The dynamics of organic cations in metal halide hybrid perovskites (MHPs) have been investigated using numerous experimental and computational techniques because of their suspected effects on the properties of MHPs. In this Perspective, we summarize and reconcile key findings and present new data to synthesize a unified understanding of the dynamics of the cations. We conclude that theory and experiment collectively paint a relatively complete picture of rotational dynamics within MHPs. This picture is then used to discuss the consequences of structural dynamics for electron−phonon interactions and their effect on material properties by providing a brief account of key studies that correlate cation dynamics with the dynamics of the inorganic sublattice and overall device properties.M etal halide perovskites (MHPs) are enjoying considerable academic and industrial interest due to their high photovoltaic power conversion efficiencies (22% as of July 2017), 1 ease and low cost of production, and broad material tuneability. 2 Besides applications in photovoltaics, MHPs may find use as solar thermoelectric materials, 3 LEDs, lasers, 4 and nonvolatile memory. 5 The macroscopic properties of MHPs emerge from diverse microscopic phenomena, including crystal structure, 6 defects, cation disorder, 7 ion migration, 8 and spin−orbit coupling. 9 Linking these phenomena to macroscopic performance is challenging because of the complex interplay between them. In this Perspective, we will address cation dynamics, their interactions with lattice vibrations (phonons), and their hypothesized effects on device performance.MHPs share a common ABX 3 (perovskite) structure as shown in Figure 1. This consists of (A) an organic molecule (e.g., methylammonium (MA) or formamidinium (FA)) or a large inorganic atom (e.g., caesium), (B) a metal dication (e.g., Pb (II) or Sn (II) ) and, (X) halide anions (Cl, Br, I, or some combination thereof). The M and X species form a cornersharing octahedral framework. The charge-balancing A-site cation occupies the central cavity generated by this framework and has a strong effect on the MHP structure, quantified by the Goldschmidt tolerance factor. 10 A-site ions just above or below the optimum size may induce tilting of the octahedra within the BX 3 sublattice away from a cubic perovskite. Mixing of ions will lead to inhomogeneity in the local structure, which may result in coupling of cation motion and equilibrium distribution to more complex local lattice dynamics.