We have computed finite temperature corrections to the electron-hadron scattering cross sections .
These are based upon the renormalized electron mass and the modified density of states due to the presence of a background thermal bath .
It is found that the electron-hadron thermal transport scattering cross section can be much larger than the zero temperature one .
In the case of electron-neutron transport scattering , we find \sigma _ { ne } ( T ) / \sigma _ { ne } ( T = 0 ) \simeq 5 at T \simeq 0.1 MeV .