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The experimental electron density distribution in glycyl-L-threonine dihydrate has been investigated using single-crystal X-ray diffraction data at 110 K to a resolution of (sin θ/λ) = 1.2 Å−1. Multipolar pseudo-atom refinement was carried out against 5417 observed data and the molecular electron density was analyzed using topological methods. The experimental electrostatic potential around the molecule is discussed in terms of molecular interactions. Crystal data: C6H12N2O4.2H2O, Mr = 212.2, orthorhombic, P212121, Z = 4, F(000) = 456 e, T = 110 K, a = 9.572 (3), b = 10.039 (3), c = 10.548 (2) Å, V = 1013.6 (4) Å3, Dx = 1.3 g cm−3, µ = 1.2 cm−1 for λMo = 0.7107 Å.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108768199014251/an0564sup1.cif
Contains datablocks global, 1

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768199014251/an0564sup2.hkl
Supplementary material

CCDC reference: 141672

Computing details top

Data collection: CAD-4 Software (Enraf-Nonius, 1989); cell refinement: CAD-4 Software (Enraf-Nonius, 1989); data reduction: DREAR (Blessing, 1987, 1989); program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); program(s) used to refine structure: MOLLY (Hansen & Coppens, 1978); molecular graphics: ORTEP (Johnson, 1970).

Glycyl-L-Threonine Dihydrate top
Crystal data top
C6H12N2O4·2(H2O)Dx = 1.390 Mg m3
Mr = 212.21Mo Kα radiation, λ = 0.71068 Å
Orthorhombic, P212121Cell parameters from 25 reflections
a = 9.572 (3) Åθ = 11–20°
b = 10.039 (3) ŵ = 0.12 mm1
c = 10.548 (3) ÅT = 110 K
V = 1013.7 (5) Å3Rectangular prism, colorless
Z = 40.30 × 0.30 × 0.15 mm
F(000) = 456
Data collection top
ENRAF-NONIUS CAD4
diffractometer
Rint = 0.023
Radiation source: fine-focus sealed tubeθmax = 54.9°, θmin = 2.8°
Graphite monochromatorh = 2222
ω/2θ scansk = 2323
15903 measured reflectionsl = 024
5417 independent reflections4 standard reflections every 120 min
3978 reflections with I > 3σ(I) intensity decay: 3%
Refinement top
Refinement on FSecondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.025Only H-atom displacement parameters refined
3978 reflections w = 1/[σ2(Fo2)]
405 parameters(Δ/σ)max = 0.05
0 restraintsΔρmax = 0.10 e Å3
Primary atom site location: structure-invariant direct methodsΔρmin = 0.10 e Å3
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
C1A0.11292 (5)0.38015 (5)0.53973 (5)0.0123 (2)
C10.17857 (5)0.24934 (5)0.49970 (4)0.0098 (2)
C2A0.13187 (5)0.04093 (5)0.38561 (4)0.0105 (2)
C2B0.11723 (6)0.04410 (6)0.24045 (5)0.0140 (2)
C2G0.21530 (7)0.14443 (7)0.18052 (6)0.0240 (3)
C20.04583 (5)0.07540 (5)0.43915 (5)0.0107 (2)
O10.30234 (4)0.22458 (4)0.52137 (4)0.0153 (2)
O2G0.02571 (4)0.07192 (4)0.21065 (4)0.0149 (2)
O210.05779 (4)0.04844 (4)0.50909 (3)0.0135 (2)
O220.08373 (4)0.18971 (4)0.40860 (4)0.0167 (2)
N10.20802 (5)0.45253 (4)0.62489 (4)0.0124 (2)
N20.09031 (4)0.16725 (4)0.43985 (4)0.0112 (2)
OW10.16550 (4)0.23049 (4)0.67630 (4)0.0166 (2)
OW20.04059 (6)0.39211 (5)0.76544 (5)0.0338 (4)
HN110.299230.483260.581260.017 (3)*
HN120.146520.517210.676510.019 (3)*
HN130.238800.391640.698610.017 (3)*
H2A0.239010.019020.411330.015 (2)*
H2G10.193340.242650.222700.033 (3)*
H2G20.324640.129090.201710.033 (3)*
H2G30.198530.139680.078950.033 (3)*
H1A10.097210.443920.457770.016 (2)*
H1A20.017960.346590.586290.017 (2)*
HN20.011830.199920.440810.015 (2)*
H2B0.143210.057300.212840.019 (3)*
H2G0.043330.154930.167310.016 (3)*
HW110.126770.188460.602350.023 (2)*
HW120.243000.276970.639450.028 (2)*
HW210.037660.341450.737150.041 (3)*
HW220.025160.430390.847320.033 (3)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C1A0.0102 (2)0.0104 (2)0.0163 (3)0.0014 (1)0.0026 (2)0.0020 (2)
C10.0079 (2)0.0099 (1)0.0116 (2)0.0002 (2)0.0004 (1)0.0009 (1)
C2A0.0088 (2)0.0103 (2)0.0123 (2)0.0006 (2)0.0000 (2)0.0012 (2)
C2B0.0153 (2)0.0151 (2)0.0116 (2)0.0029 (2)0.0019 (2)0.0007 (2)
C2G0.0178 (3)0.0326 (4)0.0216 (3)0.0010 (3)0.0066 (3)0.0082 (3)
C20.0093 (2)0.0097 (2)0.0131 (2)0.0004 (1)0.0012 (2)0.0008 (1)
O10.0088 (2)0.0149 (2)0.0223 (3)0.0016 (2)0.0025 (2)0.0055 (2)
O2G0.0157 (2)0.0144 (2)0.0147 (2)0.0011 (2)0.0030 (2)0.0019 (2)
O210.0115 (1)0.0136 (2)0.0155 (2)0.0002 (1)0.0024 (2)0.0008 (1)
O220.0145 (2)0.0095 (2)0.0260 (2)0.0004 (2)0.0009 (3)0.0040 (2)
N10.0112 (2)0.0119 (2)0.0143 (2)0.0001 (2)0.0011 (2)0.0028 (2)
N20.0083 (2)0.0099 (2)0.0153 (2)0.0001 (2)0.0010 (2)0.0027 (2)
OW10.0157 (2)0.0179 (2)0.0162 (2)0.0026 (2)0.0003 (2)0.0023 (2)
OW20.0422 (4)0.0389 (4)0.0202 (3)0.0268 (4)0.0134 (3)0.0091 (3)
Geometric parameters (Å, º) top
C1A—N11.4709 (6)C2A—C2B1.5381 (7)
C1A—C11.5159 (7)C2B—O2G1.4314 (6)
C1—O11.2319 (6)C2B—C2G1.5151 (8)
C1—N21.3385 (6)C2—O221.2459 (6)
C2A—N21.4470 (6)C2—O211.2655 (6)
C2A—C21.5366 (7)
N1—C1A—C1109.97 (4)O2G—C2B—C2G111.77 (4)
O1—C1—N2124.77 (4)O2G—C2B—C2A108.05 (4)
O1—C1—C1A121.46 (4)C2G—C2B—C2A111.89 (5)
N2—C1—C1A113.78 (4)O22—C2—O21125.17 (5)
N2—C2A—C2111.92 (4)O22—C2—C2A116.67 (4)
N2—C2A—C2B110.52 (4)O21—C2—C2A118.15 (4)
C2—C2A—C2B109.44 (4)C1—N2—C2A123.55 (4)
N1—C1A—C1—O111.01 (6)C2B—C2A—C2—O2264.61 (6)
N1—C1A—C1—N2169.30 (4)N2—C2A—C2—O218.15 (6)
N2—C2A—C2B—O2G59.23 (5)C2B—C2A—C2—O21114.72 (5)
C2—C2A—C2B—O2G64.45 (4)O1—C1—N2—C2A3.95 (9)
N2—C2A—C2B—C2G64.23 (5)C1A—C1—N2—C2A175.72 (5)
C2—C2A—C2B—C2G172.08 (4)C2—C2A—N2—C1123.48 (5)
N2—C2A—C2—O22172.52 (4)C2B—C2A—N2—C1114.26 (5)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—HN11···O21i1.0338 (7)1.7915 (4)2.8195 (6)172.20 (3)
N1—HN12···OW2ii1.0321 (6)1.6544 (5)2.6832 (6)174.39 (3)
N1—HN13···OW1iii1.0325 (7)1.9331 (4)2.8178 (6)141.85 (3)
N2—HN2···O1iv1.0312 (6)1.9742 (3)2.9907 (5)168.03 (2)
O2G—H2G···O22v0.9662 (8)1.7954 (4)2.7600 (5)177.17 (4)
OW1—HW11···O210.9591 (7)1.8384 (4)2.7413 (5)155.29 (3)
OW1—HW12···O22vi0.9613 (7)1.7662 (4)2.6843 (6)159.25 (2)
OW2—HW21···OW10.9537 (8)1.7749 (4)2.7219 (7)171.79 (4)
OW2—HW22···O21vii0.9568 (8)1.9489 (4)2.8544 (6)157.09 (3)
Symmetry codes: (i) x+1/2, y1/2, z+1; (ii) x, y1, z; (iii) x, y1/2, z+3/2; (iv) x1/2, y1/2, z+1; (v) x, y1/2, z+1/2; (vi) x1/2, y+1/2, z+1; (vii) x, y+1/2, z+3/2.
 

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