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

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

Several models <strong>and</strong> approaches for mass transfer coefficients on both the gas <strong>and</strong><br />

liquid sides are presented by Wagner et al. [40]. Various approaches <strong>and</strong> models for<br />

determination <strong>of</strong> the wetted <strong>and</strong> effective interfacial areas for mass transfer<br />

presented by Kister [32] <strong>and</strong> G<strong>and</strong>hidasan [41] were preliminary examined <strong>and</strong><br />

compared against each other.<br />

One particular problem to address here is the significant discrepancies between the<br />

predicted values <strong>of</strong> mass transfer coefficients between various approaches <strong>and</strong><br />

models. It is observed that many researchers have used Onda et al. [35] model to<br />

describe the liquid-gas interfacial areas <strong>and</strong> mass transfer coefficient in distillation<br />

columns. Klausner et al. [45] have already developed a detailed heat <strong>and</strong> mass<br />

transfer analysis for a HDH system called the diffusion driven desalination (DDD)<br />

process. They extensively tested Onda et al. [35] correlations <strong>and</strong> used it to evaluate<br />

the mass transfer coefficients on the liquid <strong>and</strong> gas sides. They reported that<br />

excellent results were obtained against experimentation measurements [47]; thus<br />

the same approach will be applied here.<br />

Nevertheless, Klausner <strong>and</strong> Mei [45-46] modified Onda et al. [35] model described<br />

by equations (4.46-4.47) by introducing a constant <strong>of</strong> 2.2 instead <strong>of</strong> 1.45 for<br />

calculating the wetted interfacial area in the (DDD) system. They argued that the<br />

model underestimates the wetted surface area <strong>of</strong> the packing <strong>and</strong> this was the<br />

reason behind this modification in equation (4.47). The model is based on the<br />

concept <strong>of</strong> wetted packing area as a geometric parameter in determining the<br />

Reynolds number for the liquid as opposed to the interfacial area.<br />

a<br />

a<br />

e<br />

<br />

<br />

<br />

c<br />

exp 1.45<br />

<br />

<br />

<br />

<br />

l <br />

0.75<br />

0.1 0.2 0.<br />

05<br />

1 Rel<br />

Wel<br />

Frl<br />

<br />

<br />

<br />

<br />

(4.46)<br />

a<br />

w<br />

a<br />

<br />

<br />

<br />

<br />

<br />

<br />

c<br />

exp <br />

2.2<br />

<br />

<br />

<br />

<br />

L <br />

0.75<br />

0.5 0.2 0.<br />

05<br />

1 Re<br />

LA<br />

WeL<br />

Fr<br />

L<br />

<br />

<br />

<br />

<br />

<br />

<br />

(4.47)<br />

Therefore, this modification could be even more crucial for the present analysis due<br />

to the existence <strong>of</strong> conductive packing media or a solid phase in the energy <strong>and</strong><br />

mass balances. However, their predicted performance using this modified correlation<br />

is always higher than their experimental measurements in terms <strong>of</strong> the outlet air<br />

humidity content, outlet water temperature, <strong>and</strong> outlet air temperature.<br />

In the original model, Onda et al. [35] assumed the wetted area was equal to the<br />

effective interfacial area. The total wetted surface area in the irrigated column is<br />

expected to be greater than the effective area for mass transfer due to existence <strong>of</strong><br />

static liquid holdup which contributes little to heat <strong>and</strong> mass transfer. This finding has<br />

been ascertained during the course <strong>of</strong> preliminary calculations <strong>of</strong> the effective<br />

83

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

Saved successfully!

Ooh no, something went wrong!