The wall friction term in a one-dimensional model vanishes under the stagnant liquid conditions (i.e. the liquid volume flux JL = 0). Hence void fraction αG(ΔP) in rod bundles have been evaluated using measured pressure gradients dP/dz. However, effects of the wall friction term on αG(ΔP) have not been quantitatively evaluated. In this study, we therefore carried out air-water experiments using a 3×3 rod bundle under the conditions of JL = 0, and measured dP/dz and αG,exp with the closing valve method. We obtained the dimensionless wall friction force Fw * (= αG(ΔP)−αG,exp) from the measured dP/dz and αG,exp. The Fw * values were expressed by using the gas volume flux JG, because the liquid flow field was induced by the gas flow (i.e. JG). The difference between αG,exp and αG(ΔP) was reduced by half after αG(ΔP) was corrected using the obtained correlation for Fw * . The Fw * correlation was applied to existing αG(ΔP) data for 4×4 and 8×8 bundles, and effects of Fw * on the αG(ΔP) values were confirmed to be small in a large rod bundle due to the small wall area per unit fluid volume.