Results 191 to 200 of about 19,123 (225)

Counter-beam thermonuclear fusion

Technical Physics, 2013
A method of organizing counter beams of deuterium and tritium in a ring with electrified walls is suggested. In such a ring, beams of ions are locked in a potential well the height of which is much larger than the energy of colliding particles. In this instance, the phase volume of the ion beams increases due to multiple scattering.
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Solid-state “thermonuclear fusion”

Physics Today, 1965
In the search for a power-producing fusion reactor the experimental devices built have usually been at least roomsize, cost millions of dollars, and taken many years to construct and debug. Each time a new idea has been proposed it has required much time, labor, and funds actually to get such a device operating.
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Joining of CMCs for thermonuclear fusion applications

Journal of Nuclear Materials, 1996
Abstract Because of their thermomechanical and nuclear peculiarities some ceramic matrix composites (CMCs), i.e. carbon fibre reinforced carbon composites (CFC), carbon, fibre reinforced silicon carbide composites (C f /SiC) and silicon carbide fibre reinforced silicon carbide composites (SiC f /Sic) are candidate materials for high temperature ...
SALVO, Milena, FERRARIS, Monica, LEMOINE P., APPENDINO, MARGHERITA, MEROLA M.   +4 more
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Condensed hydrogen for thermonuclear fusion

Journal of Applied Physics, 2010
Inertial confinement fusion (ICF) power, in either pure fusion or fission-fusion hybrid reactors, is a possible solution for future world’s energy demands. Formation of uniform layers of a condensed hydrogen fuel in ICF targets has been a long standing materials physics challenge. Here, we review the progress in this field.
S. O. Kucheyev, A. V. Hamza
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A free-electron maser for thermonuclear fusion

Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 1992
Abstract An update is given on the design effort for an electrostatic free-electron maser (FEM) producing a 1 MW cw output in the 150–250 GHz range.
Urbanus, W.H., van Amersfoort, P.W., Best, R.W. B., Sterk, A.B., Verhoeven, A.G. A., van der Wiel, M.J., Lazar, N.H., Boehmer, H., Gover, A., Pinhasi, Y., Jerby, E.   +10 more
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Status and prospects of controlled thermonuclear fusion

Hyperfine Interactions, 1993
Of all approaches to controlled thermonuclear fusion the tokamak experiments have been most successful. Over the last decade particularly three large devices have achieved plasma density,n, temperature,T, and energy confinement time,τ E, in ranges necessary for a fusion reactor plasma.
Duechs, D., Hellsten, T.
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The return of thermonuclear fusion

Nature, 1994
Four research reports from Lawrence Livermore Laboratory amply justify the decision to build a more powerful laser for fusion research.
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Thermonuclear Reactions and Nuclear Fusion

1979
Power from nuclear fission is now a reality both on land and sea, and in those countries where the coal measures are rapidly being worked out one can envisage their future economy depending on nuclear fuels, especially when oil is regarded as a costly import.
T. A. Littlefield, N. Thorley
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Tritium Problems in a Thermonuclear Fusion Device

Fusion Technology, 1985
Works under way in CEA Saclay on a fusion reactor tritium system are described. Areas covered are large components for the torus vacuum system, fuel clean-up processes, electrolytic cell, atmosphere clean-up and tritium recovery from solid wastes. All these tasks are covered theoretically and experimentally.
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Macroparticle accelerators and thermonuclear fusion

Il Nuovo Cimento B Series 10, 1966
Accelerating macroparticles to velocities in the range of 106 to 108 cm/s would lead to a large number of applications such as the simulation of meteors, the production of very dense plasmas and possibly the release of controlled thermonuclear energy.
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