EQUATION REGISTRY

Volume Jacobian and scale

Use detF for finite deformation; sigma is the small-strain density term. The second part is an isotropic frame with linear matching sigma=-3varphi; do not conflate general anisotropy, density energy kernels and independent stretch actions.

Theory · DERIVEDEquation version 1.0.0

Based on the final manuscript · Chapters 4 and 5

ASD-WEB-SD-034
nsns,0=1det⁡F,Fij=δij+∂jui,F=eφI ⟹ nsns,0=e−3φ,ns−ns,0ns,0=e−3φ−1=−3φ+O(φ2).\begin{aligned}\frac{n_s}{n_{s,0}}&=\frac{1}{\det F},\quad F_{ij}=\delta_{ij}+\partial_j u_i,\\F=e^\varphi I&\ \Longrightarrow\ \frac{n_s}{n_{s,0}}=e^{-3\varphi},\\\frac{n_s-n_{s,0}}{n_{s,0}}&=e^{-3\varphi}-1=-3\varphi+O(\varphi^2).\end{aligned}

Use detF for finite deformation; sigma is the small-strain density term. The second part is an isotropic frame with linear matching sigma=-3varphi; do not conflate general anisotropy, density energy kernels and independent stretch actions.
Chapter reference: Ch. 4 (4.14)–(4.15); Ch. 5 (5.4.5) and isotropic-frame discussion · ASD-BOOK-ddbade997b45

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ASD-WEB-SD-034 is the stable website equation ID. It retains existing links and does not replace the manuscript reference. Use the copy button to obtain LaTeX.

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Adopted source, conditions and previous versions

Ch. 4 (4.14)–(4.15); Ch. 5 (5.4.5) and isotropic-frame discussion

Registered formula checked individually against the final manuscript; semantic potential phi→varphi; finite-density Jacobian vs linear small-strain density made explicit; source-grounded scope note synchronized

Conditions retained in this adoption

  • Use detF for finite deformation; sigma is the small-strain density term. The second part is an isotropic frame with linear matching sigma=-3varphi; do not conflate general anisotropy, density energy kernels and independent stretch actions.

Source locators: p1342–1348 · p2028 · p2041

Manuscript SHA-256: ddbade997b45913248e588953b1d27ccb9c7c206c3c8d992d3aef2364a64836e

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Previous source, retained as history

SD-51779505a476 · Ch. 4 (4.15); Ch. 5 (5.4.5), §4.2

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