“…C 10 , C 01 ¼ Mooney-Rivlin material constants d, d min , d max ¼ Time-varying displacement and minimum and maximum values I 1 , I 2 ¼ Strain invariants of the right Green deformation tensor k, n ¼ Material constants of the equivalent strain amplitude parameter N f , N f,max , N f,min ¼ Average fatigue life and maximum and minimum life for a given loading case R ¼ Strain ratio, ε min /ε max R d ¼ Displacement ratio, d min /d max r 2 ¼ Correlation coefficient V ¼ Spatial stretch tensor W ¼ Strain energy density β ¼ Material constant for the equivalent parameter {ε ij } ¼ Logarithmic strain tensor ε, ε min , ε max ¼ Logarithmic normal strain and minimum and maximum strain ε m , ε a ¼ Mean strain and strain amplitude ε À1 ð Þ m ; ε À1 ð Þ a ¼ Mean strain and strain amplitude corresponding to R = À1 ε eq ¼ Equivalent strain parameter, which has the same value as ε Rubbers offer the advantage of withstanding very large strains without permanent deformation or fracture, which makes them ideal for many applications such as tires, vibration isolators, accessory drive belts and so on. 1 Some of the behaviours of the rubbers are comparable with those of commonly used linear elastic materials such as conventional metals. For example, rubbers exhibit limited fatigue strength when subject to tearing energy below a critical value.…”