Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S2056989015000663/cv5481sup1.cif | |
Rietveld powder data file (CIF format) https://doi.org/10.1107/S2056989015000663/cv5481Isup2.rtv | |
Rietveld powder data file (CIF format) https://doi.org/10.1107/S2056989015000663/cv5481IIsup3.rtv |
CCDC references: 1043290; 1043289
Key indicators
- Powder X-ray study
- T = 298 K
- Mean (C-C) = 0.020 Å
- Mean (C-C) = 0.020 Å
- R factor = 0.000
- wR factor = 0.000
- Data-to-parameter ratio = 0.0
checkCIF/PLATON results
No syntax errors found Datablock: I
Alert level B PLAT340_ALERT_3_B Low Bond Precision on C-C Bonds ............... 0.0197 Ang.
Author Response: Our data are from Powder X-Ray diffraction |
Alert level G PLAT007_ALERT_5_G Number of Unrefined Donor-H Atoms .............. 3 Report PLAT720_ALERT_4_G Number of Unusual/Non-Standard Labels .......... 3 Note PLAT981_ALERT_1_G No non-zero f" Anomalous Scattering Values Found Please Check PLAT986_ALERT_1_G No non-zero f' Anomalous Scattering Values Found Please Check
0 ALERT level A = Most likely a serious problem - resolve or explain 1 ALERT level B = A potentially serious problem, consider carefully 0 ALERT level C = Check. Ensure it is not caused by an omission or oversight 4 ALERT level G = General information/check it is not something unexpected 2 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 0 ALERT type 2 Indicator that the structure model may be wrong or deficient 1 ALERT type 3 Indicator that the structure quality may be low 1 ALERT type 4 Improvement, methodology, query or suggestion 1 ALERT type 5 Informative message, check
Datablock: II
Alert level B PLAT112_ALERT_2_B ADDSYM Detects Additional (Pseudo) Symm. Elem... c/2 Check
Author Response: There is not any pseudo translation. There is a one molecule in asymmetry unit with triclinic systsm in P-1 space group |
PLAT340_ALERT_3_B Low Bond Precision on C-C Bonds ............... 0.0197 Ang.
Author Response: Our data are from Powder X-Ray diffraction |
Alert level C PLAT213_ALERT_2_C Atom S1 has ADP max/min Ratio ..... 3.4 prolat
Alert level G PLAT007_ALERT_5_G Number of Unrefined Donor-H Atoms .............. 3 Report PLAT720_ALERT_4_G Number of Unusual/Non-Standard Labels .......... 3 Note PLAT764_ALERT_4_G Overcomplete CIF Bond List Detected (Rep/Expd) . 1.13 Ratio PLAT860_ALERT_3_G Number of Least-Squares Restraints ............. 1 Note PLAT981_ALERT_1_G No non-zero f" Anomalous Scattering Values Found Please Check PLAT986_ALERT_1_G No non-zero f' Anomalous Scattering Values Found Please Check
0 ALERT level A = Most likely a serious problem - resolve or explain 2 ALERT level B = A potentially serious problem, consider carefully 1 ALERT level C = Check. Ensure it is not caused by an omission or oversight 6 ALERT level G = General information/check it is not something unexpected 2 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 2 ALERT type 2 Indicator that the structure model may be wrong or deficient 2 ALERT type 3 Indicator that the structure quality may be low 2 ALERT type 4 Improvement, methodology, query or suggestion 1 ALERT type 5 Informative message, check
The chemistry of semicarbazones and thiosemicarbazones is especially interesting due to their special role in biological applications such as anti-proliferative, anti-tumoral, anti-convulsant, anti-trypanosomal, herbicidal and biocidal activities (Beraldo et al., 2002; Kasuga et al., 2003; Teixeira et al., 2003; Beraldo & Gambino, 2004; Mikhaleva et al., 2008; de Oliveira et al., 2008; Alomar et al., 2012; Gan et al., 2014). They are also important intermediates in organic synthesis, mainly for obtaining heterocyclic rings, such as thiazolidones, oxadiazoles, pyrazolidones, and thiadiazoles (Greenbaum et al., 2004; Küçükgüzel et al., 2006). Semicarbazones and thiosemicarbazones have received considerable attention in view of their simplicity of preparation, various complexing abilities and coordination behavior that can be used in analytical applications (Garg & Jain, 1988; Casas et al., 2000). They are of interest from a supramolecular point of view since they can be functionalized to give different supramolecular arrays.
Compounds (I) and (II) crystallize in centrosymmetric space groups P21/c and P1, respectively, with one molecule in the asymmetric unit. Each molecule has an intramolecular N—H···N hydrogen bond (Tables 1 and 2), which forms an S(5) ring. The semicarbazone and thiosemicarbazone fragments in the compounds show an E conformation around the imine C=N bond. The molecules (Fig. 1) are approximately planar, with a dihedral angle of 2.59 (5)° between the C1/C2/C3 crotonaldehyde plane and the mean plane of the C4/N1/N2/C5/O1/N3 semicarbazone fragment for (I), and of 9.12 (5)° between the C1/C2/C3 crotonaldehyde plane and the mean plane of the C4/N1/N2/C5/S1/N3 thiosemicarbazone fragment for (II). All bond lengths and angles in (I) and (II) are normal and correspond well to those observed in the crystal structures of related semi- and thiosemicarbazone derivatives, viz. acetone semicarbazone and benzaldehydesemicarbazone (Naik & Palenik, 1974), 3,4- methylenedioxybenzaldehydesemicarbazone (Wang et al., 2004), isatin 3-semicarbazone and 1-methylisatin 3-semicarbazone (Pelosi et al., 2005), 4- (methylsulfanyl)benzaldehydethiosemicarbazone (Yathirajan et al., 2006), 4-(methylsulfanyl)benzaldehydesemicarbazone (Sarojini et al., 2007), 5-hydroxy-2-nitrobenzaldehyde thiosemicarbazone (Reddy et al., 2014) and 1-(4-formylbenzylidene) thiosemicarbazone (Carballo et al., 2014).
As a result of the presence of potential hydrogen-donor sites in molecules (I) and (II), supramolecular hydrogen-bonding interactions are observed in both compounds (Tables 1 and 2). In the crystal of (I), molecules are linked by pairs of N—H···O hydrogen bonds, forming inversion dimers with R22(8) ring motifs (Fig. 2a). The resulting dimers are connected through N—H···O hydrogen bonds, forming layers parallel to bc plane. In the crystal of (II), molecules are linked by weak N—H···S hydrogen bonds, forming chains propagating in [110] (Fig. 2b).
All reactions and manipulations were carried out in air with reagent grade solvents. The IR spectra were recorded on a Jasco FT–IR 300E instrument. 1H and 13C{1H} NMR spectra were recorded on a Bruker Bio spin 400 spectrometer. Microanalysis was performed using EURO EA. Powder X-ray diffraction data were collected with Stoe Transmission diffractometer (Stadi P).
For the synthesis of (I), a mixture of semicarbazide hydrochloride (CH5N3O·HCl; 0.5 g, 4.5 mmol) and sodium acetate (CH3COONa; 0.75 g, 9.1 mmol) in 10 ml water was agitated well and crotonaldehyde (0.5 g, 7.1 mmol) was added slowly with stirring. On completion of the addition, the reaction mixture was agitated for 24 h at room temperature. The solid product which formed was separated by filtration and washed with water and finally recrystallized from absolute ethanol to produce the product (I) (white powder; m.p. 481–482 K) in 55.5 % yield.
IR (KBr, ν, cm-1): 3456, 3281, 3192 (NH2), (1668–1638) (C═O); 1H NMR (400 MHz, CD3OD) δ p.p.m. 1.76 (d, J = 4.42 Hz, 3H, –CH3), 6.43–5.46 (m, 2H, –HC═CH–), 7.39 (d, J = 7.19 Hz, 1H, HC═N–).13C NMR (100 MHz, CD3OD) δ p.p.m. 18.52 (CH3), 130.01 (–HC═CH–), 137.62 (–HC═CH–), 145.64 (N═C) , 160.19 (C═O). Analysis calculated for (I): C, 47.23; H, 7.13; N, 33.05, 12.58 O%. Found: C, 46.43; H, 6.08; N, 34.69%
For the synthesis of (II), crotonaldehyde (0.5 g, 7.1 mmol) was added to thiosemicarbazide (CH5N3S; 0.65 g, 7.1 mmol) in 5 ml water and the mixture was stirred at room temperature for 24 h. The product was separated by filtration and recrystallized from absolute ethanol to produce the product (II) (white powder; m.p. 435–436 K) in 72.5% yield.
IR (KBr, ν, cm-1): 3323, 3244, 3164 (NH2), 1650(C═S). 1H NMR (400 MHz, CDCl3) δ p.p.m. 1.90 (d, J = 5.86 Hz, 3H, –CH3), 6.07–6.27 (m, 2H, –HC═CH–), 6.49 (sb, 1H), 7.10 (sb, 1H) 7.60 (d, J = 8.57 Hz, 1H, HC═N–), 10.10 (sb, 2H). 13C NMR (100.6 MHz, CDCl3) 18.73 (CH3), 127.70 (–HC═CH–), 140.58 (–HC═CH–), 146.21 (N═C), 177.95 (C═S). Analysis calculated for (II): C, 41.93; H, 6.33; N, 29.34.05, 22.39 S%. Found: C, 41.89; H, 6.25; N, 31.88%.
Crystal data, data collection and structure refinement details are summarized in Table 2. Compounds (I) and (II) crystallized in the form of a very fine white powder. Since no single crystals of sufficient size and quality could be obtained, the crystal structures of both compounds were determined from X-ray powder diffraction patterns. The powder samples of (I) and (II) were lightly ground in a mortar, loaded into two Mylar foils and fixed onto the sample holder with a mask of suitable internal diameter (8.0 mm). The powder X-ray diffraction data were collected at room temperature with a STOE transmission STADI-P diffractometer using monochromatic Cu Ka1 radiation (λ= 1.54060 Å) selected with an incident beam curved-crystal germanium Ge(111) monochromator with a linear position-sensitive detector (PSD). The patterns were scanned over the angular range 5.0–80.0° (2θ). For pattern indexing, the extraction of the peak positions was carried out with the program WinPLOTR (Roisnel & Rodríguez-Carvajal, 2000). Pattern indexing was performed with the program DICVOL4.0 (Boultif & Louër, 2004). The first 20 lines of the powder pattern were indexed completely on the basis of a monoclinic cell for (I) and a triclinic cell for (II). The figures of merit (de Wolff et al., 1968; Smith & Snyder, 1979) are sufficiently acceptable to support the obtained indexing results [M(20) = 50.5, F(20) = 71.9 (0.0034, 83)] for (I) and [M(20) = 61.8, F(20) = 96.0 (0.0051, 41)] for (II). The best estimated space groups were P21/c in the monoclinic system for (I) and P1 in the triclinic system for (II).
The whole powder diffraction patterns from 5 to 80° (2θ) for the two compounds (I) and (II) were subsequently refined with cell and resolution constraints (Le Bail et al., 1988) using the profile-matching option of the program FULLPROF (Rodríguez-Carvajal, 2001). The number of molecules per unit cell was estimated to be Z = 4 for (I) and Z = 2 for (II). The initial crystal structures for (I) and (II) were determined by direct methods using the program EXPO2014 (Altomare et al., 2013). The models found by this program were introduced into the program GSAS (Larson & Von Dreele, 2004) implemented in EXPGUI (Toby, 2001) for Rietveld refinement. During the Rietveld refinements, the background was refined using a shifted Chebyshev polynomial with 20 coefficients. The effect of asymmetry of low-order peaks was corrected using a pseudo-Voigt description of the peak shape (Thompson et al., 1987), which allows for angle-dependent asymmetry with axial divergence (Finger et al., 1994) and microstrain broadening, as described by Stephens (1999). The two asymmetry parameters of this function, S/L and D/L, were both fixed at 0.022 during this refinement. Intensities were corrected from absorption effects with a function for a plate sample in transmission geometry with a µ·d value of 0.15 for (I) and 0.72 for (II) (µ is the absorption coefficient and d is the sample thickness). These µ·d values were determined experimentally.
Before the final refinement, all H atoms were introduced in geometrically calculated positions. The coordinates of these H atoms were refined with strict restraints on bond lengths and angles until a suitable geometry was obtained, after that they were fixed in the final stage of the refinement. No soft restraints were imposed for (I), while for (II) the bond CH3—CH was a clearly stretched (close to1.6 Å), therefore a single soft restraint was carried out to obtain a normal value (1.49 Å). The final refinement cycles were performed using isotropic atomic displacement parameters for the C, N and O atoms, an anisotropic atomic displacement parameter for S atom in (II) and a fixed global isotropic atomic displacement parameter for the H atoms. The preferred orientation was modelled with 12 coefficients using a spherical harmonics correction (Von Dreele, 1997) of intensities in the final refinement. The use of the preferred orientation correction leads to a better molecular geometry with better agreement factors. The final Rietveld plots of the X-ray diffraction patterns for both (I) and (II) are given in Fig. 3.
For both compounds, data collection: WinXPOW (Stoe & Cie, 1999). Data reduction: WinXPOW (Stoe & Cie, 1999) for (I). For both compounds, program(s) used to solve structure: EXPO2014 (Altomare et al., 2013); program(s) used to refine structure: GSAS (Larson & Von Dreele, 2004); molecular graphics: ORTEP-3 for Windows (Farrugia, 2012), Mercury (Macrae et al., 2006); software used to prepare material for publication: publCIF (Westrip, 2010).
C5H9N3O | Z = 4 |
Mr = 127.15 | F(000) = 272 |
Monoclinic, P21/c | Dx = 1.222 Mg m−3 |
Hall symbol: -P 2ybc | Cu Kα1 radiation, λ = 1.5406 Å |
a = 11.1646 (3) Å | µ = 0.74 mm−1 |
b = 5.13891 (9) Å | T = 298 K |
c = 13.0301 (2) Å | Particle morphology: fine powder |
β = 112.3496 (11)° | white |
V = 691.43 (3) Å3 | flat sheet, 8 × 8 mm |
Stoe transmission Stadi-P diffractometer | Data collection mode: transmission |
Radiation source: sealed X-ray tube | Scan method: step |
Ge 111 monochromator | 2θmin = 5°, 2θmax = 80°, 2θstep = 0.02° |
Specimen mounting: Powder loaded into two Mylar foils |
Least-squares matrix: full | Profile function: CW Profile function number 4 with 21 terms Pseudovoigt profile coefficients as parameterized in (Thompson et al., 1987) Asymmetry correction of Finger et al., 1994. Microstrain broadening by P.W. Stephens, (1999. #1(GU) = 0.000 #2(GV) = 0.000 #3(GW) = 10.054 #4(GP) = 0.000 #5(LX) = 2.972 #6(ptec) = 0.00 #7(trns) = 0.00 #8(shft) = 0.0000 #9(sfec) = 0.00 #10(S/L) = 0.0220 #11(H/L) = 0.0220 #12(eta) = 0.6000 #13(S400 ) = 2.1E-01 #14(S040 ) = 3.3E-01 #15(S004 ) = 4.2E-02 #16(S220 ) = 2.1E-02 #17(S202 ) = 4.8E-03 #18(S022 ) = 8.7E-02 #19(S301 ) = -3.5E-03 #20(S103 ) = 5.2E-02 #21(S121 ) = 5.4E-02 Peak tails are ignored where the intensity is below 0.0010 times the peak Aniso. broadening axis 0.0 0.0 1.0 |
Rp = 0.027 | 121 parameters |
Rwp = 0.036 | 0 restraints |
Rexp = 0.029 | H-atom parameters not refined |
R(F2) = 0.02795 | Weighting scheme based on measured s.u.'s |
χ2 = 1.613 | (Δ/σ)max = 0.03 |
3750 data points | Background function: GSAS Background function number 1 with 20 terms. Shifted Chebyshev function of 1st kind 1: 983.478 2: -916.772 3: 421.914 4: -92.3775 5: -9.18321 6: 30.2365 7: -2.25826 8: -10.7421 9: -19.9256 10: 25.6982 11: -24.5216 12: 4.20376 13: 6.93721 14: -3.88406 15: -7.36711 16: 7.71847 17: -1.82508 18: -0.259371 19: -0.220296 20: 0.765767 |
C5H9N3O | V = 691.43 (3) Å3 |
Mr = 127.15 | Z = 4 |
Monoclinic, P21/c | Cu Kα1 radiation, λ = 1.5406 Å |
a = 11.1646 (3) Å | µ = 0.74 mm−1 |
b = 5.13891 (9) Å | T = 298 K |
c = 13.0301 (2) Å | flat sheet, 8 × 8 mm |
β = 112.3496 (11)° |
Stoe transmission Stadi-P diffractometer | Scan method: step |
Specimen mounting: Powder loaded into two Mylar foils | 2θmin = 5°, 2θmax = 80°, 2θstep = 0.02° |
Data collection mode: transmission |
Rp = 0.027 | 3750 data points |
Rwp = 0.036 | 121 parameters |
Rexp = 0.029 | 0 restraints |
R(F2) = 0.02795 | H-atom parameters not refined |
χ2 = 1.613 |
x | y | z | Uiso*/Ueq | ||
C1 | 0.935 (2) | 0.8319 (18) | 0.3282 (11) | 0.057 (5)* | |
H1a | 0.88432 | 0.92372 | 0.25964 | 0.075* | |
H1b | 0.96701 | 0.95714 | 0.38819 | 0.075* | |
H1c | 1.00844 | 0.74948 | 0.31821 | 0.075* | |
C2 | 0.855 (2) | 0.6310 (16) | 0.3552 (13) | 0.052 (4)* | |
H2 | 0.8297 | 0.48475 | 0.30627 | 0.075* | |
C3 | 0.8056 (15) | 0.6448 (14) | 0.4352 (9) | 0.033 (4)* | |
H3 | 0.80211 | 0.8092 | 0.46492 | 0.05* | |
C4 | 0.7367 (18) | 0.4405 (17) | 0.4558 (11) | 0.032 (4)* | |
H4 | 0.73987 | 0.27746 | 0.42622 | 0.075* | |
N1 | 0.7027 (14) | 0.4632 (13) | 0.5417 (7) | 0.025 (3)* | |
N2 | 0.6313 (12) | 0.2520 (15) | 0.5530 (7) | 0.031 (3)* | |
H1n2 | 0.60928 | 0.12885 | 0.50191 | 0.05* | |
C5 | 0.5708 (15) | 0.252 (2) | 0.6285 (11) | 0.029 (4)* | |
O1 | 0.5060 (12) | 0.0728 (12) | 0.6388 (6) | 0.029 (3)* | |
N3 | 0.6041 (15) | 0.4651 (13) | 0.6956 (9) | 0.024 (3)* | |
H1n3 | 0.55477 | 0.51321 | 0.73425 | 0.05* | |
H2n3 | 0.67532 | 0.55182 | 0.70648 | 0.05* |
C1—C2 | 1.493 (17) | C4—H4 | 0.928 |
C1—H1a | 0.978 | N1—N2 | 1.387 (11) |
C1—H1b | 0.970 | N2—H1n2 | 0.883 |
C1—H1c | 0.975 | N2—C5 | 1.390 (10) |
C2—C3 | 1.353 (11) | C5—O1 | 1.210 (11) |
C2—H2 | 0.956 | C5—N3 | 1.361 (11) |
C3—C4 | 1.387 (13) | N3—H1n3 | 0.911 |
C3—H3 | 0.936 | N3—H2n3 | 0.875 |
C4—N1 | 1.317 (11) | ||
H1a—C1—H1b | 108.9 | C3—C4—N1 | 117.2 (12) |
H1a—C1—H1c | 108.1 | H4—C4—N1 | 120.1 |
H1a—C1—C2 | 111.0 | C4—N1—N2 | 112.5 (9) |
H1b—C1—H1c | 109.0 | N1—N2—H1n2 | 119.2 |
H1b—C1—C2 | 109.9 | N1—N2—C5 | 121.9 (9) |
H1c—C1—C2 | 109.9 | H1n2—N2—C5 | 117.6 |
C1—C2—H2 | 115.9 | N2—C5—O1 | 123.3 (11) |
C1—C2—C3 | 126.9 (9) | N2—C5—N3 | 111.6 (11) |
H2—C2—C3 | 116.9 | O1—C5—N3 | 124.8 (11) |
C2—C3—H3 | 117.3 | C5—N3—H1n3 | 119.9 |
C2—C3—C4 | 121.8 (10) | C5—N3—H2n3 | 121.6 |
H3—C3—C4 | 119.4 | H1n3—N3—H2n3 | 118.4 |
C3—C4—H4 | 119.5 | ||
C4—N1—N2—C5 | −171.0 (13) | N1—N2—C5—N3 | −7.4 (18) |
N2—N1—C4—C3 | 178.3 (13) | C1—C2—C3—C4 | −177.3 (16) |
N1—N2—C5—O1 | 178.6 (13) | C2—C3—C4—N1 | 174.0 (15) |
D—H···A | D—H | H···A | D···A | D—H···A |
N3—H2N3···N1 | 0.87 | 2.33 | 2.629 (19) | 100 |
N2—H1N2···O1i | 0.88 | 2.07 | 2.910 (11) | 158 |
N3—H1N3···O1ii | 0.91 | 2.04 | 2.914 (18) | 162 |
Symmetry codes: (i) −x+1, −y, −z+1; (ii) −x+1, y+1/2, −z+3/2. |
C5H9N3S | V = 382.15 (2) Å3 |
Mr = 143.21 | Z = 2 |
Triclinic, P1 | F(000) = 152 |
Hall symbol: -P 1 | Dx = 1.245 Mg m−3 |
a = 5.86650 (17) Å | Cu Kα1 radiation, λ = 1.5406 Å |
b = 8.0313 (2) Å | µ = 3.11 mm−1 |
c = 9.0795 (4) Å | T = 298 K |
α = 104.1407 (18)° | Particle morphology: fine powder |
β = 101.0403 (19)° | white |
γ = 106.3511 (17)° | flat sheet, 8 × 8 mm |
Stoe transmission Stadi-P diffractometer | Data collection mode: transmission |
Radiation source: sealed X-ray tube | Scan method: step |
Ge 111 monochromator | 2θmin = 4.980°, 2θmax = 79.960°, 2θstep = 0.02° |
Specimen mounting: Powder loaded into two Mylar foils |
Least-squares matrix: full | Profile function: CW Profile function number 4 with 21 terms Pseudovoigt profile coefficients as parameterized in (Thompson et al., 1987) Asymmetry correction of Finger et al., 1994. #1(GU) = 0.000 #2(GV) = 0.000 #3(GW) = 2.793 #4(GP) = 0.000 #5(LX) = 5.477 #6(ptec) = 2.45 #7(trns) = 0.00 #8(shft) = 0.0000 #9(sfec) = 0.00 #10(S/L) = 0.0220 #11(H/L) = 0.0220 #12(eta) = 0.6000 Peak tails are ignored where the intensity is below 0.0010 times the peak Aniso. broadening axis 0.0 0.0 1.0 |
Rp = 0.033 | 114 parameters |
Rwp = 0.043 | 1 restraint |
Rexp = 0.034 | H-atom parameters not refined |
R(F2) = 0.02670 | (Δ/σ)max = 0.03 |
χ2 = 1.664 | Background function: GSAS Background function number 1 with 20 terms. Shifted Chebyshev function of 1st kind 1: 590.360 2: -469.557 3: 198.126 4: -45.2586 5: -2.75624 6: 13.8508 7: 4.35563 8: -5.95029 9: -12.8815 10: 35.6051 11: -12.9276 12: -11.1488 13: 8.85293 14: -2.01034 15: -0.496121 16: 8.39616 17: -2.33367 18: -5.14527 19: 10.5079 20: -3.85249 |
3750 data points |
C5H9N3S | γ = 106.3511 (17)° |
Mr = 143.21 | V = 382.15 (2) Å3 |
Triclinic, P1 | Z = 2 |
a = 5.86650 (17) Å | Cu Kα1 radiation, λ = 1.5406 Å |
b = 8.0313 (2) Å | µ = 3.11 mm−1 |
c = 9.0795 (4) Å | T = 298 K |
α = 104.1407 (18)° | flat sheet, 8 × 8 mm |
β = 101.0403 (19)° |
Stoe transmission Stadi-P diffractometer | Scan method: step |
Specimen mounting: Powder loaded into two Mylar foils | 2θmin = 4.980°, 2θmax = 79.960°, 2θstep = 0.02° |
Data collection mode: transmission |
Rp = 0.033 | 3750 data points |
Rwp = 0.043 | 114 parameters |
Rexp = 0.034 | 1 restraint |
R(F2) = 0.02670 | H-atom parameters not refined |
χ2 = 1.664 |
x | y | z | Uiso*/Ueq | ||
C1 | 0.184 (2) | 0.841 (2) | 0.515 (2) | 0.103 (6)* | |
H1A | 0.15342 | 0.79934 | 0.39748 | 0.12* | |
H1B | 0.2323 | 0.97016 | 0.55142 | 0.12* | |
H1C | 0.02574 | 0.78525 | 0.53491 | 0.12* | |
C2 | 0.370 (2) | 0.7688 (17) | 0.5865 (18) | 0.054 (5)* | |
H2 | 0.53963 | 0.83335 | 0.59455 | 0.055* | |
C3 | 0.325 (2) | 0.6393 (16) | 0.6524 (15) | 0.034 (5)* | |
H3 | 0.14582 | 0.56255 | 0.63049 | 0.055* | |
C4 | 0.487 (3) | 0.5747 (19) | 0.7264 (19) | 0.039 (5)* | |
H4 | 0.66632 | 0.65671 | 0.74816 | 0.055* | |
N1 | 0.4514 (17) | 0.4461 (12) | 0.7878 (15) | 0.035 (4)* | |
N2 | 0.6486 (16) | 0.4005 (12) | 0.8462 (13) | 0.021 (4)* | |
H1n2 | 0.79218 | 0.45838 | 0.841 | 0.05* | |
C5 | 0.611 (3) | 0.2572 (16) | 0.907 (2) | 0.034 (4)* | |
N3 | 0.3681 (15) | 0.1560 (12) | 0.8849 (13) | 0.017 (4)* | |
H1n3 | 0.34725 | 0.13246 | 0.97116 | 0.05* | |
H2n3 | 0.26401 | 0.20773 | 0.84645 | 0.05* | |
S1 | 0.8446 (6) | 0.1980 (5) | 0.9772 (6) | 0.04081 |
U11 | U22 | U33 | U12 | U13 | U23 | |
S1 | 0.032 (4) | 0.039 (5) | 0.082 (8) | 0.026 (4) | 0.043 (5) | 0.035 (5) |
C1—H1A | 0.999 | C4—N1 | 1.274 (12) |
C1—H1B | 0.946 | N1—N2 | 1.361 (10) |
C1—H1C | 0.983 | N2—H1n2 | 0.856 |
C1—C2 | 1.49 (2) | N2—C5 | 1.377 (13) |
C2—H2 | 0.963 | C5—N3 | 1.376 (13) |
C2—C3 | 1.311 (13) | C5—S1 | 1.638 (13) |
C3—H3 | 1.008 | N3—C5 | 1.376 (13) |
C3—C4 | 1.352 (14) | N3—H1n3 | 0.872 |
C4—H4 | 1.024 | N3—H2n3 | 0.894 |
H1A—C1—H1B | 109.0 | C3—C4—N1 | 130.8 (16) |
H1A—C1—H1C | 106.2 | H4—C4—N1 | 116.8 |
H1A—C1—C2 | 108.5 | C4—N1—N2 | 118.6 (11) |
H1B—C1—H1C | 110.2 | N1—N2—H1n2 | 119.6 |
H1B—C1—C2 | 113.8 | N1—N2—C5 | 119.2 (10) |
H1C—C1—C2 | 108.8 | H1n2—N2—C5 | 121.2 |
C1—C2—H2 | 115.8 | N2—C5—N3 | 115.6 (12) |
C1—C2—C3 | 125.6 (13) | N2—C5—S1 | 120.4 (11) |
H2—C2—C3 | 118.2 | N3—C5—S1 | 123.5 (9) |
C2—C3—H3 | 116.8 | C5—N3—H1n3 | 110.5 |
C2—C3—C4 | 128.4 (15) | C5—N3—H2n3 | 112.2 |
H3—C3—C4 | 113.9 | H1n3—N3—H2n3 | 113.2 |
C3—C4—H4 | 111.8 | ||
C4—N1—N2—C5 | −177.4 (14) | N1—N2—C5—N3 | 8.0 (19) |
N2—N1—C4—C3 | 175.6 (15) | C1—C2—C3—C4 | −176.2 (15) |
N1—N2—C5—S1 | 179.6 (11) | C2—C3—C4—N1 | −177.6 (16) |
D—H···A | D—H | H···A | D···A | D—H···A |
N3—H2N3···N1 | 0.89 | 2.17 | 2.641 (14) | 112 |
N2—H1N2···S1i | 0.86 | 2.83 | 3.473 (11) | 133 |
N3—H1N3···S1ii | 0.87 | 2.77 | 3.398 (11) | 130 |
Symmetry codes: (i) −x+2, −y+1, −z+2; (ii) −x+1, −y, −z+2. |
D—H···A | D—H | H···A | D···A | D—H···A |
N3—H2N3···N1 | 0.87 | 2.33 | 2.629 (19) | 100 |
N2—H1N2···O1i | 0.88 | 2.07 | 2.910 (11) | 158 |
N3—H1N3···O1ii | 0.91 | 2.04 | 2.914 (18) | 162 |
Symmetry codes: (i) −x+1, −y, −z+1; (ii) −x+1, y+1/2, −z+3/2. |
D—H···A | D—H | H···A | D···A | D—H···A |
N3—H2N3···N1 | 0.89 | 2.17 | 2.641 (14) | 112 |
N2—H1N2···S1i | 0.86 | 2.83 | 3.473 (11) | 133 |
N3—H1N3···S1ii | 0.87 | 2.77 | 3.398 (11) | 130 |
Symmetry codes: (i) −x+2, −y+1, −z+2; (ii) −x+1, −y, −z+2. |
Experimental details
(I) | (II) | |
Crystal data | ||
Chemical formula | C5H9N3O | C5H9N3S |
Mr | 127.15 | 143.21 |
Crystal system, space group | Monoclinic, P21/c | Triclinic, P1 |
Temperature (K) | 298 | 298 |
a, b, c (Å) | 11.1646 (3), 5.13891 (9), 13.0301 (2) | 5.86650 (17), 8.0313 (2), 9.0795 (4) |
α, β, γ (°) | 90, 112.3496 (11), 90 | 104.1407 (18), 101.0403 (19), 106.3511 (17) |
V (Å3) | 691.43 (3) | 382.15 (2) |
Z | 4 | 2 |
Radiation type | Cu Kα1, λ = 1.5406 Å | Cu Kα1, λ = 1.5406 Å |
µ (mm−1) | 0.74 | 3.11 |
Specimen shape, size (mm) | Flat sheet, 8 × 8 | Flat sheet, 8 × 8 |
Data collection | ||
Diffractometer | Stoe transmission Stadi-P diffractometer | Stoe transmission Stadi-P diffractometer |
Specimen mounting | Powder loaded into two Mylar foils | Powder loaded into two Mylar foils |
Data collection mode | Transmission | Transmission |
Scan method | Step | Step |
2θ values (°) | 2θmin = 5 2θmax = 80 2θstep = 0.02 | 2θmin = 4.980 2θmax = 79.960 2θstep = 0.02 |
Refinement | ||
R factors and goodness of fit | Rp = 0.027, Rwp = 0.036, Rexp = 0.029, R(F2) = 0.02795, χ2 = 1.613 | Rp = 0.033, Rwp = 0.043, Rexp = 0.034, R(F2) = 0.02670, χ2 = 1.664 |
No. of data points | 3750 | 3750 |
No. of parameters | 121 | 114 |
No. of restraints | 0 | 1 |
H-atom treatment | H-atom parameters not refined | H-atom parameters not refined |
Computer programs: WinXPOW (Stoe & Cie, 1999), EXPO2014 (Altomare et al., 2013), GSAS (Larson & Von Dreele, 2004), ORTEP-3 for Windows (Farrugia, 2012), Mercury (Macrae et al., 2006), publCIF (Westrip, 2010).