Polar plots of m_proj,10° similar to Figure 4 with the NRN enabled for different TDE b values. It is clear that the ejected material is asymmetrically distributed in all cases. As b decreases, the ejecta spread out more due to greater energy injection from nuclear fusion. This change is most drastic between b = 0.20 (standard TDE with negligible nuclear burning) and b = 0.19 (some nuclear burning).