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!โˆ’3C (2) The nominal (engineering) puling stress ๐‘†=๐น/๐ด!, with ๐น puling force and ๐ด! initial cross-section area, is ๐‘†=๐œ•๐œ“/๐œ•๐œ†, giving ๐‘†=%&'(A๐œ†(*$โˆ’๐œ†*

for this study, where the strain energy density (SED) is ๐œ“=%&'(!4๐œ†ฬ…$(+๐œ†ฬ…%(+๐œ†ฬ…'(โˆ’39 (1) Here, ๐ธ is the (zero-strain) Youngโ€™s modulus, ๐›ผ is the strain-stiffening coefficient (Ogden · 1972

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Hyperelastic characterization via deep indentation

cond-mat.soft ยท 2025-05-28 ยท conditional ยท novelty 5.0

Deep indentation force-depth curves have a Hertzian and a parabolic regime, and the parabolic coefficient beta maps empirically to the Ogden strain-stiffening coefficient alpha, allowing in-situ hyperelastic characterization.

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  • Hyperelastic characterization via deep indentation cond-mat.soft ยท 2025-05-28 ยท conditional ยท none ยท ref 1972

    Deep indentation force-depth curves have a Hertzian and a parabolic regime, and the parabolic coefficient beta maps empirically to the Ogden strain-stiffening coefficient alpha, allowing in-situ hyperelastic characterization.