“…If a mass with mass moment of inertia / and a torsional spring of constant k are attached to one end of the cylinder as shown in figure 1, and the other end of the cylinder is subjected to a harmonically varying torque, then the expression for the angular acceleration response ratio of the top plane of the cylinder to the bottom plane is given by [4,5] ^ Mrgp^/^ [C,a*sin(ft*)+cos(ft*)]-' (1) (7) Thus, if R and 4> are the measured ampHtude ratio and phase angle, respectively, and all the physical and geometric parameters of the specimen are determined by other means, then G' and G" can be found using eqs (6) and (7). However, because of the complexity of these equations, G' and G" cannot be solved for explicity.…”