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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

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