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Single-crystal X-ray diffraction and quantum mechanical theories were used to examine in detail the subtle nature of non-covalent interactions in the [2:1:1] multicomponent crystal of 1,1-amino­cyclo­pentane­carb­oxy­lic acid:oxalic acid:water. The crystal, which is a hydrate salt of the amino acid with the hydrogen-oxalate ion, also contains the zwitterion of the amino acid in equal proportions. It was found that a dimeric cation [Acc5(Z)...Acc5(C)]+ bonded by an O—H...O hydrogen bond exists due to a charge transfer between acid and carboxyl­ate groups. The three-dimensional crystal is built by blocks stacked along the [101] direction by dispersion interactions, with each block growing along two directions: a hydrogen oxalate HOX...HOX catameric supramolecular structure along the [010] direction; and double ...HOXW—[Acc5(Z)... Acc5(C)]+... chains related by inversion centers along the [1 0 {\bar 1}] direction. A PBE-DFT optimization, under periodic boundary conditions, was carried out. The fully optimized structure obtained was used to extract the coordinates to calculate the stabilization energy between the dimers under the crystal field, employing the M062X/aug-cc-pVTZ level of theory. The non-covalent index isosurfaces employed here allow the visualization of where the hydrogen bond and dispersion interactions contribute within the crystal. The crystal atomic arrangements are analyzed by employing the Atoms in Molecules and electron localization function theories. Within this context, the presence of density bond critical points is employed as a criterion for proving the existence of the hydrogen bond and it was found that these results agree with those rendered by the crystallographic geometrical analysis, with only three exceptions, for which bond critical points were not found.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2052520617011775/eb5064sup1.cif
Contains datablock I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520617011775/eb5064Isup2.hkl
Contains datablock I

pdf

Portable Document Format (PDF) file https://doi.org/10.1107/S2052520617011775/eb5064sup3.pdf
Table of DFT-PBE-PBC optimized atom coordinates and three further figures

CCDC reference: 1568826

Computing details top

Data collection: CrystalClear (Rigaku/MSC Inc., 2000); cell refinement: CrystalClear (Rigaku/MSC Inc., 2000); data reduction: CrystalStructure 3.6.0 (Rigaku/MSC Inc., 2004); program(s) used to solve structure: SHELXS2016/6 (Sheldrick, 2016); program(s) used to refine structure: SHELXL2016/6 (Sheldrick, 2016); molecular graphics: DIAMOND (Brandenburg & Putz, 2006); software used to prepare material for publication: SHELXL2016/6 (Sheldrick, 2016).

(I) top
Crystal data top
C14H26N2O9F(000) = 784
Mr = 366.37Dx = 1.393 Mg m3
Dm = 1.393 Mg m3
Dm measured by not measured
Monoclinic, P21/nMo Kα radiation, λ = 0.7107 Å
a = 17.283 (3) ÅCell parameters from 19530 reflections
b = 5.7371 (8) Åθ = 1.4–28.1°
c = 18.561 (3) ŵ = 0.12 mm1
β = 108.274 (4)°T = 291 K
V = 1747.5 (5) Å3Rectangular, colourless
Z = 40.30 × 0.20 × 0.15 mm
Data collection top
RIGAKU AFC7S Mercury
diffractometer
3558 independent reflections
Radiation source: normal-focus sealed tube2320 reflections with I > 2σ(I)
Detector resolution: 14.6306 pixels mm-1Rint = 0.062
ω scansθmax = 28.1°, θmin = 1.4°
Absorption correction: multi-scan
Jacobson, R. (1998)
h = 2020
Tmin = 0.937, Tmax = 0.948k = 75
19530 measured reflectionsl = 2222
Refinement top
Refinement on F288 restraints
Least-squares matrix: fullHydrogen site location: mixed
R[F2 > 2σ(F2)] = 0.062H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.164 w = 1/[σ2(Fo2) + (0.0662P)2 + 0.7567P]
where P = (Fo2 + 2Fc2)/3
S = 1.07(Δ/σ)max < 0.001
3558 reflectionsΔρmax = 0.29 e Å3
312 parametersΔρmin = 0.29 e Å3
Special details top

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
N10.71589 (14)0.4390 (4)0.35067 (15)0.0375 (5)
H110.706 (2)0.367 (6)0.302 (2)0.071 (10)*
H120.6919 (19)0.590 (6)0.3442 (17)0.062 (9)*
H130.6902 (18)0.374 (5)0.3777 (17)0.048 (9)*
O20.79780 (12)0.7041 (3)0.28638 (11)0.0531 (5)
O10.91798 (13)0.6401 (4)0.37413 (13)0.0684 (7)
H10.950 (3)0.763 (8)0.346 (3)0.127 (15)*
C10.84098 (17)0.6130 (5)0.34402 (16)0.0413 (7)
C20.80528 (15)0.4531 (4)0.39079 (14)0.0349 (6)
C30.84390 (18)0.2095 (5)0.40022 (17)0.0509 (8)
H3A0.8030890.0908310.3974600.061*
H3B0.8684000.1799870.3607020.061*
C40.9083 (5)0.2074 (15)0.4776 (4)0.061 (2)0.678 (18)
H4A0.958 (2)0.289 (4)0.4774 (4)0.074*0.678 (18)
H4B0.9219 (8)0.049 (7)0.4970 (9)0.074*0.678 (18)
C50.8611 (6)0.3424 (19)0.5223 (6)0.073 (3)0.678 (18)
H5A0.820 (2)0.242 (5)0.5328 (7)0.088*0.678 (18)
H5B0.8982 (16)0.399 (3)0.571 (2)0.088*0.678 (18)
C4B0.8718 (18)0.180 (3)0.4868 (7)0.079 (6)0.322 (18)
H4B10.830 (5)0.100 (9)0.5015 (16)0.095*0.322 (18)
H4B20.920 (5)0.086 (10)0.5022 (17)0.095*0.322 (18)
C5B0.8889 (14)0.413 (3)0.5265 (13)0.074 (6)0.322 (18)
H5B10.8834 (13)0.407 (3)0.584 (5)0.089*0.322 (18)
H5B20.949 (5)0.482 (7)0.5290 (13)0.089*0.322 (18)
C60.82099 (19)0.5444 (5)0.47241 (15)0.0491 (7)
H6A0.8566540.6791650.4819950.059*
H6B0.7702780.5868590.4810040.059*
N21.01369 (17)1.0784 (5)0.14719 (14)0.0463 (6)
H210.966 (2)1.192 (6)0.1395 (19)0.074 (10)*
H220.996 (3)0.939 (8)0.127 (2)0.109 (15)*
H231.047 (2)1.130 (5)0.1202 (18)0.062 (9)*
O30.94629 (12)0.7709 (3)0.20984 (12)0.0509 (5)
O40.99939 (14)0.9130 (4)0.32631 (12)0.0673 (7)
C70.99324 (16)0.8976 (4)0.25728 (16)0.0398 (6)
C81.05297 (15)1.0480 (4)0.23084 (14)0.0373 (6)
C91.07420 (18)1.2831 (5)0.27099 (17)0.0482 (7)
H9A1.0651991.4074920.2338920.058*
H9B1.0398901.3110830.3026400.058*
C101.1632 (7)1.278 (3)0.3195 (11)0.080 (5)0.52 (2)
H10A1.1678 (8)1.311 (4)0.361 (3)0.096*0.52 (2)
H10B1.189 (2)1.365 (7)0.3039 (17)0.096*0.52 (2)
C111.1916 (8)1.028 (3)0.3147 (9)0.077 (4)0.48 (2)
H11A1.242 (4)1.028 (3)0.3110 (9)0.092*0.48 (2)
H11B1.1922 (8)0.949 (6)0.356 (3)0.092*0.48 (2)
C10B1.1578 (9)1.240 (4)0.3264 (12)0.087 (6)0.48 (2)
H10C1.1543 (9)1.135 (8)0.378 (3)0.104*0.48 (2)
H10D1.192 (2)1.413 (11)0.3469 (17)0.104*0.48 (2)
C11B1.1989 (4)1.1000 (17)0.2783 (9)0.058 (3)0.52 (2)
H11C1.2084 (7)1.195 (5)0.238 (2)0.070*0.52 (2)
H11D1.250 (3)1.031 (4)0.3093 (17)0.070*0.52 (2)
C121.13470 (17)0.9188 (5)0.24734 (19)0.0524 (8)
H12A1.1278970.7549470.2567290.063*
H12B1.1551280.9318910.2044290.063*
C130.60324 (16)0.0480 (4)0.54309 (15)0.0382 (6)
C140.62234 (16)0.1935 (4)0.51573 (16)0.0399 (6)
O50.63155 (14)0.2189 (3)0.51124 (12)0.0544 (6)
H550.621 (2)0.349 (6)0.5271 (19)0.067 (10)*
O60.56691 (13)0.0716 (3)0.58792 (11)0.0520 (5)
O70.60949 (14)0.3630 (3)0.55320 (12)0.0596 (6)
O80.64709 (14)0.2030 (3)0.46069 (12)0.0559 (6)
O1W0.37498 (14)0.1441 (4)0.65001 (14)0.0499 (5)
H2W0.397 (3)0.035 (8)0.682 (2)0.106 (16)*
H1W0.363 (2)0.064 (7)0.607 (2)0.095 (14)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N10.0368 (14)0.0379 (14)0.0417 (14)0.0034 (10)0.0177 (11)0.0011 (11)
O20.0491 (13)0.0630 (13)0.0456 (12)0.0036 (10)0.0125 (10)0.0179 (10)
O10.0377 (13)0.0950 (17)0.0679 (15)0.0131 (11)0.0101 (11)0.0324 (13)
C10.0392 (17)0.0408 (15)0.0451 (17)0.0018 (12)0.0148 (14)0.0043 (12)
C20.0348 (15)0.0337 (13)0.0365 (14)0.0015 (10)0.0115 (11)0.0022 (10)
C30.0511 (18)0.0391 (16)0.063 (2)0.0043 (13)0.0193 (16)0.0035 (13)
C40.043 (4)0.052 (3)0.080 (4)0.006 (3)0.006 (3)0.014 (3)
C50.074 (6)0.092 (6)0.038 (4)0.005 (4)0.007 (4)0.005 (4)
C4B0.093 (14)0.060 (8)0.060 (9)0.026 (9)0.009 (9)0.008 (6)
C5B0.056 (10)0.083 (10)0.059 (8)0.020 (8)0.019 (8)0.023 (8)
C60.0579 (19)0.0511 (17)0.0379 (16)0.0066 (14)0.0146 (14)0.0036 (13)
N20.0533 (17)0.0464 (15)0.0446 (15)0.0053 (13)0.0231 (13)0.0013 (11)
O30.0444 (12)0.0472 (11)0.0598 (13)0.0130 (9)0.0145 (10)0.0049 (9)
O40.0663 (15)0.0935 (17)0.0427 (13)0.0334 (12)0.0178 (11)0.0037 (11)
C70.0345 (15)0.0387 (15)0.0459 (17)0.0005 (12)0.0120 (13)0.0070 (12)
C80.0368 (15)0.0358 (14)0.0413 (15)0.0019 (11)0.0153 (12)0.0007 (11)
C90.0548 (19)0.0361 (15)0.0562 (19)0.0041 (13)0.0210 (15)0.0032 (13)
C100.050 (7)0.069 (9)0.100 (10)0.003 (5)0.006 (6)0.018 (6)
C110.058 (5)0.084 (7)0.077 (7)0.012 (5)0.004 (5)0.004 (6)
C10B0.105 (12)0.050 (7)0.087 (9)0.016 (6)0.002 (8)0.039 (7)
C11B0.031 (4)0.055 (5)0.082 (7)0.007 (3)0.007 (4)0.002 (4)
C120.0382 (17)0.0465 (17)0.074 (2)0.0005 (12)0.0196 (16)0.0058 (14)
C130.0419 (16)0.0360 (14)0.0382 (15)0.0020 (12)0.0150 (13)0.0005 (11)
C140.0439 (16)0.0362 (15)0.0425 (16)0.0001 (12)0.0175 (13)0.0030 (12)
O50.0816 (16)0.0323 (11)0.0664 (14)0.0038 (10)0.0478 (12)0.0041 (10)
O60.0708 (15)0.0443 (11)0.0561 (13)0.0021 (9)0.0419 (12)0.0061 (9)
O70.0944 (17)0.0328 (11)0.0712 (15)0.0004 (10)0.0540 (13)0.0021 (9)
O80.0865 (16)0.0414 (11)0.0553 (13)0.0116 (10)0.0448 (12)0.0020 (9)
O1W0.0617 (14)0.0387 (11)0.0494 (13)0.0060 (10)0.0175 (11)0.0020 (10)
Geometric parameters (Å, º) top
N1—C21.492 (3)O3—C71.230 (3)
N1—H110.96 (4)O4—C71.255 (3)
N1—H120.95 (3)O4—H11.35 (5)
N1—H130.85 (3)C7—C81.539 (4)
O2—C11.214 (3)C8—C91.529 (4)
O1—C11.281 (3)C8—C121.538 (4)
O1—H11.11 (5)C9—C10B1.507 (13)
C1—C21.521 (4)C9—C101.520 (10)
C2—C31.535 (4)C9—H9A0.9700
C2—C61.544 (4)C9—H9B0.9700
C3—C41.517 (7)C10—C111.526 (15)
C3—C4B1.536 (13)C10—H10A0.78 (6)
C3—H3A0.9700C10—H10B0.78 (6)
C3—H3B0.9700C11—C121.466 (9)
C4—C51.542 (11)C11—H11A0.89 (6)
C4—H4A0.98 (4)C11—H11B0.89 (6)
C4—H4B0.98 (4)C10B—C11B1.533 (15)
C5—C61.509 (8)C10B—H10C1.15 (7)
C5—H5A0.98 (4)C10B—H10D1.15 (7)
C5—H5B0.98 (4)C11B—C121.498 (7)
C4B—C5B1.512 (16)C11B—H11C0.98 (5)
C4B—H4B10.96 (9)C11B—H11D0.98 (5)
C4B—H4B20.96 (9)C12—H12A0.9700
C5B—C61.489 (13)C12—H12B0.9700
C5B—H5B11.09 (9)C13—O61.197 (3)
C5B—H5B21.09 (9)C13—O51.316 (3)
C6—H6A0.9700C13—C141.546 (4)
C6—H6B0.9700C14—O81.226 (3)
N2—C81.497 (4)C14—O71.255 (3)
N2—H211.03 (4)O5—H550.84 (4)
N2—H220.90 (5)O1W—H2W0.86 (5)
N2—H230.92 (3)O1W—H1W0.89 (4)
C2—N1—H11110 (2)H21—N2—H23109 (3)
C2—N1—H12110.8 (19)H22—N2—H23104 (3)
H11—N1—H12109 (3)C7—O4—H1112 (2)
C2—N1—H13112 (2)O3—C7—O4126.7 (3)
H11—N1—H13113 (3)O3—C7—C8117.4 (2)
H12—N1—H13101 (3)O4—C7—C8115.8 (2)
C1—O1—H1118 (2)N2—C8—C9111.4 (2)
O2—C1—O1126.9 (3)N2—C8—C12110.6 (2)
O2—C1—C2121.0 (2)C9—C8—C12105.2 (2)
O1—C1—C2112.1 (2)N2—C8—C7105.3 (2)
N1—C2—C1106.8 (2)C9—C8—C7114.9 (2)
N1—C2—C3110.7 (2)C12—C8—C7109.4 (2)
C1—C2—C3112.0 (2)C10B—C9—C8102.8 (8)
N1—C2—C6110.1 (2)C10—C9—C8108.3 (6)
C1—C2—C6112.2 (2)C10—C9—H9A110.0
C3—C2—C6105.1 (2)C8—C9—H9A110.0
C4—C3—C2106.2 (4)C10—C9—H9B110.0
C2—C3—C4B101.7 (7)C8—C9—H9B110.0
C4—C3—H3A110.5H9A—C9—H9B108.4
C2—C3—H3A110.5C9—C10—C11105.6 (10)
C4—C3—H3B110.5C9—C10—H10A110.6
C2—C3—H3B110.5C11—C10—H10A110.6
H3A—C3—H3B108.7C9—C10—H10B110.6
C3—C4—C598.6 (6)C11—C10—H10B110.6
C3—C4—H4A112.0H10A—C10—H10B108.8
C5—C4—H4A112.0C12—C11—C10108.0 (8)
C3—C4—H4B112.0C12—C11—H11A110.1
C5—C4—H4B112.0C10—C11—H11A110.1
H4A—C4—H4B109.7C12—C11—H11B110.1
C6—C5—C4105.9 (7)C10—C11—H11B110.1
C6—C5—H5A110.6H11A—C11—H11B108.4
C4—C5—H5A110.6C9—C10B—C11B102.0 (10)
C6—C5—H5B110.6C9—C10B—H10C111.4
C4—C5—H5B110.6C11B—C10B—H10C111.4
H5A—C5—H5B108.7C9—C10B—H10D111.4
C5B—C4B—C3111.1 (15)C11B—C10B—H10D111.4
C5B—C4B—H4B1109.4H10C—C10B—H10D109.2
C3—C4B—H4B1109.4C12—C11B—C10B99.5 (9)
C5B—C4B—H4B2109.4C12—C11B—H11C111.9
C3—C4B—H4B2109.4C10B—C11B—H11C111.9
H4B1—C4B—H4B2108.0C12—C11B—H11D111.9
C6—C5B—C4B97.3 (12)C10B—C11B—H11D111.9
C6—C5B—H5B1112.3H11C—C11B—H11D109.6
C4B—C5B—H5B1112.3C11—C12—C8107.0 (5)
C6—C5B—H5B2112.3C11B—C12—C8105.4 (4)
C4B—C5B—H5B2112.3C11—C12—H12A110.3
H5B1—C5B—H5B2109.9C8—C12—H12A110.3
C5B—C6—C2110.4 (9)C11—C12—H12B110.3
C5—C6—C2104.3 (5)C8—C12—H12B110.3
C5—C6—H6A110.9H12A—C12—H12B108.6
C2—C6—H6A110.9O6—C13—O5125.3 (2)
C5—C6—H6B110.9O6—C13—C14122.8 (2)
C2—C6—H6B110.9O5—C13—C14111.9 (2)
H6A—C6—H6B108.9O8—C14—O7126.6 (2)
C8—N2—H21107.6 (19)O8—C14—C13118.7 (2)
C8—N2—H22109 (3)O7—C14—C13114.8 (2)
H21—N2—H22111 (3)C13—O5—H55111 (2)
C8—N2—H23116 (2)H2W—O1W—H1W100 (4)
 

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