Abstract
In, K+·SO3–p-C6H4–N3 −, the conformation angle of the azido group with respect to the benzene ring is 19.1 (3)°, so that the anion is chiral within the crystal structure. In addition, the crystal structure is also chiral (Sohncke space group). The potassium ion is coordinated by three closer O atoms from three different sulfonyl groups [K⋯O 2.6486 (17) to 2.7787 (17) Å], three more distant O atoms [K⋯O 2.959 (2) to 3.206 (2) Å] and three N atoms at 3.073 (2) to 3.268 (2) Å. The anions are packed into layers perpendicular to b, only O and N atoms being at the surface of the layers. The K+ ions are located between the layers.
Keywords: crystal structure
Related literature
For the synthesis, see: Biesemeier et al. (2003 ▶). For the crystal structures of the same anion with different cations, see: Biesemeier et al. (2004a
▶,b
▶,c
▶).
Experimental
Crystal data
K(C6H4N3O3S)
M r = 237.28
Orthorhombic,
a = 5.4220 (5) Å
b = 7.9937 (7) Å
c = 19.267 (2) Å
V = 835.08 (15) Å3
Z = 4
Mo Kα radiation
μ = 0.87 mm−1
T = 193 K
0.55 × 0.33 × 0.25 mm
Data collection
STOE IPDS2 diffractometer
Absorption correction: integration (XPREP; Bruker, 2012 ▶) T min = 0.740, T max = 0.841
6140 measured reflections
1639 independent reflections
1591 reflections with I > 2σ(I)
R int = 0.038
Refinement
R[F 2 > 2σ(F 2)] = 0.018
wR(F 2) = 0.048
S = 1.09
1639 reflections
143 parameters
All H-atom parameters refined
Δρmax = 0.32 e Å−3
Δρmin = −0.25 e Å−3
Absolute structure: Flack x determined using 636 quotients [(I +)−(I −)]/[(I +)+(I −)] (Parsons & Flack, 2004 ▶)
Absolute structure parameter: 0.004 (16)
Data collection: X-AREA (Stoe & Cie, 2005 ▶); cell refinement: X-AREA; data reduction: X-AREA; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL2013 (Sheldrick, 2008 ▶); molecular graphics: DIAMOND (Brandenburg, 2000 ▶); software used to prepare material for publication: SHELXL2013.
Supplementary Material
Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536814015669/hp2068sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536814015669/hp2068Isup2.hkl
CCDC reference: 1012203
Additional supporting information: crystallographic information; 3D view; checkCIF report
supplementary crystallographic information
S1. Experimentelles
S1.1. Synthese und Kristallisation
Zur Synthese siehe Biesemeier et al. (2003). Beim letzten Schritt, der Kristallisation von K[O3S–C6H4–N3] aus Methanol, wurden die Kristalle aber nicht durch Abkühlen der Lösung erhalten, sondern durch partielle Verdunstung des Methanols bei Zimmertemperatur. Nach ihren Röntgendiagrammen haben die erhaltenen Kristalle die gleiche Struktur bei Zimmertemperatur und bei 193 K.
Elementaranalyse: C 30,30 % (ber. 30,37 %), H 1,92 % (ber. 1,70 %), N 17,68 % (ber. 17,71 %).
Infrarot-Spektrum (KBr-Pressling und Nujol-Verreibung, Absorptionsmaxima in cm–1): 2142 (νas N3), 1591, 1493, 1272 (νs N3), 1207 (νas SO3), 1143, 1117 (νs SO3), 1041, 1005, 831, 729, 711 (ν CS), 650 (δ N3), 569 (δ SO3), 524.
S1.2. Verfeinerung
Die Kristalldaten und Angaben zur Messung und Strukturverfeinerung sind in Tabelle 1 zusammengestellt.
S2. Ergebnisse und Diskussion
Die Titelverbindung wurde neben Kalium-4-pentazolylbenzolsulfonat (K+[O3S–C6H4–N5]–) wie beschrieben hergestellt (Biesemeier et al., 2003), aus 4-Diazoniumbenzolsulfonat und Natriumazid und anschließender Fällung mit KOH aus methanolischer Lösung bei –50°C. Das [O3S–C6H4N3]– -Ion eignet sich um K+ von Na+ durch Fällungsreaktion aus methanolischer Lösung zu trennen. Durch Extraktion mit Aceton, Eindampfen der Lösung und Umkristallisation aus Methanol wurden Kristalle der Titelverbindung erhalten. Wird das Umkristallisieren durch Abkühlen der methanolischen Lösung auf –45°C bewirkt, so entstehen Kristalle, die Satellitenreflexe zeigen. Lässt man dagegen das Methanol bei Zimmertemperatur verdunsten, treten keine Satellitenreflexe auf.
Das [O3S–C6H4–N3]– -Ion hat dieselbe Struktur, wie sie schon bei [THF-K-18-Krone-8][O3S–C6H4–N3] (Biesemeier et al., 2003) und mit weiteren Kationen (Biesemeier et al., 2004a,b,c) gefunden wurde (Fig. 1). Die Azidogruppe ist leicht geknickt (Winkel N–N–N 174,3°). Der Konformationswinkel der Azidogruppe relativ zum aromatischen Ring beträgt 19,1°. Damit ist das Molekül im Kristall chiral; im Kristall liegt kein Racemat vor (Sohncke-Raumgruppe P212121).
Ein Kalium-Ion ist von drei nähergelegenen O-Atomen aus drei verschiedenen Sulfonylgruppen koordiniert (S···O-Abstände 2,65 bis 2,78 Å). Dazu kommen drei etwas längere S···O-Kontakte zu drei weiteren O-Atomen. Von den insgesamt vier koordinierten Sulfonylgruppen sind zwei chelatartig an das K+ -Ion koordiniert. Etwas entfernter befinden sich Stickstoff-Atome (3,07, 3,10, 3,27 Å und weitere). Rechnet man nur die drei nächsten N-Atome zur Koordinationssphäre, so ist das Koordinationspolyeder ein 4-5-Polyeder, d.h. es hat ein verzerrtes Quadrat und ein gegenüberliegendes verzerrtes Fünfeck als Deckflächen (Fig. 2). Im Gegensatz dazu haben die N-Atome des [O3S–C6H4–N3]– -Ions im Na[O3S–C6H4–N3] keine Kontakte mit einem Na+ -Ion (Biesemeier et al., 2004a,b,c, Seite 37), ebensowenig wie mit den stark abgeschirmten Kalium-Atomen im [K-18-Krone-6-THF][O3S–C6H4–N3] (Biesemeier et al., 2003).
Die [O3S–C6H4–N3]– -Ionen sind zu Schichten senkrecht zur b-Achse gepackt. Auf den Außenseiten der Schichten befinden sich nur N- und O-Atome. Die K+ -Ionen befinden sich zwischen den Schichten (Fig. 3).
Figures
Fig. 1.

Die Molekularstruktur des [O3S–C6H4–N3]–-Ions. Schwingungsellipsoide mit 50% Aufenthaltswahrscheinlichkeit bei 193 K. Bindungslängen in Å.
Fig. 2.
Das Koordinationspolyeder um ein K+-Ion bis 3,30 Å. Kontaktabstände in Å. Man betrachte das Stereobild über Kreuz (linkes Bild für das rechte Auge).
Fig. 3.
Die Kristallpackung in K[O3S–C6H4–N3]. Beim K+-Ion im der Mitte unten sind alle koordinierten Atome bis zu einem Abstand von 3,30 Å eingezeichnet. Stereobild über Kreuz betrachten.
Crystal data
| K(C6H4N3O3S) | Dx = 1.887 Mg m−3 |
| Mr = 237.28 | Mo Kα radiation, λ = 0.71069 Å |
| Orthorhombic, P212121 | Cell parameters from 10459 reflections |
| a = 5.4220 (5) Å | θ = 2.1–26.1° |
| b = 7.9937 (7) Å | µ = 0.87 mm−1 |
| c = 19.267 (2) Å | T = 193 K |
| V = 835.08 (15) Å3 | Prism, yellow |
| Z = 4 | 0.55 × 0.33 × 0.25 mm |
| F(000) = 480 |
Data collection
| STOE IPDS2 diffractometer | 1639 independent reflections |
| Radiation source: sealed X-ray tube | 1591 reflections with I > 2σ(I) |
| Graphite monochromator | Rint = 0.038 |
| ω scans | θmax = 26.1°, θmin = 2.1° |
| Absorption correction: integration (XPREP; Bruker, 2012) | h = −6→6 |
| Tmin = 0.740, Tmax = 0.841 | k = −9→9 |
| 6140 measured reflections | l = −23→23 |
Refinement
| Refinement on F2 | Secondary atom site location: difference Fourier map |
| Least-squares matrix: full | Hydrogen site location: difference Fourier map |
| R[F2 > 2σ(F2)] = 0.018 | All H-atom parameters refined |
| wR(F2) = 0.048 | w = 1/[σ2(Fo2) + (0.0214P)2 + 0.2034P] where P = (Fo2 + 2Fc2)/3 |
| S = 1.09 | (Δ/σ)max < 0.001 |
| 1639 reflections | Δρmax = 0.32 e Å−3 |
| 143 parameters | Δρmin = −0.25 e Å−3 |
| 0 restraints | Absolute structure: Flack x determined using 636 quotients [(I+)-(I-)]/[(I+)+(I-)] (Parsons & Flack, 2004) |
| Primary atom site location: structure-invariant direct methods | Absolute structure parameter: 0.004 (16) |
Special details
| 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. |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)
| x | y | z | Uiso*/Ueq | ||
| K | −0.01018 (9) | 0.67980 (6) | 0.26487 (2) | 0.02287 (13) | |
| S | 0.49304 (10) | −0.10392 (6) | 0.33927 (2) | 0.01569 (12) | |
| O1 | 0.5157 (4) | −0.28483 (18) | 0.33948 (8) | 0.0325 (4) | |
| O2 | 0.2819 (3) | −0.0487 (2) | 0.29887 (7) | 0.0216 (3) | |
| O3 | 0.7217 (3) | −0.0217 (2) | 0.32010 (8) | 0.0274 (4) | |
| N1 | 0.3166 (3) | 0.0942 (2) | 0.63445 (9) | 0.0211 (4) | |
| N2 | 0.1000 (3) | 0.1318 (2) | 0.65003 (9) | 0.0186 (4) | |
| N3 | −0.0882 (3) | 0.1672 (3) | 0.66954 (10) | 0.0253 (4) | |
| C1 | 0.4320 (4) | −0.0448 (3) | 0.42651 (10) | 0.0170 (4) | |
| C2 | 0.2204 (4) | 0.0433 (3) | 0.44334 (10) | 0.0193 (4) | |
| C3 | 0.1787 (4) | 0.0909 (3) | 0.51178 (10) | 0.0195 (4) | |
| C4 | 0.3477 (4) | 0.0485 (3) | 0.56286 (10) | 0.0179 (4) | |
| C5 | 0.5598 (4) | −0.0410 (3) | 0.54628 (11) | 0.0203 (4) | |
| C6 | 0.6009 (4) | −0.0873 (3) | 0.47797 (11) | 0.0196 (4) | |
| H2 | 0.095 (4) | 0.065 (3) | 0.4069 (12) | 0.020 (6)* | |
| H3 | 0.047 (5) | 0.153 (3) | 0.5228 (12) | 0.019 (6)* | |
| H5 | 0.665 (5) | −0.074 (3) | 0.5797 (13) | 0.021 (6)* | |
| H6 | 0.730 (5) | −0.150 (3) | 0.4652 (13) | 0.023 (6)* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| K | 0.0214 (2) | 0.0205 (2) | 0.0268 (2) | −0.0031 (2) | 0.0020 (2) | −0.00356 (16) |
| S | 0.0137 (2) | 0.0174 (2) | 0.0159 (2) | 0.0008 (2) | 0.0016 (2) | −0.00066 (16) |
| O1 | 0.0519 (10) | 0.0183 (8) | 0.0275 (8) | 0.0083 (8) | 0.0062 (10) | −0.0005 (6) |
| O2 | 0.0165 (7) | 0.0300 (8) | 0.0183 (7) | 0.0033 (7) | −0.0023 (6) | −0.0031 (6) |
| O3 | 0.0159 (7) | 0.0446 (10) | 0.0217 (7) | −0.0074 (7) | 0.0043 (6) | −0.0003 (7) |
| N1 | 0.0184 (8) | 0.0264 (9) | 0.0185 (8) | −0.0001 (8) | 0.0012 (7) | −0.0022 (8) |
| N2 | 0.0228 (9) | 0.0187 (9) | 0.0144 (8) | −0.0008 (7) | −0.0018 (7) | −0.0022 (6) |
| N3 | 0.0252 (10) | 0.0290 (10) | 0.0218 (9) | 0.0045 (8) | 0.0000 (7) | −0.0027 (8) |
| C1 | 0.0177 (10) | 0.0166 (9) | 0.0167 (8) | −0.0022 (8) | 0.0020 (7) | −0.0003 (7) |
| C2 | 0.0162 (10) | 0.0234 (10) | 0.0182 (10) | 0.0014 (9) | −0.0010 (7) | 0.0024 (8) |
| C3 | 0.0165 (9) | 0.0213 (10) | 0.0208 (9) | 0.0024 (9) | 0.0032 (8) | −0.0001 (8) |
| C4 | 0.0178 (10) | 0.0181 (10) | 0.0177 (9) | −0.0044 (8) | 0.0014 (7) | 0.0002 (8) |
| C5 | 0.0173 (10) | 0.0228 (10) | 0.0207 (9) | 0.0002 (8) | −0.0035 (7) | 0.0014 (8) |
| C6 | 0.0147 (9) | 0.0214 (11) | 0.0228 (10) | 0.0020 (9) | 0.0012 (8) | −0.0011 (8) |
Geometric parameters (Å, º)
| K—O1i | 3.206 (2) | N1—C4 | 1.437 (3) |
| K—O1ii | 2.959 (2) | N1—N2 | 1.249 (2) |
| K—O2iii | 2.6486 (17) | N2—N3 | 1.124 (3) |
| K—O2i | 2.7652 (18) | C1—C2 | 1.385 (3) |
| K—O3iv | 2.7787 (17) | C1—C6 | 1.392 (3) |
| K—O3ii | 2.9900 (19) | C2—C3 | 1.391 (3) |
| K—N1v | 3.0731 (19) | C3—C4 | 1.387 (3) |
| K—N3vi | 3.1001 (19) | C4—C5 | 1.391 (3) |
| K—N1vii | 3.2680 (18) | C5—C6 | 1.385 (3) |
| S—O1 | 1.4514 (15) | C2—H2 | 0.99 (2) |
| S—O2 | 1.4530 (15) | C3—H3 | 0.90 (3) |
| S—O3 | 1.4510 (16) | C5—H5 | 0.90 (3) |
| S—C1 | 1.7772 (19) | C6—H6 | 0.90 (3) |
| O2iii—K—O2i | 165.85 (3) | N3vi—K—N1vii | 63.38 (5) |
| O2iii—K—O3iv | 68.91 (5) | O1i—K—N1vii | 90.59 (4) |
| O2i—K—O3iv | 105.79 (5) | O3—S—O1 | 112.31 (12) |
| O2iii—K—O1ii | 78.93 (5) | O3—S—O2 | 113.54 (9) |
| O2i—K—O1ii | 107.90 (5) | O1—S—O2 | 111.77 (11) |
| O3iv—K—O1ii | 146.17 (5) | O1—S—C1 | 106.14 (9) |
| O2iii—K—O3ii | 116.42 (5) | O2—S—C1 | 106.21 (9) |
| O2i—K—O3ii | 64.39 (4) | O3—S—C1 | 106.23 (9) |
| O3iv—K—O3ii | 161.09 (5) | S—O1—Kviii | 99.64 (10) |
| O1ii—K—O3ii | 47.81 (4) | S—O1—Kix | 90.64 (9) |
| O2iii—K—N1v | 68.35 (5) | S—O2—Kx | 153.64 (10) |
| O2i—K—N1v | 125.79 (5) | S—O2—Kix | 109.87 (9) |
| O3iv—K—N1v | 97.52 (5) | S—O3—Kxi | 153.32 (10) |
| O1ii—K—N1v | 59.72 (5) | S—O3—Kviii | 98.31 (9) |
| O3ii—K—N1v | 101.27 (5) | N2—N1—C4 | 113.74 (17) |
| O2iii—K—N3vi | 66.84 (5) | N1—N2—N3 | 174.3 (2) |
| O2i—K—N3vi | 103.47 (5) | C2—C1—C6 | 120.18 (18) |
| O3iv—K—N3vi | 105.97 (5) | C2—C1—S | 120.73 (15) |
| O1ii—K—N3vi | 68.90 (5) | C6—C1—S | 119.09 (16) |
| O3ii—K—N3vi | 63.54 (5) | C1—C2—C3 | 119.72 (19) |
| N1v—K—N3vi | 116.14 (5) | C1—C2—H2 | 119.5 (14) |
| O2iii—K—O1i | 139.77 (5) | C3—C2—H2 | 120.7 (14) |
| O2i—K—O1i | 46.78 (4) | C4—C3—C2 | 119.89 (19) |
| O3iv—K—O1i | 79.32 (5) | C4—C3—H3 | 119.6 (15) |
| O1ii—K—O1i | 123.12 (5) | C2—C3—H3 | 120.5 (15) |
| O3ii—K—O1i | 101.68 (4) | C3—C4—C5 | 120.59 (19) |
| N1v—K—O1i | 92.96 (5) | C3—C4—N1 | 122.77 (19) |
| N3vi—K—O1i | 148.83 (5) | C5—C4—N1 | 116.64 (18) |
| O2iii—K—N1vii | 101.73 (5) | C6—C5—C4 | 119.3 (2) |
| O2i—K—N1vii | 64.18 (4) | C6—C5—H5 | 119.9 (16) |
| O3iv—K—N1vii | 71.73 (5) | C4—C5—H5 | 120.8 (16) |
| O1ii—K—N1vii | 126.86 (5) | C5—C6—C1 | 120.4 (2) |
| O3ii—K—N1vii | 89.35 (5) | C5—C6—H6 | 122.5 (16) |
| N1v—K—N1vii | 167.85 (5) | C1—C6—H6 | 117.0 (16) |
| N2—N1—C4—C3 | 19.1 (3) | O1—S—C1—C2 | −121.7 (2) |
| N2—N1—C4—C5 | −161.41 (19) | O2—S—C1—C2 | −2.6 (2) |
| C3—C4—C5—C6 | 0.1 (3) | O1—S—C1—C6 | 58.7 (2) |
| N1—C4—C5—C6 | −179.5 (2) | O2—S—C1—C6 | 177.77 (17) |
| C5—C4—C3—C2 | 0.3 (3) | O3—S—C1—C2 | 118.55 (19) |
| N1—C4—C3—C2 | 179.8 (2) | O3—S—C1—C6 | −61.1 (2) |
| C1—C2—C3—C4 | −0.7 (3) | C4—C5—C6—C1 | 0.0 (3) |
| C3—C2—C1—C6 | 0.8 (3) | C2—C1—C6—C5 | −0.5 (3) |
| C3—C2—C1—S | −178.80 (17) | S—C1—C6—C5 | 179.14 (18) |
Symmetry codes: (i) x, y+1, z; (ii) x−1, y+1, z; (iii) −x, y+1/2, −z+1/2; (iv) −x+1, y+1/2, −z+1/2; (v) x−1/2, −y+1/2, −z+1; (vi) −x−1/2, −y+1, z−1/2; (vii) −x+1/2, −y+1, z−1/2; (viii) x+1, y−1, z; (ix) x, y−1, z; (x) −x, y−1/2, −z+1/2; (xi) −x+1, y−1/2, −z+1/2.
Footnotes
This paper is dedicated to Professor Dr Werner Massa on his 70th birthday.
Supporting information for this paper is available from the IUCr electronic archives (Reference: HP2068).
References
- Biesemeier, F., Harms, K. & Müller, U. (2003). Z. Anorg. Allg. Chem. 630, 787–793.
- Biesemeier, F., Harms, K. & Müller, U. (2004a). Z. Kristallogr. New Cryst. Struct. 219, 37–38.
- Biesemeier, F., Harms, K. & Müller, U. (2004b). Z. Kristallogr. New Cryst. Struct. 219, 39–40.
- Biesemeier, F., Harms, K. & Müller, U. (2004c). Z. Kristallogr. New Cryst. Struct. 219, 41–43.
- Brandenburg, K. (2000). DIAMOND Crystal Impact GbR, Bonn, Germany.
- Bruker (2012). XPREP Bruker AXS Inc., Madison, Wisconsin, USA.
- Parsons, S. & Flack, H. (2004). Acta Cryst. A60, s61.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Stoe & Cie (2005). X-AREA und X-RED32 Stoe & Cie, Darmstadt, Germany.
Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536814015669/hp2068sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536814015669/hp2068Isup2.hkl
CCDC reference: 1012203
Additional supporting information: crystallographic information; 3D view; checkCIF report


