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A form of DL-aspartic acid, C4H7NO4 is presented, which crystallizes in the same space group as the previously reported form but with a slightly different a axis. Its structure exhibits a three-dimensional supra­molecular network of N—H...O and O—H...O bonds, which stabilizes the crystal packing.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807043097/bg2096sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807043097/bg2096Isup2.hkl
Contains datablock I

CCDC reference: 663722

Key indicators

  • Single-crystal X-ray study
  • T = 293 K
  • Mean [sigma](C-C) = 0.002 Å
  • R factor = 0.038
  • wR factor = 0.103
  • Data-to-parameter ratio = 10.0

checkCIF/PLATON results

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Alert level B PLAT222_ALERT_3_B Large Non-Solvent H Ueq(max)/Ueq(min) ... 4.62 Ratio PLAT430_ALERT_2_B Short Inter D...A Contact O1 .. O1 .. 2.84 Ang.
Alert level C PLAT066_ALERT_1_C Predicted and Reported Transmissions Identical . ? PLAT088_ALERT_3_C Poor Data / Parameter Ratio .................... 9.95 PLAT250_ALERT_2_C Large U3/U1 Ratio for Average U(i,j) Tensor .... 2.19
Alert level G PLAT199_ALERT_1_G Check the Reported _cell_measurement_temperature 293 K PLAT200_ALERT_1_G Check the Reported _diffrn_ambient_temperature . 293 K PLAT793_ALERT_1_G Check the Absolute Configuration of C3 = ... S
0 ALERT level A = In general: serious problem 2 ALERT level B = Potentially serious problem 3 ALERT level C = Check and explain 3 ALERT level G = General alerts; check 4 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 2 ALERT type 2 Indicator that the structure model may be wrong or deficient 2 ALERT type 3 Indicator that the structure quality may be low 0 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check

Comment top

Interest in D,L-aspartic acid has spanned several decades, from the first structural determination by Rao (1973), due to its acting as important ligand in the preparation of transition metal complexes (Ciunik, 1987; Casellato et al., 1991; Barfod et al., 1999). In exploring the possibility of introducing D,L-aspartic acid into a phosphite system, we unexpectedly obtained the title compound. To the best of our knowledge, there are only four reports on the structure of D,L-aspartic acid (Rao et al., 1968; Rao, 1973; Sequeira et al., 1989; Flaig et al., 1998). The present structure of D,L-aspartic acid differs slightly from these previously reported ones, since it presents the same space group and a similar molecular disposition, but with an a parameter some 7–8% shorter.

The molecules (Fig. 1) are interconnected with each other by hydrogen bonds to form a 3-D supramolecular network (Table 1 and Fig. 2).

Related literature top

For related literature, see: Barfod et al. (1999); Casellato et al. (1991); Ciunik (1987); Flaig et al. (1998); Rao (1973); Rao et al. (1968); Sequeira et al. (1989).

Experimental top

The title compound was obtained by hydrothermal methods. A mixture of Zn(CH3COO)2·2H2O (0.16 g), H3PO3 (0.19 g), D,L-aspartic acid (0.25 g) and H2O (8 ml), was sealed in a 25 ml Teflon-lined steel autoclave and heated under autogenous pressure at 363 K for 3 days. Then, the filtrate was kept at room temperature and colorless prism-like crystals were obtained after three weeks.

Refinement top

All the H atoms were located from difference-density maps in a difference Fourier map and their positions and isotropic displacement parameters were refined.

Structure description top

Interest in D,L-aspartic acid has spanned several decades, from the first structural determination by Rao (1973), due to its acting as important ligand in the preparation of transition metal complexes (Ciunik, 1987; Casellato et al., 1991; Barfod et al., 1999). In exploring the possibility of introducing D,L-aspartic acid into a phosphite system, we unexpectedly obtained the title compound. To the best of our knowledge, there are only four reports on the structure of D,L-aspartic acid (Rao et al., 1968; Rao, 1973; Sequeira et al., 1989; Flaig et al., 1998). The present structure of D,L-aspartic acid differs slightly from these previously reported ones, since it presents the same space group and a similar molecular disposition, but with an a parameter some 7–8% shorter.

The molecules (Fig. 1) are interconnected with each other by hydrogen bonds to form a 3-D supramolecular network (Table 1 and Fig. 2).

For related literature, see: Barfod et al. (1999); Casellato et al. (1991); Ciunik (1987); Flaig et al. (1998); Rao (1973); Rao et al. (1968); Sequeira et al. (1989).

Computing details top

Data collection: SMART (Bruker, 1999); cell refinement: SAINT (Bruker, 1999); data reduction: SAINT (Bruker, 1999); program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Bruker, 1999); software used to prepare material for publication: SHELXTL (Bruker, 1999).

Figures top
[Figure 1] Fig. 1. The molecular structure of the title compound, showing 50% probability displacement ellipsoids.
[Figure 2] Fig. 2. Packing diagram of the title compound.
D,L-aspartic acid top
Crystal data top
C4H7NO4F(000) = 560
Mr = 133.11Dx = 1.645 Mg m3
Monoclinic, C2/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -C 2ycCell parameters from 4179 reflections
a = 17.5813 (2) Åθ = 2.6–26.5°
b = 7.4369 (5) ŵ = 0.15 mm1
c = 9.1807 (3) ÅT = 293 K
β = 116.436 (3)°Prism, colorless
V = 1074.86 (9) Å30.18 × 0.14 × 0.06 mm
Z = 8
Data collection top
Siemems SMART CCD
diffractometer
1105 independent reflections
Radiation source: fine-focus sealed tube986 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.032
φ and ω scansθmax = 26.5°, θmin = 2.6°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 2222
Tmin = 0.974, Tmax = 0.991k = 99
4179 measured reflectionsl = 1111
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)] = 0.039All H-atom parameters refined
wR(F2) = 0.103 w = 1/[σ2(Fo2) + (0.0514P)2 + 0.5964P]
where P = (Fo2 + 2Fc2)/3
S = 1.07(Δ/σ)max < 0.001
1105 reflectionsΔρmax = 0.23 e Å3
111 parametersΔρmin = 0.18 e Å3
0 restraintsExtinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.017 (2)
Crystal data top
C4H7NO4V = 1074.86 (9) Å3
Mr = 133.11Z = 8
Monoclinic, C2/cMo Kα radiation
a = 17.5813 (2) ŵ = 0.15 mm1
b = 7.4369 (5) ÅT = 293 K
c = 9.1807 (3) Å0.18 × 0.14 × 0.06 mm
β = 116.436 (3)°
Data collection top
Siemems SMART CCD
diffractometer
1105 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
986 reflections with I > 2σ(I)
Tmin = 0.974, Tmax = 0.991Rint = 0.032
4179 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0390 restraints
wR(F2) = 0.103All H-atom parameters refined
S = 1.07Δρmax = 0.23 e Å3
1105 reflectionsΔρmin = 0.18 e Å3
111 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
C10.00684 (9)0.2497 (2)0.49490 (19)0.0227 (4)
C20.09882 (9)0.2473 (2)0.52666 (19)0.0238 (4)
H20.1006 (12)0.204 (3)0.431 (3)0.035 (5)*
H30.1188 (13)0.374 (3)0.544 (3)0.042 (6)*
C30.15383 (9)0.1315 (2)0.67210 (19)0.0199 (4)
H40.1312 (10)0.014 (2)0.6575 (18)0.016 (4)*
C40.24516 (9)0.1148 (2)0.69224 (19)0.0205 (4)
O10.01739 (7)0.17330 (17)0.58347 (15)0.0342 (4)
O20.04289 (8)0.33822 (18)0.36471 (15)0.0348 (4)
H10.1002 (18)0.338 (4)0.349 (3)0.074 (8)*
O30.30295 (7)0.17660 (17)0.82024 (14)0.0319 (4)
O40.25457 (7)0.03708 (15)0.58062 (13)0.0270 (3)
N10.15498 (9)0.2014 (2)0.82518 (17)0.0232 (4)
H70.1800 (14)0.318 (3)0.855 (3)0.040 (6)*
H60.1879 (14)0.126 (3)0.911 (3)0.041 (6)*
H50.1023 (14)0.203 (3)0.818 (3)0.040 (5)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0161 (8)0.0309 (9)0.0199 (7)0.0015 (6)0.0069 (6)0.0019 (6)
C20.0165 (8)0.0321 (9)0.0227 (8)0.0018 (6)0.0085 (7)0.0036 (7)
C30.0153 (7)0.0219 (8)0.0218 (8)0.0023 (6)0.0075 (6)0.0020 (6)
C40.0158 (7)0.0196 (8)0.0253 (8)0.0012 (6)0.0084 (6)0.0024 (6)
O10.0183 (6)0.0553 (8)0.0298 (7)0.0011 (5)0.0116 (5)0.0096 (6)
O20.0165 (6)0.0565 (8)0.0287 (7)0.0073 (5)0.0077 (5)0.0144 (6)
O30.0150 (6)0.0461 (8)0.0311 (7)0.0033 (5)0.0071 (5)0.0111 (5)
O40.0217 (6)0.0301 (6)0.0302 (6)0.0014 (5)0.0125 (5)0.0050 (5)
N10.0155 (7)0.0322 (8)0.0219 (7)0.0006 (6)0.0083 (6)0.0003 (6)
Geometric parameters (Å, º) top
C1—O11.2140 (19)C3—H40.945 (17)
C1—O21.3023 (19)C4—O31.2494 (19)
C1—C21.510 (2)C4—O41.2501 (18)
C2—C31.520 (2)O2—H10.95 (3)
C2—H20.95 (2)N1—H70.95 (2)
C2—H30.99 (2)N1—H60.93 (2)
C3—N11.490 (2)N1—H50.90 (2)
C3—C41.537 (2)
O1—C1—O2123.98 (14)C2—C3—H4109.7 (10)
O1—C1—C2122.01 (14)C4—C3—H4107.0 (10)
O2—C1—C2114.01 (13)O3—C4—O4126.31 (14)
C1—C2—C3112.60 (13)O3—C4—C3116.86 (13)
C1—C2—H2107.4 (12)O4—C4—C3116.81 (13)
C3—C2—H2110.4 (12)C1—O2—H1112.0 (16)
C1—C2—H3107.0 (12)C3—N1—H7113.5 (13)
C3—C2—H3110.8 (12)C3—N1—H6109.4 (13)
H2—C2—H3108.5 (17)H7—N1—H6105.5 (18)
N1—C3—C2111.55 (13)C3—N1—H5110.9 (14)
N1—C3—C4109.87 (12)H7—N1—H5109.6 (18)
C2—C3—C4111.94 (13)H6—N1—H5107.6 (18)
N1—C3—H4106.5 (9)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O2—H1···O3i0.95 (3)1.61 (3)2.5574 (16)176 (3)
N1—H7···O4ii0.95 (2)1.93 (2)2.8782 (19)171.8 (18)
N1—H6···O4iii0.93 (2)1.91 (2)2.8381 (18)177.4 (19)
N1—H5···O1iv0.90 (2)2.07 (2)2.8992 (18)152.5 (19)
N1—H5···O10.90 (2)2.26 (2)2.8572 (18)124.0 (17)
Symmetry codes: (i) x1/2, y+1/2, z1/2; (ii) x+1/2, y+1/2, z+3/2; (iii) x, y, z+1/2; (iv) x, y, z+3/2.

Experimental details

Crystal data
Chemical formulaC4H7NO4
Mr133.11
Crystal system, space groupMonoclinic, C2/c
Temperature (K)293
a, b, c (Å)17.5813 (2), 7.4369 (5), 9.1807 (3)
β (°) 116.436 (3)
V3)1074.86 (9)
Z8
Radiation typeMo Kα
µ (mm1)0.15
Crystal size (mm)0.18 × 0.14 × 0.06
Data collection
DiffractometerSiemems SMART CCD
Absorption correctionMulti-scan
(SADABS; Sheldrick, 1996)
Tmin, Tmax0.974, 0.991
No. of measured, independent and
observed [I > 2σ(I)] reflections
4179, 1105, 986
Rint0.032
(sin θ/λ)max1)0.628
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.039, 0.103, 1.07
No. of reflections1105
No. of parameters111
H-atom treatmentAll H-atom parameters refined
Δρmax, Δρmin (e Å3)0.23, 0.18

Computer programs: SMART (Bruker, 1999), SAINT (Bruker, 1999), SHELXS97 (Sheldrick, 1990), SHELXL97 (Sheldrick, 1997), SHELXTL (Bruker, 1999).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O2—H1···O3i0.95 (3)1.61 (3)2.5574 (16)176 (3)
N1—H7···O4ii0.95 (2)1.93 (2)2.8782 (19)171.8 (18)
N1—H6···O4iii0.93 (2)1.91 (2)2.8381 (18)177.4 (19)
N1—H5···O1iv0.90 (2)2.07 (2)2.8992 (18)152.5 (19)
N1—H5···O10.90 (2)2.26 (2)2.8572 (18)124.0 (17)
Symmetry codes: (i) x1/2, y+1/2, z1/2; (ii) x+1/2, y+1/2, z+3/2; (iii) x, y, z+1/2; (iv) x, y, z+3/2.
 

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