14.05.2013 Views

estudio y caracterización de un plasma de microondas a presión ...

estudio y caracterización de un plasma de microondas a presión ...

estudio y caracterización de un plasma de microondas a presión ...

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.

Destrucción <strong>de</strong> VOCs con <strong>plasma</strong> <strong>de</strong> Aire<br />

of trichloroethylene. On the other hand, the <strong>un</strong>iformity of the C-Cl bonds in carbon<br />

tetrachlori<strong>de</strong> facilitates rupture and limits recombination.<br />

128<br />

Concentration curves of carbon tetrachlori<strong>de</strong> and trichloroethylene show an<br />

exponential <strong>de</strong>cline that ends at the same concentration; thus, the <strong>de</strong>composition of<br />

trichloroethylene is more efficient than the <strong>de</strong>composition of carbon tetrachlori<strong>de</strong><br />

because the <strong>de</strong>cline in the C2HCl3 curve is more prono<strong>un</strong>ced. To analyse this behaviour,<br />

the parameter of <strong>de</strong>cline, , can be calculated from the outlet concentration and the<br />

amo<strong>un</strong>t of energy dissipated in the <strong>plasma</strong> [28, 29]:<br />

<br />

where X is the VOC concentration after reaction and E is the <strong>de</strong>posited energy <strong>de</strong>nsity<br />

(applied microwave power/gas flow rate; J/L). β represents the energy <strong>de</strong>nsity required<br />

to reduce the concentration of trichloroethylene or carbon tetrachlori<strong>de</strong> to 1/e of X0<br />

(extrapolated zero Watts of microwave power) and is an indicator of the ease of<br />

<strong>de</strong>struction.<br />

Similar exponential behaviour was observed by Yan et al. [30] in a corona<br />

<strong>plasma</strong>. These authors suggested that a linear recombination of the active species<br />

produced VOC <strong>de</strong>struction. Thus, X0 correspon<strong>de</strong>d to the initial concentration of<br />

contaminant. However, in our case, X0 is several or<strong>de</strong>rs of magnitu<strong>de</strong> lower (653 ppbv<br />

for C2HCl3 and 1059 ppbv for CCl4) than the initial concentration (1000 ppmv for both<br />

compo<strong>un</strong>ds), as shown in Figure 5.3. Thus, to fully explain the observed concentration<br />

of contaminants, other <strong>de</strong>struction mechanisms that are in<strong>de</strong>pen<strong>de</strong>nt of the power supply<br />

must be relevant. One possibility is that chlorine released from the contaminants reacts<br />

with Cu (I), which is introduced into the <strong>plasma</strong> from the tip of the torch.<br />

The β parameter obtained for CCl4 and C2HCl3 was 9420 and 9397 J/L,<br />

respectively; thus, β does not <strong>de</strong>pend strongly on the concentration of the compo<strong>un</strong>d.<br />

Rather, β is affected by the configuration of the <strong>plasma</strong> torch such as the flow rate,<br />

microwave power and initial concentration, which makes the proposed <strong>de</strong>vice incredibly<br />

versatile.

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

Saved successfully!

Ooh no, something went wrong!