Hello,
To pick up on the issue #450, I would like to suggest a new formulation of the multi-power law.
The current multi-power law might be difficult to calibrate and first attempts (last year) to calibrate the power failed (no convergence).
Here is the current law:
$\theta(x)=\rho_0 + \rho_1 \mathcal{D}^{\rho_2}(x) $
If I understand well, the descriptor are values normalized between [0:1] before calibration. The power $\rho_2$ of the multi-power-law is calibrated such that $\rho_2 \in R$. Then the sigmoïde is applied.
Here is a plot of the multi-power law for different value of $\rho_2$, with $\rho_0=0$ and $\rho_1=1$.
We can see that these functions increases or decreases depending the value of $rho_2$ : if $rho_2<0$, $\theta(x)$ decrease, if $rho_2>0$, $\theta(x)$ increase. Moreover, these functions are not normalized between [0:1] anymore.
Thus, I suggest to use a different formulation:
$\theta(x)=\rho_0 + \rho_1 \mathcal{D}^{\beta}(x) $
with,
$\beta=10^{\rho_2}$
This lead to a more consistent variation of the descriptor in the interval [0:1]:

Hello,
To pick up on the issue #450, I would like to suggest a new formulation of the multi-power law.
The current multi-power law might be difficult to calibrate and first attempts (last year) to calibrate the power failed (no convergence).
Here is the current law:
If I understand well, the descriptor are values normalized between [0:1] before calibration. The power$\rho_2$ of the multi-power-law is calibrated such that $\rho_2 \in R$ . Then the sigmoïde is applied.
Here is a plot of the multi-power law for different value of$\rho_2$ , with $\rho_0=0$ and $\rho_1=1$ .
We can see that these functions increases or decreases depending the value of$rho_2$ : if $rho_2<0$ , $\theta(x)$ decrease, if $rho_2>0$ , $\theta(x)$ increase. Moreover, these functions are not normalized between [0:1] anymore.
Thus, I suggest to use a different formulation:
with,
This lead to a more consistent variation of the descriptor in the interval [0:1]: