research communications\(\def\hfill{\hskip 5em}\def\hfil{\hskip 3em}\def\eqno#1{\hfil {#1}}\)

Journal logoCRYSTALLOGRAPHIC
COMMUNICATIONS
ISSN: 2056-9890

The crystal structures and Hirshfeld surface analysis of the 2-iodo­phenyl- and 4,5-di­fluoro-2-iodo­phenyl derivatives of benzenesulfonamide

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aDepartment of Physics, The New College, Chennai 600 014, University of Madras, Tamil Nadu, India, and bDepartment of Organic Chemistry, University of Madras, Guindy Campus, Chennai-600 025, Tamilnadu, India
*Correspondence e-mail: [email protected]

Edited by M. Weil, Vienna University of Technology, Austria (Received 30 June 2025; accepted 24 July 2025; online 7 August 2025)

Two new benzene­sulfonyl derivatives, N-(2-iodo­phen­yl)benzene­sulfonamide, C12H10INO2, (I), and N-(4,5-di­fluoro-2-iodo­phen­yl)benzene­sulfonamide, C12H8F2INO2S, (II) were synthesized and structurally characterized. In both mol­ecular structures, the conformation of the N—C bond in the –SO2—NH—C segment is gauche relative to the S=O bond. For (I), the crystal packing is dominated by N—H⋯O hydrogen-bonding inter­actions that link the mol­ecules into chains extending parallel to [010]. In the case of (II), the mol­ecules are linked by N—H⋯O(S) hydrogen bonds into dimers that are located on centers of inversion. These findings are consistent with the results of Hirshfeld surface analyses.

1. Chemical context

Sulfonamide-containing compounds, often referred to as sulfa drugs, form a significant class of pharmacologically active agents. These mol­ecules, which may incorporate one or more pharmacological scaffolds, demonstrate a broad spectrum of biological activities including anti­viral, anti­cancer, anti­bacterial, anti-carbonic anhydrase (CA), diuretic, COX-2 inhibitory, and protease inhibitory effects (Madhan et al., 2024aView full citation,bView full citation,cView full citation). The sulfonamide moiety is recognized as an important structural unit in medicinal chemistry and is present in many widely marketed drugs (Supuran, 2003View full citation; Elgemeie et al., 2019View full citation). Since their discovery, sulfonamides have been extensively used as anti­biotics (Zhao et al., 2016View full citation), particularly for treating infections like malaria, tuberculosis, or HIV, by targeting the di­hydro­pteroate synthase (DHPS) pathway (Dennis et al., 2018View full citation). Even after the advent of penicillin, sulfa drugs have retained their relevance in clinical settings due to their diverse therapeutic actions, including anti­tumor, anti­cancer, and anti­thyroid activities (Scozzafava et al., 2003View full citation). Various sulfonamide derivatives serve as chemotherapeutic agents, exhibiting anti­bacterial, anti­fungal, anti­tumor, and hypoglycemic properties (Chohan et al., 2010View full citation; El-Sayed et al., 2011View full citation Seri et al., 2000View full citation). Benzene­sulfonamide derivatives are particularly known for their anti­tumor and anti­fungal activities. Crystallographic studies of these compounds reveal structural parameters consistent with other sulfonamide-based mol­ecules (Chakkaravarthi et al., 2007View full citation; Li & Yang, 2006View full citation). Continued inter­est in sulfonamides stems from their enduring role in treating bacterial infections, their chemical versatility, and their effectiveness despite the rise of newer anti­biotic classes. Modern synthetic approaches aim to produce sulfon­amide-functionalized heterocycles with enhanced anti­viral and anti­microbial profiles (Madhan et al., 2024aView full citation). Research into N-sulfonyl­ated I and F atom-substituted compounds is motivated by the observed enhancement of biological activity. Hence, the introduction of fluorine atoms into drugs is increasingly common due to the strong electron-withdrawing character and small atomic radius of the fluorine atom, which significantly influences the physiological, pharmacological and metabolic properties of a compound (Mueller et al., 2007View full citation; Purser et al., 2008View full citation). The availability of multiple aromatic groups in N-sulfonyl­ated 2-iodo­phenyl imposes also the possibility for versatile stacking patterns, which may be competitive to the conventional hydrogen-bonding inter­actions in the crystal packing.

[Scheme 1]

In the context given above, we report herein the crystal structure determinations and Hirshfeld surface analyses of two new 2-iodo­phenyl benzene­sulfonamides: N-(2-iodo­phen­yl)benzene­sulfonamide, C12H10INO2, (I), and N-(4,5-di­fluoro-2-iodo­phen­yl)benzene­sulfonamide, C12H8F2INO2S, (II), which feature a complex inter­play of weak hydrogen bonding and ππ inter­actions.

2. Structural commentary

The mol­ecular structures of (I) and (II) are shown in Figs. 1[link] and 2[link], respectively. In both cases, the conformation of the N—C bond in the –SO2—NH—C segment is gauche relative to the S=O bond. The mol­ecule is twisted at the S—N bond with a torsion angle of C7—N1—S1—C6 = −69.0 (2)° for (I) and −61.1 (6)° for (II) compared to the values of −72.83 (15) and 61.9 (3)° in N-(phen­yl)-2-nitro­benzene­sulfonamide (Chaithanya et al., 2012aView full citation) and 4-nitro-N-phenyl­benzene­sulfonamide (Chaithanya et al., 2012bView full citation), respectively. The two benzene rings are tilted relative to each other by 44.1 (1)° for (I) and 73.1 (1)° for (II). The mol­ecular configuration of (II) is stabilized by a weak intra­molecular hydrogen bond C12—H12⋯O1 (Table 1[link]) with one of the sulfone O-atoms as acceptor, which generates an S(6) ring motif. Other structural parameters (bond lengths and angles) in the mol­ecules of (I) and (II) agree well with those reported for related compounds (Madhan et al., 2022View full citation, 2023aView full citation,bView full citation, 2024aView full citation,bView full citation,cView full citation).

Table 1
Hydrogen-bond geometry (Å, °) for (I)[link]

D—H⋯A D—H H⋯A DA D—H⋯A
N1—H1A⋯O2i 0.86 2.37 3.144 (3) 149
C3—H3⋯O1ii 0.93 2.57 3.352 (4) 142
Symmetry codes: (i) Mathematical equation; (ii) Mathematical equation.
[Figure 1]
Figure 1
The mol­ecular structure of compound (I), with atom labeling and displacement ellipsoids drawn at the 50% probability level.
[Figure 2]
Figure 2
The mol­ecular structure of compound (II), with atom labeling and displacement ellipsoids drawn at the 50% probability level.

3. Supra­molecular features

In the crystal structure of (I), inter­molecular N—H⋯O hydrogen-bonding inter­actions (Table 1[link]) link the mol­ecules into C(4) chains (Etter et al., 1990View full citation) running parallel to [010] while C—H⋯O inter­actions inter­link these chains (Fig. 3[link]). In addition, ππ inter­actions are present with a centroid-to-centroid distance Cg2⋯Cg2 (2 − x, 1 − y, 1 − z) = 3.747 (2) Å and a slippage of 1.035 Å (Cg2 is the centroid of phenyl ring C7–C1).

[Figure 3]
Figure 3
Crystal packing of compound (I), showing the N—H⋯O and C—H⋯O inter­action that link the mol­ecules into chains.

In the crystal structure of (II), mol­ecules are linked by N—H⋯O(S) hydrogen-bonding inter­actions (Table 2[link], Fig. 4[link]) into inversion-related dimers with an R22(8) graph-set motif (Etter et al., 1990View full citation). Like for (I), ππ inter­actions are present that consolidate the crystal packing, here with centroid-to-centroid distances Cg1⋯Cg1(1 − x, 2 − y, −z) = 3.621 (2) and a slippage of 0.998 Å and Cg2⋯Cg2(2 − x, 1 − y, 1 − z) = 3.797 (2) Å and a slippage of 1.617 Å (Cg1 and Cg2 are the centroids of the C1–C6 and C7–C12 rings, respectively).

Table 2
Hydrogen-bond geometry (Å, °) for (II)[link]

D—H⋯A D—H H⋯A DA D—H⋯A
N1—H1A⋯O2i 0.86 2.58 3.169 (8) 126
C12—H12⋯O1 0.93 2.27 2.916 (11) 126
Symmetry code: (i) Mathematical equation.
[Figure 4]
Figure 4
Crystal packing of compound (II), showing the N—H⋯O(S) hydrogen-bonding inter­actions that lead to inversion-related dimers.

4. Hirshfeld surface analysis

In order to qu­antify the inter­molecular inter­actions in the crystals of (I) and (II), Hirshfeld surfaces and two-dimensional fingerprint plots were generated using CrystalExplorer (Spackman et al., 2021View full citation).

Plots of dnorm use the normalized functions di and de (Fig. 5[link]), with white surfaces indicating contacts with distances equal to the sum of van der Waals (vdW) radii, while red and blue colors reflect contacts at the distances below and above sum of the corresponding vdW radii, respectively. Two-dimensional fingerprint plots showing the occurrence of all inter­molecular contacts (McKinnon et al., 2007View full citation) and are presented in Fig. 6[link]. H⋯H in (I) and O⋯H/H⋯O contacts in (II) represent the largest contributions to the Hirshfeld surfaces (37.4 and 44.7%, respectively). Beyond these largest fractions, short contacts are O⋯H/H⋯O (21.7%) for (I) and O⋯C/C⋯O (17.2%) for (II) (Fig. 6[link]c), C⋯H/H⋯C (16.5%) for (I) and O⋯O (11%) for (II) (Fig. 6[link]d). The significant increase in the O⋯H/H⋯O contributions when moving from (I) to (II) reflects growing significance of C—H⋯O binding. This is in line with a larger number of the available inter­molecular O-atom acceptors in the latter case. Accordingly, a pair of spikes identifying O⋯H/H⋯O contacts on the plots in the case of (I) is more diffuse.

[Figure 5]
Figure 5
The Hirshfeld surfaces of compounds (I) and (II) mapped over dnorm.
[Figure 6]
Figure 6
Two-dimensional fingerprint plots for (I) and delineated into the principal contributions of H⋯H, O⋯H/H⋯O, C⋯H/H⋯C, I⋯H/H⋯I, I⋯C/C⋯I, C⋯C and I⋯O/O⋯I contacts and for (II) O⋯H/H⋯O, O⋯C/C⋯O, O⋯O, N⋯O/O⋯N, H⋯H, H⋯C/C⋯H, C⋯C, N⋯C/C⋯N and N⋯H/H⋯N. Other contributors account for less than 1.0% contacts to the surface areas.

In brief, the Hirshfeld surface analyses complement the main merit of the structure analyses, and together they suggest possibilities for controlling the supra­molecular behavior of benzene­sulfonamide as possible biomedical materials.

5. Database survey

A search of the Cambridge Structural Database (CSD, version 5.37; Groom et al., 2016View full citation) indicated 123 compounds incorporating the phenyl­sulfonamide moiety. The bond lengths and angles in (I) and (II) are very close to those observed in 2,4-dimethyl-N-(phen­yl)benzene­sulfonamide (Gowda et al., 2009aView full citation), 4-chloro-2-methyl-N-(phen­yl)benzene­sulfonamide (Gowda et al., 2009bView full citation), 4-methyl-N-(3,4-di­methyl­phen­yl)benzene­sulfonamide (Gowda et al., 2009cView full citation) and other aryl sulfonamides Perlovich et al., 2006View full citation; Tatsuta et al., 2009View full citation; Arora & Sundaralingam, 1971View full citation; Gelbrich et al., 2007View full citation). Of these, the most closely related examples are provided by structures of bromo­substituted 3-methyl-1-(phenyl­sulfon­yl)-1H-indole derivatives (Madhan et al., 2024bView full citation).

6. Synthesis and crystallization

(I): To a solution of 2-iodo­aniline (2 g, 9.17 mmol) in dry di­chloro­methane (DCM; 10 ml), benzene­sulfonyl chloride (1.42 ml, 11.01 mmol) and pyridine (1.11 ml, 13.76 mmol) were slowly added and stirred at room temperature for 8 h under nitro­gen atmosphere. After completion of the reaction (monitored by TLC), it was poured into ice water containing conc. HCl (1 ml), extracted with DCM (3 × 10 ml) then washed with water (2 × 20 ml) and dried (Na2SO4). Removal of the solvent in vacuo followed by trituration of the crude product with diethyl ether (5 ml) afforded (I) (2.43 g, 84%) as a colorless solid. M.p: 363–365 K. 1H-NMR (300 MHZ, CDCl3): δ 7.70 (d, J = 7.5 Hz, 2H), 7.61 (t, J = 7.5 Hz, 2H), 7.55–7.49 (m, 1 H), 7.41–7.36 (m, 2H), 7.28 (t, J = 7.5 Hz, 1H), 6.82–6.77 (m, 2H) ppm; 13C{1H}-NMR (75 MHz, CDCl3): δ 139.1, 138.8, 137.4, 133.3, 129.6, 127.4, 122.9, 92.5 ppm.

(II): To a solution of 4,5-di­fluoro2-iodo­aniline (2 g, 7.84 mmol) in dry DCM (10 ml), benzene­sulfonyl chloride (1.21 ml, 9.41 mmol) and pyridine (0.95 ml, 11.76 mmol) were slowly added and stirred at room temperature for 8 h under nitro­gen atmosphere. After completion of the reaction (monitored by TLC), it was poured into ice water containing conc. HCl (1 ml), extracted with DCM (3 × 10 ml) then washed with water (2 × 20 ml) and dried (Na2SO4). Removal of solvent in vacuo followed by trituration of the crude product with diethyl ether (5 mL) afforded benzene­sulfonamide (II) (2.56 g, 83%) as a colorless solid. M.p: 393–395 K. 1H-NMR (300 MHZ, CDCl3): δ 7.58 (d, J = 7.5 Hz, 2H), 7.45–7.39 (m, 2 H), 7.30–7.26 (m, 3 H)ppm; 13C{1H}-NMR (75 MHz, CDCl3): δ 150.7 (dd, 1JC–F = 249.4 Hz, 2JC–F = 12.7 Hz), 147.8 (dd, 1JC–F = 252 Hz, 2JC–F = 12.7 Hz), 138.4, 134.3 (dd, 1JC–F = 82 Hz, 2JC–F = 3 Hz), 133.7, 129.3, 127.4, 126.8 (d, JC–F = 19.5 Hz), 112.3 (d, JC–F = 21.7 Hz) ppm.

7. Refinement

Crystal data, data collection and structure refinement details are summarized in Table 3[link]. All hydrogen atoms were positioned geometrically and refined as riding with N—H = 0.86 and C—H = 0.93 Å (aromatic CH) with Uiso(H) = 1.5Ueq(C) for methyl groups and 1.2Ueq(C) for other H atoms.

Table 3
Experimental details

  (I) (II)
Crystal data
Chemical formula C12H10INO2S C12H8F2INO2S
Mr 359.17 395.15
Crystal system, space group Monoclinic, P21/c Triclinic, PMathematical equation
Temperature (K) 298 298
a, b, c (Å) 8.3648 (4), 9.8537 (4), 15.3923 (8) 8.2688 (5), 8.5178 (5), 10.4329 (7)
α, β, γ (°) 90, 90.955 (2), 90 81.291 (2), 80.503 (2), 68.383 (2)
V3) 1268.52 (10) 670.47 (7)
Z 4 2
Radiation type Mo Kα Cu Kα
μ (mm−1) 2.68 20.44
Crystal size (mm) 0.35 × 0.25 × 0.08 0.22 × 0.10 × 0.05
 
Data collection
Diffractometer Bruker D8 Venture Diffractometer Bruker D8 Venture Diffractometer
Absorption correction Multi-scan (SADABS; Krause et al., 2015View full citation) Multi-scan (SADABS; Krause et al., 2015View full citation)
Tmin, Tmax 0.672, 0.971 0.240, 0.521
No. of measured, independent and observed [I > 2σ(I)] reflections 29284, 2591, 2386 14553, 2476, 2367
Rint 0.049 0.062
(sin θ/λ)max−1) 0.625 0.605
 
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.027, 0.069, 1.09 0.072, 0.203, 1.14
No. of reflections 2591 2476
No. of parameters 155 173
H-atom treatment H-atom parameters constrained H-atom parameters constrained
Δρmax, Δρmin (e Å−3) 0.54, −0.56 1.66, −0.95
Computer programs: APEX2 and SAINT (Bruker, 2016View full citation), SHELXT (Sheldrick, 2015aView full citation), SHELXL (Sheldrick, 2015bView full citation), ORTEP-3 for Windows and WinGX (Farrugia, 2012View full citation), Mercury (Macrae et al., 2020View full citation), publCIF (Westrip, 2010View full citation) and PLATON (Spek, 2009View full citation).

Supporting information


Computing details top

N-(2-Iodophenyl)benzenesulfonamide (I) top
Crystal data top
C12H10INO2SF(000) = 696
Mr = 359.17Dx = 1.881 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 8.3648 (4) ÅCell parameters from 29284 reflections
b = 9.8537 (4) Åθ = 1.4–25.0°
c = 15.3923 (8) ŵ = 2.68 mm1
β = 90.955 (2)°T = 298 K
V = 1268.52 (10) Å3Prism, colourless
Z = 40.35 × 0.25 × 0.08 mm
Data collection top
Bruker D8 Venture Diffractometer2386 reflections with I > 2σ(I)
Radiation source: micro focus sealed tubeRint = 0.049
ω and φ scansθmax = 26.4°, θmin = 3.4°
Absorption correction: multi-scan
(SADABS; Krause et al., 2015)
h = 1010
Tmin = 0.672, Tmax = 0.971k = 1212
29284 measured reflectionsl = 1919
2591 independent reflections
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.027 w = 1/[σ2(Fo2) + (0.0319P)2 + 1.2298P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.069(Δ/σ)max = 0.002
S = 1.09Δρmax = 0.54 e Å3
2591 reflectionsΔρmin = 0.56 e Å3
155 parametersExtinction correction: SHELXL-2019/2 (Sheldrick 2015b), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraintsExtinction coefficient: 0.0085 (7)
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
C10.5786 (3)0.4285 (3)0.74857 (19)0.0393 (6)
H10.6014550.3652980.7056210.047*
C20.4228 (4)0.4717 (4)0.7611 (2)0.0488 (8)
H20.3409050.4392240.7252070.059*
C30.3886 (4)0.5624 (4)0.8263 (3)0.0539 (9)
H30.2837670.5904310.8345580.065*
C40.5092 (4)0.6113 (4)0.8791 (3)0.0576 (9)
H40.4853100.6713740.9236220.069*
C50.6662 (4)0.5720 (3)0.8666 (2)0.0451 (7)
H50.7479840.6064240.9018270.054*
C60.6996 (3)0.4810 (3)0.80115 (17)0.0310 (5)
C70.8849 (3)0.4506 (3)0.61007 (17)0.0311 (5)
C80.7791 (3)0.5277 (3)0.55998 (18)0.0342 (6)
C90.7163 (4)0.4759 (4)0.4824 (2)0.0481 (8)
H90.6465750.5284010.4488260.058*
C100.7567 (4)0.3479 (4)0.4552 (2)0.0547 (9)
H100.7138590.3134490.4035390.066*
C110.8612 (5)0.2705 (4)0.5049 (2)0.0537 (9)
H110.8880680.1835270.4867720.064*
C120.9263 (4)0.3215 (3)0.5814 (2)0.0420 (7)
H120.9980860.2693030.6138940.050*
N10.9533 (3)0.4996 (2)0.69018 (14)0.0316 (5)
H1A1.0226220.5640400.6895060.038*
O10.9978 (2)0.4978 (2)0.84793 (13)0.0405 (5)
O20.9031 (3)0.28915 (19)0.77277 (14)0.0408 (5)
S10.90001 (7)0.43340 (6)0.78303 (4)0.02932 (16)
I10.71045 (2)0.72190 (2)0.59939 (2)0.04598 (11)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0361 (15)0.0437 (16)0.0381 (15)0.0119 (12)0.0004 (12)0.0013 (13)
C20.0328 (15)0.059 (2)0.0542 (19)0.0143 (14)0.0079 (13)0.0148 (16)
C30.0307 (15)0.055 (2)0.076 (2)0.0046 (14)0.0086 (15)0.0110 (18)
C40.0435 (18)0.057 (2)0.072 (2)0.0047 (16)0.0105 (17)0.0175 (19)
C50.0360 (15)0.0491 (18)0.0500 (17)0.0010 (13)0.0013 (13)0.0111 (15)
C60.0283 (12)0.0328 (13)0.0320 (13)0.0013 (10)0.0003 (10)0.0059 (11)
C70.0291 (12)0.0344 (14)0.0300 (13)0.0044 (10)0.0080 (10)0.0005 (11)
C80.0319 (13)0.0387 (15)0.0320 (13)0.0018 (11)0.0063 (11)0.0002 (11)
C90.0418 (16)0.068 (2)0.0343 (15)0.0020 (15)0.0015 (12)0.0053 (15)
C100.053 (2)0.069 (2)0.0419 (17)0.0123 (18)0.0080 (15)0.0218 (17)
C110.060 (2)0.0462 (19)0.056 (2)0.0063 (15)0.0219 (17)0.0208 (16)
C120.0412 (16)0.0392 (15)0.0461 (16)0.0024 (13)0.0133 (13)0.0029 (13)
N10.0285 (11)0.0322 (11)0.0340 (11)0.0050 (9)0.0015 (9)0.0027 (9)
O10.0329 (10)0.0483 (12)0.0399 (11)0.0002 (9)0.0090 (8)0.0000 (9)
O20.0485 (12)0.0293 (10)0.0445 (11)0.0047 (8)0.0005 (9)0.0073 (8)
S10.0274 (3)0.0295 (3)0.0309 (3)0.0011 (2)0.0029 (2)0.0029 (3)
I10.04805 (15)0.03807 (15)0.05150 (16)0.00919 (8)0.00858 (9)0.00039 (8)
Geometric parameters (Å, º) top
C1—C61.385 (4)C7—N11.434 (3)
C1—C21.388 (5)C8—C91.393 (4)
C1—H10.9300C8—I12.091 (3)
C2—C31.377 (5)C9—C101.373 (5)
C2—H20.9300C9—H90.9300
C3—C41.372 (5)C10—C111.382 (6)
C3—H30.9300C10—H100.9300
C4—C51.386 (5)C11—C121.384 (5)
C4—H40.9300C11—H110.9300
C5—C61.380 (4)C12—H120.9300
C5—H50.9300N1—S11.640 (2)
C6—S11.768 (3)N1—H1A0.8600
C7—C81.390 (4)O1—S11.429 (2)
C7—C121.392 (4)O2—S11.430 (2)
C6—C1—C2118.8 (3)C9—C8—I1118.9 (2)
C6—C1—H1120.6C10—C9—C8120.5 (3)
C2—C1—H1120.6C10—C9—H9119.8
C3—C2—C1120.5 (3)C8—C9—H9119.8
C3—C2—H2119.7C9—C10—C11119.6 (3)
C1—C2—H2119.7C9—C10—H10120.2
C4—C3—C2120.0 (3)C11—C10—H10120.2
C4—C3—H3120.0C10—C11—C12120.5 (3)
C2—C3—H3120.0C10—C11—H11119.8
C3—C4—C5120.6 (3)C12—C11—H11119.8
C3—C4—H4119.7C11—C12—C7120.3 (3)
C5—C4—H4119.7C11—C12—H12119.8
C6—C5—C4119.1 (3)C7—C12—H12119.8
C6—C5—H5120.5C7—N1—S1120.34 (18)
C4—C5—H5120.5C7—N1—H1A119.8
C5—C6—C1121.0 (3)S1—N1—H1A119.8
C5—C6—S1119.4 (2)O1—S1—O2120.50 (13)
C1—C6—S1119.6 (2)O1—S1—N1105.77 (12)
C8—C7—C12118.9 (3)O2—S1—N1107.07 (13)
C8—C7—N1122.3 (2)O1—S1—C6107.76 (13)
C12—C7—N1118.8 (3)O2—S1—C6107.45 (13)
C7—C8—C9120.2 (3)N1—S1—C6107.72 (12)
C7—C8—I1121.0 (2)
C6—C1—C2—C31.8 (5)C9—C10—C11—C120.5 (5)
C1—C2—C3—C40.4 (5)C10—C11—C12—C71.2 (5)
C2—C3—C4—C51.0 (6)C8—C7—C12—C110.8 (4)
C3—C4—C5—C61.1 (6)N1—C7—C12—C11179.3 (3)
C4—C5—C6—C10.4 (5)C8—C7—N1—S1110.1 (3)
C4—C5—C6—S1178.5 (3)C12—C7—N1—S170.0 (3)
C2—C1—C6—C51.8 (4)C7—N1—S1—O1176.0 (2)
C2—C1—C6—S1177.1 (2)C7—N1—S1—O246.3 (2)
C12—C7—C8—C90.1 (4)C7—N1—S1—C669.0 (2)
N1—C7—C8—C9179.7 (3)C5—C6—S1—O13.3 (3)
C12—C7—C8—I1179.6 (2)C1—C6—S1—O1177.9 (2)
N1—C7—C8—I10.6 (3)C5—C6—S1—O2134.5 (2)
C7—C8—C9—C100.8 (5)C1—C6—S1—O246.6 (3)
I1—C8—C9—C10178.9 (3)C5—C6—S1—N1110.4 (2)
C8—C9—C10—C110.5 (5)C1—C6—S1—N168.4 (2)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1A···O2i0.862.373.144 (3)149
C3—H3···O1ii0.932.573.352 (4)142
Symmetry codes: (i) x+2, y+1/2, z+3/2; (ii) x1, y, z.
N-(4,5-Difluoro-2-iodophenyl)benzenesulfonamide (II) top
Crystal data top
C12H8F2INO2SZ = 2
Mr = 395.15F(000) = 380
Triclinic, P1Dx = 1.957 Mg m3
a = 8.2688 (5) ÅCu Kα radiation, λ = 1.54178 Å
b = 8.5178 (5) ÅCell parameters from 14553 reflections
c = 10.4329 (7) Åθ = 1.4–25.0°
α = 81.291 (2)°µ = 20.44 mm1
β = 80.503 (2)°T = 298 K
γ = 68.383 (2)°Prism, colourless
V = 670.47 (7) Å30.22 × 0.10 × 0.05 mm
Data collection top
Bruker D8 Venture Diffractometer2367 reflections with I > 2σ(I)
Radiation source: micro focus sealed tubeRint = 0.062
ω and φ scansθmax = 69.0°, θmin = 4.3°
Absorption correction: multi-scan
(SADABS; Krause et al., 2015)
h = 910
Tmin = 0.240, Tmax = 0.521k = 1010
14553 measured reflectionsl = 1212
2476 independent reflections
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.072 w = 1/[σ2(Fo2) + (0.1461P)2 + 0.5316P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.203(Δ/σ)max < 0.001
S = 1.14Δρmax = 1.66 e Å3
2476 reflectionsΔρmin = 0.94 e Å3
173 parametersExtinction correction: SHELXL-2019/2 (Sheldrick 2015b), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraintsExtinction coefficient: 0.017 (2)
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
C10.6043 (11)0.6893 (10)0.0209 (8)0.0690 (17)
H10.6920520.6068800.0254620.083*
C20.4337 (12)0.7289 (12)0.0029 (10)0.079 (2)
H20.4052620.6751100.0565930.095*
C30.3033 (11)0.8488 (11)0.0732 (10)0.081 (2)
H30.1866550.8758980.0616330.097*
C40.3467 (10)0.9284 (11)0.1607 (10)0.080 (2)
H40.2578091.0086900.2080750.096*
C50.5138 (10)0.8932 (9)0.1794 (8)0.0674 (16)
H50.5404880.9485020.2388100.081*
C60.6479 (9)0.7712 (8)0.1076 (6)0.0582 (14)
C70.8376 (8)0.5366 (8)0.3596 (6)0.0571 (14)
C80.7924 (10)0.3964 (9)0.4144 (7)0.0614 (15)
C90.7196 (12)0.3840 (12)0.5445 (8)0.078 (2)
H90.6920000.2891020.5810560.093*
C100.6899 (13)0.5163 (13)0.6173 (8)0.081 (2)
C110.7353 (14)0.6529 (12)0.5661 (9)0.082 (2)
C120.8116 (11)0.6642 (10)0.4384 (8)0.0700 (18)
H120.8454080.7565750.4051980.084*
N10.9216 (7)0.5461 (7)0.2298 (6)0.0597 (12)
H1A1.0040650.4570020.2029380.072*
O10.8802 (7)0.8532 (7)0.1911 (6)0.0691 (12)
O20.9746 (7)0.6771 (7)0.0082 (5)0.0717 (13)
S10.8673 (2)0.7215 (2)0.12842 (16)0.0582 (5)
I10.83499 (6)0.19041 (6)0.30905 (4)0.0749 (4)
F10.6177 (10)0.5090 (9)0.7433 (5)0.116 (2)
F20.7077 (11)0.7780 (9)0.6410 (6)0.112 (2)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.085 (5)0.061 (4)0.068 (4)0.032 (3)0.006 (3)0.014 (3)
C20.089 (5)0.080 (5)0.083 (5)0.043 (4)0.024 (4)0.005 (4)
C30.064 (4)0.076 (5)0.102 (6)0.028 (4)0.017 (4)0.007 (4)
C40.061 (4)0.074 (5)0.091 (6)0.016 (3)0.008 (4)0.010 (4)
C50.074 (4)0.057 (3)0.068 (4)0.020 (3)0.004 (3)0.014 (3)
C60.067 (3)0.054 (3)0.054 (3)0.023 (3)0.001 (3)0.007 (3)
C70.056 (3)0.059 (3)0.053 (3)0.012 (2)0.007 (2)0.015 (3)
C80.070 (4)0.061 (4)0.053 (3)0.022 (3)0.004 (3)0.010 (3)
C90.092 (5)0.084 (5)0.059 (4)0.038 (4)0.002 (4)0.006 (4)
C100.095 (5)0.092 (6)0.048 (4)0.026 (4)0.001 (3)0.014 (4)
C110.100 (6)0.078 (5)0.060 (4)0.015 (4)0.011 (4)0.023 (4)
C120.085 (5)0.062 (4)0.063 (4)0.024 (3)0.008 (3)0.014 (3)
N10.065 (3)0.056 (3)0.055 (3)0.018 (2)0.000 (2)0.014 (2)
O10.079 (3)0.064 (3)0.073 (3)0.033 (2)0.002 (2)0.020 (2)
O20.078 (3)0.076 (3)0.059 (3)0.030 (3)0.014 (2)0.018 (2)
S10.0632 (9)0.0577 (9)0.0560 (9)0.0254 (7)0.0028 (7)0.0127 (7)
I10.0903 (5)0.0698 (5)0.0695 (5)0.0344 (3)0.0010 (3)0.0166 (3)
F10.154 (6)0.122 (5)0.052 (3)0.036 (4)0.022 (3)0.018 (3)
F20.156 (6)0.104 (4)0.077 (3)0.038 (4)0.001 (3)0.045 (3)
Geometric parameters (Å, º) top
C1—C21.363 (12)C7—N11.422 (9)
C1—C61.386 (10)C8—C91.396 (10)
C1—H10.9300C8—I12.100 (7)
C2—C31.377 (14)C9—C101.378 (13)
C2—H20.9300C9—H90.9300
C3—C41.376 (14)C10—F11.353 (9)
C3—H30.9300C10—C111.360 (15)
C4—C51.343 (12)C11—F21.346 (10)
C4—H40.9300C11—C121.382 (12)
C5—C61.408 (10)C12—H120.9300
C5—H50.9300N1—S11.655 (6)
C6—S11.748 (7)N1—H1A0.8600
C7—C121.394 (10)O1—S11.425 (5)
C7—C81.394 (10)O2—S11.425 (5)
C2—C1—C6120.4 (8)C9—C8—I1116.3 (6)
C2—C1—H1119.8C10—C9—C8118.2 (8)
C6—C1—H1119.8C10—C9—H9120.9
C1—C2—C3119.9 (8)C8—C9—H9120.9
C1—C2—H2120.1F1—C10—C11118.9 (9)
C3—C2—H2120.1F1—C10—C9119.6 (9)
C4—C3—C2119.7 (7)C11—C10—C9121.4 (8)
C4—C3—H3120.2F2—C11—C10119.7 (8)
C2—C3—H3120.2F2—C11—C12119.5 (9)
C5—C4—C3121.8 (8)C10—C11—C12120.8 (8)
C5—C4—H4119.1C11—C12—C7119.7 (8)
C3—C4—H4119.1C11—C12—H12120.1
C4—C5—C6118.9 (8)C7—C12—H12120.1
C4—C5—H5120.5C7—N1—S1122.7 (4)
C6—C5—H5120.5C7—N1—H1A118.7
C1—C6—C5119.3 (7)S1—N1—H1A118.7
C1—C6—S1120.1 (6)O1—S1—O2118.7 (4)
C5—C6—S1120.6 (5)O1—S1—N1107.5 (3)
C12—C7—C8118.5 (7)O2—S1—N1105.5 (3)
C12—C7—N1119.4 (7)O1—S1—C6108.4 (3)
C8—C7—N1121.8 (6)O2—S1—C6109.5 (3)
C7—C8—C9121.3 (7)N1—S1—C6106.5 (3)
C7—C8—I1122.4 (5)
C6—C1—C2—C31.2 (12)F1—C10—C11—C12179.1 (9)
C1—C2—C3—C40.3 (13)C9—C10—C11—C120.7 (15)
C2—C3—C4—C50.4 (14)F2—C11—C12—C7178.8 (8)
C3—C4—C5—C60.2 (13)C10—C11—C12—C72.0 (13)
C2—C1—C6—C51.4 (11)C8—C7—C12—C112.8 (11)
C2—C1—C6—S1179.2 (6)N1—C7—C12—C11177.8 (7)
C4—C5—C6—C10.7 (11)C12—C7—N1—S147.0 (8)
C4—C5—C6—S1179.9 (6)C8—C7—N1—S1138.2 (6)
C12—C7—C8—C91.2 (11)C7—N1—S1—O155.0 (6)
N1—C7—C8—C9176.1 (7)C7—N1—S1—O2177.4 (5)
C12—C7—C8—I1177.3 (5)C7—N1—S1—C661.1 (6)
N1—C7—C8—I12.4 (9)C1—C6—S1—O1163.4 (6)
C7—C8—C9—C101.3 (13)C5—C6—S1—O117.1 (7)
I1—C8—C9—C10179.9 (7)C1—C6—S1—O232.5 (7)
C8—C9—C10—F1179.3 (8)C5—C6—S1—O2148.0 (6)
C8—C9—C10—C112.3 (14)C1—C6—S1—N181.1 (6)
F1—C10—C11—F20.1 (15)C5—C6—S1—N198.4 (6)
C9—C10—C11—F2178.6 (9)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1A···O2i0.862.583.169 (8)126
C12—H12···O10.932.272.916 (11)126
Symmetry code: (i) x+2, y+1, z.
Geometry of stacking interactions for I and II (Å, °). top
CompoundGroup AGroup BShortest contactsCgA···CgBPlane···CgBipasa
I(C7–C12)(C7–C12)ii3.747 (2)3.747 (2)3.602 (2)016.0 (1)
II(C1–C6)(C1–C6)ˆiii3.225 (2)3.621 (2)3.480 (2)016.0 (2)
(C7–C12)(C7–C12)iv3.499 (2)3.797 (2)3.436 (2)025.2 (2)
a) Cg is a group centroid; Plane···CgB is the distance between mean plane of Group A and centroid of the interacting Group B; ipa is interplanar angle; sa is slippage angle, which is the angle of CgA···CgB axis to the Group A mean plane normal. [Symmetry codes for I: (ii) 2-X,-Y,-Z; for II: (iii) 1-X,2-Y,-Z; (iv) 2-X,1-Y,1-Z.]

Acknowledgements

The authors thank the SAIF, IIT, Madras, India, for the data collection.

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