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The occurrence of a first-order reversible phase transition in glycine-glutaric acid co-crystals at 220-230 K has been confirmed by three different techniques - single-crystal X-ray diffraction, polarized Raman spectroscopy and differential scanning calorimetry. The most interesting feature of this phase transition is that every second glutaric acid molecule changes its conformation, and this fact results in the space-group symmetry change from P21/c to P\bar 1. The topology of the hydrogen-bonded motifs remains almost the same and hydrogen bonds do not switch to other atoms, although the hydrogen bond lengths do change and some of the bonds become inequivalent.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108768112015972/gp5050sup1.cif
Contains datablocks 300, 275, 250, 225, 200, 175, 150, 125, 100

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768112015972/gp5050300sup2.hkl
Contains datablock 300

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768112015972/gp5050275sup3.hkl
Contains datablock 275

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768112015972/gp5050250sup4.hkl
Contains datablock 250

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768112015972/gp5050225sup5.hkl
Contains datablock 225

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768112015972/gp5050100sup6.hkl
Contains datablock 100

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768112015972/gp5050125sup7.hkl
Contains datablock 125

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768112015972/gp5050150sup8.hkl
Contains datablock 150

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768112015972/gp5050175sup9.hkl
Contains datablock 175

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768112015972/gp5050200sup10.hkl
Contains datablock 200

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Portable Document Format (PDF) file https://doi.org/10.1107/S0108768112015972/gp5050sup11.pdf
Procedure of indexing diffraction patterns from domains in glycine and photographs of co-crystal

CCDC references: 889409; 889410; 889411; 889412; 889413; 889414; 889415; 889416; 889417

Computing details top

For all compounds, data collection: STOE X-AREA (Stoe & Cie, 2006); cell refinement: STOE X-AREA (Stoe & Cie, 2006); data reduction: STOE X-RED (Stoe & Cie, 2006); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008) and X-STEP32 (Stoe & Cie, 2000); molecular graphics: Mercury (Macrae et al., 2006); software used to prepare material for publication: Mercury (Macrae et al., 2006), PLATON (Spek, 2009), enCIFer (Allen et al., 2004).

Figures top
[Figure 1]
[Figure 2]
[Figure 3]
[Figure 4]
[Figure 5]
[Figure 6]
[Figure 7]
[Figure 8]
(300) Propane-1,3-dicarboxylic acid – Aminoethanoic acid (1/1) top
Crystal data top
C5H8O4·C2H5NO2F(000) = 440
Mr = 207.18Dx = 1.434 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 3307 reflections
a = 4.9110 (7) Åθ = 2.0–29.2°
b = 20.922 (3) ŵ = 0.13 mm1
c = 10.2744 (15) ÅT = 300 K
β = 114.586 (10)°Prism, colourless
V = 959.9 (2) Å30.32 × 0.17 × 0.10 mm
Z = 4
Data collection top
STOE IPDS 2
diffractometer
1421 reflections with I > 2σ(I)
Plane graphite monochromatorRint = 0.046
Detector resolution: 6.67 pixels mm-1θmax = 29.2°, θmin = 2.0°
rotation method scansh = 56
6828 measured reflectionsk = 2824
2578 independent reflectionsl = 1414
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.048Hydrogen site location: difference Fourier map
wR(F2) = 0.096H-atom parameters constrained
S = 0.89 w = 1/[σ2(Fo2) + (0.0419P)2]
where P = (Fo2 + 2Fc2)/3
2578 reflections(Δ/σ)max < 0.001
130 parametersΔρmax = 0.19 e Å3
0 restraintsΔρmin = 0.17 e Å3
Crystal data top
C5H8O4·C2H5NO2V = 959.9 (2) Å3
Mr = 207.18Z = 4
Monoclinic, P21/cMo Kα radiation
a = 4.9110 (7) ŵ = 0.13 mm1
b = 20.922 (3) ÅT = 300 K
c = 10.2744 (15) Å0.32 × 0.17 × 0.10 mm
β = 114.586 (10)°
Data collection top
STOE IPDS 2
diffractometer
1421 reflections with I > 2σ(I)
6828 measured reflectionsRint = 0.046
2578 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0480 restraints
wR(F2) = 0.096H-atom parameters constrained
S = 0.89Δρmax = 0.19 e Å3
2578 reflectionsΔρmin = 0.17 e Å3
130 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
O10.1303 (3)0.44553 (6)0.33353 (12)0.0431 (3)
O50.6180 (3)0.64113 (6)0.22044 (13)0.0492 (4)
O30.2017 (3)0.91549 (6)0.03314 (12)0.0412 (3)
N10.5566 (4)0.52554 (7)0.33624 (14)0.0360 (4)
H1A0.65990.55650.31790.054*
H1B0.68190.50000.40390.054*
H1C0.42680.54260.36610.054*
C20.3932 (4)0.48823 (8)0.20491 (17)0.0334 (4)
H2A0.53570.46490.18020.040*
H2B0.28430.51720.12680.040*
O60.8167 (4)0.59463 (6)0.09106 (14)0.0501 (4)
H60.84180.60180.01840.075*
O20.0510 (3)0.40246 (7)0.12345 (14)0.0543 (4)
C10.1753 (4)0.44149 (8)0.22259 (17)0.0332 (4)
C70.6740 (4)0.64281 (8)0.11621 (17)0.0347 (4)
O40.1063 (4)0.84677 (6)0.10598 (16)0.0565 (4)
H40.03560.87880.12600.085*
C50.4645 (5)0.75376 (9)0.06721 (18)0.0423 (5)
H5A0.31950.73830.10120.051*
H5B0.62950.77250.14810.051*
C60.5810 (5)0.69752 (8)0.01277 (18)0.0379 (4)
H6B0.42610.68310.07740.045*
H6A0.75120.71120.00500.045*
C30.2064 (4)0.86107 (8)0.01003 (17)0.0345 (4)
C40.3204 (5)0.80483 (9)0.04245 (19)0.0443 (5)
H4A0.46510.81990.07710.053*
H4B0.15460.78610.12300.053*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0537 (9)0.0417 (7)0.0454 (7)0.0153 (7)0.0319 (6)0.0063 (6)
O50.0761 (11)0.0384 (7)0.0480 (7)0.0049 (7)0.0405 (7)0.0067 (6)
O30.0536 (9)0.0293 (6)0.0473 (7)0.0004 (6)0.0275 (6)0.0027 (5)
N10.0422 (10)0.0321 (8)0.0396 (7)0.0084 (7)0.0228 (7)0.0000 (6)
C20.0348 (11)0.0350 (9)0.0344 (8)0.0021 (8)0.0186 (8)0.0002 (7)
O60.0726 (11)0.0360 (7)0.0510 (8)0.0163 (7)0.0349 (8)0.0061 (6)
O20.0612 (10)0.0556 (9)0.0575 (8)0.0243 (8)0.0358 (7)0.0237 (7)
C10.0331 (11)0.0306 (9)0.0389 (9)0.0014 (8)0.0180 (8)0.0015 (7)
C70.0408 (12)0.0277 (9)0.0377 (8)0.0027 (8)0.0184 (8)0.0020 (7)
O40.0853 (12)0.0378 (8)0.0758 (9)0.0195 (8)0.0627 (9)0.0160 (7)
C50.0587 (14)0.0335 (10)0.0419 (9)0.0103 (9)0.0280 (9)0.0057 (7)
C60.0483 (13)0.0325 (9)0.0398 (9)0.0048 (9)0.0252 (9)0.0037 (7)
C30.0374 (11)0.0328 (9)0.0367 (9)0.0041 (8)0.0189 (8)0.0041 (7)
C40.0581 (14)0.0389 (11)0.0461 (10)0.0129 (10)0.0318 (10)0.0087 (8)
Geometric parameters (Å, º) top
O1—C11.2508 (19)C7—C61.498 (2)
O5—C71.212 (2)O4—C31.306 (2)
O3—C31.219 (2)O4—H40.8200
N1—C21.474 (2)C5—C41.500 (2)
N1—H1A0.8900C5—C61.514 (2)
N1—H1B0.8900C5—H5A0.9700
N1—H1C0.8900C5—H5B0.9700
C2—C11.515 (2)C6—H6B0.9700
C2—H2A0.9700C6—H6A0.9700
C2—H2B0.9700C3—C41.497 (2)
O6—C71.313 (2)C4—H4A0.9700
O6—H60.8200C4—H4B0.9700
O2—C11.249 (2)
C2—N1—H1A109.5C4—C5—H5A108.7
C2—N1—H1B109.5C6—C5—H5A108.7
H1A—N1—H1B109.5C4—C5—H5B108.7
C2—N1—H1C109.5C6—C5—H5B108.7
H1A—N1—H1C109.5H5A—C5—H5B107.6
H1B—N1—H1C109.5C7—C6—C5112.48 (13)
N1—C2—C1112.00 (13)C7—C6—H6B109.1
N1—C2—H2A109.2C5—C6—H6B109.1
C1—C2—H2A109.2C7—C6—H6A109.1
N1—C2—H2B109.2C5—C6—H6A109.1
C1—C2—H2B109.2H6B—C6—H6A107.8
H2A—C2—H2B107.9O3—C3—O4122.19 (16)
C7—O6—H6109.5O3—C3—C4123.82 (15)
O2—C1—O1125.15 (17)O4—C3—C4113.98 (15)
O2—C1—C2117.00 (15)C3—C4—C5114.82 (14)
O1—C1—C2117.83 (15)C3—C4—H4A108.6
O5—C7—O6119.17 (15)C5—C4—H4A108.6
O5—C7—C6122.33 (16)C3—C4—H4B108.6
O6—C7—C6118.49 (14)C5—C4—H4B108.6
C3—O4—H4109.5H4A—C4—H4B107.5
C4—C5—C6114.14 (14)
N1—C2—C1—O2171.95 (16)C4—C5—C6—C7170.01 (18)
N1—C2—C1—O19.1 (2)O3—C3—C4—C5147.7 (2)
O5—C7—C6—C510.4 (3)O4—C3—C4—C533.3 (3)
O6—C7—C6—C5170.82 (17)C6—C5—C4—C3179.48 (18)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1B···O3i0.892.142.9671 (19)154
N1—H1C···O3ii0.892.002.8824 (19)169
N1—H1A···O50.892.002.7665 (18)143
O4—H4···O1iii0.821.752.5706 (18)178
O6—H6···O2iv0.821.752.5444 (18)164
Symmetry codes: (i) x+1, y1/2, z+1/2; (ii) x, y+3/2, z+1/2; (iii) x, y+1/2, z+1/2; (iv) x+1, y+1, z.
(275) Propane-1,3-dicarboxylic acid – Aminoethanoic acid (1/1) top
Crystal data top
C5H8O4·C2H5NO2F(000) = 440
Mr = 207.18Dx = 1.438 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 3205 reflections
a = 4.9022 (7) Åθ = 2.0–29.2°
b = 20.901 (3) ŵ = 0.13 mm1
c = 10.2730 (15) ÅT = 275 K
β = 114.60 (1)°Prism, colourless
V = 957.0 (2) Å30.32 × 0.17 × 0.10 mm
Z = 4
Data collection top
STOE IPDS 2
diffractometer
1461 reflections with I > 2σ(I)
Plane graphite monochromatorRint = 0.047
Detector resolution: 6.67 pixels mm-1θmax = 29.2°, θmin = 2.0°
rotation method scansh = 56
6792 measured reflectionsk = 2824
2570 independent reflectionsl = 1414
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.043Hydrogen site location: difference Fourier map
wR(F2) = 0.085H-atom parameters constrained
S = 0.87 w = 1/[σ2(Fo2) + (0.0364P)2]
where P = (Fo2 + 2Fc2)/3
2570 reflections(Δ/σ)max = 0.001
130 parametersΔρmax = 0.16 e Å3
0 restraintsΔρmin = 0.18 e Å3
Crystal data top
C5H8O4·C2H5NO2V = 957.0 (2) Å3
Mr = 207.18Z = 4
Monoclinic, P21/cMo Kα radiation
a = 4.9022 (7) ŵ = 0.13 mm1
b = 20.901 (3) ÅT = 275 K
c = 10.2730 (15) Å0.32 × 0.17 × 0.10 mm
β = 114.60 (1)°
Data collection top
STOE IPDS 2
diffractometer
1461 reflections with I > 2σ(I)
6792 measured reflectionsRint = 0.047
2570 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0430 restraints
wR(F2) = 0.085H-atom parameters constrained
S = 0.87Δρmax = 0.16 e Å3
2570 reflectionsΔρmin = 0.18 e Å3
130 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
O10.1302 (3)0.44534 (6)0.33384 (11)0.0391 (3)
O50.6205 (3)0.64085 (6)0.22111 (12)0.0434 (3)
O30.2021 (3)0.91559 (5)0.03340 (11)0.0368 (3)
N10.5575 (3)0.52520 (6)0.33659 (13)0.0325 (3)
H1A0.66130.55620.31840.049*
H1B0.68270.49960.40430.049*
H1C0.42740.54240.36640.049*
C20.3937 (4)0.48788 (8)0.20508 (15)0.0302 (4)
H2A0.53640.46430.18070.036*
H2B0.28570.51700.12690.036*
O60.8202 (3)0.59420 (6)0.09161 (12)0.0452 (3)
H60.84880.60180.02000.068*
O20.0470 (3)0.40245 (6)0.12262 (13)0.0489 (4)
C10.1736 (4)0.44130 (8)0.22219 (16)0.0304 (4)
C70.6768 (4)0.64243 (8)0.11682 (16)0.0310 (4)
O40.1064 (4)0.84659 (6)0.10554 (15)0.0518 (4)
H40.03800.87880.12640.078*
C50.4674 (4)0.75361 (8)0.06781 (16)0.0377 (4)
H5A0.32340.73820.10260.045*
H5B0.63350.77250.14820.045*
C60.5829 (4)0.69733 (7)0.01302 (17)0.0341 (4)
H6B0.42710.68300.07700.041*
H6A0.75300.71100.00510.041*
C30.2068 (4)0.86087 (8)0.00940 (16)0.0321 (4)
C40.3207 (5)0.80467 (8)0.04307 (17)0.0398 (5)
H4A0.46460.81970.07830.048*
H4B0.15430.78570.12310.048*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0477 (8)0.0394 (7)0.0401 (6)0.0147 (6)0.0281 (6)0.0068 (5)
O50.0665 (10)0.0342 (7)0.0416 (6)0.0049 (7)0.0346 (7)0.0065 (5)
O30.0474 (8)0.0267 (6)0.0414 (6)0.0001 (6)0.0234 (6)0.0021 (5)
N10.0377 (9)0.0291 (7)0.0369 (7)0.0079 (7)0.0218 (6)0.0001 (6)
C20.0314 (10)0.0312 (8)0.0310 (8)0.0021 (8)0.0158 (7)0.0006 (6)
O60.0660 (10)0.0323 (7)0.0462 (7)0.0155 (7)0.0321 (7)0.0058 (5)
O20.0540 (9)0.0498 (8)0.0525 (7)0.0223 (7)0.0318 (7)0.0231 (6)
C10.0294 (10)0.0269 (8)0.0379 (8)0.0016 (8)0.0168 (7)0.0005 (7)
C70.0349 (10)0.0251 (8)0.0340 (8)0.0020 (8)0.0153 (7)0.0016 (6)
O40.0787 (11)0.0346 (7)0.0694 (8)0.0180 (7)0.0579 (8)0.0149 (6)
C50.0517 (12)0.0303 (9)0.0382 (8)0.0092 (9)0.0256 (8)0.0048 (7)
C60.0438 (12)0.0285 (8)0.0368 (8)0.0053 (8)0.0234 (8)0.0035 (7)
C30.0347 (11)0.0317 (9)0.0326 (8)0.0033 (8)0.0166 (8)0.0037 (7)
C40.0525 (13)0.0345 (10)0.0410 (9)0.0109 (9)0.0279 (9)0.0073 (7)
Geometric parameters (Å, º) top
O1—C11.2534 (18)C7—C61.502 (2)
O5—C71.2132 (18)O4—C31.3082 (19)
O3—C31.2221 (19)O4—H40.8200
N1—C21.4749 (19)C5—C41.507 (2)
N1—H1A0.8900C5—C61.512 (2)
N1—H1B0.8900C5—H5A0.9700
N1—H1C0.8900C5—H5B0.9700
C2—C11.517 (2)C6—H6B0.9700
C2—H2A0.9700C6—H6A0.9700
C2—H2B0.9700C3—C41.494 (2)
O6—C71.3149 (19)C4—H4A0.9700
O6—H60.8200C4—H4B0.9700
O2—C11.2499 (19)
C2—N1—H1A109.5C4—C5—H5A108.8
C2—N1—H1B109.5C6—C5—H5A108.8
H1A—N1—H1B109.5C4—C5—H5B108.8
C2—N1—H1C109.5C6—C5—H5B108.8
H1A—N1—H1C109.5H5A—C5—H5B107.7
H1B—N1—H1C109.5C7—C6—C5112.43 (12)
N1—C2—C1112.07 (12)C7—C6—H6B109.1
N1—C2—H2A109.2C5—C6—H6B109.1
C1—C2—H2A109.2C7—C6—H6A109.1
N1—C2—H2B109.2C5—C6—H6A109.1
C1—C2—H2B109.2H6B—C6—H6A107.9
H2A—C2—H2B107.9O3—C3—O4121.90 (15)
C7—O6—H6109.5O3—C3—C4124.04 (14)
O2—C1—O1125.25 (16)O4—C3—C4114.06 (14)
O2—C1—C2117.19 (14)C3—C4—C5114.62 (13)
O1—C1—C2117.56 (14)C3—C4—H4A108.6
O5—C7—O6119.35 (14)C5—C4—H4A108.6
O5—C7—C6122.17 (15)C3—C4—H4B108.6
O6—C7—C6118.47 (13)C5—C4—H4B108.6
C3—O4—H4109.5H4A—C4—H4B107.6
C4—C5—C6113.85 (13)
N1—C2—C1—O2172.37 (15)C4—C5—C6—C7169.69 (17)
N1—C2—C1—O18.5 (2)O3—C3—C4—C5147.16 (18)
O5—C7—C6—C510.6 (3)O4—C3—C4—C533.7 (2)
O6—C7—C6—C5170.55 (16)C6—C5—C4—C3179.64 (16)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1B···O3i0.892.132.9564 (18)154
N1—H1C···O3ii0.892.002.8789 (18)169
N1—H1A···O50.892.002.7658 (17)143
O4—H4···O1iii0.821.752.5680 (17)176
O6—H6···O2iv0.821.742.5425 (17)165
Symmetry codes: (i) x+1, y1/2, z+1/2; (ii) x, y+3/2, z+1/2; (iii) x, y+1/2, z+1/2; (iv) x+1, y+1, z.
(250) Propane-1,3-dicarboxylic acid – Aminoethanoic acid (1/1) top
Crystal data top
C5H8O4·C2H5NO2F(000) = 440
Mr = 207.18Dx = 1.442 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 3499 reflections
a = 4.8960 (6) Åθ = 2.0–29.5°
b = 20.878 (2) ŵ = 0.13 mm1
c = 10.2701 (13) ÅT = 250 K
β = 114.634 (9)°Prism, colourless
V = 954.3 (2) Å30.32 × 0.17 × 0.10 mm
Z = 4
Data collection top
STOE IPDS 2
diffractometer
1535 reflections with I > 2σ(I)
Plane graphite monochromatorRint = 0.045
Detector resolution: 6.67 pixels mm-1θmax = 29.2°, θmin = 2.0°
rotation method scansh = 56
6775 measured reflectionsk = 2824
2562 independent reflectionsl = 1414
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.044Hydrogen site location: difference Fourier map
wR(F2) = 0.086H-atom parameters constrained
S = 0.88 w = 1/[σ2(Fo2) + (0.0377P)2]
where P = (Fo2 + 2Fc2)/3
2562 reflections(Δ/σ)max < 0.001
130 parametersΔρmax = 0.16 e Å3
0 restraintsΔρmin = 0.20 e Å3
Crystal data top
C5H8O4·C2H5NO2V = 954.3 (2) Å3
Mr = 207.18Z = 4
Monoclinic, P21/cMo Kα radiation
a = 4.8960 (6) ŵ = 0.13 mm1
b = 20.878 (2) ÅT = 250 K
c = 10.2701 (13) Å0.32 × 0.17 × 0.10 mm
β = 114.634 (9)°
Data collection top
STOE IPDS 2
diffractometer
1535 reflections with I > 2σ(I)
6775 measured reflectionsRint = 0.045
2562 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0440 restraints
wR(F2) = 0.086H-atom parameters constrained
S = 0.88Δρmax = 0.16 e Å3
2562 reflectionsΔρmin = 0.20 e Å3
130 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
O10.1300 (3)0.44533 (6)0.33405 (11)0.0352 (3)
O50.6231 (3)0.64055 (5)0.22156 (11)0.0386 (3)
O30.2029 (3)0.91557 (5)0.03367 (11)0.0332 (3)
N10.5587 (3)0.52504 (6)0.33685 (13)0.0294 (3)
H1A0.66270.55660.31820.044*
H1B0.68660.49920.40530.044*
H1C0.42700.54220.36730.044*
C20.3943 (4)0.48752 (7)0.20504 (15)0.0277 (3)
H2A0.53860.46350.18080.033*
H2B0.28600.51690.12580.033*
O60.8236 (3)0.59387 (6)0.09217 (12)0.0411 (3)
H60.85440.60180.02020.062*
O20.0439 (3)0.40249 (6)0.12210 (13)0.0446 (3)
C10.1725 (4)0.44122 (8)0.22194 (15)0.0275 (3)
C70.6793 (4)0.64212 (7)0.11717 (15)0.0280 (3)
O40.1064 (3)0.84645 (6)0.10527 (14)0.0464 (4)
H40.03380.87890.12520.070*
C50.4699 (4)0.75347 (8)0.06795 (16)0.0331 (4)
H5A0.32490.73790.10360.040*
H5B0.63810.77280.14880.040*
C60.5856 (4)0.69709 (7)0.01315 (16)0.0304 (4)
H6B0.42800.68260.07790.036*
H6A0.75790.71090.00500.036*
C30.2068 (4)0.86084 (8)0.00894 (15)0.0284 (4)
C40.3212 (4)0.80446 (8)0.04366 (17)0.0348 (4)
H4A0.46620.81970.07970.042*
H4B0.15280.78510.12430.042*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0427 (8)0.0349 (6)0.0366 (6)0.0127 (6)0.0251 (5)0.0051 (5)
O50.0582 (9)0.0310 (6)0.0371 (6)0.0045 (6)0.0304 (6)0.0058 (5)
O30.0418 (8)0.0242 (6)0.0384 (6)0.0003 (6)0.0216 (5)0.0020 (5)
N10.0346 (8)0.0264 (7)0.0326 (6)0.0066 (6)0.0193 (6)0.0002 (5)
C20.0288 (9)0.0284 (8)0.0288 (7)0.0002 (7)0.0151 (7)0.0000 (6)
O60.0596 (9)0.0301 (6)0.0415 (6)0.0143 (6)0.0291 (6)0.0057 (5)
O20.0492 (9)0.0463 (7)0.0468 (7)0.0206 (7)0.0285 (6)0.0213 (6)
C10.0272 (9)0.0254 (8)0.0326 (7)0.0016 (7)0.0152 (7)0.0007 (6)
C70.0327 (10)0.0223 (7)0.0298 (7)0.0022 (7)0.0139 (7)0.0016 (6)
O40.0712 (10)0.0300 (7)0.0632 (8)0.0166 (7)0.0529 (7)0.0134 (6)
C50.0459 (11)0.0253 (8)0.0336 (8)0.0076 (8)0.0219 (7)0.0044 (6)
C60.0391 (11)0.0256 (8)0.0321 (8)0.0036 (7)0.0205 (7)0.0029 (6)
C30.0301 (10)0.0276 (8)0.0300 (7)0.0020 (7)0.0150 (7)0.0032 (6)
C40.0460 (12)0.0296 (9)0.0352 (8)0.0106 (8)0.0234 (8)0.0069 (6)
Geometric parameters (Å, º) top
O1—C11.2553 (17)C7—C61.503 (2)
O5—C71.2133 (18)O4—C31.3098 (19)
O3—C31.2210 (18)O4—H40.8300
N1—C21.4783 (19)C5—C41.510 (2)
N1—H1A0.9000C5—C61.513 (2)
N1—H1B0.9000C5—H5A0.9800
N1—H1C0.9000C5—H5B0.9800
C2—C11.517 (2)C6—H6B0.9800
C2—H2A0.9800C6—H6A0.9800
C2—H2B0.9800C3—C41.498 (2)
O6—C71.3157 (19)C4—H4A0.9800
O6—H60.8300C4—H4B0.9800
O2—C11.2503 (19)
C2—N1—H1A109.5C4—C5—H5A108.8
C2—N1—H1B109.5C6—C5—H5A108.8
H1A—N1—H1B109.5C4—C5—H5B108.8
C2—N1—H1C109.5C6—C5—H5B108.8
H1A—N1—H1C109.5H5A—C5—H5B107.7
H1B—N1—H1C109.5C7—C6—C5112.35 (12)
N1—C2—C1112.06 (12)C7—C6—H6B109.1
N1—C2—H2A109.2C5—C6—H6B109.1
C1—C2—H2A109.2C7—C6—H6A109.1
N1—C2—H2B109.2C5—C6—H6A109.1
C1—C2—H2B109.2H6B—C6—H6A107.9
H2A—C2—H2B107.9O3—C3—O4122.06 (15)
C7—O6—H6109.5O3—C3—C4123.95 (14)
O2—C1—O1125.25 (15)O4—C3—C4113.99 (13)
O2—C1—C2117.26 (13)C3—C4—C5114.49 (12)
O1—C1—C2117.48 (13)C3—C4—H4A108.6
O5—C7—O6119.32 (14)C5—C4—H4A108.6
O5—C7—C6122.28 (14)C3—C4—H4B108.6
O6—C7—C6118.39 (13)C5—C4—H4B108.6
C3—O4—H4109.5H4A—C4—H4B107.6
C4—C5—C6113.75 (12)
N1—C2—C1—O2172.80 (15)C4—C5—C6—C7169.33 (16)
N1—C2—C1—O18.0 (2)O3—C3—C4—C5146.67 (17)
O5—C7—C6—C510.5 (2)O4—C3—C4—C533.9 (2)
O6—C7—C6—C5170.40 (15)C6—C5—C4—C3179.68 (16)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1B···O3i0.902.122.9504 (17)153
N1—H1C···O3ii0.901.992.8760 (18)170
N1—H1A···O50.901.982.7621 (17)144
O4—H4···O1iii0.831.742.5676 (16)178
O6—H6···O2iv0.831.732.5414 (16)165
Symmetry codes: (i) x+1, y1/2, z+1/2; (ii) x, y+3/2, z+1/2; (iii) x, y+1/2, z+1/2; (iv) x+1, y+1, z.
(225) Propane-1,3-dicarboxylic acid – Aminoethanoic acid (1/1) top
Crystal data top
C5H8O4·C2H5NO2F(000) = 440
Mr = 207.18Dx = 1.446 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 3782 reflections
a = 4.8888 (6) Åθ = 2.0–29.5°
b = 20.859 (2) ŵ = 0.13 mm1
c = 10.2664 (13) ÅT = 225 K
β = 114.648 (9)°Prism, colourless
V = 951.6 (2) Å30.32 × 0.17 × 0.10 mm
Z = 4
Data collection top
STOE IPDS 2
diffractometer
1594 reflections with I > 2σ(I)
Plane graphite monochromatorRint = 0.043
Detector resolution: 6.67 pixels mm-1θmax = 29.2°, θmin = 2.0°
rotation method scansh = 56
6775 measured reflectionsk = 2824
2558 independent reflectionsl = 1414
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.042Hydrogen site location: difference Fourier map
wR(F2) = 0.081H-atom parameters constrained
S = 0.88 w = 1/[σ2(Fo2) + (0.037P)2]
where P = (Fo2 + 2Fc2)/3
2558 reflections(Δ/σ)max < 0.001
130 parametersΔρmax = 0.21 e Å3
0 restraintsΔρmin = 0.18 e Å3
Crystal data top
C5H8O4·C2H5NO2V = 951.6 (2) Å3
Mr = 207.18Z = 4
Monoclinic, P21/cMo Kα radiation
a = 4.8888 (6) ŵ = 0.13 mm1
b = 20.859 (2) ÅT = 225 K
c = 10.2664 (13) Å0.32 × 0.17 × 0.10 mm
β = 114.648 (9)°
Data collection top
STOE IPDS 2
diffractometer
1594 reflections with I > 2σ(I)
6775 measured reflectionsRint = 0.043
2558 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0420 restraints
wR(F2) = 0.081H-atom parameters constrained
S = 0.88Δρmax = 0.21 e Å3
2558 reflectionsΔρmin = 0.18 e Å3
130 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
O10.1297 (3)0.44519 (5)0.33441 (10)0.0314 (3)
O50.6253 (3)0.64046 (5)0.22218 (10)0.0346 (3)
O30.2033 (3)0.91561 (5)0.03396 (10)0.0296 (3)
N10.5594 (3)0.52477 (6)0.33723 (12)0.0263 (3)
H1A0.66520.55610.31900.039*
H1B0.68590.49870.40580.039*
H1C0.42750.54220.36730.039*
C20.3944 (3)0.48745 (7)0.20527 (14)0.0251 (3)
H2A0.53870.46330.18090.030*
H2B0.28640.51700.12610.030*
O60.8268 (3)0.59350 (5)0.09291 (11)0.0366 (3)
H60.85630.60120.02050.055*
O20.0402 (3)0.40272 (6)0.12133 (12)0.0403 (3)
C10.1715 (3)0.44119 (7)0.22204 (14)0.0247 (3)
C70.6820 (4)0.64190 (7)0.11764 (14)0.0249 (3)
O40.1061 (3)0.84624 (5)0.10478 (13)0.0423 (3)
H40.04070.87900.12770.063*
C50.4719 (4)0.75334 (7)0.06844 (14)0.0300 (4)
H5A0.64030.77270.14930.036*
H5B0.32670.73770.10410.036*
C60.5880 (4)0.69689 (7)0.01334 (15)0.0276 (3)
H6B0.43010.68230.07780.033*
H6A0.76040.71070.00490.033*
C30.2072 (3)0.86082 (7)0.00868 (14)0.0259 (3)
C40.3223 (4)0.80435 (7)0.04410 (15)0.0320 (4)
H4A0.46750.81960.08010.038*
H4B0.15370.78490.12470.038*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0382 (7)0.0317 (6)0.0323 (5)0.0113 (5)0.0225 (5)0.0052 (4)
O50.0512 (8)0.0277 (6)0.0338 (5)0.0037 (5)0.0266 (5)0.0051 (4)
O30.0376 (7)0.0217 (5)0.0332 (5)0.0002 (5)0.0183 (5)0.0016 (4)
N10.0308 (7)0.0234 (6)0.0295 (6)0.0054 (6)0.0173 (5)0.0006 (5)
C20.0259 (8)0.0269 (7)0.0255 (6)0.0005 (7)0.0136 (6)0.0002 (6)
O60.0515 (8)0.0273 (6)0.0376 (6)0.0121 (6)0.0251 (6)0.0044 (5)
O20.0431 (8)0.0427 (7)0.0421 (6)0.0173 (6)0.0249 (6)0.0182 (5)
C10.0237 (8)0.0231 (7)0.0296 (7)0.0015 (6)0.0133 (6)0.0012 (6)
C70.0282 (9)0.0207 (7)0.0268 (6)0.0022 (6)0.0124 (6)0.0011 (5)
O40.0647 (9)0.0280 (6)0.0565 (7)0.0156 (6)0.0475 (7)0.0125 (5)
C50.0402 (10)0.0249 (8)0.0294 (7)0.0073 (7)0.0191 (7)0.0038 (6)
C60.0347 (9)0.0234 (7)0.0294 (7)0.0037 (7)0.0181 (6)0.0027 (6)
C30.0263 (8)0.0262 (7)0.0265 (7)0.0017 (7)0.0123 (6)0.0023 (6)
C40.0434 (11)0.0272 (8)0.0322 (7)0.0089 (7)0.0225 (7)0.0062 (6)
Geometric parameters (Å, º) top
O1—C11.2554 (16)C7—C61.5042 (19)
O5—C71.2159 (17)O4—C31.3103 (17)
O3—C31.2212 (17)O4—H40.8300
N1—C21.4766 (18)C5—C61.515 (2)
N1—H1A0.9000C5—C41.516 (2)
N1—H1B0.9000C5—H5A0.9800
N1—H1C0.9000C5—H5B0.9800
C2—C11.518 (2)C6—H6B0.9800
C2—H2A0.9800C6—H6A0.9800
C2—H2B0.9800C3—C41.501 (2)
O6—C71.3170 (17)C4—H4A0.9800
O6—H60.8300C4—H4B0.9800
O2—C11.2536 (17)
C2—N1—H1A109.5C6—C5—H5A108.9
C2—N1—H1B109.5C4—C5—H5A108.9
H1A—N1—H1B109.5C6—C5—H5B108.9
C2—N1—H1C109.5C4—C5—H5B108.9
H1A—N1—H1C109.5H5A—C5—H5B107.7
H1B—N1—H1C109.5C7—C6—C5112.19 (11)
N1—C2—C1111.98 (11)C7—C6—H6B109.2
N1—C2—H2A109.2C5—C6—H6B109.2
C1—C2—H2A109.2C7—C6—H6A109.2
N1—C2—H2B109.2C5—C6—H6A109.2
C1—C2—H2B109.2H6B—C6—H6A107.9
H2A—C2—H2B107.9O3—C3—O4122.19 (14)
C7—O6—H6109.5O3—C3—C4123.87 (13)
O2—C1—O1125.24 (14)O4—C3—C4113.93 (12)
O2—C1—C2117.27 (12)C3—C4—C5114.22 (11)
O1—C1—C2117.49 (12)C3—C4—H4A108.7
O5—C7—O6119.33 (13)C5—C4—H4A108.7
O5—C7—C6122.19 (13)C3—C4—H4B108.7
O6—C7—C6118.47 (12)C5—C4—H4B108.7
C3—O4—H4109.5H4A—C4—H4B107.6
C6—C5—C4113.44 (11)
N1—C2—C1—O2173.27 (13)C4—C5—C6—C7169.30 (14)
N1—C2—C1—O17.84 (19)O3—C3—C4—C5146.60 (16)
O5—C7—C6—C510.6 (2)O4—C3—C4—C534.2 (2)
O6—C7—C6—C5170.43 (14)C6—C5—C4—C3179.71 (14)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1B···O3i0.902.112.9420 (16)154
N1—H1C···O3ii0.901.982.8716 (16)170
N1—H1A···O50.901.992.7641 (15)143
O4—H4···O1iii0.831.742.5650 (15)175
O6—H6···O2iv0.831.732.5417 (15)165
Symmetry codes: (i) x+1, y1/2, z+1/2; (ii) x, y+3/2, z+1/2; (iii) x, y+1/2, z+1/2; (iv) x+1, y+1, z.
(200) Propane-1,3-dicarboxylic acid – Aminoethanoic acid (1/1) top
Crystal data top
C5H8O4·C2H5NO2Z = 4
Mr = 207.18F(000) = 440
Triclinic, P1Dx = 1.486 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 4.9155 (7) ÅCell parameters from 6919 reflections
b = 20.215 (3) Åθ = 2.0–29.6°
c = 10.1862 (16) ŵ = 0.13 mm1
α = 85.578 (14)°T = 200 K
β = 113.133 (11)°Prism, colourless
γ = 88.301 (13)°0.40 × 0.23 × 0.10 mm
V = 926.1 (2) Å3
Data collection top
STOE IPDS 2
diffractometer
2491 reflections with I > 2σ(I)
Plane graphite monochromatorRint = 0.055
Detector resolution: 6.67 pixels mm-1θmax = 29.2°, θmin = 2.0°
rotation method scansh = 65
9663 measured reflectionsk = 2727
4312 independent reflectionsl = 1313
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.049Hydrogen site location: difference Fourier map
wR(F2) = 0.081H-atom parameters constrained
S = 0.89 w = 1/[σ2(Fo2) + (0.0266P)2]
where P = (Fo2 + 2Fc2)/3
4312 reflections(Δ/σ)max = 0.001
259 parametersΔρmax = 0.19 e Å3
0 restraintsΔρmin = 0.21 e Å3
Crystal data top
C5H8O4·C2H5NO2γ = 88.301 (13)°
Mr = 207.18V = 926.1 (2) Å3
Triclinic, P1Z = 4
a = 4.9155 (7) ÅMo Kα radiation
b = 20.215 (3) ŵ = 0.13 mm1
c = 10.1862 (16) ÅT = 200 K
α = 85.578 (14)°0.40 × 0.23 × 0.10 mm
β = 113.133 (11)°
Data collection top
STOE IPDS 2
diffractometer
2491 reflections with I > 2σ(I)
9663 measured reflectionsRint = 0.055
4312 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0490 restraints
wR(F2) = 0.081H-atom parameters constrained
S = 0.89Δρmax = 0.19 e Å3
4312 reflectionsΔρmin = 0.21 e Å3
259 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
O230.1871 (4)0.58896 (6)0.45166 (16)0.0260 (4)
O250.6524 (4)0.84815 (6)0.75064 (16)0.0284 (4)
O260.8511 (4)0.90410 (6)0.62247 (16)0.0289 (4)
H260.87880.90110.54680.043*
O210.1282 (3)1.05514 (6)0.82424 (16)0.0261 (3)
O220.0124 (4)1.09123 (7)0.59539 (16)0.0297 (4)
O130.7719 (3)0.08769 (6)1.01431 (16)0.0250 (3)
O240.0718 (4)0.65453 (6)0.59001 (18)0.0316 (4)
H240.00200.61970.61050.047*
O160.1845 (4)0.40381 (7)0.90921 (17)0.0328 (4)
H160.18090.40420.99090.049*
O140.7927 (4)0.15354 (6)0.83429 (16)0.0297 (4)
H140.89490.12060.82910.045*
O150.4073 (4)0.34554 (6)0.80336 (18)0.0374 (4)
N210.5779 (4)0.97095 (7)0.84561 (18)0.0225 (4)
H21A0.69570.93800.83510.034*
H21B0.45200.95290.88220.034*
H21C0.69260.99920.90640.034*
C220.4041 (5)1.00798 (9)0.7040 (2)0.0200 (4)
H22A0.31190.97590.63310.024*
H22B0.53941.03350.67200.024*
C130.7020 (5)0.14025 (8)0.9381 (2)0.0197 (4)
C250.4718 (5)0.74512 (9)0.5767 (2)0.0219 (4)
H25A0.32560.76150.61330.026*
H25B0.62750.71680.65570.026*
C230.1863 (5)0.64326 (9)0.4972 (2)0.0204 (4)
C210.1633 (5)1.05543 (8)0.7089 (2)0.0190 (4)
C260.6120 (5)0.80423 (8)0.5320 (2)0.0209 (4)
H26A0.78650.78800.51510.025*
H26B0.46740.82730.44080.025*
C240.3174 (5)0.70327 (9)0.4526 (2)0.0239 (5)
H24A0.15760.73130.37490.029*
H24B0.46230.68820.41390.029*
C160.5015 (5)0.30815 (9)1.0471 (2)0.0243 (5)
H16A0.34350.29071.07480.029*
H16B0.62500.33481.12370.029*
C140.5083 (5)0.19546 (9)0.9534 (2)0.0233 (4)
H14A0.38770.17721.00420.028*
H14B0.37130.21520.85710.028*
C150.6943 (5)0.24964 (9)1.0370 (2)0.0286 (5)
H15A0.82380.23021.13490.034*
H15B0.82310.26600.98890.034*
C270.7073 (5)0.85271 (8)0.6442 (2)0.0198 (4)
C170.3605 (5)0.35270 (9)0.9092 (2)0.0245 (5)
O110.8400 (3)0.55159 (6)0.65415 (15)0.0254 (3)
O120.9335 (4)0.58758 (7)0.86847 (17)0.0301 (4)
N110.4288 (4)0.47027 (7)0.66308 (18)0.0216 (4)
H11A0.31370.44000.68320.032*
H11B0.56640.44890.63960.032*
H11C0.31310.49970.58820.032*
C120.5809 (5)0.50654 (8)0.7909 (2)0.0191 (4)
H12A0.68580.47410.87530.023*
H12B0.43140.53310.81080.023*
C110.8023 (5)0.55239 (8)0.7686 (2)0.0188 (4)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O230.0322 (10)0.0197 (7)0.0298 (9)0.0035 (6)0.0153 (8)0.0067 (6)
O250.0419 (10)0.0231 (7)0.0283 (9)0.0067 (6)0.0213 (8)0.0080 (6)
O260.0392 (10)0.0242 (7)0.0295 (9)0.0116 (6)0.0189 (8)0.0074 (6)
O210.0308 (9)0.0263 (7)0.0239 (8)0.0063 (6)0.0144 (7)0.0009 (6)
O220.0279 (9)0.0339 (8)0.0268 (9)0.0078 (6)0.0127 (7)0.0068 (6)
O130.0293 (9)0.0192 (7)0.0264 (9)0.0014 (6)0.0118 (7)0.0003 (5)
O240.0453 (11)0.0234 (7)0.0428 (10)0.0147 (7)0.0328 (9)0.0115 (6)
O160.0458 (12)0.0251 (7)0.0305 (9)0.0107 (6)0.0201 (9)0.0021 (6)
O140.0396 (11)0.0245 (7)0.0308 (9)0.0094 (6)0.0222 (8)0.0043 (6)
O150.0639 (13)0.0248 (8)0.0372 (10)0.0047 (7)0.0362 (10)0.0024 (6)
N210.0264 (10)0.0208 (8)0.0225 (9)0.0036 (7)0.0121 (8)0.0029 (6)
C220.0201 (11)0.0220 (9)0.0195 (10)0.0014 (7)0.0093 (9)0.0033 (7)
C130.0183 (11)0.0191 (9)0.0221 (11)0.0045 (7)0.0075 (9)0.0062 (7)
C250.0258 (12)0.0215 (9)0.0215 (11)0.0061 (8)0.0119 (9)0.0043 (7)
C230.0184 (11)0.0217 (9)0.0203 (11)0.0031 (7)0.0066 (9)0.0026 (7)
C210.0180 (11)0.0172 (9)0.0241 (11)0.0050 (7)0.0102 (9)0.0036 (7)
C260.0251 (12)0.0194 (9)0.0201 (11)0.0037 (7)0.0107 (9)0.0035 (7)
C240.0307 (13)0.0234 (9)0.0218 (11)0.0083 (8)0.0137 (10)0.0056 (7)
C160.0268 (12)0.0205 (9)0.0235 (11)0.0004 (8)0.0071 (10)0.0055 (7)
C140.0227 (12)0.0191 (9)0.0300 (12)0.0010 (7)0.0122 (10)0.0037 (7)
C150.0228 (12)0.0266 (10)0.0280 (12)0.0045 (8)0.0008 (10)0.0066 (8)
C270.0209 (11)0.0161 (9)0.0211 (11)0.0032 (7)0.0077 (9)0.0004 (7)
C170.0324 (13)0.0163 (9)0.0298 (12)0.0050 (8)0.0171 (11)0.0032 (8)
O110.0305 (9)0.0265 (7)0.0249 (8)0.0123 (6)0.0155 (7)0.0069 (6)
O120.0331 (10)0.0333 (8)0.0306 (9)0.0149 (7)0.0165 (8)0.0163 (6)
N110.0254 (10)0.0214 (8)0.0218 (9)0.0076 (7)0.0128 (8)0.0028 (6)
C120.0187 (11)0.0208 (9)0.0190 (10)0.0015 (7)0.0088 (9)0.0020 (7)
C110.0158 (10)0.0169 (9)0.0238 (11)0.0005 (7)0.0084 (9)0.0009 (7)
Geometric parameters (Å, º) top
O23—C231.225 (2)C25—H25B0.9900
O25—C271.214 (2)C23—C241.512 (3)
O26—C271.326 (2)C26—C271.505 (3)
O26—H260.8400C26—H26A0.9900
O21—C211.252 (2)C26—H26B0.9900
O22—C211.256 (2)C24—H24A0.9900
O13—C131.221 (2)C24—H24B0.9900
O24—C231.306 (2)C16—C171.506 (3)
O24—H240.8400C16—C151.529 (3)
O16—C171.328 (3)C16—H16A0.9900
O16—H160.8400C16—H16B0.9900
O14—C131.313 (2)C14—C151.533 (3)
O14—H140.8400C14—H14A0.9900
O15—C171.205 (3)C14—H14B0.9900
N21—C221.482 (2)C15—H15A0.9900
N21—H21A0.9100C15—H15B0.9900
N21—H21B0.9100O11—C111.252 (2)
N21—H21C0.9100O12—C111.257 (2)
C22—C211.520 (3)N11—C121.486 (3)
C22—H22A0.9900N11—H11A0.9100
C22—H22B0.9900N11—H11B0.9100
C13—C141.502 (3)N11—H11C0.9100
C25—C261.524 (2)C12—C111.522 (3)
C25—C241.530 (3)C12—H12A0.9900
C25—H25A0.9900C12—H12B0.9900
C27—O26—H26109.5C25—C24—H24B109.1
C23—O24—H24109.5H24A—C24—H24B107.8
C17—O16—H16109.5C17—C16—C15113.30 (18)
C13—O14—H14109.5C17—C16—H16A108.9
C22—N21—H21A109.5C15—C16—H16A108.9
C22—N21—H21B109.5C17—C16—H16B108.9
H21A—N21—H21B109.5C15—C16—H16B108.9
C22—N21—H21C109.5H16A—C16—H16B107.7
H21A—N21—H21C109.5C13—C14—C15111.21 (18)
H21B—N21—H21C109.5C13—C14—H14A109.4
N21—C22—C21112.13 (16)C15—C14—H14A109.4
N21—C22—H22A109.2C13—C14—H14B109.4
C21—C22—H22A109.2C15—C14—H14B109.4
N21—C22—H22B109.2H14A—C14—H14B108.0
C21—C22—H22B109.2C16—C15—C14112.17 (19)
H22A—C22—H22B107.9C16—C15—H15A109.2
O13—C13—O14122.23 (18)C14—C15—H15A109.2
O13—C13—C14124.05 (18)C16—C15—H15B109.2
O14—C13—C14113.72 (16)C14—C15—H15B109.2
C26—C25—C24112.25 (16)H15A—C15—H15B107.9
C26—C25—H25A109.2O25—C27—O26118.69 (18)
C24—C25—H25A109.2O25—C27—C26123.50 (17)
C26—C25—H25B109.2O26—C27—C26117.78 (17)
C24—C25—H25B109.2O15—C17—O16119.58 (19)
H25A—C25—H25B107.9O15—C17—C16123.7 (2)
O23—C23—O24122.74 (17)O16—C17—C16116.62 (18)
O23—C23—C24123.6 (2)C12—N11—H11A109.5
O24—C23—C24113.64 (17)C12—N11—H11B109.5
O21—C21—O22125.30 (19)H11A—N11—H11B109.5
O21—C21—C22117.85 (17)C12—N11—H11C109.5
O22—C21—C22116.85 (17)H11A—N11—H11C109.5
C27—C26—C25111.92 (17)H11B—N11—H11C109.5
C27—C26—H26A109.2N11—C12—C11111.60 (16)
C25—C26—H26A109.2N11—C12—H12A109.3
C27—C26—H26B109.2C11—C12—H12A109.3
C25—C26—H26B109.2N11—C12—H12B109.3
H26A—C26—H26B107.9C11—C12—H12B109.3
C23—C24—C25112.57 (17)H12A—C12—H12B108.0
C23—C24—H24A109.1O11—C11—O12125.71 (18)
C25—C24—H24A109.1O11—C11—C12117.77 (17)
C23—C24—H24B109.1O12—C11—C12116.51 (18)
N21—C22—C21—O214.0 (2)C17—C16—C15—C1475.0 (2)
N21—C22—C21—O22176.98 (16)C13—C14—C15—C16176.98 (18)
C24—C25—C26—C27168.16 (18)C25—C26—C27—O256.6 (3)
O23—C23—C24—C25142.3 (2)C25—C26—C27—O26175.47 (18)
O24—C23—C24—C2537.5 (3)C15—C16—C17—O154.1 (3)
C26—C25—C24—C23178.14 (18)C15—C16—C17—O16178.57 (19)
O13—C13—C14—C1599.0 (2)N11—C12—C11—O113.6 (2)
O14—C13—C14—C1580.7 (2)N11—C12—C11—O12176.97 (17)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O14—H14···O21i0.841.742.580 (2)176
O16—H16···O12ii0.841.752.565 (2)164
N11—H11A···O150.912.122.827 (2)134
N11—H11B···O23iii0.911.962.860 (2)168
N11—H11C···O230.912.112.971 (2)158
O24—H24···O11iv0.841.722.5636 (18)176
O26—H26···O22v0.841.732.555 (2)167
N21—H21A···O250.912.052.798 (2)139
N21—H21B···O13ii0.911.962.861 (2)172
N21—H21C···O13vi0.912.142.984 (2)155
Symmetry codes: (i) x+1, y1, z; (ii) x+1, y+1, z+2; (iii) x+1, y+1, z+1; (iv) x1, y, z; (v) x+1, y+2, z+1; (vi) x, y+1, z.
(175) Propane-1,3-dicarboxylic acid – Aminoethanoic acid (1/1) top
Crystal data top
C5H8O4·C2H5NO2Z = 4
Mr = 207.18F(000) = 440
Triclinic, P1Dx = 1.490 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 4.9098 (7) ÅCell parameters from 7461 reflections
b = 20.194 (3) Åθ = 2.1–29.6°
c = 10.1777 (15) ŵ = 0.13 mm1
α = 85.571 (13)°T = 175 K
β = 113.118 (10)°Prism, colourless
γ = 88.306 (12)°0.40 × 0.23 × 0.10 mm
V = 923.3 (2) Å3
Data collection top
STOE IPDS 2
diffractometer
2580 reflections with I > 2σ(I)
Plane graphite monochromatorRint = 0.052
Detector resolution: 6.67 pixels mm-1θmax = 29.2°, θmin = 2.0°
rotation method scansh = 65
9568 measured reflectionsk = 2727
4319 independent reflectionsl = 1313
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.049Hydrogen site location: difference Fourier map
wR(F2) = 0.088H-atom parameters constrained
S = 0.89 w = 1/[σ2(Fo2) + (0.0329P)2]
where P = (Fo2 + 2Fc2)/3
4319 reflections(Δ/σ)max < 0.001
259 parametersΔρmax = 0.22 e Å3
0 restraintsΔρmin = 0.23 e Å3
Crystal data top
C5H8O4·C2H5NO2γ = 88.306 (12)°
Mr = 207.18V = 923.3 (2) Å3
Triclinic, P1Z = 4
a = 4.9098 (7) ÅMo Kα radiation
b = 20.194 (3) ŵ = 0.13 mm1
c = 10.1777 (15) ÅT = 175 K
α = 85.571 (13)°0.40 × 0.23 × 0.10 mm
β = 113.118 (10)°
Data collection top
STOE IPDS 2
diffractometer
2580 reflections with I > 2σ(I)
9568 measured reflectionsRint = 0.052
4319 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0490 restraints
wR(F2) = 0.088H-atom parameters constrained
S = 0.89Δρmax = 0.22 e Å3
4319 reflectionsΔρmin = 0.23 e Å3
259 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
O230.1870 (4)0.58898 (6)0.45114 (16)0.0223 (3)
O250.6532 (4)0.84810 (6)0.75156 (17)0.0248 (3)
O260.8537 (4)0.90432 (6)0.62332 (17)0.0253 (4)
H260.87310.90230.54530.038*
O210.1280 (4)1.05536 (6)0.82397 (16)0.0232 (3)
O220.0102 (4)1.09092 (7)0.59471 (17)0.0263 (4)
O130.7721 (3)0.08762 (6)1.01479 (16)0.0206 (3)
O240.0731 (4)0.65463 (6)0.59004 (18)0.0271 (4)
H240.00110.61990.60960.041*
O160.1825 (4)0.40414 (7)0.90858 (17)0.0281 (4)
H160.17140.40360.98890.042*
O140.7902 (4)0.15354 (7)0.83352 (17)0.0262 (4)
H140.89590.12090.82960.039*
O150.4050 (4)0.34553 (7)0.80242 (18)0.0324 (4)
N210.5783 (4)0.97136 (7)0.84576 (19)0.0194 (4)
H21A0.69990.93900.83590.029*
H21B0.45250.95250.88150.029*
H21C0.68951.00000.90710.029*
C220.4044 (5)1.00819 (9)0.7039 (2)0.0174 (4)
H22A0.31350.97600.63300.021*
H22B0.53951.03400.67190.021*
C130.6991 (5)0.14026 (9)0.9372 (2)0.0167 (4)
C250.4744 (5)0.74496 (9)0.5774 (2)0.0189 (4)
H25A0.32830.76120.61440.023*
H25B0.63040.71650.65610.023*
C230.1879 (5)0.64342 (9)0.4973 (2)0.0174 (4)
C210.1618 (5)1.05536 (9)0.7083 (2)0.0172 (4)
C260.6149 (5)0.80440 (9)0.5328 (2)0.0181 (4)
H26A0.79020.78830.51630.022*
H26B0.47040.82740.44140.022*
C240.3189 (5)0.70327 (9)0.4523 (2)0.0204 (4)
H24A0.15900.73140.37480.025*
H24B0.46360.68820.41350.025*
C160.4997 (5)0.30820 (9)1.0471 (2)0.0213 (4)
H16A0.34130.29071.07470.026*
H16B0.62290.33491.12380.026*
C140.5064 (5)0.19536 (9)0.9533 (2)0.0201 (4)
H14A0.38590.17691.00420.024*
H14B0.36890.21530.85710.024*
C150.6933 (5)0.24963 (9)1.0374 (2)0.0251 (5)
H15A0.82210.23021.13550.030*
H15B0.82290.26590.98970.030*
C270.7086 (5)0.85301 (8)0.6451 (2)0.0173 (4)
C170.3590 (5)0.35270 (9)0.9092 (2)0.0202 (4)
O110.8391 (3)0.55165 (6)0.65370 (16)0.0223 (3)
O120.9358 (4)0.58730 (7)0.86881 (17)0.0259 (4)
N110.4277 (4)0.47053 (7)0.66306 (18)0.0187 (4)
H11A0.31170.44040.68300.028*
H11B0.56520.44900.63950.028*
H11C0.31260.50010.58820.028*
C120.5803 (5)0.50660 (9)0.7910 (2)0.0166 (4)
H12A0.68480.47400.87530.020*
H12B0.43110.53330.81110.020*
C110.8031 (5)0.55238 (8)0.7686 (2)0.0168 (4)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O230.0276 (9)0.0155 (7)0.0266 (9)0.0038 (6)0.0128 (7)0.0062 (5)
O250.0364 (10)0.0207 (7)0.0244 (9)0.0062 (6)0.0183 (8)0.0074 (5)
O260.0346 (10)0.0213 (7)0.0245 (9)0.0103 (6)0.0151 (8)0.0065 (6)
O210.0272 (9)0.0230 (7)0.0217 (8)0.0057 (6)0.0130 (7)0.0014 (6)
O220.0259 (9)0.0286 (8)0.0247 (9)0.0073 (6)0.0125 (7)0.0066 (6)
O130.0233 (9)0.0159 (6)0.0222 (8)0.0001 (5)0.0089 (7)0.0001 (5)
O240.0394 (10)0.0194 (7)0.0370 (10)0.0121 (7)0.0286 (9)0.0097 (6)
O160.0381 (11)0.0225 (7)0.0254 (9)0.0085 (6)0.0160 (8)0.0018 (6)
O140.0339 (10)0.0221 (7)0.0269 (9)0.0089 (6)0.0187 (8)0.0041 (6)
O150.0544 (12)0.0215 (7)0.0330 (10)0.0028 (7)0.0309 (9)0.0018 (6)
N210.0239 (10)0.0165 (8)0.0199 (9)0.0024 (6)0.0113 (8)0.0019 (6)
C220.0172 (11)0.0188 (9)0.0167 (10)0.0025 (7)0.0070 (8)0.0028 (7)
C130.0172 (11)0.0159 (8)0.0176 (11)0.0030 (7)0.0071 (9)0.0036 (7)
C250.0197 (11)0.0187 (9)0.0195 (10)0.0039 (7)0.0088 (9)0.0024 (7)
C230.0174 (11)0.0184 (9)0.0161 (10)0.0018 (7)0.0065 (9)0.0008 (7)
C210.0164 (11)0.0158 (9)0.0220 (11)0.0044 (7)0.0100 (9)0.0036 (7)
C260.0219 (11)0.0166 (9)0.0179 (10)0.0026 (7)0.0094 (9)0.0041 (7)
C240.0254 (12)0.0201 (9)0.0196 (11)0.0070 (8)0.0120 (10)0.0055 (7)
C160.0217 (12)0.0185 (9)0.0203 (11)0.0000 (8)0.0043 (9)0.0052 (7)
C140.0199 (11)0.0173 (9)0.0250 (11)0.0009 (7)0.0108 (9)0.0035 (7)
C150.0211 (12)0.0223 (10)0.0262 (12)0.0045 (8)0.0031 (10)0.0060 (8)
C270.0159 (10)0.0147 (8)0.0192 (11)0.0020 (7)0.0052 (9)0.0005 (7)
C170.0235 (12)0.0155 (9)0.0250 (12)0.0040 (8)0.0128 (10)0.0027 (7)
O110.0278 (9)0.0226 (7)0.0217 (8)0.0101 (6)0.0144 (7)0.0051 (5)
O120.0278 (9)0.0294 (8)0.0259 (9)0.0126 (6)0.0136 (7)0.0141 (6)
N110.0233 (10)0.0171 (8)0.0192 (9)0.0069 (7)0.0116 (8)0.0025 (6)
C120.0164 (11)0.0186 (9)0.0157 (10)0.0016 (7)0.0075 (8)0.0018 (7)
C110.0164 (10)0.0143 (8)0.0209 (11)0.0007 (7)0.0091 (9)0.0003 (7)
Geometric parameters (Å, º) top
O23—C231.228 (2)C25—H25B0.9900
O25—C271.214 (3)C23—C241.509 (3)
O26—C271.328 (2)C26—C271.506 (3)
O26—H260.8400C26—H26A0.9900
O21—C211.252 (3)C26—H26B0.9900
O22—C211.253 (2)C24—H24A0.9900
O13—C131.228 (2)C24—H24B0.9900
O24—C231.305 (3)C16—C171.504 (3)
O24—H240.8400C16—C151.529 (3)
O16—C171.331 (3)C16—H16A0.9900
O16—H160.8400C16—H16B0.9900
O14—C131.311 (2)C14—C151.537 (3)
O14—H140.8400C14—H14A0.9900
O15—C171.212 (3)C14—H14B0.9900
N21—C221.482 (3)C15—H15A0.9900
N21—H21A0.9100C15—H15B0.9900
N21—H21B0.9100O11—C111.251 (2)
N21—H21C0.9100O12—C111.256 (2)
C22—C211.520 (3)N11—C121.483 (3)
C22—H22A0.9900N11—H11A0.9100
C22—H22B0.9900N11—H11B0.9100
C13—C141.499 (3)N11—H11C0.9100
C25—C261.527 (3)C12—C111.525 (3)
C25—C241.534 (3)C12—H12A0.9900
C25—H25A0.9900C12—H12B0.9900
C27—O26—H26109.5C25—C24—H24B109.2
C23—O24—H24109.5H24A—C24—H24B107.9
C17—O16—H16109.5C17—C16—C15113.39 (18)
C13—O14—H14109.5C17—C16—H16A108.9
C22—N21—H21A109.5C15—C16—H16A108.9
C22—N21—H21B109.5C17—C16—H16B108.9
H21A—N21—H21B109.5C15—C16—H16B108.9
C22—N21—H21C109.5H16A—C16—H16B107.7
H21A—N21—H21C109.5C13—C14—C15111.32 (18)
H21B—N21—H21C109.5C13—C14—H14A109.4
N21—C22—C21112.08 (16)C15—C14—H14A109.4
N21—C22—H22A109.2C13—C14—H14B109.4
C21—C22—H22A109.2C15—C14—H14B109.4
N21—C22—H22B109.2H14A—C14—H14B108.0
C21—C22—H22B109.2C16—C15—C14112.01 (18)
H22A—C22—H22B107.9C16—C15—H15A109.2
O13—C13—O14122.14 (18)C14—C15—H15A109.2
O13—C13—C14123.87 (18)C16—C15—H15B109.2
O14—C13—C14113.97 (16)C14—C15—H15B109.2
C26—C25—C24112.14 (17)H15A—C15—H15B107.9
C26—C25—H25A109.2O25—C27—O26119.15 (18)
C24—C25—H25A109.2O25—C27—C26123.38 (17)
C26—C25—H25B109.2O26—C27—C26117.45 (18)
C24—C25—H25B109.2O15—C17—O16119.13 (18)
H25A—C25—H25B107.9O15—C17—C16123.97 (19)
O23—C23—O24122.57 (17)O16—C17—C16116.85 (18)
O23—C23—C24123.5 (2)C12—N11—H11A109.5
O24—C23—C24113.88 (17)C12—N11—H11B109.5
O21—C21—O22125.3 (2)H11A—N11—H11B109.5
O21—C21—C22117.76 (18)C12—N11—H11C109.5
O22—C21—C22116.92 (18)H11A—N11—H11C109.5
C27—C26—C25111.87 (17)H11B—N11—H11C109.5
C27—C26—H26A109.2N11—C12—C11111.48 (16)
C25—C26—H26A109.2N11—C12—H12A109.3
C27—C26—H26B109.2C11—C12—H12A109.3
C25—C26—H26B109.2N11—C12—H12B109.3
H26A—C26—H26B107.9C11—C12—H12B109.3
C23—C24—C25112.18 (17)H12A—C12—H12B108.0
C23—C24—H24A109.2O11—C11—O12125.87 (18)
C25—C24—H24A109.2O11—C11—C12117.66 (17)
C23—C24—H24B109.2O12—C11—C12116.47 (18)
N21—C22—C21—O213.4 (2)C17—C16—C15—C1474.9 (2)
N21—C22—C21—O22177.07 (17)C13—C14—C15—C16176.58 (18)
C24—C25—C26—C27167.68 (18)C25—C26—C27—O256.3 (3)
O23—C23—C24—C25142.6 (2)C25—C26—C27—O26175.11 (18)
O24—C23—C24—C2537.7 (3)C15—C16—C17—O153.7 (3)
C26—C25—C24—C23178.32 (18)C15—C16—C17—O16178.74 (18)
O13—C13—C14—C1598.0 (2)N11—C12—C11—O113.2 (2)
O14—C13—C14—C1580.7 (2)N11—C12—C11—O12177.22 (17)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O14—H14···O21i0.841.742.579 (2)178
O16—H16···O12ii0.841.742.567 (2)166
N11—H11A···O150.912.122.826 (2)133
N11—H11B···O23iii0.911.962.860 (2)168
N11—H11C···O230.912.102.967 (2)158
O24—H24···O11iv0.841.732.5655 (18)176
O26—H26···O22v0.841.732.552 (2)166
N21—H21A···O250.912.072.800 (2)137
N21—H21B···O13ii0.911.952.859 (2)172
N21—H21C···O13vi0.912.122.974 (2)156
Symmetry codes: (i) x+1, y1, z; (ii) x+1, y+1, z+2; (iii) x+1, y+1, z+1; (iv) x1, y, z; (v) x+1, y+2, z+1; (vi) x, y+1, z.
(150) Propane-1,3-dicarboxylic acid – Aminoethanoic acid (1/1) top
Crystal data top
C5H8O4·C2H5NO2Z = 4
Mr = 207.18F(000) = 440
Triclinic, P1Dx = 1.496 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 4.9021 (7) ÅCell parameters from 7886 reflections
b = 20.167 (3) Åθ = 2.1–29.6°
c = 10.1686 (15) ŵ = 0.13 mm1
α = 85.540 (11)°T = 150 K
β = 113.122 (10)°Prism, colourless
γ = 88.270 (11)°0.40 × 0.23 × 0.10 mm
V = 919.7 (2) Å3
Data collection top
STOE IPDS 2
diffractometer
2840 reflections with I > 2σ(I)
Plane graphite monochromatorRint = 0.040
Detector resolution: 6.67 pixels mm-1θmax = 29.2°, θmin = 2.0°
rotation method scansh = 65
10066 measured reflectionsk = 2727
4417 independent reflectionsl = 1313
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.039Hydrogen site location: difference Fourier map
wR(F2) = 0.077H-atom parameters constrained
S = 0.88 w = 1/[σ2(Fo2) + (0.0327P)2]
where P = (Fo2 + 2Fc2)/3
4417 reflections(Δ/σ)max = 0.001
259 parametersΔρmax = 0.21 e Å3
0 restraintsΔρmin = 0.20 e Å3
Crystal data top
C5H8O4·C2H5NO2γ = 88.270 (11)°
Mr = 207.18V = 919.7 (2) Å3
Triclinic, P1Z = 4
a = 4.9021 (7) ÅMo Kα radiation
b = 20.167 (3) ŵ = 0.13 mm1
c = 10.1686 (15) ÅT = 150 K
α = 85.540 (11)°0.40 × 0.23 × 0.10 mm
β = 113.122 (10)°
Data collection top
STOE IPDS 2
diffractometer
2840 reflections with I > 2σ(I)
10066 measured reflectionsRint = 0.040
4417 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0390 restraints
wR(F2) = 0.077H-atom parameters constrained
S = 0.88Δρmax = 0.21 e Å3
4417 reflectionsΔρmin = 0.20 e Å3
259 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
O230.1874 (3)0.58914 (5)0.45078 (12)0.0203 (3)
O250.6546 (3)0.84812 (5)0.75242 (13)0.0223 (3)
O260.8549 (3)0.90476 (5)0.62412 (13)0.0228 (3)
H260.87550.90280.54630.034*
O210.1276 (3)1.05551 (5)0.82410 (12)0.0206 (2)
O220.0071 (3)1.09063 (5)0.59387 (13)0.0232 (3)
O130.7716 (3)0.08766 (5)1.01507 (12)0.0190 (2)
O240.0737 (3)0.65465 (5)0.59016 (14)0.0243 (3)
H240.00570.62040.60650.036*
O160.1809 (3)0.40439 (5)0.90802 (13)0.0255 (3)
H160.17070.40400.98860.038*
O140.7880 (3)0.15347 (5)0.83294 (13)0.0232 (3)
H140.88720.12010.82660.035*
O150.4039 (3)0.34547 (5)0.80201 (14)0.0290 (3)
N210.5793 (3)0.97142 (6)0.84584 (14)0.0179 (3)
H21A0.70370.93940.83640.027*
H21B0.45310.95200.88070.027*
H21C0.68791.00020.90760.027*
C220.4054 (4)1.00833 (7)0.70355 (17)0.0160 (3)
H22A0.31510.97610.63250.019*
H22B0.54071.03430.67180.019*
C130.6982 (4)0.14032 (7)0.93729 (16)0.0157 (3)
C250.4768 (4)0.74507 (7)0.57750 (17)0.0168 (3)
H25A0.33070.76130.61460.020*
H25B0.63280.71640.65620.020*
C230.1886 (4)0.64362 (7)0.49715 (17)0.0160 (3)
C210.1611 (4)1.05547 (7)0.70778 (17)0.0155 (3)
C260.6178 (4)0.80449 (7)0.53373 (17)0.0173 (3)
H26A0.79410.78840.51780.021*
H26B0.47380.82750.44190.021*
C240.3205 (4)0.70337 (7)0.45289 (18)0.0197 (3)
H24A0.16060.73170.37530.024*
H24B0.46530.68820.41400.024*
C160.4986 (4)0.30835 (7)1.04724 (18)0.0202 (3)
H16A0.34020.29111.07520.024*
H16B0.62300.33511.12370.024*
C140.5041 (4)0.19555 (7)0.95314 (18)0.0186 (3)
H14A0.38310.17711.00380.022*
H14B0.36680.21550.85670.022*
C150.6904 (4)0.24967 (8)1.03731 (19)0.0233 (4)
H15A0.81910.23011.13550.028*
H15B0.82080.26590.98980.028*
C270.7102 (4)0.85318 (7)0.64558 (17)0.0159 (3)
C170.3573 (4)0.35294 (7)0.90864 (18)0.0196 (3)
O110.8392 (3)0.55172 (5)0.65368 (12)0.0202 (2)
O120.9381 (3)0.58701 (5)0.86944 (13)0.0231 (3)
N110.4275 (3)0.47064 (6)0.66303 (14)0.0176 (3)
H11A0.31370.43990.68340.026*
H11B0.56530.44970.63860.026*
H11C0.30970.50020.58850.026*
C120.5797 (4)0.50657 (7)0.79090 (17)0.0161 (3)
H12A0.68370.47380.87530.019*
H12B0.43010.53340.81080.019*
C110.8035 (3)0.55227 (7)0.76915 (17)0.0149 (3)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O230.0243 (7)0.0161 (5)0.0228 (6)0.0029 (4)0.0112 (5)0.0050 (4)
O250.0321 (7)0.0192 (5)0.0213 (6)0.0043 (5)0.0160 (6)0.0054 (4)
O260.0321 (7)0.0192 (5)0.0223 (6)0.0088 (5)0.0151 (6)0.0058 (4)
O210.0226 (6)0.0212 (5)0.0190 (6)0.0041 (4)0.0100 (5)0.0014 (4)
O220.0222 (7)0.0267 (6)0.0207 (6)0.0051 (5)0.0102 (5)0.0047 (4)
O130.0216 (6)0.0154 (5)0.0199 (6)0.0002 (4)0.0083 (5)0.0004 (4)
O240.0339 (7)0.0184 (5)0.0329 (7)0.0106 (5)0.0247 (6)0.0090 (5)
O160.0354 (8)0.0208 (6)0.0229 (7)0.0077 (5)0.0155 (6)0.0011 (4)
O140.0309 (7)0.0200 (5)0.0229 (6)0.0071 (5)0.0168 (6)0.0035 (4)
O150.0480 (9)0.0201 (6)0.0300 (7)0.0020 (5)0.0281 (7)0.0010 (5)
N210.0205 (7)0.0163 (6)0.0179 (7)0.0030 (5)0.0091 (6)0.0017 (5)
C220.0165 (8)0.0170 (7)0.0159 (7)0.0020 (5)0.0076 (6)0.0025 (5)
C130.0153 (8)0.0151 (7)0.0159 (8)0.0027 (6)0.0047 (7)0.0038 (5)
C250.0205 (8)0.0165 (7)0.0163 (8)0.0041 (6)0.0096 (7)0.0037 (5)
C230.0145 (8)0.0174 (7)0.0150 (8)0.0013 (5)0.0046 (6)0.0017 (5)
C210.0151 (8)0.0146 (7)0.0182 (8)0.0037 (5)0.0078 (6)0.0029 (5)
C260.0213 (8)0.0161 (7)0.0168 (8)0.0031 (6)0.0095 (7)0.0030 (5)
C240.0249 (9)0.0193 (7)0.0178 (8)0.0065 (6)0.0108 (7)0.0047 (6)
C160.0221 (9)0.0162 (7)0.0213 (8)0.0001 (6)0.0072 (7)0.0045 (6)
C140.0190 (8)0.0155 (7)0.0223 (8)0.0009 (6)0.0091 (7)0.0027 (6)
C150.0185 (9)0.0206 (8)0.0252 (9)0.0031 (6)0.0025 (7)0.0051 (6)
C270.0153 (8)0.0128 (7)0.0184 (8)0.0013 (5)0.0056 (6)0.0003 (5)
C170.0247 (9)0.0143 (7)0.0241 (9)0.0038 (6)0.0139 (7)0.0031 (6)
O110.0243 (7)0.0207 (5)0.0199 (6)0.0086 (4)0.0124 (5)0.0043 (4)
O120.0247 (7)0.0261 (6)0.0233 (6)0.0103 (5)0.0123 (5)0.0117 (4)
N110.0214 (7)0.0163 (6)0.0185 (7)0.0063 (5)0.0110 (6)0.0022 (5)
C120.0157 (8)0.0176 (7)0.0164 (7)0.0015 (6)0.0078 (6)0.0023 (5)
C110.0136 (8)0.0136 (7)0.0185 (8)0.0011 (5)0.0077 (6)0.0009 (5)
Geometric parameters (Å, º) top
O23—C231.2280 (18)C25—H25B0.9900
O25—C271.2176 (19)C23—C241.505 (2)
O26—C271.3279 (18)C26—C271.503 (2)
O26—H260.8400C26—H26A0.9900
O21—C211.2563 (19)C26—H26B0.9900
O22—C211.2518 (19)C24—H24A0.9900
O13—C131.2271 (17)C24—H24B0.9900
O24—C231.3056 (19)C16—C171.508 (2)
O24—H240.8400C16—C151.523 (2)
O16—C171.328 (2)C16—H16A0.9900
O16—H160.8400C16—H16B0.9900
O14—C131.3117 (19)C14—C151.533 (2)
O14—H140.8400C14—H14A0.9900
O15—C171.212 (2)C14—H14B0.9900
N21—C221.483 (2)C15—H15A0.9900
N21—H21A0.9100C15—H15B0.9900
N21—H21B0.9100O11—C111.2541 (19)
N21—H21C0.9100O12—C111.2557 (19)
C22—C211.523 (2)N11—C121.480 (2)
C22—H22A0.9900N11—H11A0.9100
C22—H22B0.9900N11—H11B0.9100
C13—C141.502 (2)N11—H11C0.9100
C25—C261.523 (2)C12—C111.524 (2)
C25—C241.530 (2)C12—H12A0.9900
C25—H25A0.9900C12—H12B0.9900
C27—O26—H26109.5C25—C24—H24B109.1
C23—O24—H24109.5H24A—C24—H24B107.8
C17—O16—H16109.5C17—C16—C15113.27 (14)
C13—O14—H14109.5C17—C16—H16A108.9
C22—N21—H21A109.5C15—C16—H16A108.9
C22—N21—H21B109.5C17—C16—H16B108.9
H21A—N21—H21B109.5C15—C16—H16B108.9
C22—N21—H21C109.5H16A—C16—H16B107.7
H21A—N21—H21C109.5C13—C14—C15111.24 (14)
H21B—N21—H21C109.5C13—C14—H14A109.4
N21—C22—C21111.96 (13)C15—C14—H14A109.4
N21—C22—H22A109.2C13—C14—H14B109.4
C21—C22—H22A109.2C15—C14—H14B109.4
N21—C22—H22B109.2H14A—C14—H14B108.0
C21—C22—H22B109.2C16—C15—C14112.36 (14)
H22A—C22—H22B107.9C16—C15—H15A109.1
O13—C13—O14122.15 (14)C14—C15—H15A109.1
O13—C13—C14123.87 (14)C16—C15—H15B109.1
O14—C13—C14113.97 (12)C14—C15—H15B109.1
C26—C25—C24112.64 (13)H15A—C15—H15B107.9
C26—C25—H25A109.1O25—C27—O26119.01 (14)
C24—C25—H25A109.1O25—C27—C26123.29 (13)
C26—C25—H25B109.1O26—C27—C26117.69 (14)
C24—C25—H25B109.1O15—C17—O16119.42 (14)
H25A—C25—H25B107.8O15—C17—C16123.78 (15)
O23—C23—O24122.42 (13)O16—C17—C16116.75 (14)
O23—C23—C24123.66 (15)C12—N11—H11A109.5
O24—C23—C24113.92 (13)C12—N11—H11B109.5
O22—C21—O21125.27 (15)H11A—N11—H11B109.5
O22—C21—C22117.00 (14)C12—N11—H11C109.5
O21—C21—C22117.72 (13)H11A—N11—H11C109.5
C27—C26—C25112.15 (13)H11B—N11—H11C109.5
C27—C26—H26A109.2N11—C12—C11111.57 (13)
C25—C26—H26A109.2N11—C12—H12A109.3
C27—C26—H26B109.2C11—C12—H12A109.3
C25—C26—H26B109.2N11—C12—H12B109.3
H26A—C26—H26B107.9C11—C12—H12B109.3
C23—C24—C25112.62 (13)H12A—C12—H12B108.0
C23—C24—H24A109.1O11—C11—O12125.60 (14)
C25—C24—H24A109.1O11—C11—C12117.52 (13)
C23—C24—H24B109.1O12—C11—C12116.87 (14)
N21—C22—C21—O22177.79 (13)C17—C16—C15—C1474.51 (18)
N21—C22—C21—O212.99 (18)C13—C14—C15—C16176.54 (14)
C24—C25—C26—C27167.31 (14)C25—C26—C27—O255.9 (2)
O23—C23—C24—C25142.48 (16)C25—C26—C27—O26175.38 (14)
O24—C23—C24—C2537.6 (2)C15—C16—C17—O154.0 (2)
C26—C25—C24—C23178.41 (14)C15—C16—C17—O16178.47 (14)
O13—C13—C14—C1597.87 (18)N11—C12—C11—O112.93 (19)
O14—C13—C14—C1581.22 (17)N11—C12—C11—O12177.57 (13)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O14—H14···O21i0.841.742.5745 (16)174
O16—H16···O12ii0.841.742.5658 (17)166
N11—H11A···O150.912.112.8238 (16)135
N11—H11B···O23iii0.911.962.8554 (18)169
N11—H11C···O230.912.102.9644 (17)158
O24—H24···O11iv0.841.722.5626 (14)176
O26—H26···O22v0.841.732.5550 (16)166
N21—H21A···O250.912.072.7944 (17)136
N21—H21B···O13ii0.911.952.8551 (17)171
N21—H21C···O13vi0.912.112.9719 (18)157
Symmetry codes: (i) x+1, y1, z; (ii) x+1, y+1, z+2; (iii) x+1, y+1, z+1; (iv) x1, y, z; (v) x+1, y+2, z+1; (vi) x, y+1, z.
(125) Propane-1,3-dicarboxylic acid – Aminoethanoic acid (1/1) top
Crystal data top
C5H8O4·C2H5NO2Z = 4
Mr = 207.18F(000) = 440
Triclinic, P1Dx = 1.501 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 4.8952 (6) ÅCell parameters from 8370 reflections
b = 20.151 (3) Åθ = 2.1–29.6°
c = 10.1585 (13) ŵ = 0.13 mm1
α = 85.518 (11)°T = 125 K
β = 113.088 (9)°Prism, colourless
γ = 88.264 (11)°0.40 × 0.23 × 0.10 mm
V = 916.9 (2) Å3
Data collection top
STOE IPDS 2
diffractometer
2935 reflections with I > 2σ(I)
Plane graphite monochromatorRint = 0.038
Detector resolution: 6.67 pixels mm-1θmax = 29.2°, θmin = 2.0°
rotation method scansh = 65
9997 measured reflectionsk = 2727
4391 independent reflectionsl = 1313
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.039Hydrogen site location: difference Fourier map
wR(F2) = 0.075H-atom parameters constrained
S = 0.90 w = 1/[σ2(Fo2) + (0.0331P)2]
where P = (Fo2 + 2Fc2)/3
4391 reflections(Δ/σ)max = 0.001
259 parametersΔρmax = 0.23 e Å3
0 restraintsΔρmin = 0.20 e Å3
Crystal data top
C5H8O4·C2H5NO2γ = 88.264 (11)°
Mr = 207.18V = 916.9 (2) Å3
Triclinic, P1Z = 4
a = 4.8952 (6) ÅMo Kα radiation
b = 20.151 (3) ŵ = 0.13 mm1
c = 10.1585 (13) ÅT = 125 K
α = 85.518 (11)°0.40 × 0.23 × 0.10 mm
β = 113.088 (9)°
Data collection top
STOE IPDS 2
diffractometer
2935 reflections with I > 2σ(I)
9997 measured reflectionsRint = 0.038
4391 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0390 restraints
wR(F2) = 0.075H-atom parameters constrained
S = 0.90Δρmax = 0.23 e Å3
4391 reflectionsΔρmin = 0.20 e Å3
259 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
O230.1879 (3)0.58911 (5)0.45029 (12)0.0173 (2)
O250.6557 (3)0.84815 (5)0.75302 (12)0.0188 (2)
O260.8564 (3)0.90507 (5)0.62477 (12)0.0192 (2)
H260.88120.90260.54800.029*
O210.1277 (3)1.05564 (5)0.82429 (12)0.0176 (2)
O220.0047 (3)1.09042 (5)0.59311 (12)0.0196 (2)
O130.7715 (3)0.08758 (5)1.01545 (12)0.0163 (2)
O240.0747 (3)0.65473 (5)0.59045 (13)0.0208 (3)
H240.00370.62040.60740.031*
O160.1792 (3)0.40479 (5)0.90748 (13)0.0218 (3)
H160.16930.40460.98820.033*
O140.7857 (3)0.15346 (5)0.83223 (12)0.0199 (2)
H140.88850.12040.82710.030*
O150.4030 (3)0.34543 (5)0.80176 (13)0.0248 (3)
N210.5804 (3)0.97171 (6)0.84609 (14)0.0152 (3)
H21A0.70240.93910.83660.023*
H21B0.45420.95300.88210.023*
H21C0.69171.00050.90710.023*
C220.4059 (3)1.00839 (7)0.70358 (16)0.0137 (3)
H22A0.31640.97600.63270.016*
H22B0.54081.03450.67170.016*
C130.6967 (3)0.14032 (7)0.93711 (16)0.0133 (3)
C250.4781 (4)0.74509 (7)0.57783 (16)0.0151 (3)
H25A0.33150.76130.61490.018*
H25B0.63440.71640.65660.018*
C230.1894 (3)0.64365 (7)0.49710 (16)0.0142 (3)
C210.1601 (3)1.05532 (7)0.70766 (16)0.0136 (3)
C260.6191 (4)0.80469 (7)0.53377 (16)0.0149 (3)
H26A0.79550.78860.51760.018*
H26B0.47480.82780.44210.018*
C240.3224 (4)0.70350 (7)0.45288 (17)0.0168 (3)
H24A0.16280.73190.37510.020*
H24B0.46780.68820.41420.020*
C160.4975 (4)0.30849 (7)1.04730 (17)0.0172 (3)
H16A0.33870.29141.07540.021*
H16B0.62230.33521.12370.021*
C140.5022 (4)0.19550 (7)0.95298 (17)0.0158 (3)
H14A0.38070.17701.00350.019*
H14B0.36510.21560.85650.019*
C150.6889 (4)0.24962 (7)1.03760 (18)0.0198 (3)
H15A0.81680.22991.13590.024*
H15B0.82040.26580.99040.024*
C270.7117 (3)0.85331 (7)0.64638 (16)0.0139 (3)
C170.3562 (4)0.35311 (7)0.90847 (17)0.0166 (3)
O110.8392 (3)0.55171 (5)0.65348 (12)0.0172 (2)
O120.9398 (3)0.58671 (5)0.86977 (12)0.0197 (2)
N110.4250 (3)0.47085 (6)0.66249 (14)0.0150 (3)
H11A0.30730.44090.68210.023*
H11B0.56250.44900.63900.023*
H11C0.31090.50070.58750.023*
C120.5791 (3)0.50673 (7)0.79119 (16)0.0136 (3)
H12A0.68230.47390.87560.016*
H12B0.43010.53380.81110.016*
C110.8048 (3)0.55207 (7)0.76937 (16)0.0135 (3)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O230.0199 (6)0.0139 (5)0.0194 (6)0.0023 (4)0.0087 (5)0.0043 (4)
O250.0263 (6)0.0168 (5)0.0176 (6)0.0036 (4)0.0126 (5)0.0041 (4)
O260.0264 (7)0.0163 (5)0.0197 (6)0.0069 (4)0.0133 (5)0.0050 (4)
O210.0199 (6)0.0188 (5)0.0159 (6)0.0028 (4)0.0092 (5)0.0012 (4)
O220.0188 (6)0.0216 (5)0.0180 (6)0.0037 (4)0.0085 (5)0.0041 (4)
O130.0182 (6)0.0130 (5)0.0170 (6)0.0001 (4)0.0066 (5)0.0007 (4)
O240.0291 (7)0.0156 (5)0.0282 (6)0.0091 (5)0.0210 (6)0.0072 (4)
O160.0301 (7)0.0175 (5)0.0195 (6)0.0063 (4)0.0126 (6)0.0007 (4)
O140.0268 (7)0.0164 (5)0.0201 (6)0.0056 (4)0.0144 (5)0.0023 (4)
O150.0412 (8)0.0178 (5)0.0246 (6)0.0015 (5)0.0238 (6)0.0006 (4)
N210.0173 (7)0.0144 (6)0.0148 (6)0.0023 (5)0.0075 (5)0.0014 (4)
C220.0138 (7)0.0151 (6)0.0123 (7)0.0007 (5)0.0052 (6)0.0016 (5)
C130.0129 (7)0.0128 (6)0.0141 (7)0.0027 (5)0.0049 (6)0.0033 (5)
C250.0183 (8)0.0149 (7)0.0152 (7)0.0040 (5)0.0094 (6)0.0035 (5)
C230.0117 (7)0.0160 (7)0.0135 (7)0.0008 (5)0.0036 (6)0.0014 (5)
C210.0129 (7)0.0127 (6)0.0168 (7)0.0040 (5)0.0069 (6)0.0032 (5)
C260.0178 (8)0.0144 (7)0.0141 (7)0.0022 (5)0.0080 (6)0.0016 (5)
C240.0210 (8)0.0157 (7)0.0164 (7)0.0050 (6)0.0099 (7)0.0033 (5)
C160.0186 (8)0.0147 (7)0.0172 (8)0.0004 (5)0.0054 (6)0.0047 (5)
C140.0159 (8)0.0140 (7)0.0182 (8)0.0001 (5)0.0077 (6)0.0016 (5)
C150.0161 (8)0.0180 (7)0.0206 (8)0.0020 (6)0.0019 (7)0.0048 (6)
C270.0124 (7)0.0115 (6)0.0152 (7)0.0012 (5)0.0031 (6)0.0007 (5)
C170.0206 (8)0.0120 (6)0.0204 (8)0.0046 (5)0.0109 (7)0.0033 (5)
O110.0210 (6)0.0179 (5)0.0169 (6)0.0071 (4)0.0111 (5)0.0041 (4)
O120.0200 (6)0.0229 (5)0.0197 (6)0.0079 (4)0.0097 (5)0.0094 (4)
N110.0182 (7)0.0139 (6)0.0156 (6)0.0048 (5)0.0091 (5)0.0016 (4)
C120.0131 (7)0.0145 (6)0.0137 (7)0.0016 (5)0.0058 (6)0.0021 (5)
C110.0130 (7)0.0119 (6)0.0161 (7)0.0004 (5)0.0064 (6)0.0010 (5)
Geometric parameters (Å, º) top
O23—C231.2303 (18)C25—H25B0.9900
O25—C271.2150 (19)C23—C241.5073 (19)
O26—C271.3299 (17)C26—C271.506 (2)
O26—H260.8400C26—H26A0.9900
O21—C211.2561 (19)C26—H26B0.9900
O22—C211.2561 (18)C24—H24A0.9900
O13—C131.2297 (17)C24—H24B0.9900
O24—C231.3069 (19)C16—C171.508 (2)
O24—H240.8400C16—C151.522 (2)
O16—C171.3315 (19)C16—H16A0.9900
O16—H160.8400C16—H16B0.9900
O14—C131.3122 (18)C14—C151.534 (2)
O14—H140.8400C14—H14A0.9900
O15—C171.213 (2)C14—H14B0.9900
N21—C221.4820 (19)C15—H15A0.9900
N21—H21A0.9100C15—H15B0.9900
N21—H21B0.9100O11—C111.2535 (18)
N21—H21C0.9100O12—C111.2549 (18)
C22—C211.523 (2)N11—C121.4860 (19)
C22—H22A0.9900N11—H11A0.9100
C22—H22B0.9900N11—H11B0.9100
C13—C141.501 (2)N11—H11C0.9100
C25—C261.5256 (19)C12—C111.525 (2)
C25—C241.530 (2)C12—H12A0.9900
C25—H25A0.9900C12—H12B0.9900
C27—O26—H26109.5C25—C24—H24B109.1
C23—O24—H24109.5H24A—C24—H24B107.8
C17—O16—H16109.5C17—C16—C15113.34 (13)
C13—O14—H14109.5C17—C16—H16A108.9
C22—N21—H21A109.5C15—C16—H16A108.9
C22—N21—H21B109.5C17—C16—H16B108.9
H21A—N21—H21B109.5C15—C16—H16B108.9
C22—N21—H21C109.5H16A—C16—H16B107.7
H21A—N21—H21C109.5C13—C14—C15111.18 (13)
H21B—N21—H21C109.5C13—C14—H14A109.4
N21—C22—C21111.89 (12)C15—C14—H14A109.4
N21—C22—H22A109.2C13—C14—H14B109.4
C21—C22—H22A109.2C15—C14—H14B109.4
N21—C22—H22B109.2H14A—C14—H14B108.0
C21—C22—H22B109.2C16—C15—C14112.47 (13)
H22A—C22—H22B107.9C16—C15—H15A109.1
O13—C13—O14122.16 (14)C14—C15—H15A109.1
O13—C13—C14123.89 (13)C16—C15—H15B109.1
O14—C13—C14113.94 (12)C14—C15—H15B109.1
C26—C25—C24112.40 (12)H15A—C15—H15B107.8
C26—C25—H25A109.1O25—C27—O26119.09 (13)
C24—C25—H25A109.1O25—C27—C26123.40 (13)
C26—C25—H25B109.1O26—C27—C26117.50 (13)
C24—C25—H25B109.1O15—C17—O16119.43 (14)
H25A—C25—H25B107.9O15—C17—C16123.68 (14)
O23—C23—O24122.54 (13)O16—C17—C16116.84 (13)
O23—C23—C24123.56 (15)C12—N11—H11A109.5
O24—C23—C24113.90 (13)C12—N11—H11B109.5
O22—C21—O21125.25 (15)H11A—N11—H11B109.5
O22—C21—C22117.00 (13)C12—N11—H11C109.5
O21—C21—C22117.75 (13)H11A—N11—H11C109.5
C27—C26—C25111.91 (12)H11B—N11—H11C109.5
C27—C26—H26A109.2N11—C12—C11111.46 (12)
C25—C26—H26A109.2N11—C12—H12A109.3
C27—C26—H26B109.2C11—C12—H12A109.3
C25—C26—H26B109.2N11—C12—H12B109.3
H26A—C26—H26B107.9C11—C12—H12B109.3
C23—C24—C25112.47 (13)H12A—C12—H12B108.0
C23—C24—H24A109.1O11—C11—O12125.71 (14)
C25—C24—H24A109.1O11—C11—C12117.59 (13)
C23—C24—H24B109.1O12—C11—C12116.70 (13)
N21—C22—C21—O22177.84 (12)C17—C16—C15—C1474.23 (17)
N21—C22—C21—O212.58 (18)C13—C14—C15—C16176.32 (13)
C24—C25—C26—C27167.46 (13)C25—C26—C27—O256.1 (2)
O23—C23—C24—C25142.69 (16)C25—C26—C27—O26175.42 (13)
O24—C23—C24—C2537.30 (19)C15—C16—C17—O154.1 (2)
C26—C25—C24—C23178.60 (13)C15—C16—C17—O16178.32 (13)
O13—C13—C14—C1597.45 (17)N11—C12—C11—O112.49 (18)
O14—C13—C14—C1581.62 (16)N11—C12—C11—O12177.39 (13)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O14—H14···O21i0.841.742.5739 (16)175
O16—H16···O12ii0.841.742.5644 (16)166
N11—H11A···O150.912.132.8245 (15)133
N11—H11B···O23iii0.911.962.8537 (18)168
N11—H11C···O230.912.092.9564 (17)159
O24—H24···O11iv0.841.722.5623 (14)176
O26—H26···O22v0.841.732.5539 (16)167
N21—H21A···O250.912.062.7956 (17)137
N21—H21B···O13ii0.911.952.8522 (17)172
N21—H21C···O13vi0.912.112.9639 (17)156
Symmetry codes: (i) x+1, y1, z; (ii) x+1, y+1, z+2; (iii) x+1, y+1, z+1; (iv) x1, y, z; (v) x+1, y+2, z+1; (vi) x, y+1, z.
(100) Propane-1,3-dicarboxylic acid – Aminoethanoic acid (1/1) top
Crystal data top
C5H8O4·C2H5NO2Z = 4
Mr = 207.18F(000) = 440
Triclinic, P1Dx = 1.505 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 4.8884 (7) ÅCell parameters from 8917 reflections
b = 20.136 (3) Åθ = 2.1–29.6°
c = 10.1518 (15) ŵ = 0.13 mm1
α = 85.486 (13)°T = 100 K
β = 113.065 (10)°Prism, colourless
γ = 88.263 (12)°0.40 × 0.23 × 0.10 mm
V = 914.5 (2) Å3
Data collection top
STOE IPDS 2
diffractometer
2766 reflections with I > 2σ(I)
Plane graphite monochromatorRint = 0.052
Detector resolution: 6.67 pixels mm-1θmax = 29.2°, θmin = 2.0°
rotation method scansh = 65
8816 measured reflectionsk = 2727
4247 independent reflectionsl = 1313
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.053Hydrogen site location: difference Fourier map
wR(F2) = 0.097H-atom parameters constrained
S = 0.98 w = 1/[σ2(Fo2) + (0.0367P)2]
where P = (Fo2 + 2Fc2)/3
4247 reflections(Δ/σ)max = 0.001
259 parametersΔρmax = 0.31 e Å3
0 restraintsΔρmin = 0.29 e Å3
Crystal data top
C5H8O4·C2H5NO2γ = 88.263 (12)°
Mr = 207.18V = 914.5 (2) Å3
Triclinic, P1Z = 4
a = 4.8884 (7) ÅMo Kα radiation
b = 20.136 (3) ŵ = 0.13 mm1
c = 10.1518 (15) ÅT = 100 K
α = 85.486 (13)°0.40 × 0.23 × 0.10 mm
β = 113.065 (10)°
Data collection top
STOE IPDS 2
diffractometer
2766 reflections with I > 2σ(I)
8816 measured reflectionsRint = 0.052
4247 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0530 restraints
wR(F2) = 0.097H-atom parameters constrained
S = 0.98Δρmax = 0.31 e Å3
4247 reflectionsΔρmin = 0.29 e Å3
259 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
O230.1875 (4)0.58907 (6)0.44968 (16)0.0138 (3)
O250.6555 (4)0.84827 (7)0.75344 (17)0.0154 (3)
O260.8581 (4)0.90525 (7)0.62556 (17)0.0151 (3)
H260.89610.90120.55270.023*
O210.1280 (4)1.05580 (7)0.82434 (16)0.0145 (3)
O220.0018 (4)1.09019 (7)0.59227 (17)0.0161 (3)
O130.7712 (3)0.08755 (6)1.01603 (16)0.0129 (3)
O240.0754 (4)0.65477 (7)0.59062 (18)0.0164 (3)
H240.00830.61960.61250.025*
O160.1782 (4)0.40501 (7)0.90676 (17)0.0170 (3)
H160.17370.40560.98850.025*
O140.7839 (4)0.15336 (7)0.83151 (17)0.0159 (3)
H140.89160.12080.82820.024*
O150.4030 (4)0.34543 (7)0.80174 (18)0.0197 (4)
N210.5811 (4)0.97199 (8)0.84592 (19)0.0124 (4)
H21A0.70740.94020.83690.019*
H21B0.45520.95220.88090.019*
H21C0.68811.00110.90750.019*
C220.4058 (5)1.00861 (9)0.7031 (2)0.0107 (4)
H22A0.31680.97610.63240.013*
H22B0.54061.03480.67100.013*
C130.6952 (5)0.14024 (9)0.9368 (2)0.0105 (4)
C250.4806 (5)0.74504 (9)0.5787 (2)0.0114 (4)
H25A0.33430.76100.61620.014*
H25B0.63760.71630.65700.014*
C230.1899 (5)0.64358 (9)0.4969 (2)0.0111 (4)
C210.1586 (5)1.05554 (9)0.7067 (2)0.0104 (4)
C260.6206 (5)0.80486 (9)0.5342 (2)0.0117 (4)
H26A0.79770.78900.51820.014*
H26B0.47580.82790.44240.014*
C240.3238 (5)0.70367 (9)0.4524 (2)0.0129 (4)
H24A0.16430.73220.37480.015*
H24B0.46930.68840.41360.015*
C160.4952 (5)0.30859 (9)1.0473 (2)0.0133 (4)
H16A0.33550.29151.07490.016*
H16B0.61940.33541.12380.016*
C140.5003 (5)0.19553 (9)0.9527 (2)0.0120 (4)
H14A0.37810.17701.00300.014*
H14B0.36360.21580.85620.014*
C150.6883 (5)0.24948 (10)1.0379 (2)0.0158 (4)
H15A0.81560.22961.13630.019*
H15B0.82060.26560.99110.019*
C270.7122 (5)0.85358 (9)0.6466 (2)0.0106 (4)
C170.3553 (5)0.35312 (9)0.9077 (2)0.0123 (4)
O110.8386 (4)0.55177 (7)0.65326 (16)0.0139 (3)
O120.9420 (4)0.58647 (7)0.87026 (17)0.0158 (3)
N110.4247 (4)0.47105 (8)0.66252 (19)0.0123 (4)
H11A0.30450.44160.68170.018*
H11B0.56230.44860.64000.018*
H11C0.31290.50100.58710.018*
C120.5787 (5)0.50689 (9)0.7909 (2)0.0106 (4)
H12A0.68160.47400.87540.013*
H12B0.42950.53410.81070.013*
C110.8053 (5)0.55222 (9)0.7695 (2)0.0102 (4)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O230.0166 (8)0.0109 (7)0.0153 (8)0.0032 (5)0.0071 (7)0.0045 (5)
O250.0215 (9)0.0136 (7)0.0153 (8)0.0030 (6)0.0113 (7)0.0037 (5)
O260.0203 (9)0.0134 (7)0.0149 (8)0.0055 (6)0.0099 (7)0.0037 (5)
O210.0166 (8)0.0154 (7)0.0132 (8)0.0024 (6)0.0080 (7)0.0008 (5)
O220.0156 (8)0.0177 (7)0.0153 (8)0.0030 (6)0.0074 (7)0.0022 (5)
O130.0139 (8)0.0104 (6)0.0135 (8)0.0001 (5)0.0046 (7)0.0004 (5)
O240.0226 (9)0.0125 (7)0.0226 (9)0.0079 (6)0.0166 (7)0.0061 (6)
O160.0244 (10)0.0142 (7)0.0147 (8)0.0048 (6)0.0109 (7)0.0001 (5)
O140.0214 (9)0.0119 (7)0.0172 (8)0.0045 (6)0.0118 (7)0.0027 (5)
O150.0315 (10)0.0133 (7)0.0207 (9)0.0019 (6)0.0180 (8)0.0007 (6)
N210.0146 (9)0.0100 (7)0.0131 (9)0.0019 (6)0.0065 (8)0.0006 (6)
C220.0121 (10)0.0113 (9)0.0108 (10)0.0008 (7)0.0066 (8)0.0014 (7)
C130.0096 (10)0.0101 (8)0.0116 (10)0.0024 (7)0.0035 (9)0.0035 (7)
C250.0100 (10)0.0134 (9)0.0110 (10)0.0022 (7)0.0042 (8)0.0020 (7)
C230.0090 (10)0.0135 (9)0.0098 (10)0.0002 (7)0.0028 (8)0.0011 (7)
C210.0090 (10)0.0095 (8)0.0142 (10)0.0033 (7)0.0057 (9)0.0017 (7)
C260.0145 (11)0.0097 (8)0.0130 (10)0.0018 (7)0.0075 (9)0.0025 (7)
C240.0157 (11)0.0130 (9)0.0120 (10)0.0038 (7)0.0070 (9)0.0030 (7)
C160.0135 (11)0.0112 (9)0.0128 (10)0.0002 (7)0.0024 (9)0.0030 (7)
C140.0144 (11)0.0101 (9)0.0132 (10)0.0001 (7)0.0074 (9)0.0012 (7)
C150.0128 (11)0.0155 (9)0.0157 (11)0.0020 (8)0.0018 (9)0.0038 (7)
C270.0087 (10)0.0091 (8)0.0115 (10)0.0016 (7)0.0018 (8)0.0002 (7)
C170.0127 (11)0.0094 (9)0.0155 (11)0.0032 (7)0.0063 (9)0.0017 (7)
O110.0169 (9)0.0139 (7)0.0136 (8)0.0050 (6)0.0083 (7)0.0033 (5)
O120.0162 (8)0.0182 (7)0.0156 (8)0.0067 (6)0.0075 (7)0.0079 (6)
N110.0159 (9)0.0116 (8)0.0123 (9)0.0040 (6)0.0082 (8)0.0016 (6)
C120.0121 (11)0.0117 (9)0.0097 (10)0.0017 (7)0.0058 (8)0.0020 (7)
C110.0092 (10)0.0092 (8)0.0137 (10)0.0011 (7)0.0061 (8)0.0004 (7)
Geometric parameters (Å, º) top
O23—C231.230 (2)C25—H25B0.9900
O25—C271.218 (3)C23—C241.514 (3)
O26—C271.329 (2)C26—C271.506 (3)
O26—H260.8400C26—H26A0.9900
O21—C211.261 (3)C26—H26B0.9900
O22—C211.251 (3)C24—H24A0.9900
O13—C131.232 (2)C24—H24B0.9900
O24—C231.309 (3)C16—C171.511 (3)
O24—H240.8400C16—C151.528 (3)
O16—C171.334 (3)C16—H16A0.9900
O16—H160.8400C16—H16B0.9900
O14—C131.313 (3)C14—C151.536 (3)
O14—H140.8400C14—H14A0.9900
O15—C171.206 (3)C14—H14B0.9900
N21—C221.483 (3)C15—H15A0.9900
N21—H21A0.9100C15—H15B0.9900
N21—H21B0.9100O11—C111.254 (3)
N21—H21C0.9100O12—C111.254 (3)
C22—C211.525 (3)N11—C121.483 (3)
C22—H22A0.9900N11—H11A0.9100
C22—H22B0.9900N11—H11B0.9100
C13—C141.502 (3)N11—H11C0.9100
C25—C261.526 (3)C12—C111.525 (3)
C25—C241.537 (3)C12—H12A0.9900
C25—H25A0.9900C12—H12B0.9900
C27—O26—H26109.5C25—C24—H24B109.2
C23—O24—H24109.5H24A—C24—H24B107.9
C17—O16—H16109.5C17—C16—C15113.01 (18)
C13—O14—H14109.5C17—C16—H16A109.0
C22—N21—H21A109.5C15—C16—H16A109.0
C22—N21—H21B109.5C17—C16—H16B109.0
H21A—N21—H21B109.5C15—C16—H16B109.0
C22—N21—H21C109.5H16A—C16—H16B107.8
H21A—N21—H21C109.5C13—C14—C15111.04 (18)
H21B—N21—H21C109.5C13—C14—H14A109.4
N21—C22—C21112.03 (17)C15—C14—H14A109.4
N21—C22—H22A109.2C13—C14—H14B109.4
C21—C22—H22A109.2C15—C14—H14B109.4
N21—C22—H22B109.2H14A—C14—H14B108.0
C21—C22—H22B109.2C16—C15—C14112.16 (18)
H22A—C22—H22B107.9C16—C15—H15A109.2
O13—C13—O14122.31 (19)C14—C15—H15A109.2
O13—C13—C14123.72 (19)C16—C15—H15B109.2
O14—C13—C14113.96 (16)C14—C15—H15B109.2
C26—C25—C24111.99 (17)H15A—C15—H15B107.9
C26—C25—H25A109.2O25—C27—O26119.10 (18)
C24—C25—H25A109.2O25—C27—C26123.30 (17)
C26—C25—H25B109.2O26—C27—C26117.60 (18)
C24—C25—H25B109.2O15—C17—O16119.60 (19)
H25A—C25—H25B107.9O15—C17—C16124.0 (2)
O23—C23—O24122.71 (18)O16—C17—C16116.40 (19)
O23—C23—C24123.5 (2)C12—N11—H11A109.5
O24—C23—C24113.84 (17)C12—N11—H11B109.5
O22—C21—O21125.5 (2)H11A—N11—H11B109.5
O22—C21—C22117.20 (18)C12—N11—H11C109.5
O21—C21—C22117.27 (18)H11A—N11—H11C109.5
C27—C26—C25111.88 (17)H11B—N11—H11C109.5
C27—C26—H26A109.2N11—C12—C11111.66 (17)
C25—C26—H26A109.2N11—C12—H12A109.3
C27—C26—H26B109.2C11—C12—H12A109.3
C25—C26—H26B109.2N11—C12—H12B109.3
H26A—C26—H26B107.9C11—C12—H12B109.3
C23—C24—C25112.07 (17)H12A—C12—H12B107.9
C23—C24—H24A109.2O12—C11—O11125.93 (19)
C25—C24—H24A109.2O12—C11—C12116.87 (18)
C23—C24—H24B109.2O11—C11—C12117.20 (18)
N21—C22—C21—O22178.23 (17)C17—C16—C15—C1474.2 (2)
N21—C22—C21—O212.3 (2)C13—C14—C15—C16176.23 (18)
C24—C25—C26—C27167.06 (18)C25—C26—C27—O256.2 (3)
O23—C23—C24—C25142.8 (2)C25—C26—C27—O26174.87 (18)
O24—C23—C24—C2537.3 (3)C15—C16—C17—O154.0 (3)
C26—C25—C24—C23178.91 (18)C15—C16—C17—O16178.57 (17)
O13—C13—C14—C1596.8 (2)N11—C12—C11—O12177.91 (18)
O14—C13—C14—C1582.0 (2)N11—C12—C11—O112.3 (3)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O14—H14···O21i0.841.732.571 (2)177
O16—H16···O12ii0.841.752.568 (2)164
N11—H11A···O150.912.142.824 (2)131
N11—H11B···O23iii0.911.962.851 (2)168
N11—H11C···O230.912.082.953 (2)160
O24—H24···O11iv0.841.722.5611 (19)175
O26—H26···O22v0.841.732.555 (2)168
N21—H21A···O250.912.082.793 (2)135
N21—H21B···O13ii0.911.952.849 (2)171
N21—H21C···O13vi0.912.102.961 (2)158
Symmetry codes: (i) x+1, y1, z; (ii) x+1, y+1, z+2; (iii) x+1, y+1, z+1; (iv) x1, y, z; (v) x+1, y+2, z+1; (vi) x, y+1, z.

Experimental details

(300)(275)(250)(225)
Crystal data
Chemical formulaC5H8O4·C2H5NO2C5H8O4·C2H5NO2C5H8O4·C2H5NO2C5H8O4·C2H5NO2
Mr207.18207.18207.18207.18
Crystal system, space groupMonoclinic, P21/cMonoclinic, P21/cMonoclinic, P21/cMonoclinic, P21/c
Temperature (K)300275250225
a, b, c (Å)4.9110 (7), 20.922 (3), 10.2744 (15)4.9022 (7), 20.901 (3), 10.2730 (15)4.8960 (6), 20.878 (2), 10.2701 (13)4.8888 (6), 20.859 (2), 10.2664 (13)
α, β, γ (°)90, 114.586 (10), 9090, 114.60 (1), 9090, 114.634 (9), 9090, 114.648 (9), 90
V3)959.9 (2)957.0 (2)954.3 (2)951.6 (2)
Z4444
Radiation typeMo KαMo KαMo KαMo Kα
µ (mm1)0.130.130.130.13
Crystal size (mm)0.32 × 0.17 × 0.100.32 × 0.17 × 0.100.32 × 0.17 × 0.100.32 × 0.17 × 0.10
Data collection
DiffractometerSTOE IPDS 2
diffractometer
STOE IPDS 2
diffractometer
STOE IPDS 2
diffractometer
STOE IPDS 2
diffractometer
Absorption correction
No. of measured, independent and
observed [I > 2σ(I)] reflections
6828, 2578, 1421 6792, 2570, 1461 6775, 2562, 1535 6775, 2558, 1594
Rint0.0460.0470.0450.043
(sin θ/λ)max1)0.6860.6870.6860.686
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.048, 0.096, 0.89 0.043, 0.085, 0.87 0.044, 0.086, 0.88 0.042, 0.081, 0.88
No. of reflections2578257025622558
No. of parameters130130130130
H-atom treatmentH-atom parameters constrainedH-atom parameters constrainedH-atom parameters constrainedH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.19, 0.170.16, 0.180.16, 0.200.21, 0.18


(200)(175)(150)(125)
Crystal data
Chemical formulaC5H8O4·C2H5NO2C5H8O4·C2H5NO2C5H8O4·C2H5NO2C5H8O4·C2H5NO2
Mr207.18207.18207.18207.18
Crystal system, space groupTriclinic, P1Triclinic, P1Triclinic, P1Triclinic, P1
Temperature (K)200175150125
a, b, c (Å)4.9155 (7), 20.215 (3), 10.1862 (16)4.9098 (7), 20.194 (3), 10.1777 (15)4.9021 (7), 20.167 (3), 10.1686 (15)4.8952 (6), 20.151 (3), 10.1585 (13)
α, β, γ (°)85.578 (14), 113.133 (11), 88.301 (13)85.571 (13), 113.118 (10), 88.306 (12)85.540 (11), 113.122 (10), 88.270 (11)85.518 (11), 113.088 (9), 88.264 (11)
V3)926.1 (2)923.3 (2)919.7 (2)916.9 (2)
Z4444
Radiation typeMo KαMo KαMo KαMo Kα
µ (mm1)0.130.130.130.13
Crystal size (mm)0.40 × 0.23 × 0.100.40 × 0.23 × 0.100.40 × 0.23 × 0.100.40 × 0.23 × 0.10
Data collection
DiffractometerSTOE IPDS 2
diffractometer
STOE IPDS 2
diffractometer
STOE IPDS 2
diffractometer
STOE IPDS 2
diffractometer
Absorption correction
No. of measured, independent and
observed [I > 2σ(I)] reflections
9663, 4312, 2491 9568, 4319, 2580 10066, 4417, 2840 9997, 4391, 2935
Rint0.0550.0520.0400.038
(sin θ/λ)max1)0.6860.6870.6860.686
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.049, 0.081, 0.89 0.049, 0.088, 0.89 0.039, 0.077, 0.88 0.039, 0.075, 0.90
No. of reflections4312431944174391
No. of parameters259259259259
H-atom treatmentH-atom parameters constrainedH-atom parameters constrainedH-atom parameters constrainedH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.19, 0.210.22, 0.230.21, 0.200.23, 0.20


(100)
Crystal data
Chemical formulaC5H8O4·C2H5NO2
Mr207.18
Crystal system, space groupTriclinic, P1
Temperature (K)100
a, b, c (Å)4.8884 (7), 20.136 (3), 10.1518 (15)
α, β, γ (°)85.486 (13), 113.065 (10), 88.263 (12)
V3)914.5 (2)
Z4
Radiation typeMo Kα
µ (mm1)0.13
Crystal size (mm)0.40 × 0.23 × 0.10
Data collection
DiffractometerSTOE IPDS 2
diffractometer
Absorption correction
No. of measured, independent and
observed [I > 2σ(I)] reflections
8816, 4247, 2766
Rint0.052
(sin θ/λ)max1)0.686
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.053, 0.097, 0.98
No. of reflections4247
No. of parameters259
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.31, 0.29

Computer programs: STOE X-AREA (Stoe & Cie, 2006), STOE X-RED (Stoe & Cie, 2006), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008) and X-STEP32 (Stoe & Cie, 2000), Mercury (Macrae et al., 2006), PLATON (Spek, 2009), enCIFer (Allen et al., 2004).

Hydrogen-bond geometry (Å, º) for (300) top
D—H···AD—HH···AD···AD—H···A
N1—H1B···O3i0.892.142.9671 (19)154.2
N1—H1C···O3ii0.892.002.8824 (19)169.4
N1—H1A···O50.892.002.7665 (18)143.2
O4—H4···O1iii0.821.752.5706 (18)177.5
O6—H6···O2iv0.821.752.5444 (18)164.4
Symmetry codes: (i) x+1, y1/2, z+1/2; (ii) x, y+3/2, z+1/2; (iii) x, y+1/2, z+1/2; (iv) x+1, y+1, z.
Hydrogen-bond geometry (Å, º) for (275) top
D—H···AD—HH···AD···AD—H···A
N1—H1B···O3i0.892.132.9564 (18)154.2
N1—H1C···O3ii0.892.002.8789 (18)169.4
N1—H1A···O50.892.002.7658 (17)143.2
O4—H4···O1iii0.821.752.5680 (17)176.4
O6—H6···O2iv0.821.742.5425 (17)164.5
Symmetry codes: (i) x+1, y1/2, z+1/2; (ii) x, y+3/2, z+1/2; (iii) x, y+1/2, z+1/2; (iv) x+1, y+1, z.
Hydrogen-bond geometry (Å, º) for (250) top
D—H···AD—HH···AD···AD—H···A
N1—H1B···O3i0.902.122.9504 (17)153.4
N1—H1C···O3ii0.901.992.8760 (18)169.5
N1—H1A···O50.901.982.7621 (17)143.8
O4—H4···O1iii0.831.742.5676 (16)177.9
O6—H6···O2iv0.831.732.5414 (16)164.6
Symmetry codes: (i) x+1, y1/2, z+1/2; (ii) x, y+3/2, z+1/2; (iii) x, y+1/2, z+1/2; (iv) x+1, y+1, z.
Hydrogen-bond geometry (Å, º) for (225) top
D—H···AD—HH···AD···AD—H···A
N1—H1B···O3i0.902.112.9420 (16)154.0
N1—H1C···O3ii0.901.982.8716 (16)169.5
N1—H1A···O50.901.992.7641 (15)143.2
O4—H4···O1iii0.831.742.5650 (15)174.7
O6—H6···O2iv0.831.732.5417 (15)164.9
Symmetry codes: (i) x+1, y1/2, z+1/2; (ii) x, y+3/2, z+1/2; (iii) x, y+1/2, z+1/2; (iv) x+1, y+1, z.
Hydrogen-bond geometry (Å, º) for (200) top
D—H···AD—HH···AD···AD—H···A
O14—H14···O21i0.841.742.580 (2)176.1
O16—H16···O12ii0.841.752.565 (2)163.5
N11—H11A···O150.912.122.827 (2)133.5
N11—H11B···O23iii0.911.962.860 (2)168.1
N11—H11C···O230.912.112.971 (2)158.0
O24—H24···O11iv0.841.722.5636 (18)176.0
O26—H26···O22v0.841.732.555 (2)167.3
N21—H21A···O250.912.052.798 (2)138.5
N21—H21B···O13ii0.911.962.861 (2)172.2
N21—H21C···O13vi0.912.142.984 (2)154.5
Symmetry codes: (i) x+1, y1, z; (ii) x+1, y+1, z+2; (iii) x+1, y+1, z+1; (iv) x1, y, z; (v) x+1, y+2, z+1; (vi) x, y+1, z.
Hydrogen-bond geometry (Å, º) for (175) top
D—H···AD—HH···AD···AD—H···A
O14—H14···O21i0.841.742.579 (2)177.5
O16—H16···O12ii0.841.742.567 (2)165.9
N11—H11A···O150.912.122.826 (2)133.2
N11—H11B···O23iii0.911.962.860 (2)168.2
N11—H11C···O230.912.102.967 (2)158.3
O24—H24···O11iv0.841.732.5655 (18)176.3
O26—H26···O22v0.841.732.552 (2)165.7
N21—H21A···O250.912.072.800 (2)136.8
N21—H21B···O13ii0.911.952.859 (2)171.8
N21—H21C···O13vi0.912.122.974 (2)156.1
Symmetry codes: (i) x+1, y1, z; (ii) x+1, y+1, z+2; (iii) x+1, y+1, z+1; (iv) x1, y, z; (v) x+1, y+2, z+1; (vi) x, y+1, z.
Hydrogen-bond geometry (Å, º) for (150) top
D—H···AD—HH···AD···AD—H···A
O14—H14···O21i0.841.742.5745 (16)173.6
O16—H16···O12ii0.841.742.5658 (17)165.6
N11—H11A···O150.912.112.8238 (16)134.5
N11—H11B···O23iii0.911.962.8554 (18)169.3
N11—H11C···O230.912.102.9644 (17)157.5
O24—H24···O11iv0.841.722.5626 (14)175.5
O26—H26···O22v0.841.732.5550 (16)166.1
N21—H21A···O250.912.072.7944 (17)135.6
N21—H21B···O13ii0.911.952.8551 (17)171.1
N21—H21C···O13vi0.912.112.9719 (18)157.0
Symmetry codes: (i) x+1, y1, z; (ii) x+1, y+1, z+2; (iii) x+1, y+1, z+1; (iv) x1, y, z; (v) x+1, y+2, z+1; (vi) x, y+1, z.
Hydrogen-bond geometry (Å, º) for (125) top
D—H···AD—HH···AD···AD—H···A
O14—H14···O21i0.841.742.5739 (16)175.1
O16—H16···O12ii0.841.742.5644 (16)165.7
N11—H11A···O150.912.132.8245 (15)132.5
N11—H11B···O23iii0.911.962.8537 (18)168.4
N11—H11C···O230.912.092.9564 (17)158.6
O24—H24···O11iv0.841.722.5623 (14)176.1
O26—H26···O22v0.841.732.5539 (16)167.0
N21—H21A···O250.912.062.7956 (17)136.8
N21—H21B···O13ii0.911.952.8522 (17)172.2
N21—H21C···O13vi0.912.112.9639 (17)156.0
Symmetry codes: (i) x+1, y1, z; (ii) x+1, y+1, z+2; (iii) x+1, y+1, z+1; (iv) x1, y, z; (v) x+1, y+2, z+1; (vi) x, y+1, z.
Hydrogen-bond geometry (Å, º) for (100) top
D—H···AD—HH···AD···AD—H···A
O14—H14···O21i0.841.732.571 (2)177.3
O16—H16···O12ii0.841.752.568 (2)163.8
N11—H11A···O150.912.142.824 (2)131.3
N11—H11B···O23iii0.911.962.851 (2)167.5
N11—H11C···O230.912.082.953 (2)159.5
O24—H24···O11iv0.841.722.5611 (19)174.5
O26—H26···O22v0.841.732.555 (2)167.8
N21—H21A···O250.912.082.793 (2)134.6
N21—H21B···O13ii0.911.952.849 (2)171.4
N21—H21C···O13vi0.912.102.961 (2)157.7
Symmetry codes: (i) x+1, y1, z; (ii) x+1, y+1, z+2; (iii) x+1, y+1, z+1; (iv) x1, y, z; (v) x+1, y+2, z+1; (vi) x, y+1, z.
 

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