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borderColor | wheat |
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bgColor | mintcream |
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borderWidth | 7 |
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| For the finite-volume reservoir LaTeX Math Inline |
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body | V_{\phi,1} \leq V_{\phi,2} < \infty |
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| the DTR and CTR are both going through the PSS flow regime at late transient times:
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anchor | Case2_PSS_p11 |
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alignment | left |
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| p_{u,\rm 11}(t \rightarrow \infty) \rightarrow \frac{t}{c_{t,1} V_{\phi, 1}} |
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anchor | Case2_PSS_p21 |
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alignment | left |
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| p_{u,\rm 21}(t \rightarrow \infty) \rightarrow \frac{t}{c_{t,2} V_{\phi,2}} |
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where Substituting LaTeX Math Block Reference |
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displaytextanchor | Case2_PSS_p11 |
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| and LaTeX Math Block Reference |
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displaytextanchor | Case2_PSS_p21 |
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| in LaTeX Math Block Reference |
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| one arrives to LaTeX Math Block Reference |
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displaytextanchor | Case2_PSS |
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| . |
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If pressure in producer W1 is supported by several injectors theninjectors
then over a long period of time one can assume:
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\delta q_1 =\sum_k f_{k1} \delta q_k
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with constant coefficients LaTeX Math Inline |
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body | f_{1k}, \ {k=\{1..N_{\rm inj} \} } |
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, which makes one of the key assumptions in Capacitance Resistance Model (CRM).
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