Abstract

Paracetamol (PCM) has two well-documented polymorphic forms at room temperature; monoclinic Form I is more stable than the other orthorhombic Form II. Form II exhibits improved tabletting properties compared to Form I due to low shearing forces; however, difficulties in its manufacture have limited its use in industrial manufacture. Previous studies have found that the introduction of a co-former to form co-crystals would allow the PCM molecule to exist in a conformation similar to that of the orthorhombic form while being more stable at room temperature. Experimental charge density analysis of the paracetamol-4,4′-bipyridine (PCM-44BP) co-crystal system, and its constituent molecules, has been carried out to examine the forces that drive the formation and stabilisation of the co-crystal, while allowing PCM to maintain a packing motif similar to that found in Form II. It is hoped studies on this well-known compound will help apply the knowledge gained to other drug molecules that are less successful. The PCM molecules in the co-crystal were found to exhibit similar packing motifs to that found in Form I, however, intercalation of the 44BP molecule between the PCM layers resulted in a shallower angle between molecular planes, which could result in the required lateral shear. Topological analysis identified more weak interactions in the co-crystal compared to the individual molecules, thus allowing for greater stability as evidenced by the lattice energies. Weak interactions in the PCM-44BP co-crystal were found to range in strength from 4.08–84.33 kJ mol−1, and this variety allowed the PCM-44BP planes to be held together, while a weak π–π interaction (15.14 kJ mol−1) allowed lateral shear to occur, thus mimicking the planes found in Form II PCM and offering the possibility of improved tabletting properties. A comparison of integrated atomic charges between partitions of the PCM molecules in the single and co-crystal found that the hydroxyl and amide groups were involved in greater hydrogen bonding in the co-crystal, resulting in a charge redistribution across the molecule evidenced by a larger molecular dipole moment (µ = 12.34D). These findings, in addition to the co-crystal having the largest lattice energy, form a potential basis with which to predict that the co-crystal exhibits improved solubility and stability profiles. It is anticipated that these findings will contribute to improvements in the formulation and other physical properties of PCM and other pharmaceutical compounds.

Highlights

  • Crystal engineering refers to the rational design of solids by inducing the reproducible formation of weak interactions between pairs of functional groups [1]

  • The molecular electrostatic potential (MEP) is an integral part in linking the results found in electron density distribution (EDD)

  • We present an EDD study of PCM (1), 44BP (2) and the PCM-44BP (3) co-crystal with the aim of exploring a potential contributing factor towards the poor tableting properties exhibited by Form I

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Summary

Introduction

Crystal engineering refers to the rational design of solids by inducing the reproducible formation of weak interactions between pairs of functional groups [1] This field has recently undergone a resurgence because of increased interest from pharmaceutical companies and research institutions. Due to the excessive costs associated with bringing a new drug from the design stage through to the market, many pharmaceutical companies have opted to revisit older drug candidates that did not make it to market and to seek to improve their physicochemical properties This approach encompasses a very large number of drugs as over 90% of drug candidates fail due to poor physicochemical properties, resulting in sub-optimal in vivo performance or a requirement for the development of inconvenient dosage forms [3]. There continues to be much debate regarding the definition of co-crystals, including whether solvates and hydrates are included in the same definition: the FDA has defined co-crystals as “solids that are crystalline materials composed of two or more molecules in the same crystal lattice” with the interactions between them governed by “non-ionic interactions” [5]

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