The electronic resistivity and Seebeck coefficient were measured on a dense pellet (~88%) of CuBiSeCl2, parallel to the pressing direction, between 2 and 300 K (Figure ) to understand the electronic transport within the material. The pellet was highly textured, as described above, with preferential orientation in both the a and c directions (S24). Below 250 K, the resistance of CuBiSeCl2 became too high for any meaningful resistivity or Seebeck coefficient data to be collected, hence these properties are only shown to approximately 250 K. The electronic resistivity of CuBiSeCl2 exhibits behaviour typical of a semiconductor, and a large resistivity of ~6376(3) Ωm is measured at 300 K, consistent with the prediction of heavy charge carriers. Using the Arrhenius equation and by plotting log(σ), where σ is the electronic conductivity, as a function of 1000/T, the activation energy (Ea) could be extracted and was found to be 0.4623(3) eV.