chemical physics of discharges - Argonne National Laboratory
chemical physics of discharges - Argonne National Laboratory chemical physics of discharges - Argonne National Laboratory
epcrte? the noss~kil.itv of nroduct-r carton bla ck fror hvdrocarbons usinp a nlnsna 'et. !!ethane or other hvtrccarbons which would h e introduced intc the plasma flane, uoul? be cracke2 usir.;. tvCro.ren as the ooeratinr vas an? Droducirp carbon black. LicciC as i.re11 3s' Fzseous h-:?rncar!mns car te cse? 5s a source for carbon and the '.'itrc khoratories (4) have exnerinente? ;iith carton Slack production frnv linuic! h:idrocarhons. 'P"?O5 + !Z1 j Ta (8) \!C3 t 4 :.: ' (9) ~ 1 3 + 0 Y~/CE,,+ ~ PI (10) re0 + U7+ ?e (11) The nroduction of metal nitrides (F! f* 17) from the elements has been invest ipated for three elements, titanium, -arrnesiun and tunpsten (reactions 1 to 3). The Droduction of titaniun nitride in the 1000. vield was accovplished bv usinp 200 mesh titaniur Dowder fed into a nitrooen Dlasna ;et. The titanium nitride particle size was found to be 0.75 to 7.5 microns and the nroduct was also formed in larpe, corpact, Folden .rellov crvstals. In a like manner tunpsten nitride was formed in 75p yield. 40% conversion to rnapnesiun nitride was obtained when nacnesium was fed into a nitropen olasma jet. The preDaration of'cetal carbiles has also been reDorted (12 6 17). Tipure 5 shovs the 9 conversion VS. Kwhr/a tunasten input for reaction 4. As can be seen, the XC conversion is directlv Dronortional to the power input level. The hiRhest conversions obtained were 43? for \,!2r and 11% for %'C. reaction 5 aSove is shown in riplire 6 uhere .9. conversion is plotter] VS. Kwhr/v !XI3 innut. The three products of the reaction, tunrsten (43 to Rl? cnnversicn), tunester. carhide (4 to 11% oonversion) and ditunesten carbide (9 to 35% conversion) are fomad in a total conversion of 81 to 9UQ.. ?e naior Droduct is tiinosten which is'favored at higher Kwhr/p WOg inputs. The reaction of tantalum and methane in a helium nlasma jet is shown in Fipure 7 where a water-cooled cuenchinp nroba was ~ l ~ c at e d 1/3" and 5" below the plasma jet. The effect of the ruenchinr distance is dranatic. The annunt of Ta2C formed is notapDrecfahlv different in either case, however, the TaC vield chanped considerably bv the n1acerrer.t of the ouenchinp device. Conversions UD to 72% have been produced by this reaction. Tipure e shows a nlot of the tantalur-pentoxide plus nethane reaction carried o ut in a helitic Dlasma jet. The % conversion is plotted vs. Kwhr/y tantalun nentoxide input for two different ouenchinp nrobe distances frm the plasma iet. Jn the case where the auencher was 1/7" 5elow the jet the Droduction of TaC
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- Page 281 and 282: i i (12) c (11) (14) I 281 LITERATU
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- Page 285 and 286: 285 TABLE 2 Effect of Haloqenated A
- Page 287 and 288: ANALYTICAL RESULTS Some evidence wa
- Page 289 and 290: DISCUSSION 289 The salient features
- Page 291 and 292: ? ~ MENBERSHIP IN THE DIVISION OF F
- Page 293 and 294: 292 flow of the reactant gas stream
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- Page 313: FUFARCI! INSTITUTE OF TFYDLC UNIVER
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- Page 342 and 343: RESULTS 341 Composition Dependence
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epcrte? the noss~kil.itv <strong>of</strong> nroduct-r carton bla ck fror hvdrocarbons usinp a nlnsna<br />
'et. !!ethane or other hvtrccarbons which would h e introduced intc the plasma flane,<br />
uoul? be cracke2 usir.;. tvCro.ren as the ooeratinr vas an? Droducirp carbon black.<br />
LicciC as i.re11 3s' Fzseous h-:?rncar!mns car te cse? 5s a source for carbon and the<br />
'.'itrc khoratories (4) have exnerinente? ;iith carton Slack production frnv linuic!<br />
h:idrocarhons.<br />
'P"?O5 + !Z1 j Ta (8)<br />
\!C3 t 4 :.: ' (9)<br />
~ 1 3 + 0 Y~/CE,,+ ~<br />
PI (10)<br />
re0 + U7+ ?e (11)<br />
The nroduction <strong>of</strong> metal nitrides (F! f* 17) from the elements has been<br />
invest ipated for three elements, titanium, -arrnesiun and tunpsten (reactions 1 to 3).<br />
The Droduction <strong>of</strong> titaniun nitride in the 1000. vield was accovplished bv usinp 200<br />
mesh titaniur Dowder fed into a nitrooen Dlasna ;et. The titanium nitride particle<br />
size was found to be 0.75 to 7.5 microns and the nroduct was also formed in larpe,<br />
corpact, Folden .rellov crvstals. In a like manner tunpsten nitride was formed in<br />
75p yield. 40% conversion to rnapnesiun nitride was obtained when nacnesium was<br />
fed into a nitropen olasma jet.<br />
The preDaration <strong>of</strong>'cetal carbiles has also been reDorted (12 6 17). Tipure<br />
5 shovs the 9 conversion VS. Kwhr/a tunasten input for reaction 4. As can be seen,<br />
the XC conversion is directlv Dronortional to the power input level. The hiRhest<br />
conversions obtained were 43? for \,!2r and 11% for %'C. reaction 5 aSove is shown in<br />
riplire 6 uhere .9. conversion is plotter] VS. Kwhr/v !XI3 innut. The three products <strong>of</strong><br />
the reaction, tunrsten (43 to Rl? cnnversicn), tunester. carhide (4 to 11% oonversion)<br />
and ditunesten carbide (9 to 35% conversion) are fomad in a total conversion <strong>of</strong> 81<br />
to 9UQ.. ?e naior Droduct is tiinosten which is'favored at higher Kwhr/p WOg inputs.<br />
The reaction <strong>of</strong> tantalum and methane in a helium nlasma jet is shown in Fipure 7 where<br />
a water-cooled cuenchinp nroba was ~ l ~ c at e d 1/3" and 5" below the plasma jet. The<br />
effect <strong>of</strong> the ruenchinr distance is dranatic. The annunt <strong>of</strong> Ta2C formed is notapDrecfahlv<br />
different in either case, however, the TaC vield chanped considerably bv<br />
the n1acerrer.t <strong>of</strong> the ouenchinp device. Conversions UD to 72% have been produced<br />
by this reaction. Tipure e shows a nlot <strong>of</strong> the tantalur-pentoxide plus nethane<br />
reaction carried o ut in a helitic Dlasma jet. The % conversion is plotted vs. Kwhr/y<br />
tantalun nentoxide input for two different ouenchinp nrobe distances frm the plasma<br />
iet. Jn the case where the auencher was 1/7" 5elow the jet the Droduction <strong>of</strong> TaC