Buy article online - an online subscription or single-article purchase is required to access this article.
Download citation
Download citation
link to html
The structure of the title compound, C7H7Cl2NO2S, resembles those of other methane­sulfonanilides, with similar geometric parameters. The amide H atom is roughly in the plane of the dichloro­phenyl group with a deviation of −0.021 (7) Å, while the S atom is slightly above the plane with a deviation of 0.285 (9) Å. The dihedral angle between the benzene ring and the C—N—S plane is 14.4 (5)°. The mol­ecules are packed into chains through N—H...O hydrogen bonds and weak (methyl)C—H...O inter­actions.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807026724/dn2186sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807026724/dn2186Isup2.hkl
Contains datablock I

CCDC reference: 614682

Key indicators

  • Single-crystal X-ray study
  • T = 299 K
  • Mean [sigma](C-C) = 0.008 Å
  • R factor = 0.092
  • wR factor = 0.255
  • Data-to-parameter ratio = 14.1

checkCIF/PLATON results

No syntax errors found



Alert level C RFACR01_ALERT_3_C The value of the weighted R factor is > 0.25 Weighted R factor given 0.255 PLAT062_ALERT_4_C Rescale T(min) & T(max) by ..................... 1.33 PLAT063_ALERT_3_C Crystal Probably too Large for Beam Size ....... 0.75 mm PLAT340_ALERT_3_C Low Bond Precision on C-C Bonds (x 1000) Ang ... 8
Alert level G ABSTM02_ALERT_3_G When printed, the submitted absorption T values will be replaced by the scaled T values. Since the ratio of scaled T's is identical to the ratio of reported T values, the scaling does not imply a change to the absorption corrections used in the study. Ratio of Tmax expected/reported 1.330 Tmax scaled 0.794 Tmin scaled 0.057 PLAT860_ALERT_3_G Note: Number of Least-Squares Restraints ....... 1
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 4 ALERT level C = Check and explain 2 ALERT level G = General alerts; check 0 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 5 ALERT type 3 Indicator that the structure quality may be low 1 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check

Comment top

The biological activity of sulfonanilides is thought to be due to the amide hydrogen portion of the molecules as it can align itself in relation to a receptor site. Thus the structural studies of sulfonanilides are of interest. In the present work, the structure of N-(3,5-dichlorophenyl)-methanesulfonamde (35DCPMSA) has been determined as part of our study of the substituent effects on the solid state structures of methanesulfonanilides (Gowda et al., 2007a, b). The structure of 35DCPMSA (Fig. 1) is similar to those of other methanesulfonanilides (Gowda et al., 2007a, b). 35DCPMSA crystallizes in monoclinic P21/c space group in contrast to the monoclinc P21/c, monoclinic P21/n, triclinic P-1 and triclinic P-1 space groups observed for N-(2,3-dichlorophenyl)-methanesulfonamide (23DCPMSA), N-(2,4-dichlorophenyl)-methanesulfonamide (24DCPMSA), N-(2,5-dichlorophenyl)-methanesulfonamide (25DCPMSA), N-(3,4-dichlorophenyl)-methanesulfonamide (34DCPMSA)(Gowda et al., 2007b), respectively. The substitution of a Cl atom at the meta position of N-(phenyl)-methanesulfonamde (PMSA) (Klug, 1968) to produce N-(3-chlorophenyl)-methanesulfonamide (3CPMSA) changes its space group from monoclinic P21/c to C 2/c (Gowda et al., 2007a). The substitution of an additional chloro group either at ortho, para or meta position of 3CPMSA to produce 23DCPMSA, 34DCPMSA or 35DCPMSA, respectively, changes the space group from monoclinc C 2/c to monoclinic P21/c with 23DCPMSA, triclinic P-1 with 34DCPMSA and monoclinic P21/c with 35DCPMSA. The geometric parameters in 35DCPMSA are similar to those in other methanesulfonanilides except for some difference in the bond and torsional angles. The N—H is roughly in the plane of the dichlorophenyl group with a deviation of -0.021 (7) Å from the plane, whereas the S atom is slightly above with a deviation of 0.285 (9) Å. The dihedral angle between the benzene ring and the C6—N5—S2 plane is 14.4 (5)°. The N—H···O hydrogen bonds (Table 1) build up chains which are further connected through weak C—H (methyl)···O interactions (Fig. 2).

Related literature top

For related literature, see: Gowda et al. (2007a, 2007b); Jayalakshmi & Gowda (2004); Klug (1968).

Experimental top

The title compound was prepared according to the literature method (Jayalakshmi & Gowda, 2004). The purity of the compound was checked by determining its melting point. It was characterized by recording its infrared and NMR spectra (Jayalakshmi & Gowda, 2004). Single crystals of the compound were obtained from a slow evaporation of its ethanolic solution and used for X-ray diffraction studies at room temperature.

Refinement top

H atoms attached to C atoms were fixed geometrically and treated as riding, with C—H = 0.93 Å (aromatic) or 0.96 Å (CH3) and with Uiso(H) = 1.2Ueq(aromatic) or Uiso(H) = 1.5Ueq(CH3). H atom attched to N was refined using a N—H restraint of 0.85 (1) Å.

Structure description top

The biological activity of sulfonanilides is thought to be due to the amide hydrogen portion of the molecules as it can align itself in relation to a receptor site. Thus the structural studies of sulfonanilides are of interest. In the present work, the structure of N-(3,5-dichlorophenyl)-methanesulfonamde (35DCPMSA) has been determined as part of our study of the substituent effects on the solid state structures of methanesulfonanilides (Gowda et al., 2007a, b). The structure of 35DCPMSA (Fig. 1) is similar to those of other methanesulfonanilides (Gowda et al., 2007a, b). 35DCPMSA crystallizes in monoclinic P21/c space group in contrast to the monoclinc P21/c, monoclinic P21/n, triclinic P-1 and triclinic P-1 space groups observed for N-(2,3-dichlorophenyl)-methanesulfonamide (23DCPMSA), N-(2,4-dichlorophenyl)-methanesulfonamide (24DCPMSA), N-(2,5-dichlorophenyl)-methanesulfonamide (25DCPMSA), N-(3,4-dichlorophenyl)-methanesulfonamide (34DCPMSA)(Gowda et al., 2007b), respectively. The substitution of a Cl atom at the meta position of N-(phenyl)-methanesulfonamde (PMSA) (Klug, 1968) to produce N-(3-chlorophenyl)-methanesulfonamide (3CPMSA) changes its space group from monoclinic P21/c to C 2/c (Gowda et al., 2007a). The substitution of an additional chloro group either at ortho, para or meta position of 3CPMSA to produce 23DCPMSA, 34DCPMSA or 35DCPMSA, respectively, changes the space group from monoclinc C 2/c to monoclinic P21/c with 23DCPMSA, triclinic P-1 with 34DCPMSA and monoclinic P21/c with 35DCPMSA. The geometric parameters in 35DCPMSA are similar to those in other methanesulfonanilides except for some difference in the bond and torsional angles. The N—H is roughly in the plane of the dichlorophenyl group with a deviation of -0.021 (7) Å from the plane, whereas the S atom is slightly above with a deviation of 0.285 (9) Å. The dihedral angle between the benzene ring and the C6—N5—S2 plane is 14.4 (5)°. The N—H···O hydrogen bonds (Table 1) build up chains which are further connected through weak C—H (methyl)···O interactions (Fig. 2).

For related literature, see: Gowda et al. (2007a, 2007b); Jayalakshmi & Gowda (2004); Klug (1968).

Computing details top

Data collection: CAD-4-PC Software (Enraf–Nonius, 1996); cell refinement: CAD-4-PC Software; data reduction: REDU4 (Stoe & Cie, 1987); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEPIII (Burnett & Johnson, 1996), ORTEP-3 for Windows (Farrugia, 1997) and PLATON (Spek, 2003); software used to prepare material for publication: SHELXL97.

Figures top
[Figure 1] Fig. 1. Molecular structure of the title compound showing the atom labelling scheme. Displacement ellipsoids are drawn at the 30% probability level. H atoms are represented as small spheres of arbitrary radii.
[Figure 2] Fig. 2. Partial packing view showing the formation of the hydrogen bond network through N—H···O and C—H···O hydrogen bonding interactions. H bonds are shown as dashed lines. H atoms not involved in hydrogen bonding have been omitted for clarity. [Symmetry code: (i) -x + 1, 1/2 + y, 3/2 - z; (ii) x, 1 + y, z].
N-(3,5-dichlorophenyl)methanesulfonamide top
Crystal data top
C7H7Cl2NO2SF(000) = 488
Mr = 240.10Dx = 1.627 Mg m3
Monoclinic, P21/cCu Kα radiation, λ = 1.54180 Å
Hall symbol: -P 2ybcCell parameters from 25 reflections
a = 16.076 (3) Åθ = 2.8–19.9°
b = 5.053 (2) ŵ = 7.70 mm1
c = 12.148 (3) ÅT = 299 K
β = 96.60 (2)°Long laminar, colourless
V = 980.3 (5) Å30.75 × 0.30 × 0.03 mm
Z = 4
Data collection top
Enraf–Nonius CAD4
diffractometer
1424 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.059
Graphite monochromatorθmax = 67.1°, θmin = 2.8°
ω scansh = 1919
Absorption correction: ψ scan
(North et al., 1968)
k = 06
Tmin = 0.043, Tmax = 0.597l = 141
1828 measured reflections3 standard reflections every 120 min
1731 independent reflections intensity decay: 2.5%
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.092Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.255H atoms treated by a mixture of independent and constrained refinement
S = 1.09 w = 1/[σ2(Fo2) + (0.2P)2]
where P = (Fo2 + 2Fc2)/3
1731 reflections(Δ/σ)max < 0.001
123 parametersΔρmax = 1.17 e Å3
1 restraintΔρmin = 0.70 e Å3
Crystal data top
C7H7Cl2NO2SV = 980.3 (5) Å3
Mr = 240.10Z = 4
Monoclinic, P21/cCu Kα radiation
a = 16.076 (3) ŵ = 7.70 mm1
b = 5.053 (2) ÅT = 299 K
c = 12.148 (3) Å0.75 × 0.30 × 0.03 mm
β = 96.60 (2)°
Data collection top
Enraf–Nonius CAD4
diffractometer
1424 reflections with I > 2σ(I)
Absorption correction: ψ scan
(North et al., 1968)
Rint = 0.059
Tmin = 0.043, Tmax = 0.5973 standard reflections every 120 min
1828 measured reflections intensity decay: 2.5%
1731 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0921 restraint
wR(F2) = 0.255H atoms treated by a mixture of independent and constrained refinement
S = 1.09Δρmax = 1.17 e Å3
1731 reflectionsΔρmin = 0.70 e Å3
123 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
C10.6079 (3)0.3484 (10)1.0081 (4)0.0512 (12)
H1A0.58100.26571.06580.077*
H1B0.58940.52860.99940.077*
H1C0.66750.34471.02750.077*
C60.7071 (3)0.3919 (9)0.7811 (3)0.0415 (10)
C70.7711 (3)0.2524 (11)0.8417 (4)0.0525 (12)
H70.75960.11820.89010.063*
C80.8527 (4)0.3193 (11)0.8280 (5)0.0587 (13)
C90.8727 (3)0.5086 (12)0.7540 (5)0.0611 (13)
H90.92810.54880.74560.073*
C100.8076 (4)0.6353 (11)0.6932 (5)0.0562 (12)
C110.7251 (3)0.5846 (9)0.7054 (4)0.0482 (11)
H110.68220.67700.66410.058*
N50.6212 (2)0.3432 (8)0.7865 (3)0.0437 (9)
O30.4928 (2)0.1929 (7)0.8545 (3)0.0532 (9)
O40.6204 (2)0.0779 (7)0.8935 (3)0.0618 (10)
S20.58202 (7)0.1770 (2)0.88336 (8)0.0415 (5)
Cl120.83015 (11)0.8707 (3)0.59639 (16)0.0837 (6)
Cl130.93272 (10)0.1532 (5)0.90719 (17)0.0962 (8)
H50.586 (2)0.451 (7)0.754 (3)0.033 (11)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.063 (3)0.046 (3)0.043 (2)0.002 (2)0.003 (2)0.0037 (19)
C60.046 (2)0.035 (2)0.043 (2)0.0028 (18)0.0066 (17)0.0026 (17)
C70.056 (3)0.051 (3)0.051 (2)0.007 (2)0.008 (2)0.006 (2)
C80.053 (3)0.061 (3)0.061 (3)0.006 (2)0.003 (2)0.006 (2)
C90.051 (3)0.060 (3)0.074 (3)0.006 (2)0.017 (2)0.002 (3)
C100.063 (3)0.046 (3)0.063 (3)0.001 (2)0.022 (2)0.005 (2)
C110.056 (2)0.036 (2)0.053 (2)0.004 (2)0.012 (2)0.0040 (19)
N50.043 (2)0.045 (2)0.0418 (19)0.0047 (15)0.0016 (16)0.0088 (15)
O30.0509 (18)0.048 (2)0.0596 (19)0.0087 (14)0.0031 (15)0.0066 (14)
O40.076 (2)0.0288 (18)0.082 (2)0.0097 (17)0.0151 (19)0.0060 (16)
S20.0479 (7)0.0299 (7)0.0466 (7)0.0017 (4)0.0061 (5)0.0010 (4)
Cl120.0841 (11)0.0712 (11)0.1022 (12)0.0009 (8)0.0379 (9)0.0311 (9)
Cl130.0531 (9)0.1287 (19)0.1048 (13)0.0228 (8)0.0006 (8)0.0388 (11)
Geometric parameters (Å, º) top
C1—S21.754 (5)C8—Cl131.732 (6)
C1—H1A0.9600C9—C101.369 (8)
C1—H1B0.9600C9—H90.9300
C1—H1C0.9600C10—C111.376 (7)
C6—C71.387 (7)C10—Cl121.740 (5)
C6—C111.392 (7)C11—H110.9300
C6—N51.412 (6)N5—S21.630 (4)
C7—C81.382 (8)N5—H50.85 (3)
C7—H70.9300O3—S21.439 (4)
C8—C91.376 (8)O4—S21.427 (4)
S2—C1—H1A109.5C8—C9—H9121.4
S2—C1—H1B109.5C9—C10—C11122.8 (5)
H1A—C1—H1B109.5C9—C10—Cl12118.6 (4)
S2—C1—H1C109.5C11—C10—Cl12118.6 (4)
H1A—C1—H1C109.5C10—C11—C6118.5 (5)
H1B—C1—H1C109.5C10—C11—H11120.7
C7—C6—C11120.6 (4)C6—C11—H11120.7
C7—C6—N5123.8 (4)C6—N5—S2125.8 (3)
C11—C6—N5115.5 (4)C6—N5—H5118 (3)
C8—C7—C6117.9 (5)S2—N5—H5112 (3)
C8—C7—H7121.1O4—S2—O3118.7 (2)
C6—C7—H7121.1O4—S2—N5109.2 (2)
C9—C8—C7123.0 (5)O3—S2—N5104.6 (2)
C9—C8—Cl13119.0 (4)O4—S2—C1108.3 (2)
C7—C8—Cl13117.9 (4)O3—S2—C1108.3 (2)
C10—C9—C8117.1 (5)N5—S2—C1107.2 (2)
C10—C9—H9121.4
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N5—H5···O3i0.85 (3)2.11 (4)2.949 (5)170 (4)
C1—H1B···O4ii0.962.453.233 (6)138
Symmetry codes: (i) x+1, y+1/2, z+3/2; (ii) x, y+1, z.

Experimental details

Crystal data
Chemical formulaC7H7Cl2NO2S
Mr240.10
Crystal system, space groupMonoclinic, P21/c
Temperature (K)299
a, b, c (Å)16.076 (3), 5.053 (2), 12.148 (3)
β (°) 96.60 (2)
V3)980.3 (5)
Z4
Radiation typeCu Kα
µ (mm1)7.70
Crystal size (mm)0.75 × 0.30 × 0.03
Data collection
DiffractometerEnraf–Nonius CAD4
Absorption correctionψ scan
(North et al., 1968)
Tmin, Tmax0.043, 0.597
No. of measured, independent and
observed [I > 2σ(I)] reflections
1828, 1731, 1424
Rint0.059
(sin θ/λ)max1)0.597
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.092, 0.255, 1.09
No. of reflections1731
No. of parameters123
No. of restraints1
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)1.17, 0.70

Computer programs: CAD-4-PC Software (Enraf–Nonius, 1996), CAD-4-PC Software, REDU4 (Stoe & Cie, 1987), SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), ORTEPIII (Burnett & Johnson, 1996), ORTEP-3 for Windows (Farrugia, 1997) and PLATON (Spek, 2003), SHELXL97.

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N5—H5···O3i0.85 (3)2.11 (4)2.949 (5)170 (4)
C1—H1B···O4ii0.962.453.233 (6)138.4
Symmetry codes: (i) x+1, y+1/2, z+3/2; (ii) x, y+1, z.
 

Subscribe to Acta Crystallographica Section E: Crystallographic Communications

The full text of this article is available to subscribers to the journal.

If you have already registered and are using a computer listed in your registration details, please email support@iucr.org for assistance.

Buy online

You may purchase this article in PDF and/or HTML formats. For purchasers in the European Community who do not have a VAT number, VAT will be added at the local rate. Payments to the IUCr are handled by WorldPay, who will accept payment by credit card in several currencies. To purchase the article, please complete the form below (fields marked * are required), and then click on `Continue'.
E-mail address* 
Repeat e-mail address* 
(for error checking) 

Format*   PDF (US $40)
   HTML (US $40)
   PDF+HTML (US $50)
In order for VAT to be shown for your country javascript needs to be enabled.

VAT number 
(non-UK EC countries only) 
Country* 
 

Terms and conditions of use
Contact us

Follow Acta Cryst. E
Sign up for e-alerts
Follow Acta Cryst. on Twitter
Follow us on facebook
Sign up for RSS feeds