chemical physics of discharges - Argonne National Laboratory
chemical physics of discharges - Argonne National Laboratory chemical physics of discharges - Argonne National Laboratory
156 The Dissociation of Metal Halides in Electrical Discharges F o KO MCTaggart Mdsion of Mineral Chemistry, C.S.I.R.0. Box 124, Port Melbourne, Victoria, Australia. I Introduction. in electrical discharges in dissociating gae molecules is well known, and is the basis of the chemical reactions that a H observed in plasnrs systems. Since gases such a8 02, H2, B2dC1 9 88 well a8 vapours of organic and other compounds have been diesociazed to atoms ad/m radicals, it appears Logical to suppose that many other molecules would behave similarly. This paper describes the diesociation of the halides of the Croup I, I1 and 111, and rare earth metals. &m-imental. Ideally, the halides should be introduced Into the discharge tube in the form of vapoure at suitable pressures. Due to the wide range of volatilities occurring in the above compounds and to other erperimental difficulties it proved more convenient to we carrier gmee, and to volatilize the halides from small boats contained wlthin the reaction tube by heating these boats to suitable temperatures. It was usually possible to make use of the heat generated in the plasma itself for this purpose. Samples were placed upstream from,or within the central plasma region,ln positione where heat sufficient to give the desired rate of volatilization was produced. The effect of the energetic electrons produced Since heating of solib due to atomic recombination ie largeu a surface effect it was also possible to verg the sublimation rate of samples by changing the Lmrfece area exposed to the plasma. Both inert gases (in particular He and H ) and hydrogen have been used and certain reactions which are discussed befow appear to involve E atoms aa well a dissociative effects. These gases were of coomerciel purity, the He and 5 being purified by passing them over zirconim ponder heated to 800°C; although no essential differences between the cylinder gases and the purified gases were observed. Pressures of the carrier gaaes were varied between 0.5 ad 2.3 mm. Halides wed were of A.B. grade, but in certain cases impure compounds were deliberately used in order to determine the effects of impurities on the dissociation and on the purity of the metal obtained. Ertenslve use was made of a 2450 mC magnetron generator (Mullard m2/205A) which although capable of an output in exce88 of 2 M continuow wave power, was seldom operated at inputs higher than 600 watts. B&P frequency energy from the magnetron was fed via a 50 ohm air dielectric coaxial line, to a section of waveguide operated ea a resonant cavity by means of a sliding plunger inserted into the open end. The discharge tube passed tranevereely through the guide at a point of m a r i m electrostatic field. h e investigatlons, Involving the chlorides of Li, Be, and a, which dissociate very readily, were made using au 9-f" generator consintlng of a 4-125A vacuum tube at a frequency of 30 mC, the power of which could be varied from close to zero to about 400 watts. In these
Compound Bond he rgy Li I 82 UBr 102 LICl 115 Lilr 138 157 cases the reaction tube passed through the "tank coil" of the output circuit . Conventional methods of analysis were used to determine 8/ the SmOunt of metal deposited, b/ the undissociated halide sublimed onto the reaction tube, and c/ the halogen or hydrogen halide collected in the liquid sir trap which followed the reaction tube in the flow1 syatem. - Results. From all the halides studied It was poesible to separate metals, often in good yields. 1 The lithim -UP cornpoonds dissociated in both inert carrier gmes and in H to gLve metals d the relative reaction rates were detedned for the fodides, bromides, chlorides and fluorides of Li, Ha, K end Cs. Son18 Of these are ehown in Table 1. It rill be noted that for any one metal - Table 1 Relative Reaction Ratee for the Hdidee of LI and la Re10 React. Compound Bond Bel, Bead. Bate -rgJ Bate 232.5 101.5 66.5 19.0 BaI BaBr HaCl BaF 72 89 99 108 26 e0 15.0 IOIO 5 *o I
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156<br />
The Dissociation <strong>of</strong> Metal Halides in Electrical Discharges<br />
F o KO MCTaggart<br />
Mdsion <strong>of</strong> Mineral Chemistry, C.S.I.R.0. Box 124, Port<br />
Melbourne, Victoria, Australia.<br />
I<br />
Introduction.<br />
in electrical <strong>discharges</strong> in dissociating gae molecules is well known,<br />
and is the basis <strong>of</strong> the <strong>chemical</strong> reactions that a H observed in plasnrs<br />
systems. Since gases such a8 02, H2, B2dC1 9 88 well a8 vapours <strong>of</strong><br />
organic and other compounds have been diesociazed to atoms ad/m<br />
radicals, it appears Logical to suppose that many other molecules would<br />
behave similarly. This paper describes the diesociation <strong>of</strong> the halides<br />
<strong>of</strong> the Croup I, I1 and 111, and rare earth metals.<br />
&m-imental. Ideally, the halides should be introduced Into<br />
the discharge tube in the form <strong>of</strong> vapoure at suitable pressures. Due<br />
to the wide range <strong>of</strong> volatilities occurring in the above compounds and<br />
to other erperimental difficulties it proved more convenient to we<br />
carrier gmee, and to volatilize the halides from small boats contained<br />
wlthin the reaction tube by heating these boats to suitable temperatures.<br />
It was usually possible to make use <strong>of</strong> the heat generated in the plasma<br />
itself for this purpose. Samples were placed upstream from,or within<br />
the central plasma region,ln positione where heat sufficient to give the<br />
desired rate <strong>of</strong> volatilization was produced.<br />
The effect <strong>of</strong> the energetic electrons produced<br />
Since heating <strong>of</strong> solib<br />
due to atomic recombination ie largeu a surface effect it was also<br />
possible to verg the sublimation rate <strong>of</strong> samples by changing the Lmrfece<br />
area exposed to the plasma.<br />
Both inert gases (in particular He and H ) and hydrogen have been<br />
used and certain reactions which are discussed befow appear to involve E<br />
atoms aa well a dissociative effects. These gases were <strong>of</strong> coomerciel<br />
purity, the He and 5 being purified by passing them over zirconim ponder<br />
heated to 800°C; although no essential differences between the cylinder<br />
gases and the purified gases were observed. Pressures <strong>of</strong> the carrier<br />
gaaes were varied between 0.5 ad 2.3 mm. Halides wed were <strong>of</strong> A.B. grade,<br />
but in certain cases impure compounds were deliberately used in order to<br />
determine the effects <strong>of</strong> impurities on the dissociation and on the purity<br />
<strong>of</strong> the metal obtained.<br />
Ertenslve use was made <strong>of</strong> a 2450 mC magnetron generator (Mullard<br />
m2/205A) which although capable <strong>of</strong> an output in exce88 <strong>of</strong> 2 M continuow<br />
wave power, was seldom operated at inputs higher than 600 watts. B&P<br />
frequency energy from the magnetron was fed via a 50 ohm air dielectric<br />
coaxial line, to a section <strong>of</strong> waveguide operated ea a resonant cavity by<br />
means <strong>of</strong> a sliding plunger inserted into the open end. The discharge<br />
tube passed tranevereely through the guide at a point <strong>of</strong> m a r i m electrostatic<br />
field. h e investigatlons, Involving the chlorides <strong>of</strong> Li, Be,<br />
and a, which dissociate very readily, were made using au 9-f" generator<br />
consintlng <strong>of</strong> a 4-125A vacuum tube at a frequency <strong>of</strong> 30 mC, the power <strong>of</strong><br />
which could be varied from close to zero to about 400 watts. In these