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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Jul 9;67(Pt 8):o1991. doi: 10.1107/S1600536811026080

Tetra­ethyl­ammonium bicarbonate trihydrate

Heping Li a, Yimin Hou a, Yunxia Yang b,*
PMCID: PMC3213447  PMID: 22091026

Abstract

In the title compound, C8H20N+·CHO3 ·3H2O, the bicarbon­ate anion, which has a small mean deviation from the plane of 0.0014 Å, fully utilises its three O and one H atom to form various O—H⋯O hydrogen bonds with the three water mol­ecules in the asymmetric unit, generating a hydrogen-bonded layer, which extends along (10Inline graphic). The tetra­ethyl­ammonium cations, as the guest species, are accommodated between every two neighboring layers, constructing a sandwich-like structure with an inter­layer distance of 7.28 Å.

Related literature

For the crystal structure of tetra­ethyl­ammonium bicarbonate monohydrate clathrate, see: Li et al. (2003). For O—H⋯O hydrogen bonds, see: Steiner (2002). For polymorphism see Kumar et al. (2002). graphic file with name e-67-o1991-scheme1.jpg

Experimental

Crystal data

  • C8H20N+·CHO3 ·3H2O

  • M r = 245.32

  • Monoclinic, Inline graphic

  • a = 7.6633 (1) Å

  • b = 12.9627 (3) Å

  • c = 14.2683 (3) Å

  • β = 99.932 (1)°

  • V = 1396.13 (5) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.10 mm−1

  • T = 296 K

  • 0.61 × 0.29 × 0.18 mm

Data collection

  • Bruker SMART APEX diffractometer

  • Absorption correction: multi-scan (SADABS; Sheldrick, 1996) T min = 0.854, T max = 1.000

  • 8465 measured reflections

  • 3480 independent reflections

  • 2466 reflections with I > 2σ(I)

  • R int = 0.018

Refinement

  • R[F 2 > 2σ(F 2)] = 0.045

  • wR(F 2) = 0.138

  • S = 1.02

  • 3480 reflections

  • 166 parameters

  • 10 restraints

  • H atoms treated by a mixture of independent and constrained refinement

  • Δρmax = 0.16 e Å−3

  • Δρmin = −0.17 e Å−3

Data collection: APEX2 (Bruker, 2009); cell refinement: SAINT (Bruker, 2009); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXL97 and publCIF (Westrip, 2010).

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536811026080/nr2008sup1.cif

e-67-o1991-sup1.cif (16.7KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811026080/nr2008Isup2.hkl

e-67-o1991-Isup2.hkl (170.7KB, hkl)

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

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
O1W—H1WA⋯O2i 0.83 (1) 2.00 (1) 2.8239 (16) 177 (2)
O1W—H1WB⋯O3Wii 0.82 (1) 2.05 (1) 2.8666 (19) 173 (2)
O2W—H2WA⋯O1 0.83 (1) 1.97 (1) 2.7980 (15) 172 (2)
O2W—H2WB⋯O1Wiii 0.82 (1) 2.01 (1) 2.8229 (16) 171 (2)
O3—H3⋯O1iv 0.83 (1) 1.85 (1) 2.6676 (15) 172 (2)
O3W—H3WA⋯O2 0.83 (1) 2.06 (1) 2.8422 (18) 157 (2)
O3W—H3WB⋯O2W 0.81 (1) 2.07 (2) 2.8099 (19) 152 (3)

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

Acknowledgments

We thank Northwest Normal University for supporting this study.

supplementary crystallographic information

Comment

Polymorphism is the existence of the same chemical substance in at least two different crystalline arrangements of molecules (Kumar et al. 2002). It is helpful to understand polymorphism to explore different crystal structures which are not qualified polymorphs but are also constructed with the same components. In 2003, the crystal structure of tetraethylammonium bicarbonate monohydrate clathrate (C8H20N+.CHO3-.H2O, 1) has been reported (Li et al. 2003). Here we reported the crystal structure of tetraethylammonium bicarbonate trihydrate clathrate (C8H20N+.CHO3-.3H2O, 2), in which the same components were used to obtain the crystal but the difference of the amount of water molecules in the asymmetric unit results in the final different packing model compared with compound 1. In addition, it should be noted that, in our experiment, 4,4'-oxybis(benzoic acid) was used to be the host molecule to obtain the acid-base inclusion compound, but after the data collection and determination, it was found that bicarbonate anion, which was finally determined according to the corresponding C—O bond lengths and O—C—O angles existed in the similar crystal structure of compound 1, take the place of the acid to interact with the related base to generate compound 2. In compound 1, one bicarbonate anion and one water molecule interacting with each other through O—H···O hydrogen bonds constitute a zigzag ribbon and are arranged in un-closed channels generated from tetraethylammonium cations. Comparatively, one bicarbonate anion and three water molecules in compound 2 form more O—H···O hydrogen bonds to construct the hydrogen-bonded layer and tetraethylammonium cations are contained between the layers to display the typical sandwich-like structure. Obviously, the amount of water molecules has significant effect on constructing different crystal structure between compound 1 and2. Noticeably, in compound 2, the strongest O—H···O hydrogen bond is between the centro-symmetric related bicarbonate anions (the distance of O···O is 2.6654 (16) Å) and other weaker O—H···O contacts involve the participation of water molecules (the corresponding values are from 2.7991 (16) Å to 2.868 (2) Å), which can be compared with the related O···O intervals of compound 1 (O···O distances are 2.619 Å and 2.868 Å) and the corresponding values (2.68 Å ~ 3.11 Å) of the reference (Steiner, 2002).

Experimental

4,4'-Oxybis(benzoic acid) (0.25 mmol, 0.065 g) was dissolved in a water-ethanol (50 ml/100 ml v/v) mixture. Tetraethylammonium hydroxide (25% aqueous solution) was added to neutralize the acid. The mixture was stirred for about 2 h and set aside to crystallize. Unexpectedly, the crystals involved 4,4'-oxybis(benzoic acid) were not obtained. Instead, colorless block crystals of the title compound were separated after several weeks.

Refinement

Carbon-bound H-atoms were placed in calculated positions (C—H: 0.96 Å for CH3 group and 0.97 Å for CH2 group) and were included in the refinement in the riding model approximation, with U(H) set to 1.2Ueq(C) for CH2 group and 1.5Ueq(C) for CH3 group. The anion and water H-atoms were located in a difference Fourier map, and were refined with a distance restraint of O—H 0.82±0.01 Å and with U(H) set to 1.5Ueq(O). Meanwhile, for water molecules, H—H distances were also restrained within 1.41±0.02 Å to meet the needs of H—O—H angles.

Figures

Fig. 1.

Fig. 1.

Thermal ellipsoid plot of the title compound at the 30% probability level; hydrogen atoms are drawn as spheres of arbitrary radius.

Fig. 2.

Fig. 2.

Packing diagram of the title compound; all hydrogen atoms bonded to carbon are omitted for clarity and the cations are represented with the open bonds.

Fig. 3.

Fig. 3.

Hydrogen-bonded linking pattern of the host layer in the crystal structure of the title compound.

Crystal data

C8H20N+·CHO3·3H2O F(000) = 544
Mr = 245.32 Dx = 1.167 Mg m3
Monoclinic, P21/n Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2yn Cell parameters from 2627 reflections
a = 7.6633 (1) Å θ = 3.1–26.7°
b = 12.9627 (3) Å µ = 0.10 mm1
c = 14.2683 (3) Å T = 296 K
β = 99.932 (1)° Block, colourless
V = 1396.13 (5) Å3 0.61 × 0.29 × 0.18 mm
Z = 4

Data collection

Bruker SMART APEX diffractometer 3480 independent reflections
Radiation source: fine-focus sealed tube 2466 reflections with I > 2σ(I)
graphite Rint = 0.018
phi and ω scans θmax = 28.5°, θmin = 2.1°
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) h = −10→8
Tmin = 0.854, Tmax = 1.000 k = −17→15
8465 measured reflections l = −12→19

Refinement

Refinement on F2 Primary atom site location: structure-invariant direct methods
Least-squares matrix: full Secondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.045 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.138 H atoms treated by a mixture of independent and constrained refinement
S = 1.02 w = 1/[σ2(Fo2) + (0.0697P)2 + 0.1916P] where P = (Fo2 + 2Fc2)/3
3480 reflections (Δ/σ)max = 0.001
166 parameters Δρmax = 0.16 e Å3
10 restraints Δρmin = −0.17 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 F^2^ against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F^2^, conventional R-factors R are based on F, with F set to zero for negative F^2^. The threshold expression of F^2^ > σ(F^2^) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F^2^ 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
N1 0.23247 (12) 0.27367 (8) 0.83104 (6) 0.0337 (2)
O1 0.02644 (15) 0.87654 (8) 0.97489 (8) 0.0608 (3)
O1W 0.24867 (16) 0.07251 (10) 0.33750 (8) 0.0642 (3)
H1WA 0.218 (3) 0.0994 (16) 0.2845 (10) 0.096*
H1WB 0.308 (3) 0.0199 (12) 0.3364 (16) 0.096*
C1 −0.08821 (18) 0.89307 (11) 0.90217 (9) 0.0453 (3)
O2 −0.14805 (14) 0.82902 (9) 0.84014 (8) 0.0594 (3)
O2W 0.21273 (15) 0.68993 (10) 0.99356 (9) 0.0641 (3)
H2WA 0.165 (3) 0.7475 (10) 0.9923 (15) 0.096*
H2WB 0.212 (3) 0.6570 (14) 1.0426 (11) 0.096*
C2 0.40040 (16) 0.21074 (11) 0.86043 (9) 0.0443 (3)
H2A 0.4158 0.1663 0.8077 0.053*
H2B 0.5004 0.2577 0.8714 0.053*
O3 −0.15534 (16) 0.98874 (8) 0.88939 (8) 0.0632 (3)
H3 −0.109 (3) 1.0260 (15) 0.9338 (12) 0.095*
O3W −0.05481 (19) 0.61659 (11) 0.84914 (10) 0.0767 (4)
H3WA −0.110 (3) 0.6718 (13) 0.8393 (18) 0.115*
H3WB 0.017 (3) 0.6182 (19) 0.8983 (12) 0.115*
C3 0.4058 (3) 0.14500 (13) 0.94748 (12) 0.0654 (4)
H3A 0.5164 0.1086 0.9602 0.098*
H3B 0.3099 0.0964 0.9370 0.098*
H3C 0.3945 0.1880 1.0009 0.098*
C4 0.26289 (17) 0.33841 (11) 0.74702 (9) 0.0428 (3)
H4A 0.3656 0.3819 0.7671 0.051*
H4B 0.2907 0.2926 0.6979 0.051*
C5 0.1098 (2) 0.40604 (13) 0.70431 (11) 0.0599 (4)
H5A 0.1407 0.4439 0.6517 0.090*
H5B 0.0832 0.4535 0.7516 0.090*
H5C 0.0079 0.3639 0.6825 0.090*
C6 0.19457 (17) 0.34029 (10) 0.91255 (9) 0.0418 (3)
H6A 0.0877 0.3797 0.8907 0.050*
H6B 0.1710 0.2954 0.9633 0.050*
C7 0.3400 (2) 0.41413 (12) 0.95290 (11) 0.0542 (4)
H7A 0.3047 0.4526 1.0040 0.081*
H7B 0.3621 0.4607 0.9040 0.081*
H7C 0.4460 0.3761 0.9765 0.081*
C8 0.07102 (17) 0.20495 (11) 0.80381 (10) 0.0460 (3)
H8A 0.0591 0.1620 0.8580 0.055*
H8B −0.0334 0.2484 0.7905 0.055*
C9 0.0748 (2) 0.13609 (13) 0.71913 (13) 0.0655 (4)
H9A −0.0319 0.0958 0.7070 0.098*
H9B 0.1754 0.0909 0.7321 0.098*
H9C 0.0834 0.1776 0.6644 0.098*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
N1 0.0328 (5) 0.0355 (5) 0.0333 (5) −0.0040 (4) 0.0068 (4) −0.0037 (4)
O1 0.0708 (7) 0.0493 (6) 0.0566 (6) 0.0134 (5) −0.0049 (5) 0.0020 (5)
O1W 0.0656 (7) 0.0716 (8) 0.0541 (6) −0.0014 (6) 0.0067 (5) −0.0011 (6)
C1 0.0479 (7) 0.0450 (8) 0.0446 (7) 0.0014 (6) 0.0123 (6) 0.0060 (6)
O2 0.0651 (6) 0.0528 (6) 0.0577 (6) 0.0023 (5) 0.0035 (5) −0.0053 (5)
O2W 0.0592 (6) 0.0610 (7) 0.0716 (7) 0.0131 (5) 0.0106 (5) 0.0068 (6)
C2 0.0401 (6) 0.0455 (8) 0.0464 (7) 0.0048 (5) 0.0052 (5) −0.0046 (6)
O3 0.0769 (8) 0.0459 (6) 0.0593 (7) 0.0090 (5) −0.0094 (5) 0.0057 (5)
O3W 0.0932 (10) 0.0618 (8) 0.0705 (8) 0.0027 (7) 0.0013 (7) −0.0066 (6)
C3 0.0826 (11) 0.0567 (10) 0.0540 (9) 0.0176 (8) 0.0034 (8) 0.0062 (7)
C4 0.0467 (7) 0.0460 (7) 0.0373 (6) −0.0067 (6) 0.0116 (5) 0.0010 (5)
C5 0.0662 (9) 0.0568 (9) 0.0532 (8) −0.0010 (7) 0.0005 (7) 0.0136 (7)
C6 0.0430 (6) 0.0458 (7) 0.0383 (6) 0.0007 (5) 0.0117 (5) −0.0073 (5)
C7 0.0627 (8) 0.0503 (8) 0.0483 (8) −0.0063 (7) 0.0054 (6) −0.0153 (6)
C8 0.0411 (6) 0.0475 (8) 0.0488 (7) −0.0141 (6) 0.0060 (5) −0.0028 (6)
C9 0.0682 (10) 0.0556 (10) 0.0685 (10) −0.0155 (8) −0.0001 (8) −0.0204 (8)

Geometric parameters (Å, °)

N1—C4 1.5141 (15) C3—H3C 0.9600
N1—C6 1.5162 (15) C4—C5 1.507 (2)
N1—C8 1.5197 (15) C4—H4A 0.9700
N1—C2 1.5203 (16) C4—H4B 0.9700
O1—C1 1.2569 (17) C5—H5A 0.9600
O1W—H1WA 0.829 (9) C5—H5B 0.9600
O1W—H1WB 0.823 (9) C5—H5C 0.9600
C1—O2 1.2422 (17) C6—C7 1.5064 (19)
C1—O3 1.3429 (18) C6—H6A 0.9700
O2W—H2WA 0.830 (9) C6—H6B 0.9700
O2W—H2WB 0.820 (9) C7—H7A 0.9600
C2—C3 1.501 (2) C7—H7B 0.9600
C2—H2A 0.9700 C7—H7C 0.9600
C2—H2B 0.9700 C8—C9 1.506 (2)
O3—H3 0.827 (10) C8—H8A 0.9700
O3W—H3WA 0.831 (9) C8—H8B 0.9700
O3W—H3WB 0.812 (9) C9—H9A 0.9600
C3—H3A 0.9600 C9—H9B 0.9600
C3—H3B 0.9600 C9—H9C 0.9600
C4—N1—C6 111.57 (10) C4—C5—H5A 109.5
C4—N1—C8 110.62 (9) C4—C5—H5B 109.5
C6—N1—C8 105.95 (9) H5A—C5—H5B 109.5
C4—N1—C2 106.09 (9) C4—C5—H5C 109.5
C6—N1—C2 111.05 (9) H5A—C5—H5C 109.5
C8—N1—C2 111.66 (10) H5B—C5—H5C 109.5
H1WA—O1W—H1WB 113.7 (19) C7—C6—N1 115.34 (10)
O2—C1—O1 126.42 (14) C7—C6—H6A 108.4
O2—C1—O3 115.77 (12) N1—C6—H6A 108.4
O1—C1—O3 117.81 (13) C7—C6—H6B 108.4
H2WA—O2W—H2WB 114.8 (19) N1—C6—H6B 108.4
C3—C2—N1 115.72 (12) H6A—C6—H6B 107.5
C3—C2—H2A 108.4 C6—C7—H7A 109.5
N1—C2—H2A 108.4 C6—C7—H7B 109.5
C3—C2—H2B 108.4 H7A—C7—H7B 109.5
N1—C2—H2B 108.4 C6—C7—H7C 109.5
H2A—C2—H2B 107.4 H7A—C7—H7C 109.5
C1—O3—H3 109.4 (16) H7B—C7—H7C 109.5
H3WA—O3W—H3WB 112 (2) C9—C8—N1 115.14 (11)
C2—C3—H3A 109.5 C9—C8—H8A 108.5
C2—C3—H3B 109.5 N1—C8—H8A 108.5
H3A—C3—H3B 109.5 C9—C8—H8B 108.5
C2—C3—H3C 109.5 N1—C8—H8B 108.5
H3A—C3—H3C 109.5 H8A—C8—H8B 107.5
H3B—C3—H3C 109.5 C8—C9—H9A 109.5
C5—C4—N1 115.30 (11) C8—C9—H9B 109.5
C5—C4—H4A 108.4 H9A—C9—H9B 109.5
N1—C4—H4A 108.4 C8—C9—H9C 109.5
C5—C4—H4B 108.4 H9A—C9—H9C 109.5
N1—C4—H4B 108.4 H9B—C9—H9C 109.5
H4A—C4—H4B 107.5

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
O1W—H1WA···O2i 0.83 (1) 2.00 (1) 2.8239 (16) 177 (2)
O1W—H1WB···O3Wii 0.82 (1) 2.05 (1) 2.8666 (19) 173 (2)
O2W—H2WA···O1 0.83 (1) 1.97 (1) 2.7980 (15) 172 (2)
O2W—H2WB···O1Wiii 0.82 (1) 2.01 (1) 2.8229 (16) 171 (2)
O3—H3···O1iv 0.83 (1) 1.85 (1) 2.6676 (15) 172 (2)
O3W—H3WA···O2 0.83 (1) 2.06 (1) 2.8422 (18) 157 (2)
O3W—H3WB···O2W 0.81 (1) 2.07 (2) 2.8099 (19) 152 (3)

Symmetry codes: (i) −x, −y+1, −z+1; (ii) x+1/2, −y+1/2, z−1/2; (iii) −x+1/2, y+1/2, −z+3/2; (iv) −x, −y+2, −z+2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: NR2008).

References

  1. Bruker (2009). APEX2 and SAINT Bruker AXS Inc., Madison, Wisconson, USA.
  2. Kumar, V. S. S., Addlagatta, A., Nangia, A., Robinson, W. T., Broder, C. K., Mondal, R., Evans, I. R., Howard, J. A. K. & Allen, F. H. (2002). Angew. Chem. Int. Ed. 41, 3848–3851. [DOI] [PubMed]
  3. Li, Q. & Hu, H. Y. (2003). Beijing Shifan Dax. Xue. Zir. Kex. (J. B. Norm. Univ.), 39, 645–649.
  4. Sheldrick, G. M. (1996). SADABS. University of Göttingen, Germany.
  5. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  6. Steiner, T. (2002). Angew. Chem. Int. Ed. 41, 48–76.
  7. Westrip, S. P. (2010). J. Appl. Cryst. 43, 920–925.

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/S1600536811026080/nr2008sup1.cif

e-67-o1991-sup1.cif (16.7KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811026080/nr2008Isup2.hkl

e-67-o1991-Isup2.hkl (170.7KB, hkl)

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


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