Experimental and Numerical Analysis of a PCM-Supported ...
Experimental and Numerical Analysis of a PCM-Supported ...
Experimental and Numerical Analysis of a PCM-Supported ...
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S <br />
<br />
(4.24)<br />
Sáez <strong>and</strong> Carbonell [22] analyzed data for liquid holdup <strong>and</strong> pressure drop available<br />
in the literature over a wide range <strong>of</strong> Reynolds <strong>and</strong> Galileo numbers in packed beds,<br />
to determine the dependence <strong>of</strong> the relative permeability on the saturation for each<br />
phase (Phase saturation refers to the phase volume per void volume). They<br />
correlated the available information in the form:<br />
2.43<br />
K<br />
rl<br />
<br />
(4.25)<br />
2.43<br />
K<br />
rg<br />
S g<br />
(4.26)<br />
The quantity δ in Equation (4.25) is the reduced liquid saturation:<br />
S S<br />
<br />
(4.27)<br />
0<br />
l l<br />
0<br />
1<br />
Sl<br />
where<br />
S is the reduced liquid saturation, Expressing krl in this form suggests that<br />
0<br />
l<br />
the saturation corresponding to the static liquid holdup ( S<br />
0 l<br />
0<br />
l<br />
) consists <strong>of</strong><br />
l<br />
essentially stagnant liquid. The use <strong>of</strong> a reduced liquid saturation in the formula for<br />
the liquid phase relative permeability is common practice in two-phase flow analyses<br />
[21].<br />
In the first attempt to use the so called slit model (one <strong>of</strong> the porous media flow<br />
models) to correlate experimental data, Holub et al. [23] analysis were identical in<br />
form to equations (4.25) <strong>and</strong> (4.26), but with relative permeability functions for the<br />
gas <strong>and</strong> liquid phases with a cubic dependence on saturation:<br />
3<br />
K<br />
rl<br />
S l<br />
(4.28)<br />
3<br />
K<br />
rg<br />
S g<br />
(4.29)<br />
Holub et al. [23] compared the relative permeability functions in equations (4.31) <strong>and</strong><br />
(4.29) to the empirically determined results in equations (4.25), (4.26). They were<br />
successful in fitting holdup <strong>and</strong> pressure drop data in the literature, provided that<br />
Ergun’s constants were set to the values measured experimentally in each case [21].<br />
For the laminar mixed or free convection flow induced by the combined thermal <strong>and</strong><br />
mass buoyancy forces, there is a buoyant force on the gas phase <strong>and</strong> also an<br />
acceleration term, which should be included in Darcy’s law. Taking all <strong>of</strong> these flow<br />
characteristics into consideration, we finally reach a form similar to Brinkman<br />
equation. Brinkman equation extends Darcy’s law to include a term that accounts for<br />
76