http://rdf.ncbi.nlm.nih.gov/pubchem/patent/DE-2549311-A1
Outgoing Links
Predicate | Object |
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assignee | http://rdf.ncbi.nlm.nih.gov/pubchem/patentassignee/MD5_feee2699ad31215b280c87343e819b12 |
classificationCPCInventive | http://rdf.ncbi.nlm.nih.gov/pubchem/patentcpc/B01D59-34 |
classificationIPCInventive | http://rdf.ncbi.nlm.nih.gov/pubchem/patentipc/B01D59-34 |
filingDate | 1975-11-04-04:00^^<http://www.w3.org/2001/XMLSchema#date> |
publicationDate | 1977-05-12-04:00^^<http://www.w3.org/2001/XMLSchema#date> |
publicationNumber | DE-2549311-A1 |
titleOfInvention | METHOD AND DEVICE FOR ISOTOPE SEPARATION |
abstract | Process uses a charge transfer reaction (A++B right arrow A+B+). The atomic ions A+ of one of the isotopes are formed preferentially by irradiation while the other isotope is not affected. The charged ions are then neutralised by atoms or molecules (B). Alternatively the atoms of one of the isotopes are activated by irradiation while the other remains qinescent. The activated one then reacts with ionic stream of atoms or molecules (B+). A and B are different elements or cpds. To select a suitable material for B, its first I.P. should be greater than the first I.P. of V. If the B+ system is used, its first I.P. should be less than the first I.P. of V. Used esp. for separating the isotopes of V to provide an enriched fuel for nuclear fuels. The process proceeds with the same probability as the excitation of the particles from their basic state. The transfer probability of the various excitation stages are differentiated by several orders of magnitude. Also ions are used instead of atoms, which permits acceleration, deflection, etc. Only a single resonance light source need be used. |
priorityDate | 1975-11-04-04:00^^<http://www.w3.org/2001/XMLSchema#date> |
type | http://data.epo.org/linked-data/def/patent/Publication |
Incoming Links
Total number of triples: 22.