Conceptual designs of two petawatt-class pulsed-power accelerators for high-energy-density-physics experiments
We have developed conceptual designs of two petawatt-class pulsed-power accelerators: Z 300 and Z 800. The designs are based on an accelerator architecture that is founded on two concepts: single-stage electrical-pulse compression and impedance matching [Phys. Rev. ST Accel. Beams 10, 030401 (2007)]...
Main Authors: | , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , |
---|---|
Format: | Article |
Language: | English |
Published: |
American Physical Society
2015-11-01
|
Series: | Physical Review Special Topics. Accelerators and Beams |
Online Access: | http://doi.org/10.1103/PhysRevSTAB.18.110401 |
id |
doaj-7a73205ef98b4b91b353618da8ea4981 |
---|---|
record_format |
Article |
spelling |
doaj-7a73205ef98b4b91b353618da8ea49812020-11-25T00:11:01ZengAmerican Physical SocietyPhysical Review Special Topics. Accelerators and Beams1098-44022015-11-01181111040110.1103/PhysRevSTAB.18.110401Conceptual designs of two petawatt-class pulsed-power accelerators for high-energy-density-physics experimentsW. A. StygarT. J. AweJ. E. BaileyN. L. BennettE. W. BredenE. M. CampbellR. E. ClarkR. A. CooperM. E. CuneoJ. B. EnnisD. L. FehlT. C. GenoniM. R. GomezG. W. GreiserF. R. GrunerM. C. HerrmannB. T. HutselC. A. JenningsD. O. JobeB. M. JonesM. C. JonesP. A. JonesP. F. KnappJ. S. LashK. R. LeChienJ. J. LeckbeeR. J. LeeperS. A. LewisF. W. LongD. J. LuceroE. A. MadridM. R. MartinM. K. MatzenM. G. MazarakisR. D. McBrideG. R. McKeeC. L. MillerJ. K. MooreC. B. MostromT. D. MulvilleK. J. PetersonJ. L. PorterD. B. ReismanG. A. RochauG. E. RochauD. V. RoseD. C. RovangM. E. SavageM. E. SceifordP. F. SchmitR. F. SchneiderJ. SchwarzA. B. SefkowD. B. SinarsS. A. SlutzR. B. SpielmanB. S. StoltzfusC. ThomaR. A. VeseyP. E. WakelandD. R. WelchM. L. WisherJ. R. WoodworthWe have developed conceptual designs of two petawatt-class pulsed-power accelerators: Z 300 and Z 800. The designs are based on an accelerator architecture that is founded on two concepts: single-stage electrical-pulse compression and impedance matching [Phys. Rev. ST Accel. Beams 10, 030401 (2007)]. The prime power source of each machine consists of 90 linear-transformer-driver (LTD) modules. Each module comprises LTD cavities connected electrically in series, each of which is powered by 5-GW LTD bricks connected electrically in parallel. (A brick comprises a single switch and two capacitors in series.) Six water-insulated radial-transmission-line impedance transformers transport the power generated by the modules to a six-level vacuum-insulator stack. The stack serves as the accelerator’s water-vacuum interface. The stack is connected to six conical outer magnetically insulated vacuum transmission lines (MITLs), which are joined in parallel at a 10-cm radius by a triple-post-hole vacuum convolute. The convolute sums the electrical currents at the outputs of the six outer MITLs, and delivers the combined current to a single short inner MITL. The inner MITL transmits the combined current to the accelerator’s physics-package load. Z 300 is 35 m in diameter and stores 48 MJ of electrical energy in its LTD capacitors. The accelerator generates 320 TW of electrical power at the output of the LTD system, and delivers 48 MA in 154 ns to a magnetized-liner inertial-fusion (MagLIF) target [Phys. Plasmas 17, 056303 (2010)]. The peak electrical power at the MagLIF target is 870 TW, which is the highest power throughout the accelerator. Power amplification is accomplished by the centrally located vacuum section, which serves as an intermediate inductive-energy-storage device. The principal goal of Z 300 is to achieve thermonuclear ignition; i.e., a fusion yield that exceeds the energy transmitted by the accelerator to the liner. 2D magnetohydrodynamic (MHD) simulations suggest Z 300 will deliver 4.3 MJ to the liner, and achieve a yield on the order of 18 MJ. Z 800 is 52 m in diameter and stores 130 MJ. This accelerator generates 890 TW at the output of its LTD system, and delivers 65 MA in 113 ns to a MagLIF target. The peak electrical power at the MagLIF liner is 2500 TW. The principal goal of Z 800 is to achieve high-yield thermonuclear fusion; i.e., a yield that exceeds the energy initially stored by the accelerator’s capacitors. 2D MHD simulations suggest Z 800 will deliver 8.0 MJ to the liner, and achieve a yield on the order of 440 MJ. Z 300 and Z 800, or variations of these accelerators, will allow the international high-energy-density-physics community to conduct advanced inertial-confinement-fusion, radiation-physics, material-physics, and laboratory-astrophysics experiments over heretofore-inaccessible parameter regimes.http://doi.org/10.1103/PhysRevSTAB.18.110401 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
W. A. Stygar T. J. Awe J. E. Bailey N. L. Bennett E. W. Breden E. M. Campbell R. E. Clark R. A. Cooper M. E. Cuneo J. B. Ennis D. L. Fehl T. C. Genoni M. R. Gomez G. W. Greiser F. R. Gruner M. C. Herrmann B. T. Hutsel C. A. Jennings D. O. Jobe B. M. Jones M. C. Jones P. A. Jones P. F. Knapp J. S. Lash K. R. LeChien J. J. Leckbee R. J. Leeper S. A. Lewis F. W. Long D. J. Lucero E. A. Madrid M. R. Martin M. K. Matzen M. G. Mazarakis R. D. McBride G. R. McKee C. L. Miller J. K. Moore C. B. Mostrom T. D. Mulville K. J. Peterson J. L. Porter D. B. Reisman G. A. Rochau G. E. Rochau D. V. Rose D. C. Rovang M. E. Savage M. E. Sceiford P. F. Schmit R. F. Schneider J. Schwarz A. B. Sefkow D. B. Sinars S. A. Slutz R. B. Spielman B. S. Stoltzfus C. Thoma R. A. Vesey P. E. Wakeland D. R. Welch M. L. Wisher J. R. Woodworth |
spellingShingle |
W. A. Stygar T. J. Awe J. E. Bailey N. L. Bennett E. W. Breden E. M. Campbell R. E. Clark R. A. Cooper M. E. Cuneo J. B. Ennis D. L. Fehl T. C. Genoni M. R. Gomez G. W. Greiser F. R. Gruner M. C. Herrmann B. T. Hutsel C. A. Jennings D. O. Jobe B. M. Jones M. C. Jones P. A. Jones P. F. Knapp J. S. Lash K. R. LeChien J. J. Leckbee R. J. Leeper S. A. Lewis F. W. Long D. J. Lucero E. A. Madrid M. R. Martin M. K. Matzen M. G. Mazarakis R. D. McBride G. R. McKee C. L. Miller J. K. Moore C. B. Mostrom T. D. Mulville K. J. Peterson J. L. Porter D. B. Reisman G. A. Rochau G. E. Rochau D. V. Rose D. C. Rovang M. E. Savage M. E. Sceiford P. F. Schmit R. F. Schneider J. Schwarz A. B. Sefkow D. B. Sinars S. A. Slutz R. B. Spielman B. S. Stoltzfus C. Thoma R. A. Vesey P. E. Wakeland D. R. Welch M. L. Wisher J. R. Woodworth Conceptual designs of two petawatt-class pulsed-power accelerators for high-energy-density-physics experiments Physical Review Special Topics. Accelerators and Beams |
author_facet |
W. A. Stygar T. J. Awe J. E. Bailey N. L. Bennett E. W. Breden E. M. Campbell R. E. Clark R. A. Cooper M. E. Cuneo J. B. Ennis D. L. Fehl T. C. Genoni M. R. Gomez G. W. Greiser F. R. Gruner M. C. Herrmann B. T. Hutsel C. A. Jennings D. O. Jobe B. M. Jones M. C. Jones P. A. Jones P. F. Knapp J. S. Lash K. R. LeChien J. J. Leckbee R. J. Leeper S. A. Lewis F. W. Long D. J. Lucero E. A. Madrid M. R. Martin M. K. Matzen M. G. Mazarakis R. D. McBride G. R. McKee C. L. Miller J. K. Moore C. B. Mostrom T. D. Mulville K. J. Peterson J. L. Porter D. B. Reisman G. A. Rochau G. E. Rochau D. V. Rose D. C. Rovang M. E. Savage M. E. Sceiford P. F. Schmit R. F. Schneider J. Schwarz A. B. Sefkow D. B. Sinars S. A. Slutz R. B. Spielman B. S. Stoltzfus C. Thoma R. A. Vesey P. E. Wakeland D. R. Welch M. L. Wisher J. R. Woodworth |
author_sort |
W. A. Stygar |
title |
Conceptual designs of two petawatt-class pulsed-power accelerators for high-energy-density-physics experiments |
title_short |
Conceptual designs of two petawatt-class pulsed-power accelerators for high-energy-density-physics experiments |
title_full |
Conceptual designs of two petawatt-class pulsed-power accelerators for high-energy-density-physics experiments |
title_fullStr |
Conceptual designs of two petawatt-class pulsed-power accelerators for high-energy-density-physics experiments |
title_full_unstemmed |
Conceptual designs of two petawatt-class pulsed-power accelerators for high-energy-density-physics experiments |
title_sort |
conceptual designs of two petawatt-class pulsed-power accelerators for high-energy-density-physics experiments |
publisher |
American Physical Society |
series |
Physical Review Special Topics. Accelerators and Beams |
issn |
1098-4402 |
publishDate |
2015-11-01 |
description |
We have developed conceptual designs of two petawatt-class pulsed-power accelerators: Z 300 and Z 800. The designs are based on an accelerator architecture that is founded on two concepts: single-stage electrical-pulse compression and impedance matching [Phys. Rev. ST Accel. Beams 10, 030401 (2007)]. The prime power source of each machine consists of 90 linear-transformer-driver (LTD) modules. Each module comprises LTD cavities connected electrically in series, each of which is powered by 5-GW LTD bricks connected electrically in parallel. (A brick comprises a single switch and two capacitors in series.) Six water-insulated radial-transmission-line impedance transformers transport the power generated by the modules to a six-level vacuum-insulator stack. The stack serves as the accelerator’s water-vacuum interface. The stack is connected to six conical outer magnetically insulated vacuum transmission lines (MITLs), which are joined in parallel at a 10-cm radius by a triple-post-hole vacuum convolute. The convolute sums the electrical currents at the outputs of the six outer MITLs, and delivers the combined current to a single short inner MITL. The inner MITL transmits the combined current to the accelerator’s physics-package load. Z 300 is 35 m in diameter and stores 48 MJ of electrical energy in its LTD capacitors. The accelerator generates 320 TW of electrical power at the output of the LTD system, and delivers 48 MA in 154 ns to a magnetized-liner inertial-fusion (MagLIF) target [Phys. Plasmas 17, 056303 (2010)]. The peak electrical power at the MagLIF target is 870 TW, which is the highest power throughout the accelerator. Power amplification is accomplished by the centrally located vacuum section, which serves as an intermediate inductive-energy-storage device. The principal goal of Z 300 is to achieve thermonuclear ignition; i.e., a fusion yield that exceeds the energy transmitted by the accelerator to the liner. 2D magnetohydrodynamic (MHD) simulations suggest Z 300 will deliver 4.3 MJ to the liner, and achieve a yield on the order of 18 MJ. Z 800 is 52 m in diameter and stores 130 MJ. This accelerator generates 890 TW at the output of its LTD system, and delivers 65 MA in 113 ns to a MagLIF target. The peak electrical power at the MagLIF liner is 2500 TW. The principal goal of Z 800 is to achieve high-yield thermonuclear fusion; i.e., a yield that exceeds the energy initially stored by the accelerator’s capacitors. 2D MHD simulations suggest Z 800 will deliver 8.0 MJ to the liner, and achieve a yield on the order of 440 MJ. Z 300 and Z 800, or variations of these accelerators, will allow the international high-energy-density-physics community to conduct advanced inertial-confinement-fusion, radiation-physics, material-physics, and laboratory-astrophysics experiments over heretofore-inaccessible parameter regimes. |
url |
http://doi.org/10.1103/PhysRevSTAB.18.110401 |
work_keys_str_mv |
AT wastygar conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT tjawe conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT jebailey conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT nlbennett conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT ewbreden conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT emcampbell conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT reclark conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT racooper conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT mecuneo conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT jbennis conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT dlfehl conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT tcgenoni conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT mrgomez conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT gwgreiser conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT frgruner conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT mcherrmann conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT bthutsel conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT cajennings conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT dojobe conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT bmjones conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT mcjones conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT pajones conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT pfknapp conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT jslash conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT krlechien conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT jjleckbee conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT rjleeper conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT salewis conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT fwlong conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT djlucero conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT eamadrid conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT mrmartin conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT mkmatzen conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT mgmazarakis conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT rdmcbride conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT grmckee conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT clmiller conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT jkmoore conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT cbmostrom conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT tdmulville conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT kjpeterson conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT jlporter conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT dbreisman conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT garochau conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT gerochau conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT dvrose conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT dcrovang conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT mesavage conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT mesceiford conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT pfschmit conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT rfschneider conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT jschwarz conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT absefkow conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT dbsinars conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT saslutz conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT rbspielman conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT bsstoltzfus conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT cthoma conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT ravesey conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT pewakeland conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT drwelch conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT mlwisher conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments AT jrwoodworth conceptualdesignsoftwopetawattclasspulsedpoweracceleratorsforhighenergydensityphysicsexperiments |
_version_ |
1725405584215244800 |