Applications for a neutron-emitting plasma focus

Summary form only given. The plasma focus device produces the smallest source size, highest instantaneous flux, pulsed neutron source of any fusion-reaction based system when it is operated in the high pressure mode. Specifically, the neutron emission region has been measured to be -1 cm long and /s...

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Published inIEEE Conference Record - Abstracts. 1996 IEEE International Conference on Plasma Science p. 237
Main Authors Freeman, B.L., Fowler, C.M., McDaniel, F.D.
Format Conference Proceeding
LanguageEnglish
Published United States IEEE 1996
Institute of Electrical and Electronics Engineers, Inc., Piscataway, NJ (United States)
Subjects
Online AccessGet full text
ISBN9780780333222
0780333225
ISSN0730-9244
2576-7208
DOI10.1109/PLASMA.1996.551453

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Abstract Summary form only given. The plasma focus device produces the smallest source size, highest instantaneous flux, pulsed neutron source of any fusion-reaction based system when it is operated in the high pressure mode. Specifically, the neutron emission region has been measured to be -1 cm long and /spl lsim/2 mm diameter. Neutron yields as high as /spl gsim/10/sup 12/ neutrons/pulse (n/p) have been produced from the D(D,n)/sup 3/He reaction (DD). The scaling of such yields to their equivalent D(T,n)/sup 4/He neutron (DT) yields by a factor of 80 to 100 has been demonstrated. The pulse width of these neutron yields is /spl lsim/100 ns, from many measurements, Therefore, the plasma focus can produce DD neutron yields of /spl gsim/10/sup 12/ n/p and DT neutron yields of /spl sim/10/sup 14/ n/p without any extension of this machine's demonstrated operating range. At the upper end of these yields, the DT reaction provides instantaneous fluxes of /spl gsim/10/sup 21/ n/s, neutron densities of /spl lsim/10/sup 9/ n/cm/sup 2/ at 1 m from the source, and instantaneous flux densities of /spl lsim/10/sup 16/ n/cm/sup 2/-s. Given these characteristics as a starting point, such a neutron source can be utilized for several applications within the presently recognized operating bounds of the plasma focus.
AbstractList The plasma focus device produces the smallest source size, highest instantaneous flux, pulsed neutron source of any fusion-reaction based system when it is operated in the high pressure mode. Neutron yields as high as {ge} 10{sup 12} neutrons/pulse (n/p) have been produced from the D(D,n){sup 3}He reaction (DD). The scaling of such yields to their equivalent D(T,n){sup 4}He neutron (DT) yields by a factor of 80 to 100 has been demonstrated. The pulse width of these neutron yields is {le} 100 ns, from many measurements. Therefore, the plasma focus can produce DD neutron yields of {ge} 10{sup 12} n/p and DT neutron yields of {approximately} 10{sup 14} n/p without any extension of this machine`s demonstrated operating range. At the upper end of these yields, the DT reaction provides instantaneous fluxes of {approx_gt} 10{sup 21} n/s, neutron densities of {approx_lt} 10{sup 9} n/cm{sup 2} at 1m from the source, and instantaneous flux densities of {approx_lt} 10{sup 16} n/cm{sup 2}-s. Given these characteristics as a starting point, such a neutron source can be utilized for several applications within the presently recognized operating bounds of the plasma focus. With scaling, several other applications are possible.
It is shown that a neutron source can be utilized for several applications within the presently recognized operating bounds of a plasma focus. With scaling, several other applications are possible. With suitable scintillators and image intensifiers, a low-resolution, static neutron radiograph can be obtained with a neutron density of about 3x10 super(5) n/cm super(2) from either the 'DD' or 'DT' reaction. This requires only 10 super(10) n/p at a distance of 0.5m. DT neutron yields of approx.10 super(13) n/p are more appropriate for relatively opaque objects. The DT neutron is also better suited for biological radiography since the range of the 14.1MeV neutron is typically longer than the subject thickness. Neutron physics studies become accessible with instantaneous DT neutron flux densities of less than or approximate to 10 super(16)n/cm super(2)-s, achievable with total neutron yields of approx.10 super(14)n/p at 1m. Beyond these operational levels, 10 super(15)n/p DT provides the lower-level neutron yields, with a repetitively-pulsed machine, to begin radioisotope production for medical applications. Given total DT neutron yields of approx.10 super(16)n/p, one can begin to study fusion-driven fission systems with fissile multipliers of a few 10's as indicated by Teller (1991).
Summary form only given. The plasma focus device produces the smallest source size, highest instantaneous flux, pulsed neutron source of any fusion-reaction based system when it is operated in the high pressure mode. Specifically, the neutron emission region has been measured to be -1 cm long and /spl lsim/2 mm diameter. Neutron yields as high as /spl gsim/10/sup 12/ neutrons/pulse (n/p) have been produced from the D(D,n)/sup 3/He reaction (DD). The scaling of such yields to their equivalent D(T,n)/sup 4/He neutron (DT) yields by a factor of 80 to 100 has been demonstrated. The pulse width of these neutron yields is /spl lsim/100 ns, from many measurements, Therefore, the plasma focus can produce DD neutron yields of /spl gsim/10/sup 12/ n/p and DT neutron yields of /spl sim/10/sup 14/ n/p without any extension of this machine's demonstrated operating range. At the upper end of these yields, the DT reaction provides instantaneous fluxes of /spl gsim/10/sup 21/ n/s, neutron densities of /spl lsim/10/sup 9/ n/cm/sup 2/ at 1 m from the source, and instantaneous flux densities of /spl lsim/10/sup 16/ n/cm/sup 2/-s. Given these characteristics as a starting point, such a neutron source can be utilized for several applications within the presently recognized operating bounds of the plasma focus.
Author Fowler, C.M.
Freeman, B.L.
McDaniel, F.D.
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Snippet Summary form only given. The plasma focus device produces the smallest source size, highest instantaneous flux, pulsed neutron source of any fusion-reaction...
It is shown that a neutron source can be utilized for several applications within the presently recognized operating bounds of a plasma focus. With scaling,...
The plasma focus device produces the smallest source size, highest instantaneous flux, pulsed neutron source of any fusion-reaction based system when it is...
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StartPage 237
SubjectTerms 07 ISOTOPE AND RADIATION SOURCE TECHNOLOGY
70 PLASMA PHYSICS AND FUSION
Character recognition
FUSION YIELD
Helium
NEUTRON FLUX
NEUTRON SOURCES
Neutrons
Plasma applications
Plasma devices
PLASMA FOCUS DEVICES
Plasma measurements
Plasma sources
Pulse measurements
Radioactive decay
SCALING LAWS
Space vector pulse width modulation
USES
Title Applications for a neutron-emitting plasma focus
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