If a new heavy particle φ is produced in association with the top quark in a hadron collider, the production cross section exhibits a collinear singularity of the form log(m φ /m t ), which can be resummed by introducing a top quark parton distribution function (PDF). We reassess the necessity of such resummation in the context of a high energy pp collider. We find that the introduction of a top PDF typically has a small effect at √ S ∼ 100 TeV due to three factors: 1) α s at the scale µ = m φ is quite small when log(m φ /m t ) is large, 2) the Bjorken x 1 for m φ 10 TeV, and 3) the kinematic region where log(m φ /m t ) 1 is suppressed by phase space. We consider the example of pp → tH + at next-to-leading logarithm (NLL) order and show that, in terms of the total cross section, the effect of a top PDF is generically smaller than that of a bottom PDF in the associated production of bφ. However, in the p T distribution of the charged Higgs, the NLL calculation using a top PDF is crucial to generate the p T distribution for p T m t .