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- fast-track
- based on the most robust input data
- does not involve full-field 3D dynamic modelling and associtated assumptions
CRM – Single-Tank
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Capacitance Resistance Model
The simulation is based on the following equation:
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q_m\bar q^{\uparrow}(t) = f \, Iq^{\downarrow}(t) - \tau \, \cdot \, \frac{ d q_m(t) }\bar q^{\uparrow}}{ dt } - J \, \tau \, \frac{d p_{wf }(t)}{dt} |
The target function is:
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\sum_k \big( qq^*_p(t_k) - q_mp(t_k) \big)^2 \rightarrow \min |
CRMP – Multi-tank Producer-based
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Capacitance Resistance Model
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q_jq^*_{p, \, j} (t) = \sum_i^{n_i} f_{ij} I_iq_{in, \,i}(t) - \tau_j \, \frac{ d q_jq^*_{p, \, j}(t) }{ dt } - J_j \, \tau_j \, \frac{d p_{wf, \, j }(t)}{dt} \, |
ICRM – Multi-Tank
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Integrated Capacitance Resistance Model
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qQ_j (t) = \sum_i^{n_i} f_{ij} I_i(t) - \tau_j \, \frac{ d q_j(t) }{ dt } - J_j \, \tau_j \, \frac{d p_{wf, j }(t)}{dt} |
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