3D printed shape
Otimization Pb
IMPOSSIBLE
$$
-\nabla\cdot A e(u)=f
$$
$$
-\nabla\cdot A^* e(u)=\theta f
$$
Coarse mesh !!!
Doable :)
Homogenization
Orientation of
the cells
$$\alpha$$
Parameters of
the micro-structures
$$m$$
Sequence $\Omega_\varepsilon$
$\varepsilon=$16.00
A 1+2 steps program
Step 0 - Preprocessing
Compute $A^*(\alpha,m)$
Step 1 - Homogenization
Compute optimal $(\alpha,m)$
Step 2 - Dehomogenization
$$
\Omega_\varepsilon \rightarrow (\alpha,m)
$$
$\omega=(0,1)^2$-periodic
$\Omega_\varepsilon=\varepsilon \omega$
$\omega \cap (0,1)^2$
$A^*\xi:\xi=$
$$
\inf_{w\in H^1_\#((0,1)^2)} \int_{\omega\cap(0,1)^2} A(\xi+e(w)):(\xi+e(w))
$$
Correctors
$$
w_{ij}:=\textrm{argmin} \int_{\Omega} A(e_{ij}+e(w)):(e_{ij}+e(w))
$$
$e_{ij}=e_i\otimes e_j$
Compression along $e_1$
$w_{11}$
Compression along $e_2$
$w_{22}$
Shearing
$w_{12}$
Hooke's law
$$
A^*_{ijkl}:=\int_{\Omega} A(e_{ij}+e(w_{ij})):(e_{kl}+e(w_{kl}))
$$
$\small A^*(m_1,m_2)$
$\small A^*(m_1,m_2,\alpha)$
$\small = S(\alpha)^TA^*(m_1,m_2)S(\alpha)$
Compliance
$$
\min_{\alpha,m} \left\{J^*(\theta,A^*):=\int_\Omega A^*e(u^*):e(u^*)\,dx\right\}
$$
$$
\int_D \theta\,dx \leq V
$$
Stress Formulation
$$
\inf_{m,\sigma} J^*(m,\alpha) = \inf_{\alpha,m,\sigma} \int_D (A^*)^{-1}(m,\alpha) \sigma\cdot \sigma \,dx.
$$
$$
\left\{
\begin{array}{ll}
\nabla\cdot\sigma=0&\text{in } D\\
\sigma n = g&\text{on }\Gamma_N
\end{array}
\right.
$$
Alternate minimization
- Stress $\sigma$
Solve elasticity problem for current $A^*$.
- Orientation of the cell $\alpha$
Pedersen.
- Size of the micro-holes $m$
One step of gradient method.
Step 2 : Dehomogenization
Periodic Composite on structured Lattice
$$\Omega_\varepsilon=\Big\{x\in D : x\in \varepsilon\omega\Big\}$$
Locally Periodic Composite on structured Lattice
$$\Omega_\varepsilon=\Big\{x\in D : x\in \varepsilon\omega(\color{red} x)\Big\}$$
Locally Periodic on
unstructured
Square Lattice
$$\Omega_\varepsilon=\Big\{x\in D : \color{orange} \varphi(x)\in \varepsilon\omega(\color{red}x)\Big\}$$
$\color{orange} \varphi$ = Conform mapping from $D$ into $\mathbb R^2$
Grid Map $\varphi$
$D \varphi^{-1}(Y)$-periodic shape
$$
\xrightarrow[\quad\quad]{\varphi}
$$
$Y$-periodic shape $\omega$
Definition of the shape sequence $\Omega_\varepsilon$
$$
\Omega_\varepsilon(\varphi,m)=\left\{x\in D~:~\cssId{phi}{\varphi}(x) \in \cssId{vepsilon}{\varepsilon} \omega(\cssId{m}{m}(x)) \right\}.
$$
$\varphi$ Grid Map
${m}$ parameters of the micro-structure
${\varepsilon}$ length scale
Computation of the grid Map $\varphi$
$D\varphi^{-1}=$periodicity cell$=$$e^r a$
$a=$ Rotation field of the cells of angle $\alpha$
$r=$ Dilatation of the cells
$$
\nabla^T r = \nabla\alpha.
$$
Step 1. Compute $r$
$$
\min_r \left\|\nabla^T r-\nabla\alpha\right\|
$$
Step 2.
Compute $\varphi$
$$
\min_{\varphi} \left\|D\varphi - e^{-r}a^T\right\|
$$
Conformity Condition
$$
\nabla^T r = \nabla\alpha
$$
$$
\Delta \alpha=0
$$
Optimization Steps
- Homogenization
-
Add conformity constaint $\Delta\alpha=0$
- Compute dilatation and grid map
Main features
Post-treatment of the homogenization
Find $\Omega_\varepsilon$ converging toward the optimal composite
$\varepsilon$=Length scale of the fine details
One UNIQUE computation for ALL $\varepsilon$
Thank you for your attention