FRX-L: A field-reversed configuration plasma injector for magnetized target fusion
We describe the experiment and technology leading to a target plasma for the magnetized target fusion research effort, an approach to fusion wherein a plasma with embedded magnetic fields is formed and subsequently adiabatically compressed to fusion conditions. The target plasmas under consideration...
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| Veröffentlicht in: | Review of scientific instruments 2003-10, Vol.74 (10), p.4314-4323 |
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| creator | Taccetti, J. M. Intrator, T. P. Wurden, G. A. Zhang, S. Y. Aragonez, R. Assmus, P. N. Bass, C. M. Carey, C. deVries, S. A. Fienup, W. J. Furno, I. Hsu, S. C. Kozar, M. P. Langner, M. C. Liang, J. Maqueda, R. J. Martinez, R. A. Sanchez, P. G. Schoenberg, K. F. Scott, K. J. Siemon, R. E. Tejero, E. M. Trask, E. H. Tuszewski, M. Waganaar, W. J. Grabowski, C. Ruden, E. L. Degnan, J. H. Cavazos, T. Gale, D. G. Sommars, W. |
| description | We describe the experiment and technology leading to a target plasma for the magnetized target fusion research effort, an approach to fusion wherein a plasma with embedded magnetic fields is formed and subsequently adiabatically compressed to fusion conditions. The target plasmas under consideration, field-reversed configurations (FRCs), have the required closed-field-line topology and are translatable and compressible. Our goal is to form high-density
(10
17
cm
−3
)
FRCs on the field-reversed experiment-liner (FRX-L) device, inside a 36 cm long, 6.2 cm radius theta coil, with 5 T peak magnetic field and an azimuthal electric field as high as 1 kV/cm. FRCs have been formed with an equilibrium density
n
e
≈(1
to
2)×10
16
cm
−3
,
T
e
+T
i
≈250
eV
,
and excluded flux ≈2 to 3 mWb. |
| doi_str_mv | 10.1063/1.1606534 |
| format | Article |
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(10
17
cm
−3
)
FRCs on the field-reversed experiment-liner (FRX-L) device, inside a 36 cm long, 6.2 cm radius theta coil, with 5 T peak magnetic field and an azimuthal electric field as high as 1 kV/cm. FRCs have been formed with an equilibrium density
n
e
≈(1
to
2)×10
16
cm
−3
,
T
e
+T
i
≈250
eV
,
and excluded flux ≈2 to 3 mWb.</description><identifier>ISSN: 0034-6748</identifier><identifier>EISSN: 1089-7623</identifier><identifier>DOI: 10.1063/1.1606534</identifier><identifier>CODEN: RSINAK</identifier><language>eng</language><ispartof>Review of scientific instruments, 2003-10, Vol.74 (10), p.4314-4323</ispartof><rights>American Institute of Physics</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c363t-590b1c82ef349bbf15d712c7ce1d8a9b7cfdbe715555078c5bad869d4273845e3</citedby><cites>FETCH-LOGICAL-c363t-590b1c82ef349bbf15d712c7ce1d8a9b7cfdbe715555078c5bad869d4273845e3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://pubs.aip.org/rsi/article-lookup/doi/10.1063/1.1606534$$EHTML$$P50$$Gscitation$$H</linktohtml><link.rule.ids>314,776,780,790,1553,4498,27901,27902,76126,76132</link.rule.ids></links><search><creatorcontrib>Taccetti, J. M.</creatorcontrib><creatorcontrib>Intrator, T. P.</creatorcontrib><creatorcontrib>Wurden, G. A.</creatorcontrib><creatorcontrib>Zhang, S. Y.</creatorcontrib><creatorcontrib>Aragonez, R.</creatorcontrib><creatorcontrib>Assmus, P. N.</creatorcontrib><creatorcontrib>Bass, C. M.</creatorcontrib><creatorcontrib>Carey, C.</creatorcontrib><creatorcontrib>deVries, S. A.</creatorcontrib><creatorcontrib>Fienup, W. J.</creatorcontrib><creatorcontrib>Furno, I.</creatorcontrib><creatorcontrib>Hsu, S. C.</creatorcontrib><creatorcontrib>Kozar, M. P.</creatorcontrib><creatorcontrib>Langner, M. C.</creatorcontrib><creatorcontrib>Liang, J.</creatorcontrib><creatorcontrib>Maqueda, R. J.</creatorcontrib><creatorcontrib>Martinez, R. A.</creatorcontrib><creatorcontrib>Sanchez, P. G.</creatorcontrib><creatorcontrib>Schoenberg, K. F.</creatorcontrib><creatorcontrib>Scott, K. J.</creatorcontrib><creatorcontrib>Siemon, R. E.</creatorcontrib><creatorcontrib>Tejero, E. M.</creatorcontrib><creatorcontrib>Trask, E. H.</creatorcontrib><creatorcontrib>Tuszewski, M.</creatorcontrib><creatorcontrib>Waganaar, W. J.</creatorcontrib><creatorcontrib>Grabowski, C.</creatorcontrib><creatorcontrib>Ruden, E. L.</creatorcontrib><creatorcontrib>Degnan, J. H.</creatorcontrib><creatorcontrib>Cavazos, T.</creatorcontrib><creatorcontrib>Gale, D. G.</creatorcontrib><creatorcontrib>Sommars, W.</creatorcontrib><title>FRX-L: A field-reversed configuration plasma injector for magnetized target fusion</title><title>Review of scientific instruments</title><description>We describe the experiment and technology leading to a target plasma for the magnetized target fusion research effort, an approach to fusion wherein a plasma with embedded magnetic fields is formed and subsequently adiabatically compressed to fusion conditions. The target plasmas under consideration, field-reversed configurations (FRCs), have the required closed-field-line topology and are translatable and compressible. Our goal is to form high-density
(10
17
cm
−3
)
FRCs on the field-reversed experiment-liner (FRX-L) device, inside a 36 cm long, 6.2 cm radius theta coil, with 5 T peak magnetic field and an azimuthal electric field as high as 1 kV/cm. FRCs have been formed with an equilibrium density
n
e
≈(1
to
2)×10
16
cm
−3
,
T
e
+T
i
≈250
eV
,
and excluded flux ≈2 to 3 mWb.</description><issn>0034-6748</issn><issn>1089-7623</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2003</creationdate><recordtype>article</recordtype><recordid>eNqd0E1LAzEQBuAgCtbqwX-Qq0JqZrP5WG-lWBUWhKLgbcnmo6S0uyVJC_rru9qCd18Y5vIwMC9Ct0AnQAV7gAkIKjgrz9AIqKqIFAU7RyNKWUmELNUlukppRYdwgBFazBefpH7EU-yDW1sS3d7F5Cw2fefDchd1Dn2Ht2udNhqHbuVM7iP2w2z0snM5fA8467h0GftdGvA1uvB6ndzNaY_Rx_zpffZC6rfn19m0JoYJlgmvaAtGFc6zsmpbD9xKKIw0DqzSVSuNt62TwIdQqQxvtVWismUhmSq5Y2N0d7xrYp9SdL7ZxrDR8asB2vyU0UBzKmOw90ebTMi_L_0P7_v4B5ut9ewA5RRt4w</recordid><startdate>200310</startdate><enddate>200310</enddate><creator>Taccetti, J. M.</creator><creator>Intrator, T. P.</creator><creator>Wurden, G. A.</creator><creator>Zhang, S. Y.</creator><creator>Aragonez, R.</creator><creator>Assmus, P. N.</creator><creator>Bass, C. M.</creator><creator>Carey, C.</creator><creator>deVries, S. A.</creator><creator>Fienup, W. 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H.</au><au>Cavazos, T.</au><au>Gale, D. G.</au><au>Sommars, W.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>FRX-L: A field-reversed configuration plasma injector for magnetized target fusion</atitle><jtitle>Review of scientific instruments</jtitle><date>2003-10</date><risdate>2003</risdate><volume>74</volume><issue>10</issue><spage>4314</spage><epage>4323</epage><pages>4314-4323</pages><issn>0034-6748</issn><eissn>1089-7623</eissn><coden>RSINAK</coden><abstract>We describe the experiment and technology leading to a target plasma for the magnetized target fusion research effort, an approach to fusion wherein a plasma with embedded magnetic fields is formed and subsequently adiabatically compressed to fusion conditions. The target plasmas under consideration, field-reversed configurations (FRCs), have the required closed-field-line topology and are translatable and compressible. Our goal is to form high-density
(10
17
cm
−3
)
FRCs on the field-reversed experiment-liner (FRX-L) device, inside a 36 cm long, 6.2 cm radius theta coil, with 5 T peak magnetic field and an azimuthal electric field as high as 1 kV/cm. FRCs have been formed with an equilibrium density
n
e
≈(1
to
2)×10
16
cm
−3
,
T
e
+T
i
≈250
eV
,
and excluded flux ≈2 to 3 mWb.</abstract><doi>10.1063/1.1606534</doi><tpages>10</tpages></addata></record> |
| fulltext | fulltext |
| identifier | ISSN: 0034-6748 |
| ispartof | Review of scientific instruments, 2003-10, Vol.74 (10), p.4314-4323 |
| issn | 0034-6748 1089-7623 |
| language | eng |
| recordid | cdi_crossref_primary_10_1063_1_1606534 |
| source | AIP Journals Complete; AIP Digital Archive |
| title | FRX-L: A field-reversed configuration plasma injector for magnetized target fusion |
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