Effects of rotating field frequency on the ROTAMAK configuration.
dc.contributor.author | Durance, G | en_AU |
dc.contributor.author | Hogg, GR | en_AU |
dc.contributor.author | Tendys, J | en_AU |
dc.date.accessioned | 2007-11-22T04:06:37Z | en_AU |
dc.date.accessioned | 2010-04-30T04:43:05Z | en_AU |
dc.date.available | 2007-11-22T04:06:37Z | en_AU |
dc.date.available | 2010-04-30T04:43:05Z | en_AU |
dc.date.issued | 1984-12 | en_AU |
dc.description.abstract | Experiments have been undertaken at three rotating field frequencies 1.0 1.85 and 3.5 MHz to determine the effect upon the rotamak configuration and the driven toroidal current. Toroidal current has been driven at all three rotating field frequencies for each of the gases studied. The results indicate that the 1.0 MHz frequency chosen for the rotating field in the high power AAEC rotamak experiments appears to be satisfactory. | en_AU |
dc.identifier.citation | Durance, G., Hogg, G. R., Tendys, J. (1984). Effects of rotating field frequency on the ROTAMAK configuration. (AAEC/E603). Lucas Heights, NSW: Australia Atomic Energy Commission. | en_AU |
dc.identifier.govdoc | 966 | en_AU |
dc.identifier.isbn | 0642598118 | en_AU |
dc.identifier.other | AAEC-E-603 | en_AU |
dc.identifier.placeofpublication | Lucas Heights, New South Wales | en_AU |
dc.identifier.uri | http://apo.ansto.gov.au/dspace/handle/10238/35 | en_AU |
dc.language.iso | en_au | en_AU |
dc.publisher | Australian Atomic Energy Commission | en_AU |
dc.subject | Tokamak devices | en_AU |
dc.subject | Plasma | en_AU |
dc.subject | Cyclotron frequency | en_AU |
dc.subject | Hydrogen | en_AU |
dc.subject | Electric currents | en_AU |
dc.title | Effects of rotating field frequency on the ROTAMAK configuration. | en_AU |
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