Neo-Hookean Hyperelastic Model

Category: Structural Analysis | Integrated 2026-04-06
CAE visualization for hyperelastic neo hookean theory - technical simulation diagram
Neo-Hookean Hyperelastic Model

Neo-Hookean Hyperelastic: Theoretical Foundations

Neo-Hookean Hyperelasticity

🧑‍🎓

Professor, what kind of model is Neo-Hookean?


🎓

The simplest hyperelastic model. Strain energy:


$$ W = C_{10}(I_1 - 3) + \frac{1}{D_1}(J-1)^2 $$

Defined by a single parameter $C_{10}$ ($= G/2$, where $G$ is the shear modulus). A special case of Mooney-Rivlin with $C_{01} = 0$.


🧑‍🎓

Just one parameter! It can be used when there's limited test data.


🎓

Neo-Hookean is reasonable up to moderate strains (around 50%). For large strains (over 100%), Mooney-Rivlin or Ogden models are needed.


Summary

🎓
  • $W = C_{10}(I_1-3)$ — One-parameter hyperelasticity
  • $C_{10} = G/2$ — Half of the shear modulus
  • Reasonable up to 50% strain — Beyond that, use Mooney-Rivlin/Ogden
  • First choice when test data is limited

  • Coffee Break Yomoyama Talk

    The Naming of Neo-Hookean

    The name Neo-Hookean (New Hookean) was given with the meaning of "modernizing (neo)" Hookean, i.e., Hooke's linear elastic law, for the nonlinear finite deformation regime. Ronald Rivlin established this term in his 1948 paper. The strain energy function W = C₁(I₁−3) is the simplest hyperelastic model with only one parameter, and because the stress-strain relationship can be solved analytically, it is still frequently used as a benchmark for verifying numerical algorithms.

    Computational Methods for Neo-Hookean Hyperelastic

    FEM Settings for Neo-Hookean

    🎓

    ```

    *HYPERELASTIC, NEO HOOKE

    C10, D1

    ```

    Nastran: MATHE, 1, MOONEY + $C_{01}=0$.


    Summary

    🎓
    • Abaqus *HYPERELASTIC, NEO HOOKE — The simplest setting
    • NLGEOM=YES + Hybrid elements — Standard for hyperelasticity

    • Coffee Break Yomoyama Talk

      Small Strain Limit and Shear Modulus Relationship

      The parameter C₁ of the Neo-Hookean model matches C₁ = μ/2 (μ: shear stiffness) in the small strain limit. That is, C₁ can be calculated from the elastic modulus E and Poisson's ratio ν without experiments (μ = E/2(1+ν)). This property justifies the practical approximation of directly using linear elastic material data to run Neo-Hookean analysis in the preliminary design stage of rubber components where detailed large deformation test data is unavailable.

      Neo-Hookean Hyperelastic in Practice

      Neo-Hookean in Practice

      🎓

      Used for conceptual design of rubber components, modeling of biological tissues (brain, muscle). First choice when test data is limited.


      Practical Checklist

      🎓
      • [ ] Does $C_{10}$ align with the material's shear modulus? ($C_{10} = G/2$)
      • [ ] Is the applied strain below 50%? (Consider Mooney-Rivlin/Ogden if above)
      • [ ] Are hybrid elements being used?

      • Coffee Break Yomoyama Talk

        Medical Implants and Neo-Hookean

        FEM analysis of silicone rubber breast implants and heart valve prostheses most frequently uses Neo-Hookean and Mooney-Rivlin models. The US FDA, in its guidance on structural analysis of medical devices (2019), recommends using hyperelastic models with confirmed Drucker stability for soft tissue/rubber-like material computational models. Neo-Hookean is designated as a First-choice model due to its proven property of always being stable if C₁>0.

        Neo-Hookean Hyperelastic: Software & Solver Comparison

        Tools

        🎓

        Supported by all solvers. The simplest hyperelastic model.


        Coffee Break Yomoyama Talk

        Comparison of Hyperelastic Model Implementations Across Vendors

        ABAQUS, ANSYS, and Nastran all support Neo-Hooke, Mooney-Rivlin, and Ogden models, but their material constant fitting UIs differ. ABAQUS can simultaneously fit Mooney-Rivlin C10/C01 to tensile, compressive, and shear test data, while ANSYS uses uniaxial fitting as standard. A case study published in the Journal of Constitutive Models of Rubber reported that differences in fitting methods led to up to a 2x variation in predicted durability life for tire sidewall analysis.

        Advanced Technology

        Advanced

        🎓
        • Biomechanics — Neo-Hookean modeling of brain tissue, arterial walls
        • Soft Robotics — Large deformation of flexible materials

        • Coffee Break Yomoyama Talk

          Origin of the Neo-Hooke Model: Statistical Mechanics of Rubber Elasticity

          The Neo-Hookean hyperelastic model was derived in 1943 by Flory and Rehn from the molecular chain network theory of vulcanized natural rubber. It is a practical model with errors within 10% even at an elongation ratio of λ=3 for natural rubber with shear modulus G≈0.4 MPa. Today, it is widely used in ABAQUS and ANSYS for applications ranging from medical silicone catheters (G≈0.1 MPa) to tire compounds (G≈1.2 MPa).

          Neo-Hookean Hyperelastic: Common Issues & Debugging

          Troubles

          🎓
          • Inaccurate at large strains → Switch to Mooney-Rivlin or Ogden
          • Volumetric locking → Hybrid elements are mandatory
          • $D_1$ is zero → Perfectly incompressible. Hybrid elements are mandatory

          • Coffee Break Yomoyama Talk

            Accuracy Degradation at Excessive Strains

            It is well known from many experiments that Neo-Hookean underestimates stress when the stretch ratio λ≧2.5. For uniaxial tension of natural rubber, the stress difference between Mooney-Rivlin and Neo-Hookean at λ=3 can reach 20-40%. This discrepancy is due to the absence of the C₂ term (I₂ dependence). For parts where large deformation is expected (tire bead, O-ring compression), switching to a multi-parameter model like Mooney-Rivlin or higher should always be considered.

            Related Simulators

            Experience the theory firsthand with the interactive simulator for this field

            All Simulators

            Related fields

            Thermal AnalysisManufacturing Process AnalysisV&V · Quality Assurance
            Rate this article
            Thank you for your feedback!
            Helpful
            More details
            Report error
            Helpful
            0
            More details
            0
            Report error
            0
            Written by NovaSolver Contributors
            Anonymous Engineers & AI — Sitemap
            About the Authors