  \displaystyle \frac{1}{\omega_{base}} L \displaystyle \frac{di_{q}}{dt} + \omega L i_{d} + Ri_{q}
            \end{array} 
            \right.
        \end{equation}
        
        Considering static behavior of the inductive element in a reduced model:
        
        \begin{equation}
            \left\{
            \begin{array}{l}
                v_{d} =  - \omega L i_{q} + Ri_{d} \\ 
                v_{q} =   \omega L i_{d} + Ri_{q} 
            \end{array} 
            \right.
            \rightar