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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2012 May 12;68(Pt 6):m749. doi: 10.1107/S1600536812017540

Lithium bis­(2-methyl­lactato)borate monohydrate

Joshua L Allen a, Elie Paillard a, Paul D Boyle b, Wesley A Henderson a,*
PMCID: PMC3379088  PMID: 22719309

Abstract

The title compound {systematic name: poly[[aqua­lithium]-μ-3,3,8,8-tetra­methyl-1,4,6,9-tetra­oxa-5λ4-borataspiro­[4.4]nonane-2,7-dione]}, [Li(C8H12BO6)(H2O)]n (LiBMLB), forms a 12-membered macrocycle, which lies across a crystallographic inversion center. The lithium cations are pseudo-tetra­hedrally coordinated by three methyl­lactate ligands and a water mol­ecule. The asymmetric units couple across crystallographic inversion centers, forming the 12-membered macrocycles. These macrocycles, in turn, cross-link through the Li+ cations, forming an infinite polymeric structure in two dimensions parallel to (101).

Related literature  

For the synthesis and purification of HBMLB [BMLB is bis­(2-methyl­lactato)borate], see: Lamande et al. (1987). For the synthesis and properties of LiBMLB and BMLB-based ionic liquids, see: Xu et al. (2003). For crystallographic data of similar lithium salts, see: Zavalij et al. (2004); Allen et al. (2011).graphic file with name e-68-0m749-scheme1.jpg

Experimental  

Crystal data  

  • [Li(C8H12BO6)(H2O)]

  • M r = 239.94

  • Orthorhombic, Inline graphic

  • a = 12.7034 (4) Å

  • b = 11.3939 (4) Å

  • c = 15.8258 (5) Å

  • V = 2290.65 (13) Å3

  • Z = 8

  • Mo Kα radiation

  • μ = 0.12 mm−1

  • T = 110 K

  • 0.34 × 0.23 × 0.18 mm

Data collection  

  • Bruker–Nonius Kappa X8 APEXII diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2007) T min = 0.961, T max = 0.979

  • 97648 measured reflections

  • 5663 independent reflections

  • 4436 reflections with I > 2σ(I)

  • R int = 0.037

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.036

  • wR(F 2) = 0.098

  • S = 1.05

  • 5663 reflections

  • 210 parameters

  • All H-atom parameters refined

  • Δρmax = 0.51 e Å−3

  • Δρmin = −0.26 e Å−3

Data collection: APEX2 (Bruker, 2007); cell refinement: SAINT (Bruker, 2007); data reduction: SAINT; program(s) used to solve structure: SIR92 (Altomare et al., 1994); program(s) used to refine structure: XL (Sheldrick, 2008); molecular graphics: ORTEP-3 (Farrugia, 1997); software used to prepare material for publication: cif2tables.py (Boyle, 2008).

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812017540/vn2036sup1.cif

e-68-0m749-sup1.cif (18.7KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812017540/vn2036Isup2.hkl

e-68-0m749-Isup2.hkl (277.4KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Selected bond lengths (Å).

Li1—O1 1.9725 (13)
Li1—O1W 1.9487 (13)
Li1—O3i 2.0059 (13)
Li1—O6ii 1.9155 (13)

Symmetry codes: (i) Inline graphic; (ii) Inline graphic.

Acknowledgments

This work was fully supported by the US DOE BATT Program (contract DE—AC02–05-CH11231). The authors wish to thank the Department of Chemistry of North Carolina State University and the State of North Carolina for funding the purchase of the APEXII diffractometer. JLA would like to thank the SMART Scholarship Program and the American Society for Engineering Education (ASEE) for the award of a SMART Graduate Research Fellowship.

supplementary crystallographic information

Comment

Various lithium salts for lithium-ion batteries have been proposed in recent years either as alternatives to the commonly used lithium hexafluorophosphate (LiPF6) or as electrolyte additives. Of these salts, lithium bis(oxalato)borate [LiBOB] remains one of the most promising (Zavalij et al.). The title compound, lithium bis(2-methyllactato)borate [LiBMLB] is based on this structure, differing only by replacing the oxygen of a carbonyl group of each ligand with two methyl groups. Although this salt has previously been synthesized (Lamande et al., Xu et al.), the crystal structure and ion coordination have not yet been reported. The structure of the monohydrate solvate of this salt is reported in the present manuscript.

The Li+ cation coordination in the title compound is different from what has been previously reported for similar cyclic structures (Allen et al., Zavalij et al.). For salts such as LiBOB, the Li+ cations are exclusively coordinated by the anion carbonyl oxygen atoms. In the present structure, however, the anion ring pseudo-ether oxygen also participates in the Li+ cation coordination (Fig. 1). Thus, each Li+ cation is coordinated by two carbonyl oxygen atoms from two BMLB- anions, one ring oxygen from a third BMLB- anion and an oxygen from a single water molecule. The asymmetric unit couples across crystallographic inversion centers to form 12-membered macrocycles (Fig. 2). These macrocycles are cross-linked through the Li+ cation coordination, forming the infinite polymeric crystal structure in two dimensions parallel to (101) (Fig. 3).

Experimental

Lithium bis(2-methyllactato)borate was synthesized by dissolving 2-methyllactic acid, boric acid and lithium carbonate (mole ratio 4:2:1) in water. The aqueous solution was allowed to slowly evaporate, forming colorless crystals suitable for X-ray analysis.

Refinement

The hydrogen atom positional and isotropic displacement parameters were included in the refinement.

Figures

Fig. 1.

Fig. 1.

Asymmetric unit of LiBMLB-H2O showing naming and numbering scheme. Thermal ellipsoids are at 50% probability (Li-purple, O-red, B-tan, C-grey).

Fig. 2.

Fig. 2.

A 12-membered macrocycle formed from two LiBMLB-H2O units. Thermal ellipsoids are at 50% probability (Li-purple, O-red, B-tan, C-grey).

Fig. 3.

Fig. 3.

A portion of the unit cell of [LiBMLB-H2O]n. Thermal ellipsoids are at 50% probability (Li-purple, O-red, B-tan, C-grey).

Crystal data

[Li(C8H12BO6)(H2O)] F(000) = 1008
Mr = 239.94 Dx = 1.392 Mg m3
Orthorhombic, Pbca Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ac 2ab Cell parameters from 9969 reflections
a = 12.7034 (4) Å θ = 2.7–35.0°
b = 11.3939 (4) Å µ = 0.12 mm1
c = 15.8258 (5) Å T = 110 K
V = 2290.65 (13) Å3 Prism, colourless
Z = 8 0.34 × 0.23 × 0.18 mm

Data collection

Bruker–Nonius Kappa X8 APEXII diffractometer 5663 independent reflections
Radiation source: fine-focus sealed tube 4436 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.037
ω and φ scans θmax = 37.4°, θmin = 2.6°
Absorption correction: multi-scan (SADABS; Bruker, 2007) h = −21→21
Tmin = 0.961, Tmax = 0.979 k = −19→19
97648 measured reflections l = −24→26

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)] = 0.036 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.098 All H-atom parameters refined
S = 1.05 w = 1/[σ2(Fo2) + (0.0519P)2 + 0.3146P] where P = (Fo2 + 2Fc2)/3
5663 reflections (Δ/σ)max = 0.001
210 parameters Δρmax = 0.51 e Å3
0 restraints Δρmin = −0.26 e Å3

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
Li1 0.50924 (9) 0.90999 (11) 0.30769 (8) 0.0141 (2)
O1 0.36589 (3) 0.97594 (4) 0.31383 (3) 0.01110 (9)
O2 0.21632 (3) 1.07434 (4) 0.36227 (3) 0.01158 (9)
O3 0.09643 (4) 1.00827 (4) 0.27079 (3) 0.01399 (9)
O4 0.38947 (4) 1.16989 (4) 0.37533 (3) 0.01216 (9)
O5 0.34797 (4) 1.01520 (4) 0.46522 (3) 0.01186 (9)
O6 0.42797 (4) 1.07518 (5) 0.58279 (3) 0.01560 (10)
B1 0.33286 (5) 1.05967 (6) 0.37751 (4) 0.01016 (11)
C1 0.28304 (4) 0.95743 (5) 0.25349 (4) 0.00955 (10)
C2 0.18775 (5) 1.01423 (5) 0.29565 (4) 0.01021 (10)
C3 0.30791 (5) 1.02291 (6) 0.17184 (4) 0.01333 (11)
H3A 0.3167 (9) 1.1064 (10) 0.1823 (7) 0.024 (3)*
H3B 0.2509 (10) 1.0133 (10) 0.1323 (7) 0.023 (3)*
H3C 0.3744 (9) 0.9899 (9) 0.1465 (7) 0.020 (2)*
C4 0.26552 (5) 0.82752 (5) 0.23795 (4) 0.01314 (11)
H4A 0.3291 (9) 0.7933 (10) 0.2120 (7) 0.025 (3)*
H4B 0.2057 (9) 0.8176 (9) 0.1987 (7) 0.020 (2)*
H4C 0.2505 (8) 0.7861 (9) 0.2889 (7) 0.019 (2)*
C5 0.42313 (5) 1.20239 (5) 0.45830 (4) 0.01192 (11)
C6 0.40175 (5) 1.09179 (5) 0.50964 (4) 0.01110 (11)
C7 0.35561 (7) 1.30226 (7) 0.49223 (5) 0.02424 (16)
H7A 0.3687 (10) 1.3751 (11) 0.4564 (8) 0.033 (3)*
H7B 0.3770 (11) 1.3184 (12) 0.5514 (9) 0.041 (3)*
H7C 0.2815 (11) 1.2823 (12) 0.4919 (8) 0.036 (3)*
C8 0.53960 (6) 1.23386 (7) 0.45795 (5) 0.01929 (13)
H8A 0.5830 (10) 1.1701 (11) 0.4330 (8) 0.032 (3)*
H8B 0.5636 (9) 1.2482 (10) 0.5166 (8) 0.030 (3)*
H8C 0.5506 (9) 1.3071 (10) 0.4247 (7) 0.026 (3)*
O1W 0.51220 (4) 0.74779 (4) 0.26871 (3) 0.01548 (10)
H1WA 0.5426 (12) 0.7243 (12) 0.2236 (10) 0.046 (4)*
H1WB 0.4774 (11) 0.6878 (12) 0.2863 (9) 0.041 (3)*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Li1 0.0132 (5) 0.0162 (5) 0.0128 (5) 0.0010 (4) −0.0010 (4) 0.0001 (4)
O1 0.00863 (17) 0.0148 (2) 0.00990 (19) 0.00106 (14) −0.00213 (14) −0.00282 (15)
O2 0.00987 (18) 0.01454 (19) 0.0103 (2) 0.00099 (14) −0.00098 (14) −0.00277 (15)
O3 0.00931 (18) 0.0180 (2) 0.0147 (2) 0.00129 (15) −0.00238 (16) −0.00252 (17)
O4 0.0154 (2) 0.01258 (19) 0.00853 (18) −0.00325 (15) −0.00187 (15) 0.00066 (15)
O5 0.01270 (19) 0.01361 (19) 0.00925 (19) −0.00208 (15) −0.00121 (15) 0.00105 (15)
O6 0.0148 (2) 0.0233 (2) 0.0087 (2) 0.00015 (17) −0.00136 (16) 0.00053 (17)
B1 0.0099 (2) 0.0121 (3) 0.0085 (3) −0.0002 (2) −0.0005 (2) −0.0001 (2)
C1 0.0085 (2) 0.0109 (2) 0.0092 (2) −0.00022 (17) −0.00104 (18) −0.00056 (19)
C2 0.0104 (2) 0.0109 (2) 0.0094 (2) 0.00061 (18) −0.00024 (18) 0.00053 (18)
C3 0.0150 (3) 0.0149 (3) 0.0101 (2) −0.0014 (2) 0.0006 (2) 0.0015 (2)
C4 0.0122 (2) 0.0107 (2) 0.0166 (3) −0.00059 (18) −0.0002 (2) −0.0010 (2)
C5 0.0137 (2) 0.0123 (2) 0.0098 (2) −0.00051 (19) −0.00179 (19) −0.00122 (19)
C6 0.0093 (2) 0.0145 (2) 0.0095 (2) 0.00077 (18) 0.00041 (18) −0.0008 (2)
C7 0.0333 (4) 0.0180 (3) 0.0214 (3) 0.0094 (3) 0.0012 (3) −0.0049 (3)
C8 0.0167 (3) 0.0213 (3) 0.0198 (3) −0.0076 (2) −0.0040 (2) 0.0027 (3)
O1W 0.0147 (2) 0.0146 (2) 0.0172 (2) −0.00084 (16) 0.00323 (17) −0.00317 (17)

Geometric parameters (Å, º)

Li1—O1 1.9725 (13) C1—C2 1.5263 (8)
Li1—O1W 1.9487 (13) C3—H3A 0.972 (11)
Li1—O3i 2.0059 (13) C3—H3B 0.963 (12)
Li1—O6ii 1.9155 (13) C3—H3C 1.007 (11)
O1—C1 1.4366 (7) C4—H4A 0.987 (12)
O1—B1 1.4498 (8) C4—H4B 0.988 (11)
O2—C2 1.3086 (7) C4—H4C 0.953 (11)
O2—B1 1.5094 (8) C5—C8 1.5223 (9)
O3—C2 1.2268 (7) C5—C7 1.5228 (10)
O3—Li1iii 2.0059 (13) C5—C6 1.5238 (9)
O4—C5 1.4297 (8) C7—H7A 1.019 (13)
O4—B1 1.4476 (8) C7—H7B 0.993 (14)
O5—C6 1.3125 (8) C7—H7C 0.968 (13)
O5—B1 1.4901 (8) C8—H8A 0.994 (13)
O6—C6 1.2193 (8) C8—H8B 0.990 (12)
O6—Li1ii 1.9155 (13) C8—H8C 0.997 (12)
C1—C4 1.5169 (8) O1W—H1WA 0.854 (16)
C1—C3 1.5251 (9) O1W—H1WB 0.861 (14)
O6ii—Li1—O1W 111.23 (6) H3A—C3—H3C 109.7 (9)
O6ii—Li1—O1 107.84 (6) H3B—C3—H3C 109.3 (10)
O1W—Li1—O1 113.25 (6) C1—C4—H4A 109.4 (7)
O6ii—Li1—O3i 106.33 (6) C1—C4—H4B 109.1 (6)
O1W—Li1—O3i 108.83 (6) H4A—C4—H4B 108.8 (9)
O1—Li1—O3i 109.12 (6) C1—C4—H4C 112.0 (6)
C1—O1—B1 110.28 (5) H4A—C4—H4C 108.7 (9)
C1—O1—Li1 125.99 (5) H4B—C4—H4C 108.7 (9)
B1—O1—Li1 123.51 (5) O4—C5—C8 110.39 (5)
C2—O2—B1 110.05 (5) O4—C5—C7 110.42 (6)
C2—O3—Li1iii 138.72 (6) C8—C5—C7 111.88 (6)
C5—O4—B1 110.58 (5) O4—C5—C6 102.84 (5)
C6—O5—B1 109.87 (5) C8—C5—C6 111.71 (5)
C6—O6—Li1ii 163.55 (6) C7—C5—C6 109.24 (6)
O4—B1—O1 114.25 (5) O6—C6—O5 123.19 (6)
O4—B1—O5 104.66 (5) O6—C6—C5 125.87 (6)
O1—B1—O5 112.74 (5) O5—C6—C5 110.92 (5)
O4—B1—O2 112.80 (5) C5—C7—H7A 108.7 (7)
O1—B1—O2 104.22 (5) C5—C7—H7B 108.4 (8)
O5—B1—O2 108.23 (5) H7A—C7—H7B 109.3 (11)
O1—C1—C4 111.01 (5) C5—C7—H7C 111.7 (8)
O1—C1—C3 109.85 (5) H7A—C7—H7C 110.3 (11)
C4—C1—C3 111.74 (5) H7B—C7—H7C 108.4 (11)
O1—C1—C2 103.20 (5) C5—C8—H8A 111.6 (7)
C4—C1—C2 111.60 (5) C5—C8—H8B 109.5 (7)
C3—C1—C2 109.10 (5) H8A—C8—H8B 108.8 (10)
O3—C2—O2 123.33 (6) C5—C8—H8C 109.6 (7)
O3—C2—C1 125.90 (6) H8A—C8—H8C 109.0 (10)
O2—C2—C1 110.74 (5) H8B—C8—H8C 108.3 (9)
C1—C3—H3A 111.0 (7) Li1—O1W—H1WA 124.8 (9)
C1—C3—H3B 109.8 (7) Li1—O1W—H1WB 129.9 (9)
H3A—C3—H3B 107.9 (9) H1WA—O1W—H1WB 104.7 (13)
C1—C3—H3C 109.2 (6)
O6ii—Li1—O1—C1 −163.76 (5) B1—O1—C1—C2 −12.51 (6)
O1W—Li1—O1—C1 −40.24 (9) Li1—O1—C1—C2 172.64 (6)
O3i—Li1—O1—C1 81.15 (8) Li1iii—O3—C2—O2 −164.56 (7)
O6ii—Li1—O1—B1 22.04 (9) Li1iii—O3—C2—C1 17.31 (12)
O1W—Li1—O1—B1 145.56 (6) B1—O2—C2—O3 177.79 (6)
O3i—Li1—O1—B1 −93.05 (7) B1—O2—C2—C1 −3.83 (7)
C5—O4—B1—O1 −132.62 (5) O1—C1—C2—O3 −171.56 (6)
C5—O4—B1—O5 −8.84 (6) C4—C1—C2—O3 −52.29 (8)
C5—O4—B1—O2 108.60 (6) C3—C1—C2—O3 71.68 (8)
C1—O1—B1—O4 −112.92 (6) O1—C1—C2—O2 10.11 (6)
Li1—O1—B1—O4 62.07 (8) C4—C1—C2—O2 129.38 (5)
C1—O1—B1—O5 127.75 (5) C3—C1—C2—O2 −106.65 (6)
Li1—O1—B1—O5 −57.25 (8) B1—O4—C5—C8 130.06 (6)
C1—O1—B1—O2 10.61 (6) B1—O4—C5—C7 −105.70 (6)
Li1—O1—B1—O2 −174.39 (5) B1—O4—C5—C6 10.76 (6)
C6—O5—B1—O4 2.75 (6) Li1ii—O6—C6—O5 172.88 (18)
C6—O5—B1—O1 127.49 (5) Li1ii—O6—C6—C5 −8.8 (2)
C6—O5—B1—O2 −117.77 (5) B1—O5—C6—O6 −177.52 (6)
C2—O2—B1—O4 120.53 (5) B1—O5—C6—C5 3.98 (7)
C2—O2—B1—O1 −3.95 (6) O4—C5—C6—O6 172.41 (6)
C2—O2—B1—O5 −124.16 (5) C8—C5—C6—O6 54.03 (8)
B1—O1—C1—C4 −132.19 (5) C7—C5—C6—O6 −70.29 (8)
Li1—O1—C1—C4 52.96 (8) O4—C5—C6—O5 −9.14 (6)
B1—O1—C1—C3 103.72 (6) C8—C5—C6—O5 −127.51 (6)
Li1—O1—C1—C3 −71.13 (7) C7—C5—C6—O5 108.16 (6)

Symmetry codes: (i) x+1/2, y, −z+1/2; (ii) −x+1, −y+2, −z+1; (iii) x−1/2, y, −z+1/2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: VN2036).

References

  1. Allen, J. L., Han, S.-D., Boyle, P. D. & Henderson, W. A. (2011). J. Power Sources, 196, 9737–9742.
  2. Altomare, A., Cascarano, G., Giacovazzo, C., Guagliardi, A., Burla, M. C., Polidori, G. & Camalli, M. (1994). J. Appl. Cryst. 27, 435.
  3. Boyle, P.D. (2008). http://www.xray.ncsu.edu/PyCIFUtils/
  4. Bruker (2007). SADABS, APEX2 and SAINT Bruker AXS Inc., Madison, Wisconsin, USA.
  5. Farrugia, L. J. (1997). J. Appl. Cryst. 30, 565.
  6. Lamande, L., Boyer, D. & Munoz, A. (1987). J. Organomet. Chem. 329, 1–29.
  7. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  8. Xu, W., Wang, L.-M., Nieman, R. A. & Angell, C. A. (2003). J. Phys. Chem. B, 107, 11749–11749.
  9. Zavalij, P. Y., Yang, S. & Whittingham, M. S. (2004). Acta Cryst. B60, 716–724. [DOI] [PubMed]

Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812017540/vn2036sup1.cif

e-68-0m749-sup1.cif (18.7KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812017540/vn2036Isup2.hkl

e-68-0m749-Isup2.hkl (277.4KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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