Hello,
I want to solve a system of PDEs in a two-dimensional domain \Omega. The unknowns are the three components of a vector field X^\alpha(x), where \alpha = 1,2,3 and x = {x^1,x^2} are the coordinates on \Omega.
The system of PDEs is given by
- One fourth-order PDE
- Two constraints for \partial X, which enforce that the mapping x → X is conformal:
- {\bf e}_1 \cdot {\bf e}_1 = {\bf e}_2 \cdot {\bf e}_2
- {\bf e}_1 \cdot {\bf e}_2 = 0
where {\bf e}_i \equiv \partial_i X
I can derive the variational formulation of the first PDE. What is te correct way to formulate in a variational way the two additional constraints ?
Thank you