Previous research has found that the pairing symmetry in the iron-based superconductor B a1 -xKxF e2A s2 changes from nodeless s wave near optimally doped, x ≈0.4 -0.55 and Tc>30 K , to nodal (either d wave or s wave) at the pure end point, x =1 and Tc<4 K . Intense theoretical interest has been focused on this possibility of changing pairing symmetry, where in the transition region both order parameters would be present and time-reversal symmetry would be broken. Here we report specific heat measurements in zero and applied magnetic fields down to 0.4 K of three individual single crystals, free of low-temperature magnetic anomalies, of heavily overdoped B a1 -xKxF e2A s2 ,x =0 .91 , 0.88, and 0.81. The values for Tc mid are 5.6, 7.2, and 13 K and for Hc 2≈4.5 , 6, and 20 T, respectively. The data can be analyzed in a two-gap scenario, Δ2/Δ1≈4 , with the magnetic field dependence of γ (=C /T as T →0 ) showing an anisotropic "S -shaped" behavior vs H , with the suppression of the lower gap by 1 T and γ ≈H1 /2 overall. Although such a nonlinear γ vs H is consistent with deep minima or nodes in the gap structure, it is not clear evidence for one, or both, of the gaps being nodal in these overdoped samples. Thus, following the established theoretical analysis of the specific heat of d -wave cuprate superconductors containing line nodes, we present the specific heat normalized by H1 /2 plotted vs T /H1 /2 of these heavily overdoped B a1 -xKxF e2A s2 samples which—thanks to the absence of magnetic impurities in our sample—convincingly shows the expected scaling for line node behavior for the larger gap for all three compositions. There is, however, no clear observation of the nodal behavior C ∝α T2 in zero field at low temperatures, with α ≤2 mJ /mol K3 being consistent with the data. This, together with the scaling, leaves open the possibility of extreme anisotropy in a nodeless larger gap, Δ2, such that the scaling works for fields above 0.25-0.5 T (0.2-0.4 K in temperature units), where this is an estimate for the size of the deep minima in the Δ2∼20 -25 K gap. Therefore, the location of the change from nodeless to nodal gaps between optimally doped and heavily overdoped B a1 -xKxF e2A s2 based on the present work may be closer to the KF e2A s2 end point than x = 0.91 .