Home Crystal structure of benzylthiouronium chloride, C8H11ClN2S
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Crystal structure of benzylthiouronium chloride, C8H11ClN2S

  • Marius Maritz , Eric C. Hosten ORCID logo and Richard Betz ORCID logo EMAIL logo
Published/Copyright: October 5, 2020

Abstract

C8H11ClN2S, orthorhombic, Pbca (no. 61), a = 11.3126(6) Å, b = 8.3567(4) Å, c = 20.4130(11) Å, V = 1929.76(17) Å3, Z = 8, Rgt(F) = 0.0240, wRref(F2) = 0.0680, T = 200 K.

CCDC no.: 2033285

The molecular structure is shown in the figure. Table 1 contains crystallographic data and Table 2 contains the list of the atoms including atomic coordinates and displacement parameters.

Table 1:

Data collection and handling.

Crystal:Colourless block
Size:0.51 × 0.45 × 0.29 mm
Wavelength:Mo Kα radiation (0.71073 Å)
μ:0.56 mm−1
Diffractometer, scan mode:Bruker APEX-II, φ and ω
θmax, completeness:28.3°, >99 %
N(hkl)measured, N(hkl)unique, Rint:16553, 2398, 0.022
Criterion for Iobs, N(hkl)gt:Iobs > 2 σ(Iobs), 2077
N(param)refined:125
Programs:Bruker [1], [2], SHELX [3], WinGX/ORTEP [4], Mercury [5], PLATON [6]
Table 2:

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2).

AtomxyzUiso*/Ueq
S10.55112 (3)0.39898 (4)0.404030 (15)0.02740 (9)
N10.41950 (10)0.66140 (14)0.42571 (6)0.0283 (2)
H7110.4078 (14)0.753 (2)0.4414 (8)0.036 (4)*
H7120.3581 (14)0.606 (2)0.4219 (8)0.036 (4)*
N20.61698 (10)0.67443 (14)0.45016 (6)0.0310 (2)
H7210.6812 (16)0.627 (2)0.4586 (9)0.047 (5)*
H7220.6070 (14)0.766 (2)0.4670 (8)0.043 (5)*
C10.52448 (11)0.59542 (14)0.42863 (6)0.0235 (2)
C20.41370 (11)0.33877 (14)0.36493 (6)0.0274 (2)
H2A0.41260.22060.36130.033*
H2B0.34700.37060.39350.033*
C30.39410 (10)0.40884 (14)0.29786 (6)0.0241 (2)
C40.47472 (11)0.38159 (14)0.24754 (6)0.0281 (3)
H40.54460.32190.25590.034*
C50.45361 (12)0.44104 (16)0.18535 (6)0.0331 (3)
H50.50890.42160.15120.040*
C60.35232 (13)0.52865 (17)0.17262 (7)0.0372 (3)
H60.33800.56870.12980.045*
C70.27218 (12)0.55783 (19)0.22206 (7)0.0397 (3)
H70.20290.61860.21340.048*
C80.29289 (11)0.49806 (16)0.28464 (7)0.0326 (3)
H80.23750.51830.31860.039*
Cl10.66773 (3)0.50164 (3)0.027813 (16)0.02983 (9)

Source of material

The compound was obtained commerciually (Hopkin & Williams Ltd.). Crystals suitable for the diffraction study were taken directly from the provided product.

Experimental details

Carbon-bound H atoms were placed in calculated positions (C–H 0.95 Å for aromatic carbon atoms, C–H 0.99 Å for methylene groups) and were included in the refinement in the riding model approximation, with U(H) set to 1.2Ueq(C).

All nitrogen-bound H atoms were located on a difference Fourier map and refined freely.

Comment

The effect of size and steric presence of large ions on chemical and spectroscopic properties of compounds have been a focus of research for many decades. Among the many effects that can be attributed to the spatial requirements of counterions have been the glass transition temperature in ionomers [7], surfactant modifying properties [8], the charge transfer in radical ions [9] and polymer-modified electrodes [10] as well as the structural and vibrational spectroscopic behaviour of DNA building blocks [11]. The benefit of chosing the adequate size of counterions to crystallize ionic compounds has been confirmed and reviewed several times [12]. Thiouronium derivatives are especially interesting in this context as they constitute a compound class that has been known for many decades. Their ease of synthesis in connection with their ready crystallizability – especially as picrates – has played a major role in the identification of alkyl halides [13]. However, due to the size of the picrate anion the metrical parameters of the pertaining thiouronium cations might not be free from crystal-packing-induced distortions. To eliminate this potential biased view, the crystal structure of the title compound was determined to account for this factor by opting for chloride as a much smaller anion.

The structure solution shows the presence of the benzylthiouronium cation with chloride as the counterion. The two sulphur-carbon bond lengths differ markedly from one another with values of 1.7430(12) Å and 1.8186(13) Å with the shorter bond formed towards the thiourea motif. The formal C=S double bond is longer than the most-commonly reported values for the pertaining bond in other thiouronium derivatives whose metrical parameters have been deposited with the Cambridge Structural Database [14]. The least squares planes as defined by the non-hydrogen atoms of the aromatic moiety and the thiourea moiety enclose an angle of 82.04(4)°.

In the crystal structure, all nitrogen-bonded hydrogen atoms act as donors in classical N–H⃛Cl hydrogen bonds. Furthermore, one of the hydrogen atoms of the methylene group gives rise to C–H⃛Cl contacts whose range falls by more than 0.1 Å below the sum of van-der–Waals radii of the atoms participating in them. In terms of graph-set analysis, [15], [16], the descriptor for these contacts is DDDDD at the unary level. In total, these interactions connect the entities present in the crystal structure to double layers perpendicular to the crystallographic c axis. π Stacking is not a prominent stabilizing feature of the structure as the shortest intercentroid distance was measured at 5.0240(8) Å.


Corresponding author: Richard Betz, Department of Chemistry, Nelson Mandela University, Summerstrand Campus (South), UniversityWay, Summerstrand, PO Box 77000, Port Elizabeth, 6031, South Africa, E-mail:

  1. Author contribution: All the authors have accepted responsibility for the entire content of this submitted manuscript and approved submission.

  2. Research funding: R. Betz thanks the NRF for financial support.

  3. Conflict of interest statement: The authors declare no conflicts of interest regarding this article.

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Received: 2020-08-30
Accepted: 2020-09-22
Published Online: 2020-10-05
Published in Print: 2021-01-26

© 2020 Marius Maritz et al., published by De Gruyter, Berlin/Boston

This work is licensed under the Creative Commons Attribution 4.0 International License.

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