In materials engineering, one of the key challenges is to model materials that exhibit both hyperelastic and creep characteristics, that is, materials that exhibit both large elastic deformations and time-dependent deformations under long-term loading. Examples of such materials are:
These materials are characterized by high elasticity, meaning that they can undergo large deformations and return to their original shape when the load is removed. However, under prolonged loading, rubber can also exhibit creep (e.g., in car tires, gaskets, or vibrating components).
Soft tissues, such as skin, muscles, and tendons, exhibit both hyperelastic behavior and creep. Modeling this phenomenon is important in biomechanics, such as in the design of prostheses or the analysis of the behavior of human organs under load, such as during surgical procedures.
Many plastics and polymeric materials, such as polyethylene and polypropylene, exhibit hyperelasticity under short-term loading and creep under long-term loading. These properties are important in many industries: automotive (vehicle components), consumer products, and packaging.
For Abaqus software, which is used to simulate the mechanics of solids, the question is often how to combine these two behaviors in a single material definition.
At the level of direct material definition using keywords, the answer is no. The keyword *HYPERELASTIC cannot be directly combined with *CREEP, because creep (*CREEP) requires the use of the classical definition of elasticity (*ELASTIC), not hyperelasticity. Nevertheless, there are alternative approaches that allow both behaviors to be modeled simultaneously.
Additional elements can also be included in the PRF model to further represent the actual behavior of the material:
The parallel rheological approach is based on a parallel combination of several nonlinear viscoelastic models, with the possibility of adding a nonlinear elasto-plastic model. Nonlinear elasticity in this model is described using hyperelasticity, while viscous behavior is modeled using creep potential. Importantly, to correctly represent large elastic deformations, it is assumed that the strain gradient is divided into elastic and creep-related components.
There are other options in Abaqus for combining hyperelasticity with time-dependent plastic behavior:
Although hyperelasticity and creep cannot be directly linked in Abaqus using basic keywords, PRF (parallel rheological framework) and other advanced features allow such phenomena to be modeled. With the combination of nonlinear elasticity and creep models, it is possible to accurately represent the complex behavior of materials in response to different loads.
If you would like to learn more about material modeling in Abaqus, we invite you to take a look at our training courses.