The model described in Eq. (9) (black curves) is compared to the measured Dante drive (red curves) for four shots, which use various Hohlraum sizes, ablators, laser powers, and LEH fractions (defined as the radius of the laser-entrance-hole divided by the Hohlraum radius). The foot of the pulse is not well reproduced by the model, but the main rise and peak are captured quite well—in some cases, we do not have a Dante unfold in the foot.