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q^{\uparrow}(t) = f \, q^{\downarrow}(t) - \tau \cdot \frac{ d q^{\uparrow}}{ dt } - J \cdot \tau \cdot \frac{d p_{wf }}{dt} |
The target function is:
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q^{\uparrow}_j (t) = \sum_i^{n_i} f_{ij} q^{\downarrow}_i(t) - \tau_j \cdot \frac{ d q^{\uparrow}_j}{ dt } - J_j \cdot \tau_j \cdot \frac{d p_{wf, \, j }}{dt}j}{dt} |
The target function is:
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\sum_k \sum_j \big[ q^{\uparrow}_j(t_k) - \tilde q^{\uparrow}_j(t_k) \big]^2 \rightarrow \min |
ICRM – Multi-Tank Integrated Capacitance Resistance Model
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Q^{\uparrow}_j (t) = \sum_i^{n_i} f_{ij} Q^{\downarrow}_i(t) - \tau_j \cdot \big[ q^{\uparrow}_j(t) - q^{\uparrow}_j(0) \big] - J_j \cdot \tau_j \cdot \big[ p_j - p_{wf, \, j }(t) - p_{wf, \, j }(00) \big] |
The target function is:
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\sum_k \sum_j \big[ Q^{\uparrow}_j(t_k) - \tilde Q^{\uparrow}_j(t_k) \big]^2 \rightarrow \min |
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