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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liquid <strong>and</strong> solid phases, respectively. At steady state conditions, the energy flow from<br />
gas to solid phase equilibrates with the energy flow from solid to liquid phase <strong>and</strong> the<br />
local temperatures <strong>of</strong> all phases remain constant. Any change <strong>of</strong> the system<br />
parameters will break steady state conditions, <strong>and</strong> the local temperatures will<br />
change.<br />
The condensation rate depends mainly on the vapor pressure gradient between the<br />
bulk gas phase from one side <strong>and</strong> both the gas-liquid interface <strong>and</strong> the gas-solid<br />
interface from the other side. The vapor pressure is a direct function <strong>of</strong> the<br />
respective local temperatures, assuming saturation conditions in closed loop cycles.<br />
However, the sensible energy flow components also affect the film temperature at<br />
gas-liquid interface <strong>and</strong> gas-solid interface, which indirectly affects the condensation<br />
rate. On the other h<strong>and</strong>, condensation contributes a considerable fraction <strong>of</strong> latent<br />
heat to the liquid <strong>and</strong> solid phases <strong>and</strong> leads to rising their temperatures, which in<br />
turn affects both heat <strong>and</strong> mass balances. In fact, the microscopic analysis <strong>of</strong> the<br />
condensation process is much more complicated than the described macroscopic<br />
analysis, while the later is sufficiently accurate for the present application <strong>and</strong> range<br />
<strong>of</strong> operation conditions in comparison with the experimental measurements as will<br />
be presented later.<br />
4.2.4 Closure relationships<br />
Predictive models for packed column performance incorporate macroscopic<br />
properties <strong>of</strong> the entire column based on volume or spatial averaging technique<br />
which was developed by Slattery [26], rather than focusing rigorously on underlying<br />
local variations <strong>of</strong> momentum, heat, <strong>and</strong> mass transfer processes. Hence, closure<br />
models have to be provided in the numerical scheme to capture the information that<br />
is lost in the averaging process. Careful selection <strong>of</strong> the appropriate closure<br />
relationships from literature is therefore a fundamental factor for achieving high<br />
accuracy <strong>of</strong> the simulation model. Modeling <strong>and</strong> design <strong>of</strong> a r<strong>and</strong>omly packed<br />
distillation column requires a reliable specification <strong>of</strong> effective interfacial areas,<br />
phase fractions, heat <strong>and</strong> mass transfer coefficients, <strong>and</strong> pressure drop. The next<br />
sections will be devoted to the adopted modeling procedures <strong>and</strong> calculations <strong>of</strong><br />
such critical parameters.<br />
4.2.3.1 Evaporation <strong>and</strong> condensation rates<br />
The evaporation rate, the condensation rates at the gas/liquid interface <strong>and</strong> the<br />
gas/solid interface can be written respectively as a function <strong>of</strong> the difference<br />
between the vapor pressure or vapor concentration at these interfaces <strong>and</strong> the vapor<br />
pressure or vapor concentration at the bulk gas:<br />
<br />
m<br />
evap<br />
k<br />
g<br />
a<br />
e<br />
<br />
c<br />
inter<br />
<br />
( T ) c<br />
(4.36)<br />
l<br />
79