research papers 682 https://doi.org/10.1107/S2053229617011172 Acta Cryst. (2017). C73, 682–687 Received 6 May 2017 Accepted 28 July 2017 Edited by M. Kubicki, Adam Mickiewicz University, Poland Keywords: bifurcated hydrogen bonding; fluorous weak interaction; crystal structure; halogen bonding; pyridinium salt; supra- molecular interactions; synthon. CCDC references: 1565383; 1565382 Supporting information: this article has supporting information at journals.iucr.org/c Weak hydrogen and halogen bonding in 4-[(2,2-difluoroethoxy)methyl]pyridinium iodide and 4-[(3-chloro-2,2,3,3-tetrafluoropropoxy)- methyl]pyridinium iodide Norman Lu, a * Rong-Jyun Wei, a Hsing-Fang Chiang, a,b Joseph S. Thrasher, b Yuh-Sheng Wen c and Ling-Kang Liu a,c a Institute of Organic and Polymeric Materials, National Taipei University of Technology, Taipei 106, Taiwan, b Department of Chemistry, Clemson University, Advanced Materials Research Laboratory, 91 Technology Drive, Anderson, SC, USA, and c Institute of Chemistry, Academia Sinica, Taipei 115, Taiwan. *Correspondence e-mail: normanlu@mail.ntut.edu.tw To enable a comparison between a C—HX hydrogen bond and a halogen bond, the structures of two fluorous-substituted pyridinium iodide salts have been determined. 4-[(2,2-Difluoroethoxy)methyl]pyridinium iodide, C 8 H 10 F 2 - NO + I , (1), has a –CH 2 OCH 2 CF 2 H substituent at the para position of the pyridinium ring and 4-[(3-chloro-2,2,3,3-tetrafluoropropoxy)methyl]pyridinium iodide, C 9 H 9 ClF 4 NO + I , (2), has a –CH 2 OCH 2 CF 2 CF 2 Cl substituent at the para position of the pyridinium ring. In salt (1), the iodide anion is involved in one N—HI and three C—HI hydrogen bonds, which, together with C—HF hydrogen bonds, link the cations and anions into a three-dimensional network. For salt (2), the iodide anion is involved in one N—HI hydrogen bond, two C—HI hydrogen bonds and one C—ClI halogen bond; additional C— HF and C—FF interactions link the cations and anions into a three- dimensional arrangement. 1. Introduction The role of hydrogen bonding has long been recognized as controlling structures in a wide variety of materials (Jeffrey & Saenger, 1991; Jeffrey, 2003; Steiner, 2002; Nagy, 2014). In general, hydrogen bonding spans from the covalent limit (e.g. HF 2 anion, 40 kcal mol 1 ; 1 kcal mol 1 = 4.184 kJ mol 1 ) to the electrostatic limit (e.g. NH 4 + Cl , 15 kcal mol 1 ). The even weaker C—HF hydrogen bond is on the van der Waals limit (0.25 kcal mol 1 ) (Desiraju, 2002; Desiraju & Steiner, 1999). Alternatively, studies on halogen-bonding interactions with other electronegative species have shown that halogen bonding, where the halogen atom acts as a Lewis base acceptor, is driven by a region of positive electrostatic potential (i.e. the -hole) which arises from the anisotropic distribution of electron density within the halogen atom (Jagarlapudi et al., 1986; Price et al. , 1994; Metrangolo et al. , 2008; Politzer et al., 2010). Halogen bonds have found increasing practical applications, such as in the discovery and development of active pharmaceutical ingredients (APIs) (Wilcken et al., 2012; Baldrighi et al., 2013). A halide ion may serve as a hydrogen-bond acceptor or as a halogen-bond acceptor. For example, pyridinium halides in the solid state were known to have the halide ion exhibiting four hydrogen bonds, arranged in a distorted tetrahedral geometry (Mootz & Hocken, 1989), forming alternating cation–anion chains that are crosslinked using halide ions as ISSN 2053-2296 # 2017 International Union of Crystallography