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Accurate structure factors have been measured for the two known conformational polymorphs (A and B) of famotidine up to a maximum resolution of sin(θ)/λ = 1.2 Å−1 at 100 K using a conventional X-ray source and a CCD-based diffractometer. The experimental electron-density distribution was modelled using a multipole model and the interatomic interactions were analysed following the atoms-in-molecules theory. Excellent equivalence between most electronic and electrostatic properties in the polymorphs exists and no significant differences were found to exist across polymorphs either in the interatomic interactions (via the topological analysis) or in the atomic charges from integration of the atomic basins. Additional derived properties, such as the molecular dipole moment, similarly did not distinguish between the polymorphs. Only the molecular electrostatic potential mapped on top of the molecular surface, i.e. the isodensity contoured at 0.00675 e Å−3, was able to uncover the differences between A and B. In both conformations, the sizes of the electronegative and electropositive areas match. However, the average electrostatic potential in the electronegative area of A is −40 kJ mol−1, while the corresponding value in B is −55 kJ mol−1. Together with the physical shape and dimensions of A and B, this leads to a conclusion that the polymorphs are mutually exclusive at the same receptor binding site.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108767304017891/xc5012sup1.cif
Contains datablocks global, fama, famb

pdf

Portable Document Format (PDF) file https://doi.org/10.1107/S0108767304017891/xc5012sup2.pdf
Residual and static model densities

fcf

Structure factor file (CIF format) https://doi.org/10.1107/S0108767304017891/xc5012famasup3.fcf
Contains datablock fama0m

fcf

Structure factor file (CIF format) https://doi.org/10.1107/S0108767304017891/xc5012fambsup4.fcf
Contains datablock fambm

CCDC references: 215086; 215087

Computing details top

Figures top
[Figure 1]
[Figure 2]
[Figure 3]
(fama) top
Crystal data top
C8H15N7O2S3F(000) = 504
Mr = 337.45Dx = 1.595 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.7107 Å
Hall symbol: -P 2ybcCell parameters from 16250 reflections
a = 11.9115 (3) Åθ = 2.3–59.3°
b = 7.1876 (2) ŵ = 0.54 mm1
c = 16.6236 (4) ÅT = 100 K
β = 100.045 (1)°Block, white
V = 1401.4 (1) Å30.35 × 0.35 × 0.30 mm
Z = 4
Data collection top
Bruker CCD area detector
diffractometer
20197 independent reflections
Radiation source: fine-focus sealed tube16610 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.020
ω–scans and π–scansθmax = 59.5°, θmin = 1.8°
Absorption correction: analytical
?
h = 2828
Tmin = 0.787, Tmax = 0.887k = 017
68907 measured reflectionsl = 039
Refinement top
Refinement on FSecondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.023Riding
wR(F2) = 0.021 w = 1/[σ2(Fo2)]
S = 1.70(Δ/σ)max < 0.001
16610 reflectionsΔρmax = 0.29 e Å3
459 parametersΔρmin = 0.28 e Å3
1 restraintExtinction correction: SHELXL, none
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0
Crystal data top
C8H15N7O2S3V = 1401.4 (1) Å3
Mr = 337.45Z = 4
Monoclinic, P21/cMo Kα radiation
a = 11.9115 (3) ŵ = 0.54 mm1
b = 7.1876 (2) ÅT = 100 K
c = 16.6236 (4) Å0.35 × 0.35 × 0.30 mm
β = 100.045 (1)°
Data collection top
Bruker CCD area detector
diffractometer
20197 independent reflections
Absorption correction: analytical
?
16610 reflections with I > 2σ(I)
Tmin = 0.787, Tmax = 0.887Rint = 0.020
68907 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0231 restraint
wR(F2) = 0.021Riding
S = 1.70Δρmax = 0.29 e Å3
16610 reflectionsΔρmin = 0.28 e Å3
459 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
S(1)0.315075 (6)0.561307 (10)0.678851 (5)0.016
S(11)0.189700 (7)0.058633 (9)0.780479 (5)0.016
S(17)0.165730 (5)0.480806 (8)0.985180 (4)0.011
O(19)0.28332 (3)0.43673 (5)0.98160 (2)0.017
O(20)0.12947 (4)0.66963 (4)0.96721 (2)0.019
N(3)0.37674 (2)0.21698 (4)0.69832 (2)0.014
N(6)0.44159 (2)0.38131 (3)0.58723 (2)0.015
N(8)0.52513 (3)0.08170 (4)0.60768 (2)0.018
N(9)0.56204 (4)0.27215 (4)0.50447 (2)0.022
N(15)0.15104 (3)0.06788 (3)0.97858 (2)0.018
N(16)0.07858 (2)0.35592 (3)0.92209 (1)0.012
N(18)0.14725 (2)0.41919 (4)1.07640 (2)0.015
C(2)0.38629 (2)0.36292 (4)0.65144 (2)0.013
C(4)0.31408 (2)0.25961 (4)0.75872 (2)0.014
C(5)0.27197 (2)0.43651 (4)0.75710 (2)0.016
C(7)0.50809 (2)0.24405 (4)0.56790 (2)0.015
C(10)0.29956 (3)0.11283 (5)0.81953 (2)0.016
C(12)0.06027 (3)0.07637 (4)0.77651 (2)0.015
C(13)0.00932 (2)0.07211 (4)0.85552 (2)0.015
C(14)0.08440 (2)0.17164 (3)0.92439 (1)0.012
H(8A)0.578890.013380.590840.033
H(8B)0.486410.056300.655920.031
H(9A)0.556550.395930.475410.032
H(9B)0.614860.171540.491000.034
H(15A)0.208500.124741.023660.039
H(15B)0.145090.071330.971230.029
H(18A)0.217590.442941.118590.033
H(18B)0.076190.471291.093270.031
H(5)0.219440.490520.798750.023
H(10A)0.277150.178910.873930.027
H(10B)0.381010.040930.838080.024
H(12A)0.078570.221040.762680.021
H(12B)0.003710.024400.726130.022
H(13A)0.074900.137810.844170.024
H(13B)0.001750.072590.873210.022
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S(1)0.01534 (2)0.01255 (2)0.01842 (3)0.00217 (2)0.00433 (2)0.00062 (2)
S(11)0.02180 (3)0.01146 (2)0.01574 (3)0.00180 (2)0.00622 (2)0.00028 (2)
S(17)0.01237 (2)0.00824 (2)0.01259 (2)0.00089 (1)0.00240 (1)0.00048 (1)
O(19)0.01226 (9)0.01737 (10)0.02166 (12)0.00249 (8)0.00450 (8)0.00304 (9)
O(20)0.0255 (1)0.0081 (1)0.0217 (1)0.0003 (1)0.0036 (1)0.0010 (1)
N(3)0.01436 (7)0.01354 (7)0.01522 (8)0.00179 (6)0.00414 (6)0.00106 (6)
N(6)0.01615 (8)0.01193 (6)0.01693 (8)0.00192 (6)0.00599 (6)0.00060 (6)
N(8)0.0185 (1)0.0155 (1)0.0204 (1)0.0060 (1)0.0057 (1)0.0040 (1)
N(9)0.0268 (1)0.0159 (1)0.0246 (1)0.0068 (1)0.0144 (1)0.0036 (1)
N(15)0.0284 (1)0.0092 (1)0.0154 (1)0.0009 (1)0.0020 (1)0.0003 (1)
N(16)0.01315 (6)0.00943 (6)0.01218 (6)0.00028 (5)0.00137 (5)0.00017 (5)
N(18)0.01661 (9)0.01667 (8)0.01149 (8)0.00036 (7)0.00127 (6)0.00075 (6)
C(2)0.01206 (7)0.01225 (7)0.01466 (8)0.00076 (6)0.00268 (6)0.00024 (6)
C(4)0.01240 (7)0.01525 (8)0.01364 (8)0.00102 (6)0.00222 (6)0.00010 (6)
C(5)0.01496 (8)0.01612 (8)0.01654 (9)0.00217 (7)0.00411 (7)0.00158 (7)
C(7)0.01450 (8)0.01263 (7)0.01637 (9)0.00214 (6)0.00417 (6)0.00058 (6)
C(10)0.01516 (9)0.01987 (10)0.01398 (9)0.00219 (8)0.00249 (6)0.00240 (7)
C(12)0.01654 (9)0.01365 (8)0.01274 (8)0.00182 (7)0.00069 (6)0.00119 (6)
C(13)0.01462 (8)0.01503 (8)0.01594 (9)0.00440 (7)0.00298 (7)0.00381 (7)
C(14)0.01431 (7)0.00953 (6)0.01184 (7)0.00147 (6)0.00242 (5)0.00084 (5)
Geometric parameters (Å, º) top
S(1)—C(2)1.7594 (3)C(12)—C(13)1.5404 (4)
S(1)—C(5)1.7301 (3)C(13)—C(14)1.5050 (4)
S(11)—C(10)1.8320 (4)N(8)—H(8A)1.0090
S(11)—C(12)1.8131 (3)N(8)—H(8B)1.0090
S(17)—O(19)1.4473 (3)N(9)—H(9A)1.0090
S(17)—O(20)1.4397 (3)N(9)—H(9B)1.0090
S(17)—N(16)1.6136 (2)N(15)—H(15A)1.0090
S(17)—N(18)1.6311 (2)N(15)—H(15B)1.0090
N(3)—C(2)1.3234 (4)N(18)—H(18A)1.0090
N(3)—C(4)1.3858 (4)N(18)—H(18B)1.0090
N(6)—C(2)1.3548 (4)C(5)—H(5)1.0830
N(6)—C(7)1.3390 (3)C(10)—H(10A)1.0950
N(8)—C(7)1.3392 (4)C(10)—H(10B)1.0950
N(9)—C(7)1.3425 (4)C(12)—H(12A)1.0950
N(15)—C(14)1.3223 (4)C(12)—H(12B)1.0950
N(16)—C(14)1.3266 (3)C(13)—H(13A)1.0950
C(4)—C(5)1.3654 (4)C(13)—H(13B)1.0950
C(4)—C(10)1.4919 (4)
C(2)—S(1)—C(5)89.671 (13)C(7)—N(8)—H(8B)119.95
C(10)—S(11)—C(12)101.723 (13)H(8A)—N(8)—H(8B)119.87
O(19)—S(17)—O(20)117.08 (2)C(7)—N(9)—H(9A)120.58
O(19)—S(17)—N(16)111.654 (16)C(7)—N(9)—H(9B)117.97
O(19)—S(17)—N(18)105.51 (2)H(9A)—N(9)—H(9B)121.10
O(20)—S(17)—N(16)104.704 (18)C(14)—N(15)—H(15A)121.76
O(20)—S(17)—N(18)111.381 (19)C(14)—N(15)—H(15B)117.11
N(16)—S(17)—N(18)106.106 (12)H(15A)—N(15)—H(15B)121.05
C(2)—N(3)—C(4)111.34 (2)S(17)—N(18)—H(18A)111.71
C(2)—N(6)—C(7)120.42 (3)S(17)—N(18)—H(18B)114.42
S(17)—N(16)—C(14)120.81 (2)H(18A)—N(18)—H(18B)112.29
S(1)—C(2)—N(3)113.26 (2)S(1)—C(5)—H(5)125.11
S(1)—C(2)—N(6)116.59 (2)C(4)—C(5)—H(5)124.92
N(3)—C(2)—N(6)130.15 (3)S(11)—C(10)—H(10A)108.81
N(3)—C(4)—C(5)115.72 (3)S(11)—C(10)—H(10B)108.99
N(3)—C(4)—C(10)118.38 (2)C(4)—C(10)—H(10A)109.07
C(5)—C(4)—C(10)125.90 (3)C(4)—C(10)—H(10B)108.84
S(1)—C(5)—C(4)109.97 (2)H(10A)—C(10)—H(10B)107.68
N(6)—C(7)—N(8)124.65 (3)S(11)—C(12)—H(12A)108.47
N(6)—C(7)—N(9)117.51 (3)S(11)—C(12)—H(12B)108.62
N(8)—C(7)—N(9)117.83 (3)C(13)—C(12)—H(12A)108.69
S(11)—C(10)—C(4)113.31 (2)C(13)—C(12)—H(12B)108.67
S(11)—C(12)—C(13)114.66 (2)H(12A)—C(12)—H(12B)107.51
C(12)—C(13)—C(14)111.65 (2)C(12)—C(13)—H(13A)109.26
N(15)—C(14)—N(16)127.23 (3)C(12)—C(13)—H(13B)109.37
N(15)—C(14)—C(13)117.17 (2)C(14)—C(13)—H(13A)109.34
N(16)—C(14)—C(13)115.56 (2)C(14)—C(13)—H(13B)109.31
C(7)—N(8)—H(8A)120.14H(13A)—C(13)—H(13B)107.84
(famb) top
Crystal data top
C8H15N7O2S3F(000) = 504
Mr = 337.45Dx = 1.561 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.7107 Å
Hall symbol: -P 2ybcCell parameters from 8948 reflections
a = 16.980 (2) Åθ = 2.2–29.5°
b = 5.285 (1) ŵ = 0.54 mm1
c = 17.639 (2) ÅT = 100 K
β = 116.416 (1)°Block, white
V = 1418.0 (4) Å30.40 × 0.30 × 0.25 mm
Z = 4
Data collection top
Bruker CCD area detector
diffractometer
17385 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.025
Graphite monochromatorθmax = 60.0°, θmin = 2.2°
ω–scans and π–scansh = 4137
70467 measured reflectionsk = 012
21282 independent reflectionsl = 043
Refinement top
Refinement on FSecondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.024Riding
wR(F2) = 0.021 w = 1/[σ2(Fo2)]
S = 1.62(Δ/σ)max < 0.001
17385 reflectionsΔρmax = 0.36 e Å3
459 parametersΔρmin = 0.27 e Å3
1 restraintExtinction correction: SHELXL, none
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0
Crystal data top
C8H15N7O2S3V = 1418.0 (4) Å3
Mr = 337.45Z = 4
Monoclinic, P21/nMo Kα radiation
a = 16.980 (2) ŵ = 0.54 mm1
b = 5.285 (1) ÅT = 100 K
c = 17.639 (2) Å0.40 × 0.30 × 0.25 mm
β = 116.416 (1)°
Data collection top
Bruker CCD area detector
diffractometer
17385 reflections with I > 2σ(I)
70467 measured reflectionsRint = 0.025
21282 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0241 restraint
wR(F2) = 0.021Riding
S = 1.62Δρmax = 0.36 e Å3
17385 reflectionsΔρmin = 0.27 e Å3
459 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
S(1)0.867925 (5)0.033416 (14)0.724949 (5)0.015
S(11)0.574210 (4)0.230221 (13)0.465606 (5)0.013
S(17)0.811208 (4)0.136561 (12)0.376405 (4)0.010
O(19)0.88904 (2)0.05994 (8)0.45002 (2)0.015
O(20)0.80780 (2)0.07776 (7)0.29470 (2)0.015
N(3)0.76934 (2)0.35216 (5)0.61233 (2)0.013
N(6)0.92556 (2)0.40819 (6)0.66020 (2)0.015
N(8)0.83836 (2)0.68654 (6)0.54881 (2)0.014
N(9)0.98867 (2)0.71086 (12)0.61104 (3)0.030
N(15)0.61229 (2)0.17846 (6)0.26752 (2)0.014
N(16)0.73205 (2)0.00285 (5)0.38788 (2)0.013
N(18)0.80726 (2)0.44097 (5)0.37908 (2)0.015
C(2)0.85278 (2)0.29462 (5)0.65851 (2)0.012
C(4)0.71446 (2)0.18750 (5)0.62646 (2)0.013
C(5)0.75520 (2)0.00140 (6)0.68423 (2)0.016
C(7)0.91587 (2)0.59775 (6)0.60691 (2)0.015
C(10)0.61732 (2)0.22663 (7)0.58035 (2)0.016
C(12)0.60209 (2)0.08930 (5)0.44891 (2)0.013
C(13)0.58560 (2)0.12241 (6)0.35702 (2)0.014
C(14)0.64808 (2)0.03272 (5)0.33575 (2)0.011
H(8A)0.783450.629220.552430.026
H(8B)0.841680.850580.521110.030
H(9A)0.988190.844050.569850.043
H(9B)1.046100.617060.641250.054
H(15A)0.546400.172970.232770.028
H(15B)0.649320.272060.245090.027
H(18A)0.762410.505830.322460.033
H(18B)0.807000.509750.432330.033
H(5)0.721900.144690.702060.022
H(10A)0.600940.406500.600720.023
H(10B)0.584530.075590.598040.023
H(12A)0.671390.126690.491200.017
H(12B)0.562080.225040.463550.016
H(13A)0.592870.322620.345450.021
H(13B)0.517890.066540.315130.021
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S(1)0.01489 (2)0.01349 (2)0.01206 (2)0.00118 (2)0.00514 (2)0.00351 (2)
S(11)0.01099 (2)0.01157 (2)0.01386 (2)0.00004 (2)0.00460 (2)0.00019 (2)
S(17)0.00776 (2)0.01011 (2)0.00880 (2)0.00033 (1)0.00338 (1)0.00064 (1)
O(19)0.00820 (7)0.01947 (12)0.01366 (10)0.00016 (8)0.00199 (7)0.00574 (9)
O(20)0.01492 (9)0.01591 (10)0.01202 (10)0.00055 (8)0.00749 (8)0.00216 (8)
N(3)0.00894 (6)0.01374 (7)0.01269 (7)0.00110 (6)0.00382 (5)0.00281 (6)
N(6)0.00833 (6)0.01985 (9)0.01396 (8)0.00051 (6)0.00296 (6)0.00628 (7)
N(8)0.01184 (7)0.01539 (9)0.01215 (8)0.00024 (7)0.00442 (6)0.00409 (6)
N(9)0.01190 (9)0.0409 (2)0.02998 (18)0.00494 (12)0.00586 (10)0.01889 (17)
N(15)0.00933 (6)0.01675 (9)0.01144 (8)0.00046 (6)0.00328 (6)0.00259 (6)
N(16)0.00806 (6)0.01426 (7)0.01238 (7)0.00085 (5)0.00366 (5)0.00291 (6)
N(18)0.01778 (9)0.01034 (8)0.01252 (8)0.00131 (7)0.00554 (7)0.00085 (6)
C(2)0.00926 (7)0.01337 (8)0.01078 (7)0.00047 (6)0.00356 (6)0.00227 (6)
C(4)0.01094 (7)0.01374 (8)0.01179 (8)0.00275 (6)0.00540 (6)0.00045 (6)
C(5)0.01650 (9)0.01368 (9)0.01388 (9)0.00308 (8)0.00741 (8)0.00132 (7)
C(7)0.00941 (7)0.01923 (10)0.01323 (9)0.00182 (7)0.00369 (6)0.00500 (8)
C(10)0.01098 (8)0.01891 (11)0.01500 (10)0.00291 (8)0.00691 (7)0.00223 (8)
C(12)0.01116 (7)0.01236 (8)0.01350 (9)0.00025 (6)0.00630 (7)0.00163 (6)
C(13)0.01057 (7)0.01417 (9)0.01337 (9)0.00325 (7)0.00534 (7)0.00073 (7)
C(14)0.00826 (6)0.01206 (7)0.01037 (7)0.00095 (6)0.00383 (6)0.00023 (6)
Geometric parameters (Å, º) top
S(1)—C(2)1.7542 (3)C(12)—C(13)1.5272 (4)
S(1)—C(5)1.7278 (4)C(13)—C(14)1.5142 (4)
S(11)—C(10)1.8205 (3)N(8)—H(8A)1.0090
S(11)—C(12)1.8129 (3)N(8)—H(8B)1.0090
S(17)—O(19)1.4387 (3)N(9)—H(9A)1.0090
S(17)—O(20)1.4501 (3)N(9)—H(9B)1.0090
S(17)—N(16)1.6090 (3)N(15)—H(15A)1.0090
S(17)—N(18)1.6118 (3)N(15)—H(15B)1.0090
N(3)—C(2)1.3177 (4)N(18)—H(18A)1.0090
N(3)—C(4)1.3764 (4)N(18)—H(18B)1.0090
N(6)—C(2)1.3622 (4)C(5)—H(5)1.0830
N(6)—C(7)1.3329 (4)C(10)—H(10A)1.0950
N(8)—C(7)1.3425 (4)C(10)—H(10B)1.0950
N(9)—C(7)1.3457 (4)C(12)—H(12A)1.0950
N(15)—C(14)1.3267 (4)C(12)—H(12B)1.0950
N(16)—C(14)1.3179 (4)C(13)—H(13A)1.0950
C(4)—C(5)1.3627 (4)C(13)—H(13B)1.0950
C(4)—C(10)1.4938 (4)
C(2)—S(1)—C(5)89.616 (14)C(7)—N(8)—H(8B)115.03
C(10)—S(11)—C(12)99.556 (15)H(8A)—N(8)—H(8B)122.74
O(19)—S(17)—O(20)116.82 (2)C(7)—N(9)—H(9A)123.91
O(19)—S(17)—N(16)104.250 (16)C(7)—N(9)—H(9B)117.32
O(19)—S(17)—N(18)106.74 (2)H(9A)—N(9)—H(9B)114.80
O(20)—S(17)—N(16)111.389 (18)C(14)—N(15)—H(15A)118.11
O(20)—S(17)—N(18)105.021 (19)C(14)—N(15)—H(15B)121.76
N(16)—S(17)—N(18)112.752 (17)H(15A)—N(15)—H(15B)119.46
C(2)—N(3)—C(4)111.75 (3)S(17)—N(18)—H(18A)109.45
C(2)—N(6)—C(7)119.31 (3)S(17)—N(18)—H(18B)113.85
S(17)—N(16)—C(14)124.38 (2)H(18A)—N(18)—H(18B)119.03
S(1)—C(2)—N(3)113.10 (2)S(1)—C(5)—H(5)125.04
S(1)—C(2)—N(6)118.04 (2)C(4)—C(5)—H(5)125.08
N(3)—C(2)—N(6)128.85 (3)S(11)—C(10)—H(10A)108.70
N(3)—C(4)—C(5)115.62 (3)S(11)—C(10)—H(10B)108.69
N(3)—C(4)—C(10)119.11 (3)C(4)—C(10)—H(10A)108.76
C(5)—C(4)—C(10)125.26 (3)C(4)—C(10)—H(10B)108.79
S(1)—C(5)—C(4)109.88 (2)H(10A)—C(10)—H(10B)107.68
N(6)—C(7)—N(8)124.93 (3)S(11)—C(12)—H(12A)109.67
N(6)—C(7)—N(9)118.26 (3)S(11)—C(12)—H(12B)109.73
N(8)—C(7)—N(9)116.81 (3)C(13)—C(12)—H(12A)109.66
S(11)—C(10)—C(4)114.027 (19)C(13)—C(12)—H(12B)109.59
S(11)—C(12)—C(13)109.96 (2)H(12A)—C(12)—H(12B)108.21
C(12)—C(13)—C(14)112.53 (2)C(12)—C(13)—H(13A)109.02
N(15)—C(14)—N(16)128.26 (3)C(12)—C(13)—H(13B)109.09
N(15)—C(14)—C(13)116.77 (3)C(14)—C(13)—H(13A)109.11
N(16)—C(14)—C(13)114.97 (2)C(14)—C(13)—H(13B)109.14
C(7)—N(8)—H(8A)117.80H(13A)—C(13)—H(13B)107.85

Experimental details

(fama)(famb)
Crystal data
Chemical formulaC8H15N7O2S3C8H15N7O2S3
Mr337.45337.45
Crystal system, space groupMonoclinic, P21/cMonoclinic, P21/n
Temperature (K)100100
a, b, c (Å)11.9115 (3), 7.1876 (2), 16.6236 (4)16.980 (2), 5.285 (1), 17.639 (2)
β (°) 100.045 (1) 116.416 (1)
V3)1401.4 (1)1418.0 (4)
Z44
Radiation typeMo KαMo Kα
µ (mm1)0.540.54
Crystal size (mm)0.35 × 0.35 × 0.300.40 × 0.30 × 0.25
Data collection
DiffractometerBruker CCD area detector
diffractometer
Bruker CCD area detector
diffractometer
Absorption correctionAnalytical
Tmin, Tmax0.787, 0.887
No. of measured, independent and
observed [I > 2σ(I)] reflections
68907, 20197, 16610 70467, 21282, 17385
Rint0.0200.025
(sin θ/λ)max1)1.2121.219
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.023, 0.021, 1.70 0.024, 0.021, 1.62
No. of reflections1661017385
No. of parameters459459
No. of restraints11
H-atom treatmentRidingRiding
Δρmax, Δρmin (e Å3)0.29, 0.280.36, 0.27

Selected geometric parameters (Å, º) for (fama) top
S(1)—C(2)1.7594 (3)N(6)—C(2)1.3548 (4)
S(1)—C(5)1.7301 (3)N(6)—C(7)1.3390 (3)
S(11)—C(10)1.8320 (4)N(8)—C(7)1.3392 (4)
S(11)—C(12)1.8131 (3)N(9)—C(7)1.3425 (4)
S(17)—O(19)1.4473 (3)N(15)—C(14)1.3223 (4)
S(17)—O(20)1.4397 (3)N(16)—C(14)1.3266 (3)
S(17)—N(16)1.6136 (2)C(4)—C(5)1.3654 (4)
S(17)—N(18)1.6311 (2)C(4)—C(10)1.4919 (4)
N(3)—C(2)1.3234 (4)C(12)—C(13)1.5404 (4)
N(3)—C(4)1.3858 (4)C(13)—C(14)1.5050 (4)
C(2)—S(1)—C(5)89.671 (13)N(3)—C(4)—C(5)115.72 (3)
C(10)—S(11)—C(12)101.723 (13)N(3)—C(4)—C(10)118.38 (2)
O(19)—S(17)—O(20)117.08 (2)C(5)—C(4)—C(10)125.90 (3)
O(19)—S(17)—N(16)111.654 (16)S(1)—C(5)—C(4)109.97 (2)
O(19)—S(17)—N(18)105.51 (2)N(6)—C(7)—N(8)124.65 (3)
O(20)—S(17)—N(16)104.704 (18)N(6)—C(7)—N(9)117.51 (3)
O(20)—S(17)—N(18)111.381 (19)N(8)—C(7)—N(9)117.83 (3)
N(16)—S(17)—N(18)106.106 (12)S(11)—C(10)—C(4)113.31 (2)
C(2)—N(3)—C(4)111.34 (2)S(11)—C(12)—C(13)114.66 (2)
C(2)—N(6)—C(7)120.42 (3)C(12)—C(13)—C(14)111.65 (2)
S(17)—N(16)—C(14)120.81 (2)N(15)—C(14)—N(16)127.23 (3)
S(1)—C(2)—N(3)113.26 (2)N(15)—C(14)—C(13)117.17 (2)
S(1)—C(2)—N(6)116.59 (2)N(16)—C(14)—C(13)115.56 (2)
N(3)—C(2)—N(6)130.15 (3)
Selected geometric parameters (Å, º) for (famb) top
S(1)—C(2)1.7542 (3)N(6)—C(2)1.3622 (4)
S(1)—C(5)1.7278 (4)N(6)—C(7)1.3329 (4)
S(11)—C(10)1.8205 (3)N(8)—C(7)1.3425 (4)
S(11)—C(12)1.8129 (3)N(9)—C(7)1.3457 (4)
S(17)—O(19)1.4387 (3)N(15)—C(14)1.3267 (4)
S(17)—O(20)1.4501 (3)N(16)—C(14)1.3179 (4)
S(17)—N(16)1.6090 (3)C(4)—C(5)1.3627 (4)
S(17)—N(18)1.6118 (3)C(4)—C(10)1.4938 (4)
N(3)—C(2)1.3177 (4)C(12)—C(13)1.5272 (4)
N(3)—C(4)1.3764 (4)C(13)—C(14)1.5142 (4)
C(2)—S(1)—C(5)89.616 (14)N(3)—C(4)—C(5)115.62 (3)
C(10)—S(11)—C(12)99.556 (15)N(3)—C(4)—C(10)119.11 (3)
O(19)—S(17)—O(20)116.82 (2)C(5)—C(4)—C(10)125.26 (3)
O(19)—S(17)—N(16)104.250 (16)S(1)—C(5)—C(4)109.88 (2)
O(19)—S(17)—N(18)106.74 (2)N(6)—C(7)—N(8)124.93 (3)
O(20)—S(17)—N(16)111.389 (18)N(6)—C(7)—N(9)118.26 (3)
O(20)—S(17)—N(18)105.021 (19)N(8)—C(7)—N(9)116.81 (3)
N(16)—S(17)—N(18)112.752 (17)S(11)—C(10)—C(4)114.027 (19)
C(2)—N(3)—C(4)111.75 (3)S(11)—C(12)—C(13)109.96 (2)
C(2)—N(6)—C(7)119.31 (3)C(12)—C(13)—C(14)112.53 (2)
S(17)—N(16)—C(14)124.38 (2)N(15)—C(14)—N(16)128.26 (3)
S(1)—C(2)—N(3)113.10 (2)N(15)—C(14)—C(13)116.77 (3)
S(1)—C(2)—N(6)118.04 (2)N(16)—C(14)—C(13)114.97 (2)
N(3)—C(2)—N(6)128.85 (3)
 

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