research communications
of a (carboxymethyl)triethylazanium bromide–2-(triethylazaniumyl)acetate (1/1) hydrogen-bonded dimer
aDepartment of Chemistry, Grand Valley State University, Allendale, MI 49401, USA, and bCenter for Crystallographic Research, Department of Chemistry, Michigan State University, East Lansing, MI 48824, USA
*Correspondence e-mail: biross@gvsu.edu
The title compound, C8H18NO2+·Br−·C8H17NO2, crystallizes as the bromide salt of a 50:50 mixture of (triethylazaniumyl)carboxylic acid and the zwitterionic (triethylazaniumyl)carboxylate. The two organic entities are linked by a half-occupied bridging carboxylic acid hydrogen atom that is hydrogen-bonded to the carboxylate group of the second molecule. The tetralkylammonium group adopts a nearly perfect tetrahedral shape around the nitrogen atom with bond lengths that agree with known values. The carboxylic acid/carboxylate group is oriented anti to one of the ethyl groups on the ammonium group, and the carbonyl oxygen atom is engaged in intramolecular C—H⋯O hydrogen bonds.
Keywords: crystal structure; asymmetric hydrogen bond; bromide salt; intermolecular O—H⋯O hydrogen bond; intramolecular C—H⋯O hydrogen bond.
CCDC reference: 2286618
1. Chemical context
The β-carbonylphosphonate moiety is commonly used as a reagent in the Horner–Wadsworth–Emmons reaction (Horner et al., 1958; Wadsworth & Emmons, 1961; Bisceglia & Orelli, 2015). These molecules are reacted with or to prepare α,β-unsaturated where a preference for the Z-configuration of the alkene group is often observed. When the phosphonate group is replaced with a phosphine oxide, these sets of compounds have found use as ligands and extraction agents for f-elements (Babecki et al., 1989, 1990, 1992). Our research group has also characterized the ability of these types of compounds to sensitize the luminescence of lanthanide ions (Leach et al., 2017; Sartain et al., 2015). To this end, our group has been working to develop a synthetic route to the target compound shown in Fig. 1, following the procedure reported by Ando (1999). The title compound was an undesired byproduct of this reaction, and serendipitously crystallized from the aqueous washings upon standing. A proposed mechanism for the formation of the title compound I is also shown in Fig. 1.
2. Structural commentary
The title salt crystallizes as a 50:50 mixture of the ammonium carboxylate zwitterion and the ammonium bromide. The molecular entities of this compound are shown in Fig. 2 along with the atom-numbering scheme. The is composed of all of the atoms shown in Fig. 2 where the carboxylic acid hydrogen atom H1 has a 0.50 occupancy, and the Br− anion is located on a twofold rotation axis (Wyckoff position 4e) of I2/a. The ammonium group has C—N bond lengths ranging from 1.514 (3) to 1.526 (3) Å with a nearly perfect tetrahedral arrangement of around the nitrogen atom with a τ4 descriptor for fourfold coordination of 0.97 (where 0.00 = square-planar, 0.85 = trigonal–pyramidal, and 1.00 = tetrahedral; Yang et al., 2007). The carboxylic acid group has C—O bond lengths of 1.286 (3) and 1.224 (3) Å. When the molecule is viewed down the C2—N1 bond the groups adopt a with the carboxylic acid group being anti to the C5–C6 ethyl group. The torsion angle between these two groups (C1—C2—N1—C5) is 168.8 (2)°. Two intramolecular C—H⋯O hydrogen bonds are present between the carbonyl oxygen atom O2 and hydrogen atoms H3A and H7B of the gauche (Table 1, Fig. 3).
3. Supramolecular features
Molecules of the title compound exist as hydrogen-bonded dimers in the solid state. The carboxylic acid hydrogen atom H1 is a half-occupied bridging hydrogen atom (Fábry, 2018), and within this dimer it is either bonded to oxygen atom O1 or to its symmetry derived counterpart O1i [symmetry code: (i) –x + , –y + , –z + ; Fig. 3]. When this atom H1 is covalently bonded to O1, it is engaged in a very strong asymmetric hydrogen bond with the symmetry-derived oxygen atom O1i (Table 1). The bromide counter-ions are located away from the carboxylate/carboxylic acid sites and occupy a layer that lies parallel to the ab plane. These layers are bordered by the ethyl chains of the ammonium groups (Fig. 4).
4. Database survey
A search of the Cambridge Structural Database (CSD version 5.43, Jun. 2022; Groom et al., 2016) for structures with a hydrogen atom shared between two carboxylate sites resulted in 274 hits. One of the simplest structures in this set is that of ammonium diacetate (ACAMAC; Nahringbauer, 1969). The structures ALUNIE (Dega-Szafran et al., 2003) and CIVKUQ (Ghazaryan et al., 2018) are similar to the title compound with either a piperidinium ring or a trimethylammonium group, respectively, in the place of the triethylammonium groups. Both compounds were isolated with a halide counter-ion: ALUNIE was isolated with one chloride anion and CIVKUQ was isolated as the iodide salt.
5. Synthesis and crystallization
Dibutyl phosphite (1.4 ml, 1.4 g, 7.17 mmol) was added via syringe to a two-necked 25 ml round-bottom flask under an atmosphere of nitrogen. The reagent was dissolved in 7.0 ml of dichloromethane and the flask was placed in an ice–water bath. Benzyl bromoacetate (1.1 ml, 1.6 g, 6.94 mmol) and triethylamine (1.4 ml, 1.0 g, 10.0 mmol) were added and the reaction mixture was stirred for 15 minutes in the ice bath followed by one hour at room temperature. Water (10 ml) was added to the reaction, and the aqueous layer was washed with ethyl acetate (3×10 ml). The organic extracts were combined and washed with 1 M HCl (3×10 ml) and brine (1×10 ml), then dried over MgSO4. The title compound crystallized serendipitously from the combined aqueous washings after standing for ca three days.
6. Refinement
Crystal data, data collection and structure . All hydrogen atoms bonded to carbon atoms were placed in calculated positions and refined as riding: C—H = 0.95 – 1.00 Å with Uiso(H) = 1.2Ueq(C) for methylene hydrogen atoms and Uiso(H) = 1.5Ueq(C) for the hydrogen atoms of the methyl groups. The carboxylic acid hydrogen atom H1 was located using electron-density difference maps. The position of this hydrogen atom was fixed and the occupancy constrained to 0.5. Its isotropic displacement parameter was refined as suggested by Fábry (2018).
details are summarized in Table 2Supporting information
CCDC reference: 2286618
https://doi.org/10.1107/S2056989023006850/wm5689sup1.cif
contains datablock I. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S2056989023006850/wm5689Isup2.hkl
Supporting information file. DOI: https://doi.org/10.1107/S2056989023006850/wm5689Isup3.cml
Data collection: CrysAlis PRO (Oxford Diffraction, 2006); cell
CrysAlis PRO (Oxford Diffraction, 2006); data reduction: CrysAlis PRO (Oxford Diffraction, 2006); program(s) used to solve structure: SHELXT (Sheldrick, 2015a); program(s) used to refine structure: SHELXL (Sheldrick, 2015b); molecular graphics: CrystalMaker (Palmer, 2007); software used to prepare material for publication: Olex2 (Dolomanov et al., 2009; Bourhis et al., 2015).C8H18NO2+·Br−·C8H17NO2 | F(000) = 848 |
Mr = 399.37 | Dx = 1.355 Mg m−3 |
Monoclinic, I2/a | Cu Kα radiation, λ = 1.54184 Å |
a = 12.6692 (4) Å | Cell parameters from 3269 reflections |
b = 7.0967 (3) Å | θ = 6.6–79.4° |
c = 22.3413 (9) Å | µ = 3.03 mm−1 |
β = 103.022 (4)° | T = 100 K |
V = 1957.04 (13) Å3 | Plate, colourless |
Z = 4 | 0.42 × 0.13 × 0.02 mm |
XtaLAB Synergy, Dualflex, HyPix diffractometer | 1785 reflections with I > 2σ(I) |
Detector resolution: 10.0000 pixels mm-1 | Rint = 0.052 |
ω scans | θmax = 80.0°, θmin = 4.1° |
Absorption correction: gaussian (CrysAlisPro; Oxford Diffraction, 2006) | h = −11→16 |
Tmin = 0.568, Tmax = 1.000 | k = −8→8 |
6198 measured reflections | l = −28→25 |
1998 independent reflections |
Refinement on F2 | 0 restraints |
Least-squares matrix: full | Hydrogen site location: mixed |
R[F2 > 2σ(F2)] = 0.040 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.109 | w = 1/[σ2(Fo2) + (0.0638P)2 + 1.4873P] where P = (Fo2 + 2Fc2)/3 |
S = 1.08 | (Δ/σ)max < 0.001 |
1998 reflections | Δρmax = 0.89 e Å−3 |
109 parameters | Δρmin = −0.42 e Å−3 |
Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes. |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
Br1 | 0.250000 | 0.39582 (5) | 0.500000 | 0.01824 (16) | |
O1 | 0.70415 (15) | 0.3474 (3) | 0.28191 (9) | 0.0250 (4) | |
H1 | 0.734798 | 0.280169 | 0.252098 | 0.07 (3)* | 0.5 |
O2 | 0.57904 (15) | 0.1209 (3) | 0.27312 (9) | 0.0235 (4) | |
N1 | 0.49061 (15) | 0.3014 (3) | 0.36825 (9) | 0.0146 (4) | |
C1 | 0.61984 (19) | 0.2698 (4) | 0.29428 (11) | 0.0181 (5) | |
C2 | 0.57456 (19) | 0.3923 (3) | 0.33887 (12) | 0.0155 (5) | |
H2A | 0.635817 | 0.434190 | 0.372016 | 0.019* | |
H2B | 0.542009 | 0.506334 | 0.316589 | 0.019* | |
C3 | 0.5279 (2) | 0.1112 (3) | 0.39641 (12) | 0.0187 (5) | |
H3A | 0.522278 | 0.017911 | 0.362887 | 0.022* | |
H3B | 0.477980 | 0.070888 | 0.422252 | 0.022* | |
C4 | 0.6431 (2) | 0.1076 (4) | 0.43539 (14) | 0.0242 (6) | |
H4A | 0.694224 | 0.132344 | 0.409276 | 0.036* | |
H4B | 0.658203 | −0.016535 | 0.454658 | 0.036* | |
H4C | 0.651144 | 0.204548 | 0.467320 | 0.036* | |
C5 | 0.47364 (19) | 0.4306 (4) | 0.41955 (11) | 0.0168 (5) | |
H5A | 0.419692 | 0.371758 | 0.439611 | 0.020* | |
H5B | 0.542724 | 0.439647 | 0.450705 | 0.020* | |
C6 | 0.4358 (2) | 0.6278 (4) | 0.39983 (14) | 0.0255 (6) | |
H6A | 0.369669 | 0.621107 | 0.367223 | 0.038* | |
H6B | 0.492434 | 0.693461 | 0.384459 | 0.038* | |
H6C | 0.420881 | 0.696650 | 0.435042 | 0.038* | |
C7 | 0.38591 (18) | 0.2757 (4) | 0.31950 (11) | 0.0170 (5) | |
H7A | 0.360683 | 0.400804 | 0.302461 | 0.020* | |
H7B | 0.401558 | 0.198822 | 0.285550 | 0.020* | |
C8 | 0.2954 (2) | 0.1824 (4) | 0.34289 (13) | 0.0242 (6) | |
H8A | 0.228952 | 0.182944 | 0.310402 | 0.036* | |
H8B | 0.283092 | 0.251692 | 0.378634 | 0.036* | |
H8C | 0.315681 | 0.052079 | 0.354755 | 0.036* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Br1 | 0.0155 (2) | 0.0211 (2) | 0.0191 (2) | 0.000 | 0.00614 (14) | 0.000 |
O1 | 0.0209 (9) | 0.0313 (10) | 0.0264 (10) | −0.0062 (8) | 0.0132 (8) | −0.0083 (8) |
O2 | 0.0214 (9) | 0.0270 (10) | 0.0242 (10) | −0.0037 (7) | 0.0091 (8) | −0.0089 (7) |
N1 | 0.0128 (8) | 0.0161 (10) | 0.0154 (10) | −0.0009 (7) | 0.0043 (8) | 0.0001 (8) |
C1 | 0.0161 (10) | 0.0229 (13) | 0.0149 (12) | 0.0010 (9) | 0.0029 (9) | −0.0013 (9) |
C2 | 0.0138 (10) | 0.0171 (12) | 0.0162 (12) | −0.0029 (8) | 0.0050 (9) | −0.0002 (9) |
C3 | 0.0212 (12) | 0.0158 (12) | 0.0186 (12) | 0.0001 (8) | 0.0035 (10) | 0.0024 (9) |
C4 | 0.0213 (12) | 0.0252 (14) | 0.0233 (14) | 0.0057 (10) | −0.0010 (10) | 0.0019 (10) |
C5 | 0.0151 (10) | 0.0214 (12) | 0.0140 (11) | 0.0015 (9) | 0.0033 (9) | −0.0002 (9) |
C6 | 0.0315 (14) | 0.0214 (14) | 0.0255 (15) | 0.0075 (10) | 0.0107 (12) | 0.0003 (10) |
C7 | 0.0136 (9) | 0.0218 (12) | 0.0145 (11) | −0.0025 (9) | 0.0008 (9) | −0.0003 (9) |
C8 | 0.0159 (11) | 0.0331 (15) | 0.0231 (13) | −0.0068 (10) | 0.0032 (10) | −0.0005 (11) |
O1—H1 | 0.9686 | C4—H4B | 0.9800 |
O1—C1 | 1.286 (3) | C4—H4C | 0.9800 |
O2—C1 | 1.224 (3) | C5—H5A | 0.9900 |
N1—C2 | 1.514 (3) | C5—H5B | 0.9900 |
N1—C3 | 1.519 (3) | C5—C6 | 1.512 (4) |
N1—C5 | 1.520 (3) | C6—H6A | 0.9800 |
N1—C7 | 1.526 (3) | C6—H6B | 0.9800 |
C1—C2 | 1.528 (3) | C6—H6C | 0.9800 |
C2—H2A | 0.9900 | C7—H7A | 0.9900 |
C2—H2B | 0.9900 | C7—H7B | 0.9900 |
C3—H3A | 0.9900 | C7—C8 | 1.515 (3) |
C3—H3B | 0.9900 | C8—H8A | 0.9800 |
C3—C4 | 1.522 (4) | C8—H8B | 0.9800 |
C4—H4A | 0.9800 | C8—H8C | 0.9800 |
C1—O1—H1 | 114.7 | H4A—C4—H4C | 109.5 |
C2—N1—C3 | 112.00 (18) | H4B—C4—H4C | 109.5 |
C2—N1—C5 | 107.61 (18) | N1—C5—H5A | 108.4 |
C2—N1—C7 | 108.91 (18) | N1—C5—H5B | 108.4 |
C3—N1—C5 | 107.89 (19) | H5A—C5—H5B | 107.5 |
C3—N1—C7 | 109.20 (19) | C6—C5—N1 | 115.3 (2) |
C5—N1—C7 | 111.24 (17) | C6—C5—H5A | 108.4 |
O1—C1—C2 | 110.4 (2) | C6—C5—H5B | 108.4 |
O2—C1—O1 | 125.8 (2) | C5—C6—H6A | 109.5 |
O2—C1—C2 | 123.7 (2) | C5—C6—H6B | 109.5 |
N1—C2—C1 | 116.35 (19) | C5—C6—H6C | 109.5 |
N1—C2—H2A | 108.2 | H6A—C6—H6B | 109.5 |
N1—C2—H2B | 108.2 | H6A—C6—H6C | 109.5 |
C1—C2—H2A | 108.2 | H6B—C6—H6C | 109.5 |
C1—C2—H2B | 108.2 | N1—C7—H7A | 108.7 |
H2A—C2—H2B | 107.4 | N1—C7—H7B | 108.7 |
N1—C3—H3A | 108.5 | H7A—C7—H7B | 107.6 |
N1—C3—H3B | 108.5 | C8—C7—N1 | 114.2 (2) |
N1—C3—C4 | 114.9 (2) | C8—C7—H7A | 108.7 |
H3A—C3—H3B | 107.5 | C8—C7—H7B | 108.7 |
C4—C3—H3A | 108.5 | C7—C8—H8A | 109.5 |
C4—C3—H3B | 108.5 | C7—C8—H8B | 109.5 |
C3—C4—H4A | 109.5 | C7—C8—H8C | 109.5 |
C3—C4—H4B | 109.5 | H8A—C8—H8B | 109.5 |
C3—C4—H4C | 109.5 | H8A—C8—H8C | 109.5 |
H4A—C4—H4B | 109.5 | H8B—C8—H8C | 109.5 |
O1—C1—C2—N1 | −167.3 (2) | C3—N1—C7—C8 | 56.4 (3) |
O2—C1—C2—N1 | 13.8 (4) | C5—N1—C2—C1 | 168.8 (2) |
C2—N1—C3—C4 | 46.5 (3) | C5—N1—C3—C4 | −71.8 (3) |
C2—N1—C5—C6 | 59.1 (3) | C5—N1—C7—C8 | −62.6 (3) |
C2—N1—C7—C8 | 179.0 (2) | C7—N1—C2—C1 | −70.5 (3) |
C3—N1—C2—C1 | 50.4 (3) | C7—N1—C3—C4 | 167.2 (2) |
C3—N1—C5—C6 | −179.9 (2) | C7—N1—C5—C6 | −60.1 (3) |
D—H···A | D—H | H···A | D···A | D—H···A |
O1—H1···O1i | 0.97 | 1.50 | 2.457 (4) | 167 |
C3—H3A···O2 | 0.99 | 2.39 | 2.969 (3) | 116 |
C7—H7B···O2 | 0.99 | 2.39 | 3.068 (3) | 125 |
Symmetry code: (i) −x+3/2, −y+1/2, −z+1/2. |
Acknowledgements
We thank the GVSU Chemistry Department Weldon Fund and the Library Open Access fund for financial support, and Professor Randy Winchester (GVSU) for fruitful conversations regarding the chemistry described in this paper.
Funding information
Funding for this research was provided by: National Science Foundation, Directorate for Mathematical and Physical Sciences (grant No. CHE-1725699 to SB; grant No. CHE-2102576 to SB; grant No. CHE-1919565 to RJS).
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