Abundances of selected isotopes after explosive nucleosynthesis for three selected progenitors from LC18 (left) and WH07 (middle and right). The solid lines show the results from the explosion simulated in this work with GR1D, the dashed lines show the bomb model of LC18, and the dotted lines show the piston model of WH07. The progenitor on the left was chosen to be the one for which the mass cut derived with GR1D is closest to that in the original work. The progenitor in the middle was chosen instead to be the one for which the explosion energy derived with GR1D differs most from that in the original work of 1.4 B. The progenitor on the right was chosen to be the one for which the explosion energy derived with GR1D is closest to that in the original work of 1.4 B. As one can see, the left and middle panels are quite similar, showing that the main difference in explosion dynamics is due to the explosion energy, regardless of whether a piston or a bomb is used. When the explosion energies are similar (i.e., the right panel), the differences are smaller.