Concepts for an affordable high current imploding plasma generator

Sincerny, P.; Danforth, M.; Gilbert, C.; Miller, A.R.; Naff, T.; Rix, W.; Stallings, C.; Waisman, E.; Schlitt, L.

doi:10.1109/ppc.1999.825515

Cited by 13 publications

(13 citation statements)

References 11 publications

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“…1 are one of the most distinguishing features of the accelerator architecture described in this article. The transformers offer the follow-ing advantages over previous approaches to the design of a high-current z-pinch accelerator [60,[69][70][71][72][73][74][75][76][77][78][79].…”

Section: A Descriptionmentioning

confidence: 99%

“…A number of architectures have been proposed in the literature for the design of future pulsed-power z-pinch drivers [60,[69][70][71][72][73][74][75][76][77][78][79]. In this article, we describe an architecture that was motivated by, and builds upon, the previous designs.…”

Section: Introductionmentioning

confidence: 99%

“…The combination of the above 15 features distinguishes this architecture from the accelerator designs presented in Refs. [60,[69][70][71][72][73][74][75][76][77][78][79].…”

Section: Introductionmentioning

confidence: 99%

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Architecture of petawatt-classz-pinch accelerators

Stygar

Cuneo

Headley³

et al. 2007

Phys. Rev. ST Accel. Beams

211

128

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We have developed an accelerator architecture that can serve as the basis of the design of petawatt-class z-pinch drivers. The architecture has been applied to the design of two z-pinch accelerators, each of which can be contained within a 104-m-diameter cylindrical tank. One accelerator is driven by slow ( 1 s) Marx generators, which are a mature technology but which necessitate significant pulse compression to achieve the short pulses ( 1 s) required to drive z pinches. The other is powered by linear transformer drivers (LTDs), which are less mature but produce much shorter pulses than conventional Marxes. Consequently, an LTD-driven accelerator promises to be (at a given pinch current and implosion time) more efficient and reliable. The Marx-driven accelerator produces a peak electrical power of 500 TW and includes the following components: (i) 300 Marx generators that comprise a total of 1:8 10 4 capacitors, store 98 MJ, and erect to 5 MV; (ii) 600 water-dielectric triplate intermediate-store transmission lines, which also serve as pulse-forming lines; (iii) 600 5-MV laser-triggered gas switches; (iv) three monolithic radial-transmission-line impedance transformers, with triplate geometries and exponential impedance profiles; (v) a 6-level 5.5-m-diameter 15-MV vacuum insulator stack; (vi) six magnetically insulated vacuum transmission lines (MITLs); and (vii) a triple-post-hole vacuum convolute that adds the output currents of the six MITLs, and delivers the combined current to a z-pinch load. The accelerator delivers an effective peak current of 52 MA to a 10-mm-length z pinch that implodes in 95 ns, and 57 MA to a pinch that implodes in 120 ns. The LTD-driven accelerator includes monolithic radial transformers and a MITL system similar to those described above, but does not include intermediate-store transmission lines, multimegavolt gas switches, or a laser trigger system. Instead, this accelerator is driven by 210 LTD modules that include a total of 1 10 6 capacitors and 5 10 5 200-kV electrically triggered gas switches. The LTD accelerator stores 182 MJ and produces a peak electrical power of 1000 TW. The accelerator delivers an effective peak current of 68 MA to a pinch that implodes in 95 ns, and 75 MA to a pinch that implodes in 120 ns. Conceptually straightforward upgrades to these designs would deliver even higher pinch currents and faster implosions.

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Section: A Descriptionmentioning

confidence: 99%

Section: Introductionmentioning

confidence: 99%

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Architecture of petawatt-classz-pinch accelerators

Stygar

Cuneo

Headley³

et al. 2007

Phys. Rev. ST Accel. Beams

211

128

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“…For this reason we simply use a 0.8 safety factor to obtain Eqs. (4) and (10)- (14). Applying this approach to obtain Eqs.…”

Section: Referencementioning

confidence: 99%

“…Large-area water-insulated electrical components are often incorporated in the designs of multiterawatt pulsedpower accelerators, such as the Z [1-10] and ZR [11] machines. Water-insulated components are also proposed for use in future accelerators [12][13][14][15][16][17][18][19]. Optimizing the design of such an accelerator requires a knowledge of the conditions under which its water-insulated components can be operated reliably.…”

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confidence: 99%

Dielectric-breakdown tests of water at 6 MV

Stygar

Savage

Wagoner

et al. 2009

Phys. Rev. ST Accel. Beams

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We have conducted dielectric-breakdown tests on water subject to a single unipolar pulse. The peak voltages used for the tests range from 5.8 to 6.8 MV; the effective pulse widths range from 0.60 to 1:1 s; and the effective areas tested range from 1:8 Â 10 5 to 3:6 Â 10 6 cm 2 . The tests were conducted on waterinsulated coaxial capacitors. Large-area water-insulated electrical components are often incorporated in the designs of multiterawatt pulsedpower accelerators, such as the Z [1-10] and ZR [11] machines. Water-insulated components are also proposed for use in future accelerators [12][13][14][15][16][17][18][19]. Optimizing the design of such an accelerator requires a knowledge of the conditions under which its water-insulated components can be operated reliably.Reference [20] proposes that the characteristic time delay delay between the application of a voltage to a water-insulated anode-cathode gap, and the completion of dielectric failure of that gap, can be approximated as follows:In this expression stat is the statistical component of the delay time; i.e., the characteristic time between the application of the voltage and the appearance of free electrons and ions that initiate the formation of streamers in the water. We define form to be the formative component: the time required for the streamers to propagate across the gap and evolve sufficiently to produce complete dielectric failure.To inhibit electrical breakdown, water-insulated components are usually designed to produce a nominally uniform electric field over most of the component's area. We assume that, when the area of a water-insulated system with a uniform field is sufficiently large, the appearance of free electrons and ions necessary to initiate a breakdown occurs somewhere in the system very early in the voltage pulse [20]. Under this condition the statistical time delay stat can be neglected, and the breakdown delay is dominated by its formative component:In principle, dielectric breakdown dominated by the formative component can be studied with an electrode geometry that consists of a point anode and a planar cathode [20][21][22]. Although measurements with an infinitely field-enhanced anode point and an infinitely extended flat cathode are not possible, a number of dielectric-breakdown measurements between a significantly field-enhanced anode electrode and a less-enhanced cathode have been described in the literature.Using these measurements, Ref.[20] finds that complete dielectric failure is likely to occur in water between a fieldenhanced anode and a less-enhanced cathode when In this expression E p V p =d is the peak value in time of the spatially averaged electric field between the anode and cathode (in MV=cm, where V p is the peak voltage difference and d is the minimum distance between the electrodes), and eff is the temporal width (in s) of the voltage pulse at 63% of peak. This relation is based on 25 measurements for which 1 V p 4:10 MV, 1:25 d 22 cm, and 0:011 eff 0:6 s.To develop a tentative design criterion for a large-area...

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