14.09.2014 Views

Experimental and Numerical Analysis of a PCM-Supported ...

Experimental and Numerical Analysis of a PCM-Supported ...

Experimental and Numerical Analysis of a PCM-Supported ...

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

where β t , β c , ρ ref , c ref , <strong>and</strong> Т ref are the volumetric thermal expansion coefficient,<br />

volumetric diffusion (concentration) expansion coefficient, reference density,<br />

reference concentration, <strong>and</strong> reference temperature respectively. Single phase flow<br />

in a dense porous medium with low flow velocity is typically governed by Darcy’s<br />

law, which relates the fluid velocity v to the pressure drop ∆P over a distance ∆L,<br />

using the viscosity μ <strong>and</strong> the absolute permeability K <strong>of</strong> the medium as proportional<br />

constants.<br />

K P<br />

v <br />

L<br />

(4.20)<br />

Ergun determined an empirical relationship between K, d, the pore size, <strong>and</strong> the void<br />

fraction ε for spherical particles:<br />

2 3<br />

d <br />

K <br />

(4.21)<br />

150 <br />

1<br />

2<br />

It can also be derived from Karman-Kozeny’s hydraulic radius theory [19]; in this<br />

case the constant is 180 instead <strong>of</strong> 150 <strong>and</strong> d represents the particle (bead)<br />

diameter. Darcy’s law can then be used to derive relations between the velocity <strong>and</strong><br />

the pressure gradient for each <strong>of</strong> the two fluid phases as follows, (Nield <strong>and</strong> Bejan<br />

[20]):<br />

v<br />

v<br />

l<br />

g<br />

K<br />

rlK<br />

P<br />

l<br />

g<br />

(4.22)<br />

<br />

l<br />

K<br />

rgK<br />

P<br />

<br />

g<br />

g<br />

(4.23)<br />

<br />

g<br />

For the case <strong>of</strong> two phase flow in equations (4.22) <strong>and</strong> (4.23), the concept <strong>of</strong> relative<br />

permeability K r has been introduced by Sáez <strong>and</strong> Carbonell [22] in momentum<br />

balance equations. The idea behind the concept <strong>of</strong> relative permeability is that an<br />

expression for the drag force for single-phase flow is used. However, this has to be<br />

altered (divided) by a certain parameter to take into account the presence <strong>of</strong> the<br />

second phase. This parameter is known as the relative permeability <strong>of</strong> a certain<br />

phase (krα). The relative permeability can in fact be viewed as the ratio between the<br />

effective permeability <strong>of</strong> a certain phase within two-phase flow (keff,α) <strong>and</strong> the<br />

permeability <strong>of</strong> the bed (k). The relative permeabilities <strong>of</strong> the gas <strong>and</strong> liquid phases<br />

are normally assumed to be primarily a function <strong>of</strong> the saturation S <strong>of</strong> each phase<br />

[21]:<br />

75

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!