Untitled - Technische Universiteit Eindhoven

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9.4. Outlook 13712Fig. 9.6: T 1 -weighted NMR images of a glass bead pack saturated with water (lower phase)and oil/TMOS (upper phase). The images were acquired at the beginning of theexperiment (left frame), and after 17 hours (right frame), respectively. Region ofinterests (ROIs) are indicated in the left panel by the white rectangles.100008000oil phasewater phaseROI 1ROI 2average signal [a.u.]60004000200000 2 4 6 8 10 12 14 16 18t R[h]Fig. 9.7: Average NMR signal intensity of the ROIs in the glass bead pack (see Figure 9.6 fordetails) as a function of time.
138 9. Concluding remarks and outlookis to adopt a non-equilibrium thermodynamical model (Cahn-Hilliard models [150] ordiffusive interface models [151]) and to include the description of multi-components andchemical reactions. With a proper free energy expression the effect of solubility of TMOSboth in oil and water can be modeled, and thus also the partitioning behavior of TMOS.Such a model could be used both for bulk systems as for pore-scale models.As noted in Section 9.3 a reservoir model could be used to simulate the gel placementand flow profiles (after treatment) on the the scale of a reservoir. This would answer thequestion for which situation (i.e. reservoir structure, water breakthrough scenario, etc.)the gel treatment works best, and also how the procedure could be optimized.
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TWO-PHASE REACTIVE TRANSPORTOF AN O
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2 1. Introductionproducerbarrierlow
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4 1. IntroductionTwo inter-European
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Part ITwo-phase bulk systems7
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Part IIGel placement in porous mate
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Page 159 and 160: 150 Appendix CwhereΩ A (θ) = −2
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Page 165 and 166: 156 Appendix Eand equal to zero in
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Page 169 and 170: 160 Bibliography[12] B. Vinot, R. S
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Page 177 and 178: 168 Bibliography[127] G. W. Scherer
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Page 181 and 182: 172 Summaryand gelation rates. The
Page 183 and 184: 174 Samenvattingwaterfase. De T 1 v
Page 185 and 186: 176 List of publications
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Untitled - Technische Universiteit Eindhoven

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