Page 51 - gas transport in porous media
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                                           30                            +  All Gas        Ho
                                                                           All Gas
                                         Cumulative Drawdown (mm 3 )  20  +  +  +  +  6.0 mm LI
                                           25
                                                                           5.6 mm LI
                                                                           7.5 mm LI
                                           15
                                                                           7.5 mm LI
                                           10
                                                                           8.0 mm LI
                                            0 5  +  +  +  +  +  +  +       7.8 mm LI
                                             0    10   20   30  40   50    8.9 mm LI
                                                       Time (hr)
                           Figure 3.11.  Drawdown rates of water for different liquid-island (LI) lengths in the pore (Silverman,
                           1998)

                             Additional experiments were performed by Gu et al. (1998) to investigate enhanced
                           vapor diffusion processes in a porous packed bed. The apparatus consisted of an
                           acrylic chamber (51 mm wide × 51 mm deep × 95 mm high). A bed of glass beads
                           were packed in the chamber, which was capped with a water-circulated jacket that was
                           maintained at a constant temperature. Beneath the water jacket was a fibrous wick that
                           was connected to an external reservoir that provided a supply of saturated water at a
                           fixed temperature. An electronic balance was used to monitor the water loss from the
                           reservoir. The bottom of the chamber consisted of a desiccant tray and a water jacket.
                           The tray could be removed for weighing to determine the accumulation of water. The
                           entire apparatus was insulated with foam, and thermocouples were fitted along the
                           chamber. A gamma attenuation system was used to measure the saturation profile
                           of the packed bed during the experiment. During the experiment, water vapor would
                           diffuse from the top toward the bottom desiccant. The rate of diffusion was monitored
                           and compared with conditions when no porous media were present (i.e., diffusion in
                           free space). Results showed that significant enhancement of vapor diffusion occurred
                           under both transient and steady-state conditions when moist porous media was present
                           in the chamber.



                           3.5.4  Field Studies
                           Evidence for enhanced vapor diffusion has also been observed in field studies. The
                                                          3
                           distribution of anthropogenic  36 Cl and H in the unsaturated zone in the Chihuahuan
                           and Sonoran Deserts (Southwest United States) were used to evaluate liquid and
                           vapor transport (Phillips et al., 1988; Scanlon, 1992). Chlorine-36 is nonvolatile and
                           restricted to liquid phase flow whereas tritiated water is volatile and can move in both
                           liquid and vapor phases. In the Chihuahuan Desert, tritium penetrated 1 m deeper
                                           3
                           than  36 Cl although H fallout occurred later than that of  36 Cl. Deeper penetration
                             3
                           of H (1.4 m) relative to that of  36 Cl (0.5 m) was attributed to enhanced downward
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