The warping function $\omega(x, \ y)$ is needed to compute torsion. Although we can let the user define the place of the source points, a method to decide the best points is desirable.
Description
The approximative solution $\overline{\omega}$ should be as near as possible of the exact (and unknown) solution $\omega$.
At first sight, there are three ways to mesure how good a solution $\overline{\omega}$ is
- Torsion constant $J$
$$J = I_{xx} + I_{yy} - \int_{t_{min}}^{t_{max}} \omega \cdot \langle \mathbf{p}, \ \mathbf{p}'\rangle \ dt$$
- Residual square on the domain
$$I_{\omega \omega} = \int_{\Omega} \omega^2 \ dx \ dy$$
- Residual square on the boundary
$$I = \int_{t_{min}}^{t_{max}} \omega^2 \ \langle \mathbf{p}, \ \mathbf{p}'\rangle dt$$
The warping function$\omega(x, \ y)$ is needed to compute torsion. Although we can let the user define the place of the source points, a method to decide the best points is desirable.
Description
The approximative solution$\overline{\omega}$ should be as near as possible of the exact (and unknown) solution $\omega$ .
At first sight, there are three ways to mesure how good a solution$\overline{\omega}$ is