We observe two Meyer-Neldel rules for the dc conductivity in porous si
licon. One rule corresponds to extended-states transport and the other
to transport by thermally activated hopping. The quantitative resembl
ance of the first rule to the one found in hydrogenated amorphous sili
con (a-Si:H) indicates that in samples in which it is observed the con
duction takes place in an a-Si:H-like tissue that wraps the luminescen
t crystallites. In samples where the second rule is observed the condu
ction appears to be either by activated hopping in this disordered tis
sue, or by intercrystallite hopping.