Ninety-two sets of observed dislocation densities for crept specimens of 21 types of ferritic/martensitic and austenitic steels, Al, W, Mo, and Mg alloys, Cu, and Ti including germanium single crystals were collected to verify an equation for evaluating the dislocation density during steady-state creep proposed by Tamura and Abe (2015). The activation energy, , activation volume, , and Larson-Miller constant, , were calculated from the creep data. Using these parameter constants, the strain rate, and the temperature dependence of the shear modulus, a correction term, , was back-calculated from the observed dislocation density for each material. is defined in the present paper as a function of the temperature dependences of both the shear modulus and pre-exponential factor of the strain rate. The values of range from −394 to 233 kJmol and average 2.1 kJmol , which is a value considerably lower than the average value of (410.4 kJmol ), and values of are mainly within the range from 0 to 50 kJmol . The change in Gibbs free energy, ∆ , for creep deformation is obtained using the calculated value of , and the empirical relation ∆ ≅ ∆ is found, where ∆ is the change in Gibbs free energy for self-diffusion of the main componential element of each material. Experimental data confirm the validity of the evaluation equation for the dislocation density.