“…It is known that convolution integrals do not in general have a closed analytical form, however, they can be obtained as such for the simple loading (stimulation) patterns, for example, creep, linear ramp, or harmonic case [ 25 ]. For the latter, authors [ 10 , 25 , 26 ] have previously shown that the dynamic stress/strain ratio (“dynamic stiffness”) can be expressed as: where σ dyn is the applied dynamic stress amplitude, ω —Circular frequency, C ω0 = E 0 × (τ 0 ×ω) α is the viscostiffness (quasi-property in units of kPa·s α ) [ 25 ], α —Dynamic material memory parameter, E 0 —Intrinsic dynamic elasticity, τ 0 —Intrinsic characteristic time. This Equation (2) time-convolutes the specimen loading history at every frequency without Fourier transform or assumptions of a material model (Maxwell, Burger, standard linear solid, Prony series, etc.…”