Buy article online - an online subscription or single-article purchase is required to access this article.
The crystal structure of β-glycine, C2H5NO2, has been refined. Single crystals of the metastable β-polymorph of glycine were obtained by cooling a saturated solution of glycine containing acetic acid. The crystal of the β-polymorph was preserved in dry air for several months. As the humidity of the air increased, a polymorphic transformation into the α-form was observed. The cell parameters of β-glycine have already been determined by Kozhin [Kristallografiya (1978), 23, 1211–1215], but the coordinates have not been published so far.
Supporting information
CCDC reference: 189379
Key indicators
- Single-crystal X-ray study
- T = 294 K
- Mean (C-C) = 0.001 Å
- R factor = 0.025
- wR factor = 0.076
- Data-to-parameter ratio = 13.3
checkCIF results
No syntax errors found
Alert Level B:
PLAT_111 Alert B ADDSYM detects (pseudo) centre of symmetry ... 80 Perc Fit
PLAT_113 Alert B ADDSYM suggests Pseudo/New Spacegroup ........ P21/m
| Author response: See response to previous problem
(see _publ_section_exptl_refinement).
|
General Notes
REFLT_03
From the CIF: _diffrn_reflns_theta_max 37.52
From the CIF: _reflns_number_total 894
Count of symmetry unique reflns 894
Completeness (_total/calc) 100.00%
TEST3: Check Friedels for noncentro structure
Estimate of Friedel pairs measured 0
Fraction of Friedel pairs measured 0.000
Are heavy atom types Z>Si present no
Please check that the estimate of the number of Friedel pairs is
correct. If it is not, please give the correct count in the
_publ_section_exptl_refinement section of the submitted CIF.
0 Alert Level A = Potentially serious problem
2 Alert Level B = Potential problem
0 Alert Level C = Please check
Data collection: STADI4 (Stoe & Cie, 1997); cell refinement: STADI4; data reduction: X-RED (Stoe & Cie, 1998); program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: X-STEP (Stoe & Cie, 1998) and Pcw (Kraus & Nolze, 1999); software used to prepare material for publication: SHELXL97.
Crystal data top
C2H5NO2 | F(000) = 80 |
Mr = 75.07 | Dx = 1.576 Mg m−3 |
Monoclinic, P21 | Mo Kα radiation, λ = 0.71069 Å |
a = 5.0935 (11) Å | Cell parameters from 26 reflections |
b = 6.274 (2) Å | θ = 15.1–24.7° |
c = 5.3847 (12) Å | µ = 0.14 mm−1 |
β = 113.19 (2)° | T = 294 K |
V = 158.18 (8) Å3 | Prism, colourless |
Z = 2 | 0.5 × 0.4 × 0.2 mm |
Data collection top
Stoe STADI4 four-circle diffractometer | 823 reflections with I > 2σ(I) |
Radiation source: fine-focus sealed tube | Rint = 0.039 |
Planar graphite monochromator | θmax = 37.5°, θmin = 3.3° |
Scan width (ω) = 1.42° – 1.87°, scan ratio 2θ:ω = 1.00
I(Net) and sigma(I) calculated according to Blessing (1987) | h = −8→8 |
Absorption correction: ψ scan (X-RED; Stoe, 1998) | k = −10→10 |
Tmin = 0.909, Tmax = 0.998 | l = −9→9 |
6548 measured reflections | 2 standard reflections every 180 min |
894 independent reflections | intensity decay: 4.3% |
Refinement top
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.025 | All H-atom parameters refined |
wR(F2) = 0.076 | w = 1/[σ2(Fo2) + (0.0501P)2 + 0.0031P] where P = (Fo2 + 2Fc2)/3 |
S = 1.12 | (Δ/σ)max < 0.001 |
894 reflections | Δρmax = 0.29 e Å−3 |
67 parameters | Δρmin = −0.18 e Å−3 |
1 restraint | Extinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.58 (7) |
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 | x | y | z | Uiso*/Ueq | |
O1 | −0.09265 (13) | 0.40990 (13) | 0.59741 (13) | 0.02586 (16) | |
N1 | 0.35024 (16) | 0.28161 (13) | 0.23730 (13) | 0.02090 (14) | |
H3 | 0.349 (4) | 0.301 (3) | 0.071 (3) | 0.029 (4)* | |
H4 | 0.520 (4) | 0.324 (3) | 0.353 (4) | 0.029 (4)* | |
H5 | 0.340 (4) | 0.142 (4) | 0.266 (3) | 0.034 (4)* | |
C1 | 0.13352 (15) | 0.38405 (13) | 0.56103 (15) | 0.01851 (13) | |
O2 | 0.37739 (15) | 0.35815 (17) | 0.74274 (12) | 0.0298 (2) | |
C2 | 0.11150 (17) | 0.39417 (16) | 0.26993 (14) | 0.02195 (15) | |
H1 | 0.123 (4) | 0.538 (4) | 0.222 (4) | 0.035 (5)* | |
H2 | −0.063 (4) | 0.332 (3) | 0.143 (4) | 0.029 (4)* | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
O1 | 0.0234 (3) | 0.0326 (4) | 0.0268 (3) | 0.0000 (2) | 0.0154 (2) | −0.0038 (2) |
N1 | 0.0218 (3) | 0.0272 (3) | 0.0151 (2) | 0.0026 (2) | 0.0087 (2) | 0.0000 (2) |
C1 | 0.0204 (3) | 0.0210 (3) | 0.0163 (2) | −0.0023 (3) | 0.0096 (2) | −0.0014 (2) |
O2 | 0.0208 (2) | 0.0532 (5) | 0.0156 (2) | −0.0029 (3) | 0.00725 (19) | 0.0007 (3) |
C2 | 0.0232 (3) | 0.0286 (4) | 0.0151 (3) | 0.0055 (3) | 0.0087 (2) | 0.0023 (3) |
Geometric parameters (Å, º) top
O1—C1 | 1.2528 (9) | C1—O2 | 1.2529 (11) |
N1—C2 | 1.4753 (11) | C1—C2 | 1.5281 (11) |
N1—H3 | 0.899 (16) | C2—H1 | 0.95 (3) |
N1—H4 | 0.88 (2) | C2—H2 | 0.964 (18) |
N1—H5 | 0.89 (3) | | |
| | | |
C2—N1—H3 | 111.6 (12) | O2—C1—C2 | 117.15 (7) |
C2—N1—H4 | 113.3 (12) | N1—C2—C1 | 111.79 (6) |
H3—N1—H4 | 106.5 (16) | N1—C2—H1 | 106.4 (10) |
C2—N1—H5 | 110.1 (11) | C1—C2—H1 | 109.3 (11) |
H3—N1—H5 | 109.1 (17) | N1—C2—H2 | 107.2 (11) |
H4—N1—H5 | 106.1 (17) | C1—C2—H2 | 112.6 (11) |
O1—C1—O2 | 125.78 (8) | H1—C2—H2 | 109.4 (16) |
O1—C1—C2 | 117.03 (7) | | |
| | | |
O1—C1—C2—N1 | −157.41 (8) | O2—C1—C2—N1 | 25.03 (12) |
Hydrogen-bond geometry (Å, º) top
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H4···O1i | 0.88 (2) | 1.97 (2) | 2.8509 (13) | 176.6 (17) |
N1—H3···O2ii | 0.899 (16) | 1.866 (16) | 2.7626 (11) | 174.4 (17) |
N1—H5···O2iii | 0.89 (3) | 2.30 (2) | 2.9795 (15) | 132.6 (14) |
N1—H5···O1iv | 0.89 (3) | 2.23 (2) | 2.9785 (13) | 140.7 (16) |
Symmetry codes: (i) x+1, y, z; (ii) x, y, z−1; (iii) −x+1, y−1/2, −z+1; (iv) −x, y−1/2, −z+1. |
Subscribe to Acta Crystallographica Section E: Crystallographic Communications
The full text of this article is available to subscribers to the journal.
If you have already registered and are using a computer listed in your registration details, please email
support@iucr.org for assistance.