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The adipic acid complexes of DL-arginine and L-arginine are made up of zwitterionic, singularly positively charged arginium ions and doubly negatively charged adipate ions, with a 2:1 stoichiometry. One of the two crystallographically independent arginium ions in the L-arginine complex has a conformation hitherto unobserved in crystal structures containing the amino acid. In the present study the structural data on arginine complexes of saturated dicarboxylic acids with 0-5 C atoms separating the two carboxyl functions are given. In terms of molecular aggregation, formic and acetic acid complexes behave in a similar way to those involving fairly long carboxylic acids such as adipic acid. By and large, the supramolecular assembly in complexes involving dicarboxylic acids with 3 or more C atoms separating the carboxyl groups (glutaric, adipic and pimelic acids), and those involving formic and acetic acids, have common features. The aggregation patterns in complexes involving oxalic, malonic and maleic acids do not share striking features among themselves (except for the mode of hydrogen-bonded dimerization of arginium ions) or with those involving larger dicarboxylic acids. Complexes of succinic acid, the shortest linear dicarboxylic acid, share features with those involving shorter as well as longer dicarboxylic acids. The difference in the behaviour of long and short dicarboxylic acids and the ambiguous behaviour of succinic acid can be broadly related to their lengths.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108768104030010/de5013sup1.cif
Contains datablocks global, dlarad_m, larad_m

fcf

Structure factor file (CIF format) https://doi.org/10.1107/S0108768104030010/de5013dlarad_msup2.fcf
Contains datablock dl_arg

fcf

Structure factor file (CIF format) https://doi.org/10.1107/S0108768104030010/de5013larad_msup3.fcf
Contains datablock largadi

CCDC references: 263171; 263172

Computing details top

For both compounds, data collection: Bruker SMART; cell refinement: Bruker SMART; data reduction: Bruker SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3; software used to prepare material for publication: PLATON (Spek, 1990).

Figures top
[Figure 1]
[Figure 2]
[Figure 3]
[Figure 4]
[Figure 5]
View of the title compound with the atom numbering scheme. Displacement ellipsoids for non-H atoms are drawn at the 50% probability level.
(dlarad_m) top
Crystal data top
C6H15N4O2·0.5(C6H8O4)·H2OF(000) = 572
Mr = 265.30Dx = 1.376 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 2581 reflections
a = 13.825 (4) Åθ = 1.5–26.4°
b = 5.0531 (16) ŵ = 0.11 mm1
c = 18.804 (6) ÅT = 298 K
β = 102.900 (6)°Plate, colourless
V = 1280.5 (7) Å30.59 × 0.11 × 0.02 mm
Z = 4
Data collection top
Bruker SMART CCD area detector
diffractometer
2581 independent reflections
Radiation source: fine-focus sealed tube2150 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.031
phi and ω scansθmax = 26.4°, θmin = 1.5°
Absorption correction: multi-scan
SADABS,Sheldrick, 1997
h = 1516
Tmin = 0.937, Tmax = 0.998k = 66
9412 measured reflectionsl = 2323
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.054All H-atom parameters refined
wR(F2) = 0.128 w = 1/[σ2(Fo2) + (0.0354P)2 + 0.8605P]
where P = (Fo2 + 2Fc2)/3
S = 1.05(Δ/σ)max < 0.001
2581 reflectionsΔρmax = 0.28 e Å3
247 parametersΔρmin = 0.17 e Å3
0 restraintsAbsolute structure: Flack H.D. (1983), Acta Cryst. A39, 876-881
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: centrosymmetric
Crystal data top
C6H15N4O2·0.5(C6H8O4)·H2OV = 1280.5 (7) Å3
Mr = 265.30Z = 4
Monoclinic, P21/cMo Kα radiation
a = 13.825 (4) ŵ = 0.11 mm1
b = 5.0531 (16) ÅT = 298 K
c = 18.804 (6) Å0.59 × 0.11 × 0.02 mm
β = 102.900 (6)°
Data collection top
Bruker SMART CCD area detector
diffractometer
2581 independent reflections
Absorption correction: multi-scan
SADABS,Sheldrick, 1997
2150 reflections with I > 2σ(I)
Tmin = 0.937, Tmax = 0.998Rint = 0.031
9412 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.054All H-atom parameters refined
wR(F2) = 0.128Δρmax = 0.28 e Å3
S = 1.05Δρmin = 0.17 e Å3
2581 reflectionsAbsolute structure: Flack H.D. (1983), Acta Cryst. A39, 876-881
247 parametersAbsolute structure parameter: centrosymmetric
0 restraints
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
N10.62752 (14)0.6252 (4)0.51182 (10)0.0281 (4)
O20.53502 (11)1.2185 (3)0.41877 (8)0.0346 (4)
O10.47059 (11)0.8150 (3)0.41053 (10)0.0468 (5)
C10.53967 (15)0.9713 (4)0.42921 (10)0.0253 (4)
C20.64106 (14)0.8607 (4)0.46758 (10)0.0243 (4)
C30.69967 (16)0.7768 (4)0.41130 (11)0.0278 (5)
C40.73618 (17)1.0090 (4)0.37272 (12)0.0300 (5)
C50.80091 (17)0.9200 (5)0.32166 (12)0.0322 (5)
N60.74420 (14)0.7534 (4)0.26397 (10)0.0345 (5)
C70.78389 (15)0.5899 (4)0.22320 (11)0.0298 (5)
N80.87995 (14)0.5456 (4)0.23660 (12)0.0350 (5)
N90.72569 (17)0.4649 (5)0.16773 (12)0.0453 (6)
O110.95427 (11)0.1802 (3)0.14957 (8)0.0365 (4)
O120.80437 (11)0.0837 (4)0.08604 (10)0.0509 (5)
C130.89578 (15)0.0407 (4)0.10453 (11)0.0294 (5)
C140.93856 (18)0.1875 (5)0.06947 (13)0.0348 (5)
C151.01776 (18)0.1011 (5)0.02977 (13)0.0365 (5)
O160.53048 (13)0.8619 (4)0.22510 (11)0.0437 (4)
H1A0.689 (2)0.569 (5)0.5375 (14)0.042 (7)*
H1B0.584 (2)0.671 (5)0.5432 (14)0.045 (7)*
H1C0.5970 (17)0.484 (5)0.4806 (13)0.035 (6)*
H20.6770 (15)0.995 (4)0.5028 (12)0.025 (5)*
H3A0.6547 (18)0.658 (5)0.3759 (13)0.038 (6)*
H3B0.7588 (18)0.669 (4)0.4382 (12)0.034 (6)*
H4A0.6783 (18)1.109 (5)0.3454 (12)0.035 (6)*
H4B0.7750 (19)1.122 (5)0.4091 (14)0.045 (7)*
H5A0.8568 (17)0.816 (4)0.3486 (12)0.029 (6)*
H5B0.8256 (18)1.084 (5)0.2994 (13)0.039 (6)*
H60.683 (2)0.782 (5)0.2507 (13)0.042 (7)*
H8A0.9202 (19)0.606 (5)0.2703 (14)0.037 (7)*
H8B0.905 (2)0.431 (5)0.2078 (15)0.050 (8)*
H9A0.751 (2)0.346 (6)0.1439 (15)0.048 (8)*
H9B0.662 (2)0.471 (5)0.1588 (14)0.048 (8)*
H14A0.964 (2)0.308 (5)0.1058 (15)0.048 (7)*
H14B0.8877 (18)0.285 (5)0.0373 (13)0.037 (6)*
H15A1.0758 (19)0.026 (5)0.0637 (14)0.044 (7)*
H15B1.0446 (18)0.262 (5)0.0072 (13)0.047 (7)*
H16A0.518 (2)1.015 (7)0.2352 (18)0.066 (11)*
H16B0.510 (3)0.847 (7)0.182 (2)0.076 (11)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N10.0232 (9)0.0310 (10)0.0292 (9)0.0050 (8)0.0041 (8)0.0046 (8)
O20.0404 (9)0.0259 (8)0.0358 (8)0.0079 (6)0.0047 (7)0.0019 (6)
O10.0246 (8)0.0395 (9)0.0678 (12)0.0008 (7)0.0076 (8)0.0086 (8)
C10.0249 (11)0.0302 (11)0.0221 (9)0.0055 (8)0.0081 (8)0.0010 (8)
C20.0214 (10)0.0266 (10)0.0236 (9)0.0017 (8)0.0027 (8)0.0008 (8)
C30.0254 (11)0.0302 (11)0.0286 (10)0.0036 (9)0.0076 (9)0.0006 (9)
C40.0269 (11)0.0319 (11)0.0320 (11)0.0011 (9)0.0086 (9)0.0040 (9)
C50.0305 (12)0.0360 (12)0.0315 (11)0.0036 (10)0.0099 (9)0.0023 (10)
N60.0206 (10)0.0516 (12)0.0308 (10)0.0055 (8)0.0046 (8)0.0073 (8)
C70.0253 (11)0.0396 (12)0.0244 (10)0.0004 (9)0.0052 (8)0.0013 (9)
N80.0208 (10)0.0496 (12)0.0336 (10)0.0019 (8)0.0036 (8)0.0135 (9)
N90.0248 (11)0.0663 (15)0.0419 (12)0.0023 (10)0.0012 (9)0.0222 (11)
O110.0254 (8)0.0448 (9)0.0359 (8)0.0019 (7)0.0005 (6)0.0107 (7)
O120.0220 (9)0.0632 (12)0.0631 (12)0.0012 (8)0.0002 (8)0.0308 (9)
C130.0258 (11)0.0348 (11)0.0282 (10)0.0008 (9)0.0074 (9)0.0004 (9)
C140.0378 (13)0.0293 (11)0.0378 (12)0.0006 (10)0.0097 (10)0.0015 (10)
C150.0368 (13)0.0346 (12)0.0405 (13)0.0063 (10)0.0134 (11)0.0041 (10)
O160.0426 (10)0.0497 (12)0.0347 (10)0.0037 (8)0.0001 (8)0.0018 (8)
Geometric parameters (Å, º) top
N1—C21.487 (3)N6—H60.83 (3)
N1—H1A0.92 (3)C7—N81.315 (3)
N1—H1B0.96 (3)C7—N91.326 (3)
N1—H1C0.96 (3)N8—H8A0.81 (3)
O2—C11.264 (2)N8—H8B0.91 (3)
O1—C11.229 (3)N9—H9A0.87 (3)
C1—C21.532 (3)N9—H9B0.87 (3)
C2—C31.529 (3)O11—C131.250 (3)
C2—H21.00 (2)O12—C131.253 (3)
C3—C41.524 (3)C13—C141.513 (3)
C3—H3A1.00 (2)C14—C151.521 (3)
C3—H3B1.02 (2)C14—H14A0.92 (3)
C4—C51.519 (3)C14—H14B0.96 (2)
C4—H4A0.99 (2)C15—C15i1.514 (5)
C4—H4B0.96 (3)C15—H15A0.98 (3)
C5—N61.456 (3)C15—H15B1.02 (3)
C5—H5A0.98 (2)O16—H16A0.83 (3)
C5—H5B1.02 (3)O16—H16B0.81 (4)
N6—C71.326 (3)
C2—N1—H1A108.8 (16)C4—C5—H5B108.4 (13)
C2—N1—H1B108.9 (15)H5A—C5—H5B110.5 (19)
H1A—N1—H1B113 (2)C7—N6—C5124.57 (19)
C2—N1—H1C110.2 (14)C7—N6—H6117.0 (18)
H1A—N1—H1C109 (2)C5—N6—H6117.5 (18)
H1B—N1—H1C108 (2)N8—C7—N6121.7 (2)
O1—C1—O2125.56 (19)N8—C7—N9118.6 (2)
O1—C1—C2118.12 (18)N6—C7—N9119.6 (2)
O2—C1—C2116.31 (18)C7—N8—H8A125.2 (18)
N1—C2—C3108.51 (16)C7—N8—H8B119.7 (17)
N1—C2—C1109.83 (16)H8A—N8—H8B115 (2)
C3—C2—C1110.22 (16)C7—N9—H9A119.3 (18)
N1—C2—H2106.3 (12)C7—N9—H9B123.3 (18)
C3—C2—H2112.6 (12)H9A—N9—H9B116 (3)
C1—C2—H2109.3 (12)O11—C13—O12123.4 (2)
C4—C3—C2113.52 (17)O11—C13—C14117.94 (19)
C4—C3—H3A111.5 (13)O12—C13—C14118.7 (2)
C2—C3—H3A106.2 (14)C13—C14—C15112.90 (19)
C4—C3—H3B109.6 (13)C13—C14—H14A107.5 (16)
C2—C3—H3B107.1 (13)C15—C14—H14A111.0 (17)
H3A—C3—H3B108.7 (18)C13—C14—H14B111.4 (14)
C5—C4—C3112.16 (18)C15—C14—H14B110.2 (14)
C5—C4—H4A110.3 (13)H14A—C14—H14B103 (2)
C3—C4—H4A109.0 (13)C15i—C15—C14114.0 (2)
C5—C4—H4B108.3 (15)C15i—C15—H15A107.6 (15)
C3—C4—H4B108.1 (15)C14—C15—H15A111.4 (15)
H4A—C4—H4B109 (2)C15i—C15—H15B108.5 (14)
N6—C5—C4110.30 (18)C14—C15—H15B110.0 (14)
N6—C5—H5A108.0 (13)H15A—C15—H15B105 (2)
C4—C5—H5A109.9 (13)H16A—O16—H16B106 (3)
N6—C5—H5B109.8 (13)
Symmetry code: (i) x+2, y, z.
(larad_m) top
Crystal data top
2(C6H15N4O2)·C6H8O4F(000) = 532
Mr = 494.56Dx = 1.374 Mg m3
Monoclinic, P21Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2ybCell parameters from 3711 reflections
a = 12.494 (4) Åθ = 1.3–24.7°
b = 5.9510 (17) ŵ = 0.11 mm1
c = 16.719 (5) ÅT = 298 K
β = 105.977 (5)°Platy, colourless
V = 1195.1 (6) Å30.25 × 0.07 × 0.06 mm
Z = 2
Data collection top
Bruker SMART CCD area detector
diffractometer
3711 independent reflections
Radiation source: fine-focus sealed tube3396 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.019
phi and ω scansθmax = 24.7°, θmin = 1.3°
Absorption correction: multi-scan
Sheldrick, 1999
h = 1414
Tmin = 0.973, Tmax = 0.994k = 66
6142 measured reflectionsl = 1918
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.039All H-atom parameters refined
wR(F2) = 0.113 w = 1/[σ2(Fo2) + (0.1P)2]
where P = (Fo2 + 2Fc2)/3
S = 0.86(Δ/σ)max = 0.012
3711 reflectionsΔρmax = 0.17 e Å3
459 parametersΔρmin = 0.17 e Å3
1 restraintAbsolute structure: Flack H.D. (1983), Acta Cryst. A39, 876-881
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 0.1 (11)
Crystal data top
2(C6H15N4O2)·C6H8O4V = 1195.1 (6) Å3
Mr = 494.56Z = 2
Monoclinic, P21Mo Kα radiation
a = 12.494 (4) ŵ = 0.11 mm1
b = 5.9510 (17) ÅT = 298 K
c = 16.719 (5) Å0.25 × 0.07 × 0.06 mm
β = 105.977 (5)°
Data collection top
Bruker SMART CCD area detector
diffractometer
3711 independent reflections
Absorption correction: multi-scan
Sheldrick, 1999
3396 reflections with I > 2σ(I)
Tmin = 0.973, Tmax = 0.994Rint = 0.019
6142 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.039All H-atom parameters refined
wR(F2) = 0.113Δρmax = 0.17 e Å3
S = 0.86Δρmin = 0.17 e Å3
3711 reflectionsAbsolute structure: Flack H.D. (1983), Acta Cryst. A39, 876-881
459 parametersAbsolute structure parameter: 0.1 (11)
1 restraint
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
N11.01548 (17)0.9154 (4)0.88174 (12)0.0240 (4)
O10.96221 (14)0.5244 (3)0.95135 (9)0.0366 (4)
O20.96334 (19)0.3583 (3)0.83320 (12)0.0566 (6)
C10.95512 (17)0.5228 (4)0.87500 (13)0.0252 (5)
C20.93201 (17)0.7539 (4)0.83210 (13)0.0233 (5)
H20.85860.80300.83570.028*
C30.92912 (17)0.7552 (4)0.74139 (12)0.0271 (5)
H3A0.88820.62440.71470.033*
H3B1.00470.74260.73690.033*
C40.87581 (19)0.9652 (5)0.69515 (12)0.0302 (6)
H4A0.80600.99400.70800.036*
H4B0.92441.09280.71460.036*
C50.85417 (19)0.9446 (5)0.60204 (13)0.0309 (5)
H5A0.82751.08740.57620.037*
H5B0.92330.90920.58910.037*
N60.77239 (15)0.7705 (4)0.56788 (11)0.0296 (5)
C70.78677 (18)0.5905 (4)0.52479 (13)0.0271 (5)
N80.88506 (17)0.5337 (5)0.51713 (15)0.0428 (6)
N90.69899 (17)0.4645 (4)0.48849 (14)0.0385 (6)
N110.47199 (16)0.3474 (4)0.62115 (13)0.0278 (5)
O110.53182 (13)0.7147 (3)0.55435 (10)0.0370 (5)
O120.5459 (2)0.9183 (3)0.66813 (13)0.0640 (7)
C110.53475 (19)0.7406 (4)0.62924 (15)0.0304 (6)
C120.52925 (17)0.5288 (4)0.67927 (13)0.0249 (5)
H120.48470.56170.71780.030*
C130.64495 (17)0.4533 (4)0.73018 (13)0.0300 (5)
H13A0.68220.38340.69280.036*
H13B0.68750.58570.75350.036*
C140.6474 (2)0.2896 (5)0.80096 (13)0.0345 (6)
H14A0.59340.17150.78020.041*
H14B0.72040.22030.81850.041*
C150.6223 (2)0.3985 (5)0.87609 (14)0.0362 (6)
H15A0.55390.48450.85830.043*
H15B0.61200.28300.91420.043*
N160.71339 (17)0.5462 (4)0.91837 (12)0.0338 (5)
C170.70469 (19)0.7180 (5)0.96698 (14)0.0313 (6)
N180.60849 (18)0.7865 (5)0.97442 (16)0.0460 (7)
N190.79692 (18)0.8235 (5)1.00812 (14)0.0436 (6)
O210.21705 (13)0.2818 (3)0.89309 (11)0.0462 (5)
O220.39213 (14)0.3812 (4)0.91304 (12)0.0506 (6)
C230.31072 (19)0.2600 (5)0.87990 (14)0.0330 (6)
C240.3284 (2)0.0812 (6)0.82081 (16)0.0458 (7)
H24A0.38860.01520.85110.055*
H24B0.35340.15480.77740.055*
C250.2318 (2)0.0652 (5)0.77992 (15)0.0371 (6)
H25A0.20830.14660.82240.045*
H25B0.17020.02880.75020.045*
C260.25825 (19)0.2315 (5)0.71983 (15)0.0372 (6)
H26A0.32030.32440.74950.045*
H26B0.28130.14970.67720.045*
C270.1621 (2)0.3808 (5)0.67872 (16)0.0400 (7)
H27A0.13760.45590.72210.048*
H27B0.10130.28600.64830.048*
C280.18174 (18)0.5578 (5)0.61971 (13)0.0301 (6)
O290.27334 (13)0.5652 (3)0.60343 (10)0.0388 (5)
O300.10253 (13)0.6905 (3)0.58914 (11)0.0420 (5)
H1A1.088 (2)0.877 (4)0.8829 (14)0.036 (7)*
H1B0.999 (2)1.052 (5)0.8635 (15)0.026 (6)*
H1C1.0151 (19)0.908 (5)0.9380 (15)0.041 (7)*
H6A0.702 (2)0.810 (5)0.5692 (14)0.037 (7)*
H8A0.8889 (17)0.419 (5)0.4860 (14)0.023 (6)*
H8B0.953 (2)0.613 (6)0.5431 (17)0.065 (10)*
H9A0.630 (2)0.480 (5)0.4972 (15)0.050 (8)*
H9B0.709 (2)0.339 (6)0.4639 (18)0.058 (10)*
H11A0.494 (2)0.174 (6)0.6427 (17)0.051 (8)*
H11B0.398 (2)0.369 (4)0.6104 (14)0.034 (7)*
H11C0.4946 (19)0.360 (5)0.5700 (16)0.040 (7)*
H16A0.7788 (19)0.506 (5)0.9261 (13)0.029 (7)*
H18A0.549 (2)0.727 (5)0.9525 (14)0.028 (7)*
H18B0.603 (2)0.898 (6)1.0223 (18)0.072 (10)*
H19A0.794 (2)0.930 (6)1.0417 (16)0.042 (8)*
H19B0.8621 (19)0.784 (5)1.0010 (13)0.035 (7)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N10.0338 (11)0.0160 (12)0.0211 (10)0.0006 (9)0.0058 (8)0.0020 (8)
O10.0515 (10)0.0331 (11)0.0272 (8)0.0077 (8)0.0145 (7)0.0094 (8)
O20.1109 (17)0.0189 (11)0.0342 (11)0.0077 (11)0.0104 (11)0.0028 (9)
C10.0250 (11)0.0223 (14)0.0268 (12)0.0021 (10)0.0046 (9)0.0008 (11)
C20.0244 (11)0.0218 (13)0.0227 (11)0.0036 (9)0.0049 (9)0.0012 (10)
C30.0307 (11)0.0251 (13)0.0246 (11)0.0011 (10)0.0061 (9)0.0027 (10)
C40.0419 (13)0.0213 (14)0.0256 (11)0.0020 (11)0.0063 (10)0.0017 (11)
C50.0430 (13)0.0223 (13)0.0245 (11)0.0012 (11)0.0046 (10)0.0015 (11)
N60.0307 (10)0.0324 (13)0.0250 (10)0.0011 (9)0.0066 (8)0.0036 (9)
C70.0296 (12)0.0266 (15)0.0221 (11)0.0008 (10)0.0022 (9)0.0022 (11)
N80.0298 (12)0.0434 (16)0.0550 (14)0.0037 (11)0.0113 (10)0.0242 (13)
N90.0291 (11)0.0383 (15)0.0462 (13)0.0027 (10)0.0072 (10)0.0164 (12)
N110.0279 (11)0.0238 (12)0.0308 (11)0.0017 (9)0.0066 (9)0.0003 (9)
O110.0426 (10)0.0335 (11)0.0387 (10)0.0017 (8)0.0174 (8)0.0071 (9)
O120.1078 (18)0.0206 (11)0.0476 (12)0.0001 (12)0.0054 (12)0.0052 (10)
C110.0273 (12)0.0241 (14)0.0355 (14)0.0011 (11)0.0017 (10)0.0017 (12)
C120.0245 (11)0.0241 (13)0.0256 (11)0.0006 (10)0.0064 (9)0.0042 (10)
C130.0286 (11)0.0313 (14)0.0280 (11)0.0020 (10)0.0044 (9)0.0018 (11)
C140.0417 (13)0.0268 (15)0.0303 (12)0.0018 (12)0.0021 (10)0.0013 (12)
C150.0426 (13)0.0362 (17)0.0297 (13)0.0080 (12)0.0095 (10)0.0006 (11)
N160.0285 (11)0.0397 (13)0.0319 (10)0.0008 (10)0.0063 (9)0.0098 (10)
C170.0324 (12)0.0362 (16)0.0255 (12)0.0040 (11)0.0081 (10)0.0041 (12)
N180.0299 (12)0.0527 (17)0.0562 (15)0.0051 (12)0.0130 (11)0.0271 (14)
N190.0333 (12)0.0515 (17)0.0456 (14)0.0072 (11)0.0101 (10)0.0223 (13)
O210.0346 (9)0.0459 (13)0.0623 (12)0.0070 (9)0.0206 (9)0.0232 (11)
O220.0304 (9)0.0513 (14)0.0691 (13)0.0060 (9)0.0118 (9)0.0335 (11)
C230.0304 (12)0.0314 (15)0.0368 (13)0.0016 (12)0.0086 (10)0.0067 (13)
C240.0361 (13)0.053 (2)0.0508 (16)0.0046 (14)0.0171 (12)0.0189 (15)
C250.0396 (14)0.0345 (17)0.0399 (14)0.0028 (12)0.0154 (11)0.0091 (13)
C260.0359 (13)0.0380 (17)0.0408 (14)0.0057 (13)0.0158 (11)0.0128 (14)
C270.0371 (13)0.0393 (18)0.0474 (15)0.0059 (12)0.0178 (11)0.0169 (14)
C280.0278 (12)0.0313 (15)0.0303 (12)0.0001 (11)0.0064 (10)0.0026 (12)
O290.0309 (9)0.0404 (12)0.0474 (10)0.0054 (8)0.0149 (7)0.0181 (10)
O300.0290 (9)0.0395 (12)0.0564 (11)0.0044 (8)0.0099 (8)0.0177 (10)
Geometric parameters (Å, º) top
N1—C21.491 (3)C13—C141.527 (3)
N1—H1A0.93 (2)C13—H13A0.9700
N1—H1B0.88 (3)C13—H13B0.9700
N1—H1C0.94 (2)C14—C151.521 (3)
O1—C11.255 (3)C14—H14A0.9700
O2—C11.224 (3)C14—H14B0.9700
C1—C21.541 (3)C15—N161.457 (3)
C2—C31.507 (3)C15—H15A0.9700
C2—H20.9800C15—H15B0.9700
C3—C41.523 (3)N16—C171.329 (3)
C3—H3A0.9700N16—H16A0.83 (2)
C3—H3B0.9700C17—N181.307 (3)
C4—C51.510 (3)C17—N191.326 (3)
C4—H4A0.9700N18—H18A0.81 (3)
C4—H4B0.9700N18—H18B1.06 (3)
C5—N61.457 (3)N19—H19A0.85 (3)
C5—H5A0.9700N19—H19B0.89 (2)
C5—H5B0.9700O21—C231.256 (3)
N6—C71.330 (3)O22—C231.245 (3)
N6—H6A0.92 (2)C23—C241.509 (4)
C7—N81.314 (3)C24—C251.494 (4)
C7—N91.329 (3)C24—H24A0.9700
N8—H8A0.87 (3)C24—H24B0.9700
N8—H8B0.97 (3)C25—C261.511 (3)
N9—H9A0.91 (3)C25—H25A0.9700
N9—H9B0.88 (3)C25—H25B0.9700
N11—C121.496 (3)C26—C271.500 (4)
N11—H11A1.10 (3)C26—H26A0.9700
N11—H11B0.90 (2)C26—H26B0.9700
N11—H11C0.97 (2)C27—C281.509 (3)
O11—C111.252 (3)C27—H27A0.9700
O12—C111.229 (3)C27—H27B0.9700
C11—C121.525 (3)C28—O291.248 (3)
C12—C131.529 (3)C28—O301.259 (3)
C12—H120.9800
C2—N1—H1A112.4 (15)C14—C13—C12115.66 (19)
C2—N1—H1B110.1 (17)C14—C13—H13A108.4
H1A—N1—H1B112 (2)C12—C13—H13A108.4
C2—N1—H1C109.3 (16)C14—C13—H13B108.4
H1A—N1—H1C104 (2)C12—C13—H13B108.4
H1B—N1—H1C109 (2)H13A—C13—H13B107.4
O2—C1—O1126.4 (2)C15—C14—C13113.8 (2)
O2—C1—C2118.85 (19)C15—C14—H14A108.8
O1—C1—C2114.8 (2)C13—C14—H14A108.8
N1—C2—C3112.08 (19)C15—C14—H14B108.8
N1—C2—C1107.66 (18)C13—C14—H14B108.8
C3—C2—C1115.00 (19)H14A—C14—H14B107.7
N1—C2—H2107.2N16—C15—C14110.3 (2)
C3—C2—H2107.2N16—C15—H15A109.6
C1—C2—H2107.2C14—C15—H15A109.6
C2—C3—C4113.64 (19)N16—C15—H15B109.6
C2—C3—H3A108.8C14—C15—H15B109.6
C4—C3—H3A108.8H15A—C15—H15B108.1
C2—C3—H3B108.8C17—N16—C15125.2 (2)
C4—C3—H3B108.8C17—N16—H16A111.9 (18)
H3A—C3—H3B107.7C15—N16—H16A120.3 (19)
C5—C4—C3112.7 (2)N18—C17—N19119.6 (3)
C5—C4—H4A109.1N18—C17—N16122.0 (2)
C3—C4—H4A109.1N19—C17—N16118.4 (2)
C5—C4—H4B109.1C17—N18—H18A125.0 (18)
C3—C4—H4B109.1C17—N18—H18B121.7 (16)
H4A—C4—H4B107.8H18A—N18—H18B111 (2)
N6—C5—C4111.7 (2)C17—N19—H19A120.5 (18)
N6—C5—H5A109.3C17—N19—H19B120.2 (18)
C4—C5—H5A109.3H19A—N19—H19B119 (3)
N6—C5—H5B109.3O22—C23—O21123.3 (2)
C4—C5—H5B109.3O22—C23—C24116.8 (2)
H5A—C5—H5B107.9O21—C23—C24120.0 (2)
C7—N6—C5126.87 (19)C25—C24—C23117.7 (2)
C7—N6—H6A119.5 (17)C25—C24—H24A107.9
C5—N6—H6A112.6 (17)C23—C24—H24A107.9
N8—C7—N9119.1 (2)C25—C24—H24B107.9
N8—C7—N6122.0 (2)C23—C24—H24B107.9
N9—C7—N6118.9 (2)H24A—C24—H24B107.2
C7—N8—H8A117.9 (14)C24—C25—C26112.9 (2)
C7—N8—H8B124.4 (19)C24—C25—H25A109.0
H8A—N8—H8B118 (2)C26—C25—H25A109.0
C7—N9—H9A124.3 (18)C24—C25—H25B109.0
C7—N9—H9B119 (2)C26—C25—H25B109.0
H9A—N9—H9B115 (3)H25A—C25—H25B107.8
C12—N11—H11A115.4 (15)C27—C26—C25113.48 (19)
C12—N11—H11B107.9 (16)C27—C26—H26A108.9
H11A—N11—H11B111 (2)C25—C26—H26A108.9
C12—N11—H11C108.3 (16)C27—C26—H26B108.9
H11A—N11—H11C104 (2)C25—C26—H26B108.9
H11B—N11—H11C110 (2)H26A—C26—H26B107.7
O12—C11—O11127.1 (3)C26—C27—C28117.4 (2)
O12—C11—C12115.9 (2)C26—C27—H27A108.0
O11—C11—C12117.0 (2)C28—C27—H27A108.0
N11—C12—C11109.02 (19)C26—C27—H27B108.0
N11—C12—C13111.08 (19)C28—C27—H27B108.0
C11—C12—C13111.69 (19)H27A—C27—H27B107.2
N11—C12—H12108.3O29—C28—O30123.7 (2)
C11—C12—H12108.3O29—C28—C27119.4 (2)
C13—C12—H12108.3O30—C28—C27116.88 (19)
O2—C1—C2—N1129.5 (2)N11—C12—C13—C1475.6 (2)
O1—C1—C2—N151.4 (2)C11—C12—C13—C14162.4 (2)
O2—C1—C2—C33.8 (3)C12—C13—C14—C1574.6 (3)
O1—C1—C2—C3177.07 (18)C13—C14—C15—N1669.4 (3)
N1—C2—C3—C472.4 (2)C14—C15—N16—C17156.6 (2)
C1—C2—C3—C4164.17 (19)C15—N16—C17—N187.6 (4)
C2—C3—C4—C5169.23 (19)C15—N16—C17—N19173.2 (2)
C3—C4—C5—N664.8 (3)O22—C23—C24—C25179.6 (3)
C4—C5—N6—C7121.6 (2)O21—C23—C24—C250.1 (4)
C5—N6—C7—N89.1 (4)C23—C24—C25—C26177.8 (2)
C5—N6—C7—N9170.9 (2)C24—C25—C26—C27179.6 (3)
O12—C11—C12—N11157.6 (2)C25—C26—C27—C28178.0 (2)
O11—C11—C12—N1125.1 (3)C26—C27—C28—O294.3 (4)
O12—C11—C12—C1379.3 (3)C26—C27—C28—O30176.1 (2)
O11—C11—C12—C1398.0 (2)

Experimental details

(dlarad_m)(larad_m)
Crystal data
Chemical formulaC6H15N4O2·0.5(C6H8O4)·H2O2(C6H15N4O2)·C6H8O4
Mr265.30494.56
Crystal system, space groupMonoclinic, P21/cMonoclinic, P21
Temperature (K)298298
a, b, c (Å)13.825 (4), 5.0531 (16), 18.804 (6)12.494 (4), 5.9510 (17), 16.719 (5)
β (°) 102.900 (6) 105.977 (5)
V3)1280.5 (7)1195.1 (6)
Z42
Radiation typeMo KαMo Kα
µ (mm1)0.110.11
Crystal size (mm)0.59 × 0.11 × 0.020.25 × 0.07 × 0.06
Data collection
DiffractometerBruker SMART CCD area detector
diffractometer
Bruker SMART CCD area detector
diffractometer
Absorption correctionMulti-scan
SADABS,Sheldrick, 1997
Multi-scan
Sheldrick, 1999
Tmin, Tmax0.937, 0.9980.973, 0.994
No. of measured, independent and
observed [I > 2σ(I)] reflections
9412, 2581, 2150 6142, 3711, 3396
Rint0.0310.019
(sin θ/λ)max1)0.6250.588
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.054, 0.128, 1.05 0.039, 0.113, 0.86
No. of reflections25813711
No. of parameters247459
No. of restraints01
H-atom treatmentAll H-atom parameters refinedAll H-atom parameters refined
Δρmax, Δρmin (e Å3)0.28, 0.170.17, 0.17
Absolute structureFlack H.D. (1983), Acta Cryst. A39, 876-881Flack H.D. (1983), Acta Cryst. A39, 876-881
Absolute structure parametercentrosymmetric0.1 (11)

Computer programs: Bruker SMART, Bruker SAINT, SHELXS97 (Sheldrick, 1990), SHELXL97 (Sheldrick, 1997), ORTEP-3, PLATON (Spek, 1990).

 

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