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| P_{\Psi} \left[ p_{e,n} \ (t) \right] = P_{\Psi} \left[ p_{i,n} \ (0) \right] + \gamma_n^{-1} \cdot \left[
B_{og} \cdot Q^{\uparrow}_{O,nn} + f^{\uparrow}_{W,nn} \cdot B_w \cdot Q^{\uparrow}_{W,n} + \sum_{m \neq n} Q^{\uparrow}_{nm} + \sum_k Q^{\downarrow}_{nk} \right] |
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| p_{{\rm wf}, n} \ \ \ (t) = p_e \ (t) + 0.5 \cdot J_{On}^{-1} \cdot \left[ q^{\uparrow}_{On}(t) + f^{\uparrow}_{W,nn} \cdot \frac{\mu_W}{\mu_O} \cdot \frac{k_{ro}(s_{w,n})}{k_{rw}(s_{w,n})} \cdot q^{\uparrow}_{Wn}(t) \right] |
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| s_{w,n} = \left[ 1 + \frac{B_o}{B_w} \cdot \frac{q^{\uparrow}_{On}}{f^{\uparrow}_{W,nn} \cdot q^{\uparrow}_{Wn}} \right]^{-1} |
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| Q(t) = \int_0^t q(t) \, dt |
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| Q^{\uparrow}_{nm} \ =
\ - \ f^{\uparrow}_{O,nm} \ \cdot B_{ob} \cdot \, Q^{\uparrow}_{O,m}
\ - \ f^{\uparrow}_{G,nm} \ \cdot B_{go} \cdot Q^{\uparrow}_{G,m}
\ - \ f^{\uparrow}_{W,nm} \ \cdot B_w \cdot Q^{\uparrow}_{W,m}
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| Q^{\downarrow}_{nk} \ =
f^{\downarrow}_{G,nk} \ \cdot B_{go} \cdot Q^{\downarrow}_{G,k}
\ + \ f^{\downarrow}_{W,nk} \ \cdot B_w \cdot Q^{\downarrow}_{W,k}
\ + \ B_{go} \cdot Q^{\downarrow}_{GCAP,k} \
\ + \ B_w \cdot Q^{\downarrow}_{WAQ,k}
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| B_{og} = \frac{B_o - R_s \, B_g}{1- R_s \, R_v} |
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| B_{go} = \frac{ B_g - R_v \, B_o}{1- R_s \, R_v} |
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where
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body | B_o, \, B_g, \, B_w, \, R_s, \, R_v |
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are
Dynamic fluid properties and LaTeX Math Inline |
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body | --uriencoded--P_%7B\Psi%7D [] |
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is Normalized Pseudo-Pressure .
The value of cumulative Gas Cap influx
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body | --uriencoded--Q%5e%7B\downarrow%7D_%7BGCAP%7D |
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is modelled as in
Gas Cap Drive @model.
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