We study the phenomenon of pole-skipping in holographic CFTs dual to diffeomorphism invariant theories containing an arbitrary number of bosonic fields in the large N limit. Defining a weight to organize the bulk equations of motion and field components, a set of general pole-skipping conditions are derived. In particular, the frequencies simply follow from general covariance and weight matching. Relating the highest-weight pole-skipping frequency to an exponential growth rate, i.e., the Lyapunov exponent, we show that the chaos bound is generally violated in the presence of finitely many higher spin fields, consistent with existing evidence. In the absence of such pathological fields, we show that the energy density Green's function has its highest-weight pole-skipping happening at a location related to the OTOC for arbitrary higher-derivative gravity, with a Lyapunov exponent saturating the chaos bound and a butterfly velocity matching that extracted from a shockwave calculation. We also suggest a physical explanation for this matching by obtaining the shockwave metric from a regularized limit of the metric perturbation at the skipped pole.