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| Expand |
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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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| LaTeX Math Block |
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| anchor | Case2_PSS_p21 |
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| alignment | left |
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| p_{u,\rm 21}(t \rigtharrow \infty) \rightarrow \frac{t}{c_{t,2} V_{\phi,2}} |
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where
Substituting | LaTeX Math Block Reference |
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and | LaTeX Math Block Reference |
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in | LaTeX Math Block Reference |
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one arrives to | LaTeX Math Block Reference |
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If pressure in producer W1 is supported by several injectors then:
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\delta q_1 =\sum_k f_{k1} \delta q_k
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which makes one of the key assumptions in Capacitance Resistance Model (CRM).
See also
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Capacitance Resistance Model (CRM)
