315 (3)0.0232 (12)
H10A0.42370.13480.34690.028*
H10B0.49330.26950.30590.028*
C110.2767 (6)0.3004 (5)0.2659 (3)0.0262 (13)
H11A0.27760.39840.23340.031*
H11B0.29510.23070.21970.031*
O170.3143 (4)0.3204 (3)0.4110 (2)0.0226 (8)
O180.1310 (4)0.3107 (3)0.3265 (2)0.0242 (8)
C121.2452 (6)0.5233 (5)0.1015 (3)0.0207 (12)
H12A1.19450.45720.11890.025*
H12B1.26380.59240.15630.025*
C131.1763 (5)0.4946 (5)0.0509 (3)0.0224 (12)
H13A1.10830.43110.05780.027*
H13B1.15640.54240.10820.027*
C141.3479 (5)0.4052 (5)0.0303 (3)0.0165 (11)
H14A1.41320.43470.06530.020*
H14B1.36300.29800.04620.020*
O190.2522 (4)0.3053 (3)0.6116 (2)0.0204 (8)
O200.1837 (4)0.1345 (3)0.7242 (2)0.0209 (8)
C150.2878 (6)0.1522 (5)0.6399 (3)0.0192 (12)
H15A0.39840.10970.65100.023*
H15B0.27190.10090.59150.023*
C160.1723 (6)0.3795 (5)0.6919 (3)0.0219 (12)
H16A0.10290.48020.67460.026*
H16B0.24740.38610.73020.026*
C170.0797 (5)0.2806 (4)0.7412 (3)0.0168 (11)
H17A0.05510.29110.80810.020*
H17B0.01920.30240.71540.020*
O211.1491 (4)0.6030 (3)0.0277 (2)0.0187 (8)
O221.3872 (4)0.4402 (3)0.0685 (2)0.0195 (8)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Li10.025 (3)0.028 (3)0.025 (3)0.0060 (19)0.0018 (19)0.0029 (19)
Li20.018 (3)0.023 (3)0.022 (3)0.0065 (19)0.0016 (19)0.0012 (19)
B10.011 (2)0.019 (2)0.016 (2)0.0031 (16)0.0015 (16)0.0017 (17)
C10.0150 (19)0.0177 (18)0.0148 (19)0.0040 (16)0.0011 (15)0.0018 (15)
C20.0114 (16)0.0186 (16)0.0156 (16)0.0019 (13)0.0022 (13)0.0009 (13)
C30.0079 (18)0.0148 (18)0.0122 (18)0.0013 (15)0.0007 (15)0.0021 (15)
C40.0129 (19)0.0156 (18)0.0136 (19)0.0014 (15)0.0008 (16)0.0034 (15)
O10.0109 (15)0.0191 (14)0.0161 (15)0.0018 (12)0.0028 (12)0.0035 (12)
O20.0126 (15)0.0247 (15)0.0186 (15)0.0036 (13)0.0019 (12)0.0020 (13)
O30.0114 (15)0.0203 (14)0.0159 (15)0.0053 (12)0.0038 (12)0.0011 (12)
O40.0127 (15)0.0207 (14)0.0188 (15)0.0030 (12)0.0020 (12)0.0035 (12)
O50.0103 (15)0.0197 (14)0.0126 (14)0.0024 (12)0.0000 (12)0.0006 (12)
O60.0128 (15)0.0211 (15)0.0182 (15)0.0021 (13)0.0007 (12)0.0033 (13)
O70.0137 (15)0.0191 (14)0.0159 (15)0.0056 (12)0.0005 (12)0.0000 (12)
O80.0134 (15)0.0221 (15)0.0153 (14)0.0038 (12)0.0000 (12)0.0027 (12)
B20.009 (2)0.014 (2)0.011 (2)0.0001 (16)0.0016 (16)0.0008 (16)
C50.0118 (19)0.0203 (19)0.0118 (18)0.0002 (15)0.0028 (15)0.0043 (16)
C60.0151 (19)0.0205 (19)0.0116 (18)0.0028 (16)0.0005 (15)0.0030 (15)
C70.0132 (19)0.0189 (18)0.0153 (19)0.0031 (15)0.0004 (15)0.0004 (16)
C80.0157 (19)0.0178 (18)0.0168 (19)0.0038 (16)0.0012 (16)0.0006 (16)
O90.0081 (15)0.0216 (15)0.0145 (14)0.0005 (12)0.0012 (12)0.0004 (12)
O100.0119 (15)0.0199 (14)0.0181 (15)0.0016 (12)0.0039 (12)0.0002 (13)
O110.0115 (15)0.0188 (14)0.0139 (14)0.0014 (12)0.0008 (12)0.0007 (12)
O120.0123 (15)0.0246 (15)0.0157 (15)0.0020 (12)0.0001 (12)0.0015 (12)
O130.0106 (15)0.0200 (14)0.0125 (14)0.0027 (12)0.0012 (12)0.0000 (12)
O140.0175 (15)0.0251 (15)0.0148 (15)0.0002 (12)0.0003 (12)0.0011 (13)
O150.0112 (15)0.0195 (14)0.0120 (14)0.0007 (12)0.0013 (12)0.0003 (12)
O160.0141 (15)0.0248 (15)0.0191 (15)0.0009 (13)0.0007 (12)0.0013 (13)
O1W0.0070 (18)0.0229 (18)0.0103 (17)0.0031 (15)0.0037 (14)0.0023 (14)
C90.014 (3)0.038 (3)0.023 (3)0.010 (2)0.002 (2)0.008 (2)
C100.009 (3)0.035 (3)0.021 (3)0.002 (2)0.007 (2)0.012 (2)
C110.015 (3)0.040 (3)0.020 (3)0.007 (2)0.007 (2)0.006 (2)
O170.0129 (15)0.0322 (15)0.0206 (15)0.0044 (12)0.0006 (12)0.0060 (13)
O180.0164 (15)0.0327 (15)0.0189 (15)0.0018 (13)0.0002 (12)0.0048 (13)
C120.017 (3)0.026 (3)0.014 (3)0.000 (2)0.004 (2)0.001 (2)
C130.015 (3)0.025 (3)0.019 (3)0.001 (2)0.002 (2)0.002 (2)
C140.012 (2)0.020 (2)0.014 (2)0.000 (2)0.000 (2)0.002 (2)
O190.0166 (19)0.0212 (17)0.0168 (18)0.0033 (15)0.0083 (15)0.0016 (15)
O200.0173 (15)0.0226 (14)0.0162 (14)0.0026 (12)0.0060 (12)0.0003 (12)
C150.015 (3)0.023 (3)0.016 (3)0.007 (2)0.009 (2)0.003 (2)
C160.021 (3)0.022 (2)0.017 (3)0.002 (2)0.006 (2)0.006 (2)
C170.009 (2)0.023 (2)0.014 (2)0.001 (2)0.003 (2)0.006 (2)
O210.0130 (18)0.0243 (18)0.0118 (17)0.0005 (15)0.0050 (14)0.0017 (14)
O220.0085 (18)0.0303 (19)0.0123 (17)0.0000 (15)0.0037 (14)0.0001 (15)
Geometric parameters (Å, º) top
Li1—O212.006 (8)B2—O111.476 (6)
Li1—O14i2.055 (9)B2—O131.489 (6)
Li1—O22.068 (9)C5—O101.198 (5)
Li1—O8ii2.158 (9)C5—O91.322 (5)
Li1—O4iii2.223 (9)C5—C61.522 (6)
Li1—O2iii2.443 (8)C6—O121.208 (5)
Li1—Li1iii3.534 (16)C6—O111.329 (5)
Li2—O172.057 (8)C7—O141.199 (5)
Li2—O1W2.104 (8)C7—O131.321 (5)
Li2—O12iv2.110 (8)C7—C81.543 (6)
Li2—O1Wiv2.113 (8)C8—O161.203 (5)
Li2—O192.141 (8)C8—O151.323 (5)
Li2—O102.214 (8)C9—O171.416 (5)
Li2—Li2iv3.091 (15)C9—O181.418 (5)
B1—O31.444 (6)C10—O171.446 (5)
B1—O71.458 (6)C10—C111.505 (6)
B1—O51.486 (6)C11—O181.445 (5)
B1—O11.497 (6)C12—O221.406 (5)
C1—O21.224 (5)C12—O211.424 (5)
C1—O11.295 (5)C13—O211.431 (5)
C1—C21.519 (6)C13—C141.519 (6)
C2—O41.201 (5)C14—O221.453 (5)
C2—O31.333 (5)O19—C151.411 (5)
C3—O61.207 (5)O19—C161.440 (5)
C3—O51.331 (5)O20—C171.446 (5)
C3—C41.525 (6)O20—C151.447 (5)
C4—O81.201 (5)C16—C171.495 (6)
C4—O71.325 (5)O1W—H1W0.99
B2—O91.443 (5)O1W—H2W0.99
B2—O151.474 (6)
O21—Li1—O14i94.0 (3)C2—O4—Li1iii109.3 (4)
O21—Li1—O2112.4 (4)C3—O5—B1108.6 (3)
O14i—Li1—O292.6 (4)C4—O7—B1110.4 (4)
O21—Li1—O8ii87.5 (3)C4—O8—Li1v145.4 (4)
O14i—Li1—O8ii175.9 (5)O9—B2—O15112.2 (4)
O2—Li1—O8ii90.3 (3)O9—B2—O11105.6 (4)
O21—Li1—O4iii93.9 (4)O15—B2—O11112.9 (4)
O14i—Li1—O4iii88.6 (3)O9—B2—O13112.8 (4)
O2—Li1—O4iii153.4 (4)O15—B2—O13104.8 (3)
O8ii—Li1—O4iii87.4 (3)O11—B2—O13108.7 (4)
O21—Li1—O2iii168.0 (5)O10—C5—O9126.1 (4)
O14i—Li1—O2iii92.7 (3)O10—C5—C6126.6 (4)
O2—Li1—O2iii77.2 (3)O9—C5—C6107.3 (4)
O8ii—Li1—O2iii85.1 (3)O12—C6—O11124.8 (4)
O4iii—Li1—O2iii76.3 (3)O12—C6—C5127.3 (4)
O17—Li2—O1W92.4 (3)O11—C6—C5107.9 (4)
O17—Li2—O12iv91.4 (3)O14—C7—O13126.2 (4)
O1W—Li2—O12iv90.1 (3)O14—C7—C8126.3 (4)
O17—Li2—O1Wiv173.6 (4)O13—C7—C8107.5 (4)
O1W—Li2—O1Wiv85.7 (3)O16—C8—O15126.5 (4)
O12iv—Li2—O1Wiv94.7 (3)O16—C8—C7125.7 (4)
O17—Li2—O1987.7 (3)O15—C8—C7107.9 (4)
O1W—Li2—O19179.9 (4)C5—O9—B2110.3 (4)
O12iv—Li2—O1990.0 (3)C5—O10—Li2140.6 (4)
O1Wiv—Li2—O1994.2 (3)C6—O11—B2108.5 (3)
O17—Li2—O1089.6 (3)C6—O12—Li2iv134.4 (4)
O1W—Li2—O1086.4 (3)C7—O13—B2109.8 (3)
O12iv—Li2—O10176.4 (4)C7—O14—Li1i154.0 (4)
O1Wiv—Li2—O1084.3 (3)C8—O15—B2109.9 (4)
O19—Li2—O1093.5 (3)Li2—O1W—Li2iv94.3 (3)
O3—B1—O7112.9 (4)H1W—O1W—H2W110.3
O3—B1—O5112.2 (4)O17—C9—O18108.5 (4)
O7—B1—O5105.2 (4)O17—C10—C11101.5 (4)
O3—B1—O1105.6 (4)H10A—C10—H10B109.3
O7—B1—O1111.5 (4)O18—C11—C10102.8 (4)
O5—B1—O1109.5 (4)C9—O17—C10105.4 (3)
O2—C1—O1127.4 (4)C9—O17—Li2123.8 (3)
O2—C1—C2122.5 (4)C10—O17—Li2130.7 (4)
O1—C1—C2110.1 (4)C9—O18—C11106.7 (4)
O4—C2—O3127.5 (4)O22—C12—O21106.2 (3)
O4—C2—C1126.1 (4)O21—C13—C14104.1 (4)
O3—C2—C1106.4 (4)O22—C14—C13104.1 (3)
O6—C3—O5124.0 (4)C15—O19—C16106.6 (3)
O6—C3—C4127.7 (4)C15—O19—Li2123.7 (3)
O5—C3—C4108.2 (4)C16—O19—Li2121.0 (3)
O8—C4—O7127.1 (4)C17—O20—C15106.8 (3)
O8—C4—C3125.5 (4)O19—C15—O20107.2 (3)
O7—C4—C3107.4 (4)O19—C16—C17102.1 (3)
C1—O1—B1107.9 (4)O20—C17—C16103.1 (3)
C1—O2—Li1151.0 (4)C12—O21—C13102.5 (3)
C1—O2—Li1iii103.5 (3)C12—O21—Li1120.4 (4)
Li1—O2—Li1iii102.8 (3)C13—O21—Li1128.9 (3)
C2—O3—B1110.0 (4)C12—O22—C14106.1 (3)
O2—C1—C2—O42.6 (8)O13—B2—O11—C6115.0 (4)
O1—C1—C2—O4177.2 (4)O11—C6—O12—Li2iv142.7 (5)
O2—C1—C2—O3178.5 (4)C5—C6—O12—Li2iv37.0 (8)
O1—C1—C2—O31.6 (5)O14—C7—O13—B2179.1 (4)
O6—C3—C4—O81.3 (8)C8—C7—O13—B22.6 (5)
O5—C3—C4—O8177.7 (4)O9—B2—O13—C7119.6 (4)
O6—C3—C4—O7177.7 (4)O15—B2—O13—C72.8 (5)
O5—C3—C4—O73.3 (5)O11—B2—O13—C7123.7 (4)
O2—C1—O1—B1180.0 (5)O13—C7—O14—Li1i115.4 (9)
C2—C1—O1—B10.2 (5)C8—C7—O14—Li1i66.7 (10)
O3—B1—O1—C11.2 (5)O16—C8—O15—B2179.0 (4)
O7—B1—O1—C1121.8 (4)C7—C8—O15—B20.2 (5)
O5—B1—O1—C1122.2 (4)O9—B2—O15—C8121.0 (4)
O1—C1—O2—Li113.2 (11)O11—B2—O15—C8119.9 (4)
C2—C1—O2—Li1166.6 (6)O13—B2—O15—C81.7 (5)
O1—C1—O2—Li1iii167.6 (4)O17—Li2—O1W—Li2iv173.9 (4)
C2—C1—O2—Li1iii12.2 (5)O12iv—Li2—O1W—Li2iv94.7 (3)
O21—Li1—O2—C133.2 (10)O1Wiv—Li2—O1W—Li2iv0.0
O14i—Li1—O2—C162.3 (9)O10—Li2—O1W—Li2iv84.5 (3)
O8ii—Li1—O2—C1120.6 (7)O17—C10—C11—O1837.4 (4)
O4iii—Li1—O2—C1154.5 (8)O18—C9—O17—C1021.2 (5)
O2iii—Li1—O2—C1154.5 (8)O18—C9—O17—Li2160.6 (4)
Li1iii—Li1—O2—C1154.5 (8)C11—C10—O17—C935.9 (4)
O21—Li1—O2—Li1iii172.4 (5)C11—C10—O17—Li2146.1 (4)
O14i—Li1—O2—Li1iii92.2 (3)O1W—Li2—O17—C9137.0 (4)
O8ii—Li1—O2—Li1iii84.9 (3)O12iv—Li2—O17—C9132.9 (4)
O4iii—Li1—O2—Li1iii0.0 (9)O19—Li2—O17—C942.9 (5)
O2iii—Li1—O2—Li1iii0.0O10—Li2—O17—C950.6 (5)
O4—C2—O3—B1176.5 (5)Li2iv—Li2—O17—C9131.2 (6)
C1—C2—O3—B12.3 (5)O1W—Li2—O17—C1045.3 (5)
O7—B1—O3—C2119.8 (4)O12iv—Li2—O17—C1044.8 (5)
O5—B1—O3—C2121.5 (4)O19—Li2—O17—C10134.8 (4)
O1—B1—O3—C22.2 (5)O10—Li2—O17—C10131.7 (4)
O3—C2—O4—Li1iii168.3 (4)Li2iv—Li2—O17—C1051.2 (9)
C1—C2—O4—Li1iii10.3 (6)O17—C9—O18—C113.4 (5)
O6—C3—O5—B1176.9 (4)C10—C11—O18—C925.4 (5)
C4—C3—O5—B14.1 (5)O21—C13—C14—O2217.4 (4)
O3—B1—O5—C3126.7 (4)O17—Li2—O19—C1574.0 (4)
O7—B1—O5—C33.5 (5)O12iv—Li2—O19—C1517.4 (5)
O1—B1—O5—C3116.4 (4)O1Wiv—Li2—O19—C15112.1 (4)
O8—C4—O7—B1180.0 (5)O10—Li2—O19—C15163.4 (3)
C3—C4—O7—B11.0 (5)Li2iv—Li2—O19—C15112.2 (7)
O3—B1—O7—C4124.1 (4)O17—Li2—O19—C16142.7 (3)
O5—B1—O7—C41.4 (5)O12iv—Li2—O19—C16126.0 (4)
O1—B1—O7—C4117.2 (4)O1Wiv—Li2—O19—C1631.3 (5)
O7—C4—O8—Li1v7.4 (9)O10—Li2—O19—C1653.2 (4)
C3—C4—O8—Li1v171.5 (5)Li2iv—Li2—O19—C1631.2 (9)
O10—C5—C6—O121.8 (8)C16—O19—C15—O2020.4 (5)
O9—C5—C6—O12177.4 (4)Li2—O19—C15—O20168.1 (4)
O10—C5—C6—O11178.4 (4)C17—O20—C15—O193.6 (5)
O9—C5—C6—O112.3 (5)C15—O19—C16—C1735.3 (5)
O14—C7—C8—O161.0 (8)Li2—O19—C16—C17175.9 (4)
O13—C7—C8—O16179.2 (4)C15—O20—C17—C1624.9 (4)
O14—C7—C8—O15179.8 (4)O19—C16—C17—O2036.5 (4)
O13—C7—C8—O151.6 (5)O22—C12—O21—C1342.2 (4)
O10—C5—O9—B2177.5 (4)O22—C12—O21—Li1109.0 (4)
C6—C5—O9—B21.7 (5)C14—C13—O21—C1235.6 (4)
O15—B2—O9—C5128.1 (4)C14—C13—O21—Li1112.1 (5)
O11—B2—O9—C54.8 (5)O14i—Li1—O21—C1259.8 (5)
O13—B2—O9—C5113.8 (4)O2—Li1—O21—C12154.3 (4)
O9—C5—O10—Li2136.8 (5)O8ii—Li1—O21—C12116.4 (4)
C6—C5—O10—Li242.3 (8)O4iii—Li1—O21—C1229.1 (5)
O17—Li2—O10—C5104.5 (6)O2iii—Li1—O21—C1264 (2)
O1W—Li2—O10—C512.1 (6)O14i—Li1—O21—C13157.4 (4)
O1Wiv—Li2—O10—C574.0 (6)O2—Li1—O21—C1362.9 (6)
O19—Li2—O10—C5167.8 (5)O8ii—Li1—O21—C1326.4 (5)
Li2iv—Li2—O10—C531.0 (7)O4iii—Li1—O21—C13113.7 (4)
O12—C6—O11—B2174.5 (4)O2iii—Li1—O21—C1379 (2)
C5—C6—O11—B25.3 (5)O21—C12—O22—C1431.0 (4)
O9—B2—O11—C66.2 (5)C13—C14—O22—C127.9 (4)
O15—B2—O11—C6129.2 (4)
Symmetry codes: (i) x+1, y+2, z; (ii) x+1, y, z; (iii) x+2, y+2, z; (iv) x+1, y+1, z+1; (v) x1, y, z.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1W—H1W···O60.991.932.880 (4)160
O1W—H2W···O16vi0.991.882.865 (4)176
Symmetry code: (vi) x+1, y1, z.
(VI) Lithium tetrakis-ethylenecarbonate bis(oxalato)borate top
Crystal data top
C12H16LiO12·C4BO8Dx = 1.599 Mg m3
Mr = 546.04Mo Kα radiation, λ = 0.71073 Å
Tetragonal, I4Cell parameters from 3376 reflections
Hall symbol: I -4θ = 2.7–31.5°
a = 10.2343 (5) ŵ = 0.15 mm1
c = 10.8245 (7) ÅT = 110 K
V = 1133.77 (11) Å3Prism, colorless
Z = 20.51 × 0.46 × 0.38 mm
F(000) = 560
Data collection top
Three-circle
diffractometer
876 independent reflections
Radiation source: fine-focus sealed tube871 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.020
Detector resolution: 8.33 pixels mm-1θmax = 30.0°, θmin = 2.7°
ω scansh = 1314
Absorption correction: multi-scan
SADABS (Sheldrick, 1996)
k = 1014
Tmin = 0.905, Tmax = 0.945l = 1515
7169 measured reflections
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.024H-atom parameters constrained
wR(F2) = 0.050 w = 1/[σ2(Fo2) + (0.01P)2 + 0.921P], P = (max(Fo2,0) + 2Fc2)/3
S = 1.00(Δ/σ)max < 0.001
876 reflectionsΔρmax = 0.29 e Å3
103 parametersΔρmin = 0.15 e Å3
0 restraintsExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0190 (12)
Crystal data top
C12H16LiO12·C4BO8Z = 2
Mr = 546.04Mo Kα radiation
Tetragonal, I4µ = 0.15 mm1
a = 10.2343 (5) ÅT = 110 K
c = 10.8245 (7) Å0.51 × 0.46 × 0.38 mm
V = 1133.77 (11) Å3
Data collection top
Three-circle
diffractometer
876 independent reflections
Absorption correction: multi-scan
SADABS (Sheldrick, 1996)
871 reflections with I > 2σ(I)
Tmin = 0.905, Tmax = 0.945Rint = 0.020
7169 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0240 restraints
wR(F2) = 0.050H-atom parameters constrained
S = 1.00Δρmax = 0.29 e Å3
876 reflectionsΔρmin = 0.15 e Å3
103 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.

Friedel pairs have been averaged during the refinement using MERG 3 instruction because of absence the atoms with noticeable anoumalous scatering.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Li10.50000.50000.00000.0192 (10)
C10.17553 (16)0.26669 (18)0.28798 (16)0.0257 (3)
H110.099 (2)0.320 (2)0.293 (2)0.035 (6)*
H120.199 (2)0.232 (2)0.366 (2)0.029 (5)*
C20.17070 (15)0.16338 (15)0.18697 (16)0.0220 (3)
H210.0943 (19)0.1690 (18)0.1376 (18)0.017 (5)*
H220.183 (2)0.077 (2)0.219 (2)0.028 (5)*
O10.27950 (11)0.35363 (11)0.24743 (12)0.0229 (2)
O20.28314 (10)0.19381 (10)0.11039 (10)0.0184 (2)
C30.33366 (14)0.30701 (14)0.14573 (13)0.0178 (3)
O30.42228 (11)0.35924 (12)0.09178 (13)0.0286 (3)
B10.50000.00000.25000.0138 (5)
C40.44843 (13)0.05450 (13)0.44948 (13)0.0164 (3)
O40.42176 (10)0.08350 (10)0.33220 (9)0.0159 (2)
O50.40114 (12)0.10327 (12)0.53880 (10)0.0255 (3)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Li10.0182 (14)0.0182 (14)0.021 (2)0.0000.0000.000
C10.0211 (7)0.0367 (9)0.0193 (7)0.0035 (6)0.0040 (6)0.0033 (6)
C20.0176 (6)0.0216 (7)0.0268 (8)0.0027 (5)0.0006 (6)0.0073 (6)
O10.0242 (5)0.0223 (5)0.0222 (5)0.0011 (4)0.0042 (5)0.0033 (5)
O20.0185 (5)0.0180 (5)0.0187 (5)0.0010 (4)0.0010 (4)0.0009 (4)
C30.0162 (6)0.0172 (6)0.0200 (6)0.0026 (5)0.0047 (5)0.0055 (5)
O30.0193 (5)0.0304 (6)0.0360 (7)0.0036 (4)0.0007 (5)0.0157 (5)
B10.0136 (7)0.0136 (7)0.0141 (12)0.0000.0000.000
C40.0154 (6)0.0170 (6)0.0168 (6)0.0016 (5)0.0005 (5)0.0004 (5)
O40.0160 (5)0.0171 (5)0.0145 (4)0.0045 (3)0.0003 (4)0.0002 (4)
O50.0285 (6)0.0298 (6)0.0181 (5)0.0068 (5)0.0034 (5)0.0051 (5)
Geometric parameters (Å, º) top
Li1—O3i1.9222 (11)O1—C31.3216 (19)
Li1—O3ii1.9222 (11)O2—C31.3251 (18)
Li1—O31.9222 (11)C3—O31.2039 (18)
Li1—O3iii1.9222 (11)B1—O4iv1.4707 (10)
C1—O11.455 (2)B1—O4v1.4707 (10)
C1—C21.522 (2)B1—O41.4707 (10)
C1—H110.96 (2)B1—O4vi1.4707 (10)
C1—H120.95 (2)C4—O51.1908 (17)
C2—O21.4520 (18)C4—O41.3320 (17)
C2—H210.949 (19)C4—C4v1.536 (3)
C2—H220.96 (2)
O3i—Li1—O3ii105.49 (4)H21—C2—H22111.6 (17)
O3i—Li1—O3117.76 (8)C3—O1—C1109.71 (12)
O3ii—Li1—O3105.49 (4)C3—O2—C2109.39 (11)
O3i—Li1—O3iii105.49 (4)O3—C3—O1124.03 (15)
O3ii—Li1—O3iii117.76 (8)O3—C3—O2122.83 (15)
O3—Li1—O3iii105.49 (4)O1—C3—O2113.11 (12)
O1—C1—C2103.41 (12)C3—O3—Li1153.53 (11)
O1—C1—H11105.4 (14)O4iv—B1—O4v111.47 (4)
C2—C1—H11114.1 (14)O4iv—B1—O4111.47 (4)
O1—C1—H12108.3 (12)O4v—B1—O4105.55 (8)
C2—C1—H12113.0 (13)O4iv—B1—O4vi105.55 (8)
H11—C1—H12111.9 (18)O4v—B1—O4vi111.47 (4)
O2—C2—C1103.61 (12)O4—B1—O4vi111.47 (4)
O2—C2—H21108.5 (12)O5—C4—O4126.67 (13)
C1—C2—H21112.9 (11)O5—C4—C4v125.72 (9)
O2—C2—H22107.6 (13)O4—C4—C4v107.62 (7)
C1—C2—H22112.1 (13)C4—O4—B1109.61 (8)
O1—C1—C2—O27.34 (15)O3i—Li1—O3—C386.6 (3)
C2—C1—O1—C33.68 (16)O3ii—Li1—O3—C3156.0 (3)
C1—C2—O2—C38.92 (15)O3iii—Li1—O3—C330.7 (3)
C1—O1—C3—O3179.93 (14)O5—C4—O4—B1179.35 (14)
C1—O1—C3—O22.02 (17)C4v—C4—O4—B10.40 (17)
C2—O2—C3—O3174.69 (13)O4iv—B1—O4—C4121.00 (8)
C2—O2—C3—O17.23 (16)O4v—B1—O4—C40.17 (7)
O1—C3—O3—Li163.0 (3)O4vi—B1—O4—C4121.34 (8)
O2—C3—O3—Li1119.1 (3)
Symmetry codes: (i) x+1, y+1, z; (ii) y+1, x, z; (iii) y, x+1, z; (iv) y+1/2, x1/2, z+1/2; (v) x+1, y, z; (vi) y+1/2, x+1/2, z+1/2.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C1—H11···O1vii0.96 (2)2.74 (2)3.350 (2)121.8 (17)
C1—H12···O2viii0.95 (2)2.76 (2)3.539 (2)140.4 (17)
C2—H21···O1vii0.949 (19)2.810 (19)3.3728 (19)118.9 (14)
C2—H22···O3iv0.96 (2)2.62 (2)3.452 (2)144.9 (17)
C2—H22···O4iv0.96 (2)2.92 (2)3.5335 (19)122.6 (16)
Symmetry codes: (iv) y+1/2, x1/2, z+1/2; (vii) y1/2, x+1/2, z+1/2; (viii) x+1/2, y+1/2, z+1/2.

Experimental details

(I)(II)(III)(IV)
Crystal data
Chemical formulaC4H2BLiO9C12H6B2Li2N2O16·3(C2H3N)C7H6BLiO9·0.33(C3H6O)C8H10BLiO10
Mr211.81592.85271.21283.91
Crystal system, space groupOrthorhombic, PbcaMonoclinic, P21/nMonoclinic, C2/mTriclinic, P1
Temperature (K)294110110110
a, b, c (Å)16.075 (3), 15.880 (3), 5.6008 (9)7.6346 (8), 22.631 (2), 14.9338 (16)16.3987 (16), 7.6308 (7), 10.9904 (11)8.6690 (7), 8.8519 (7), 9.3328 (8)
α, β, γ (°)90, 90, 9090, 91.879 (2), 9090, 121.201 (2), 90114.159 (2), 94.764 (2), 106.412 (2)
V3)1429.7 (4)2578.9 (5)1176.4 (2)610.45 (9)
Z8442
Radiation typeMo KαMo KαMo KαMo Kα
µ (mm1)0.200.130.140.14
Crystal size (mm)0.38 × 0.09 × 0.020.48 × 0.36 × 0.300.50 × 0.16 × 0.110.51 × 0.36 × 0.26
Data collection
DiffractometerThree-circle
diffractometer
Three-circle
diffractometer
Three-circle
diffractometer
Three-circle
diffractometer
Absorption correctionMulti-scan
XPREP (Sheldrick, 1997)
Multi-scan
XPREP (Sheldrick, 1997)
Multi-scan
XPREP (Sheldrick, 1997)
Multi-scan
XPREP (Sheldrick, 1997)
Tmin, Tmax0.873, 0.9960.873, 0.9610.914, 0.9850.841, 0.964
No. of measured, independent and
observed [I > 2σ(I)] reflections
9124, 1440, 1044 14456, 4542, 3039 4923, 1437, 1116 7526, 3509, 3051
Rint0.0820.0390.0410.021
(sin θ/λ)max1)0.6250.5950.6490.704
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.060, 0.089, 1.00 0.042, 0.090, 1.00 0.047, 0.129, 1.00 0.035, 0.096, 1.00
No. of reflections1440454214373509
No. of parameters144393134221
No. of restraints00380
H-atom treatmentH-atom parameters constrainedH-atom parameters constrainedH-atom parameters constrainedH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.23, 0.300.21, 0.260.40, 0.320.53, 0.22


(V)(VI)
Crystal data
Chemical formulaC17H20B2Li2O23C12H16LiO12·C4BO8
Mr627.83546.04
Crystal system, space groupTriclinic, P1Tetragonal, I4
Temperature (K)110110
a, b, c (Å)9.1327 (14), 9.6378 (15), 14.812 (2)10.2343 (5), 10.2343 (5), 10.8245 (7)
α, β, γ (°)80.640 (3), 79.414 (3), 70.642 (3)90, 90, 90
V3)1201.8 (3)1133.77 (11)
Z22
Radiation typeMo KαMo Kα
µ (mm1)0.160.15
Crystal size (mm)0.27 × 0.14 × 0.080.51 × 0.46 × 0.38
Data collection
DiffractometerThree-circle
diffractometer
Three-circle
diffractometer
Absorption correctionMulti-scan
XPREP (Sheldrick, 1997)
Multi-scan
SADABS (Sheldrick, 1996)
Tmin, Tmax0.881, 0.9870.905, 0.945
No. of measured, independent and
observed [I > 2σ(I)] reflections
9591, 4074, 2144 7169, 876, 871
Rint0.0980.020
(sin θ/λ)max1)0.5880.703
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.058, 0.110, 0.89 0.024, 0.050, 1.00
No. of reflections4074876
No. of parameters398103
No. of restraints2820
H-atom treatmentH-atom parameters constrainedH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.38, 0.360.29, 0.15

Computer programs: SMART (Bruker, 1999), SAINT (Bruker, 1999), SAINT, SHELXS97 (Sheldrick, 1990), SHELXL97 (Sheldrick, 1997), Materials Studio (2001), ATOMS (Dowty,1999), SHELXL97.

Hydrogen-bond geometry (Å, º) for (I) top
D—H···AD—HH···AD···AD—H···A
O1w—H2···O3i0.84 (4)2.57 (4)3.039 (3)117 (3)
O1w—H2···O8ii0.84 (4)2.11 (4)2.910 (3)159 (4)
O1w—H1···O4iii0.87 (4)2.09 (4)2.960 (3)174 (4)
Symmetry codes: (i) x+1/2, y+1/2, z+2; (ii) x+1, y1/2, z+5/2; (iii) x+1/2, y, z+3/2.
Hydrogen-bond geometry (Å, º) for (V) top
D—H···AD—HH···AD···AD—H···A
O1W—H1W···O60.991.932.880 (4)160.3
O1W—H2W···O16i0.991.882.865 (4)176.0
Symmetry code: (i) x+1, y1, z.
Hydrogen-bond geometry (Å, º) for (VI) top
D—H···AD—HH···AD···AD—H···A
C1—H11···O1i0.96 (2)2.74 (2)3.350 (2)121.8 (17)
C1—H12···O2ii0.95 (2)2.76 (2)3.539 (2)140.4 (17)
C2—H21···O1i0.949 (19)2.810 (19)3.3728 (19)118.9 (14)
C2—H22···O3iii0.96 (2)2.62 (2)3.452 (2)144.9 (17)
C2—H22···O4iii0.96 (2)2.92 (2)3.5335 (19)122.6 (16)
Symmetry codes: (i) y1/2, x+1/2, z+1/2; (ii) x+1/2, y+1/2, z+1/2; (iii) y+1/2, x1/2, z+1/2.
 

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