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Uranium prices steady as EIA releases annual market report
The end-of-July spot price for uranium was $86.36 per pound, as reported by Cameco—roughly the same as it has been since February. Analytics firm Trading Economics reported a uranium futures price of $86.60 per pound, a figure that also has been holding steady since early April.
These updates come as the U.S. Energy Information Administration has released its 2025 Uranium Marketing Annual Report, which examines in detail multiple aspects of the U.S. uranium market. Data are derived from answers given in the Uranium Marketing Annual Survey, which collects information on contracts, deliveries (during the past year and projected for the next 10 years), purchased enrichment services, inventories, fuel assembly usage, and market requirements.
J. Hosea, J. H. Adler, P. Alling, C. Ancher, H. Anderson, J.L. Anderson,a) J.W. Anderson, V. Arunasalam, G. Ascione, D. Ashcroft, C.W. Barnes,a) G. Barnes, S. Batha,b) M.G. Bell, R. Bell, M. Bitter, W. Blanchard, N.L. Bretz, C. Brunkhorst, R. Budny, T. Burgess,c) H. Bush,e) C.E. Bush,c) R. Camp, M. Caorlin, H. Carnevale, S. Cauffman, Z. Chang,f) C.Z. Cheng, J. Chrzanowski, J. Collins, G. Coward, M. Cropper, D.S. Darrow, R. Daugert, J. DeLooper, H. Duong,h) L. Dudek, R. Durst,f) P.C. Efthimion, D. Ernst,d) J. Faunce, R. Fisher, R.J. Fonck,f) E, Fredd, E. Fredrickson, N. Fromm, G.Y. Fu, H.P. Furth, V. Garzotto, C. Gentile, G. Gettelfinger, J. Gilbert, J. Gioia, T. Golian, N. Gorelenkov,i) B. Grek, L.R. Grisham, G. Hammett, G.R. Hanson,c) R.J. Hawryluk, W. Heidbrink,j) H.W. Herrmann, K.W. Hill, H. Hsuan, A. Janos, D.L. Jassby, F.C. Jobes, D.W. Johnson, L.C. Johnson, J. Kamperschroer, J. Kesner,d) H. Kugel, S. Kwon,e) G. Labik, N.T. Lam,f) P.H. LaMarche, E. Lawson, B. LeBlanc, M. Leonard, J. Levine, F.M. Levinton,b) D. Loesser, D. Long, M.J. Loughlin,k) J. Machuzak,d) D.K. Mansfield, M. Marchlik,e) E. S. Marmar,d) R. Marsala, A. Martin, G. Martin, V. Mastrocola, E. Mazzucato, R. Majeski, M. Mauel,l) M.P. McCarthy, B. McCormack, D.C. McCune, K.M. McGuire, D.M. Meade, S.S. Medley, D.R. Mikkelsen, S.L. Milora,c) D. Mueller, M. Murakami,c) J.A. Murphy, A. Nagy, G.A. Navratil,l) R. Nazikian, R. Newman, T. Nishitani,m) M. Norris, T. O'Connor, M. Oldaker, J. Ongena,n) M. Osakabe,o) D.K. Owens, H. Park, W. Park, S.F. Paul, Yu.I. Pavlov,p) G. Pearson, F. Perkins, E. Perry, R. Persing, M. Petrov,q) C.K. Phillips, S. Pitcher,r) S. Popovichev,p) R. Pysher, A.L. Qualls,c) S. Raftopoulos, R. Ramakrishnan, A. Ramsey, D.A. Rasmussen,c) M.H. Redi, G. Renda, G. Rewoldt, D. Roberts,f) J. Rogers, R. Rossmassler, A.L. Roquemore, E. Ruchov,j) S.A. Sabbagh,l) M. Sasao,o) G. Schilling, J. Schivell, G.L. Schmidt, R. Scillia, S.D. Scott, T. Senko, R. Sissingh, C. Skinner, J. Snipes,d) P. Snook, J. Stencel, J. Stevens, T. Stevenson, B.C. Stratton, J.D. Strachan, W. Stodiek, E. Synakowski, W. Tang, G. Taylor, J. Terry,d) M.E. Thompson, J.R. Timberlake, H.H. Towner, A. von Halle, C. Vannoy, R. Wester, R. Wieland, J.B. Wilgen,c) M. Williams, J.R. Wilson, J. Winston, K. Wright, D. Wong,r) K.L. Wong, P. Woskov,d) G.A. Wurden,a) M. Yamada, A. Yeun,r) S. Yoshikawa, K.M. Young, M.C. Zarnstorff, S.J. Zweben
Fusion Science and Technology | Volume 26 | Number 3 | November 1994 | Pages 389-398
Magnetic Fusion Experiment | Proceedings of the Eleventh Topical Meeting on the Technology of Fusion Energy New Orleans, Louisiana June 19-23, 1994 | doi.org/10.13182/FST94-A40191
Articles are hosted by Taylor and Francis Online.
The deuterium-tritium (D-T) experimental program on the Tokamak Fusion Test Reactor (TFTR) is underway and routine tritium operations have been established. The technology upgrades made to the TFTR facility have been demonstrated to be sufficient for supporting both operations and maintenance for an extended D-T campaign. To date fusion power has been increased to ∼9 MW and several physics results of importance to the D-T reactor regime have been obtained: electron temperature, ion temperature, and plasma stored energy all increase substantially in the D-T regime relative to the D-D regime at the same neutral beam power and comparable limiter conditioning; possible alpha electron heating is indicated and energy confinement improvement with average ion mass is observed; and alpha particle losses appear to be classical with no evidence of TAE mode activity up to the PFUS ∼ 6 MW level. Instability in the TAE mode frequency range has been observed at PFUS > 7 MW and its effect on performance is under investigation. Preparations are underway to enhance the alpha particle density further by increasing fusion power and by extending the neutral beam pulse length to permit alpha particle effects of relevance to the ITER regime to be more fully explored.