The behavior of the electrical conductivity in hydrogenated microcrystalline silicon ͑c-Si: H͒ that is frequently observed is explained by considering the statistical shift in the chemical potential as a function of the crystalline fraction ͑X c ͒, the dangling bond density ͑N db ͒, and the doping density ͑N d ͒. Our model shows that temperature dependent dc conductivity measurements above room temperature can be very well explained by ͑unintentional͒ micro doping of c-Si: H. It is shown that the statistical shift in the chemical potential ͑͒ is influenced mostly by the ratio between N d and N db . It is concluded that the anomalous dependence of the apparent activation energy ͑E a ͒ and the apparent exponential prefactor ͑ 0 ͒ on X c can be explained by behavior of , that can be induced by a change in this ratio between N d and N db . We used an effective medium approximation for the electron density of states ͑DOS͒ of c-Si: H. The DOS is calculated as a weighted sum of the DOS of c-Si and the DOS of a-Si:H, parameterized by X c , N db , and N d . The conductivity is deduced assuming a single dominant conduction path above the conduction edge of a-Si:H.