View source for Z Pulsed Power Facility

{{Update|date=April 2022}}{{short description|World's largest pulsed power facility}}
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[[File:The Z Machine (8056998596).jpg|thumb|Overhead view from a [[fisheye lens]] of the Z machine at Sandia National Laboratory. Due to the extremely [[high voltage]], the power feeding equipment is submerged in concentric chambers of 2 megalitres (2,000 m³) of [[transformer oil]] and 2.3 megalitres (2,300 m³) of [[deionized water]], which act as [[Electrical insulation|insulator]]s. Nevertheless, the [[electromagnetic pulse]] when the machine is discharged causes impressive lightning, referred to as a "flashover", which can be seen around many of the metallic objects in the machine.]]

[[File:Z machine cross section.jpg|thumb|Z machine cross section]]
[[File:Z machine diagram.jpg|thumb|Z machine diagram]]
The '''Z Pulsed Power Facility''', informally known as the '''Z machine''' or simply '''Z''',<ref>{{cite news |last1=Stein |first1=Ben |title=The Con-Artist Physics of "Ocean's Eleven" |url=https://www.aps.org/publications/apsnews/200203/oceans-eleven.cfm#:~:text=In%20the%20film%2C%20eleven%20con,grid%20for%20a%20few%20moments. |access-date=28 July 2020 |work=APS News |issue=3 |date=March 2002|volume=11 }}</ref> is the largest high frequency [[electromagnetic wave]] generator in the world, operated by [[Sandia National Laboratories]] in [[Albuquerque, New Mexico]].

It has primarily been used as an [[inertial confinement fusion]] (ICF) research facility, including the [[magnetized liner inertial fusion]] (MagLIF) approach, and for testing materials in conditions of extreme temperature and pressure.
In particular, it gathers data to aid in [[computer modeling]] of [[nuclear weapon]]s and eventual [[Fusion power|fusion pulsed power plants]].

==History==
{{see also|Fusion power#History of research}}
The Z machine's origins can be traced to the [[United States Department of Energy|Department of Energy]] (DoE) needing to replicate the [[Nuclear fusion|fusion reactions]] of a [[Thermonuclear weapon|thermonuclear bomb]] in a lab environment to better understand the physics involved.
Since the 1970s, the DoE has also been looking into ways to [[fusion power|generate electricity from fusion reactions]].

The first research at Sandia, headed by Gerold Yonas<ref>{{YouTube|Rd2P4Mvj7vw}}</ref><ref>{{cite web |url=http://www.bnsl.org/Documents/GerryYonas_shortbio.pdf |title=Gerry Yonas : Resume |publisher=Bnsl.org |access-date=2015-06-20 |url-status=dead |archive-url=https://web.archive.org/web/20150620231327/http://www.bnsl.org/Documents/GerryYonas_shortbio.pdf |archive-date=2015-06-20 }}</ref> – the particle-beam fusion program – dates back to 1971.<ref>{{cite book |title=Particle beam fusion program publications and related reports, January 1971 to July 1979 (Book, 1979) |publisher=WorldCat.org |date=2015-05-02 |isbn=9780553589955 |oclc = 079670227}}</ref> This program tried to generate fusion by compressing fuel with beams of charged particles. Electrons were the first particles to be thought of, because the pulsed power accelerators at the time had already concentrated them at high power in small areas. However, shortly thereafter it was realized that electrons can not possibly heat the fusion fuel rapidly enough for the purpose. The program then moved away from electrons in favor of protons. These turned out to be too light to control well enough to concentrate onto a target, and the program moved on to light ions, lithium. The accelerators names reflect the change in emphasis: first
the accelerator's name was EBFA-I (electron beam fusion accelerator), shortly thereafter PBFA-I, which became Saturn. Protons demanded another accelerator, PBFA-II, which became Z.

The November 1978 issue of ''[[Scientific American]]'' carried Yonas' first general-public article, "Fusion power with particle beams".<ref>{{cite journal|title=Fusion power with particle beams |journal=[[Scientific American]] |volume=239 |issue=5 |pages=50–61 |publisher=Adsabs.harvard.edu |bibcode=1978SciAm.239e..50Y|last1=Yonas |first1=G. |year=1978 |doi=10.1038/scientificamerican1178-50 }}</ref>

In 1985, the PBFA-II was created.<ref>{{cite web |url=http://www.sandia.gov/media/saturn.htm |title=Saturn News Release |publisher=Sandia.gov |access-date=2015-06-20 |archive-url=https://web.archive.org/web/20150924094201/http://www.sandia.gov/media/saturn.htm |archive-date=2015-09-24 |url-status=live }}</ref><ref>{{Cite conference| publisher = EG and G, Inc., Albuquerque, NM (USA)| last = Harrison| first = J. L.| title = PBFA control and monitor system| access-date = 2024-10-20| date = 1979-10-01| url = https://www.osti.gov/biblio/5700471}}</ref> Sandia continued to target heavy ion fusion at a slow pace despite the National Academies report.

Meanwhile, defense-related research was also ongoing at Sandia with the Hermes III machine and Saturn (1987), upgraded from PBFA-I, which operated at lower total power than PBFA-II but advanced Sandia's knowledge in high voltage and high current and was therefore a useful predecessor to the Z machine.

Also in 1996, the PBFA-II machine was once again upgraded<ref>{{Cite conference| publisher = Sandia National Lab. (SNL-NM), Albuquerque, NM (United States)| last1 = Spielman| first1 = R. B.| last2 = Breeze| first2 = S. F.| last3 = Deeney| first3 = C.| title = PBFA Z: A 20-MA z-pinch driver for plasma radiation sources| access-date = 2024-10-20| date = 1996-07-01| url = https://www.osti.gov/biblio/251439}}</ref> into PBFA-Z<ref name="sandia.gov">{{cite web |url=http://www.sandia.gov/media/zpinch.htm |title=Sandia National Laboratories - News Releases |publisher=Sandia.gov |access-date=2015-06-20 |archive-url=https://web.archive.org/web/20150609044428/http://www.sandia.gov/media/zpinch.htm |archive-date=2015-06-09 |url-status=live }}</ref> or simply "Z machine", described for the first time to the general public in August 1998 in ''Scientific American''.<ref>{{cite web |url=http://www.pescadoo.net/malc/art-6.htm |title=Fusion nucléaire et striction axiale. Pour la Science - février 1998 |website=www.pescadoo.net |access-date=17 January 2022 |archive-url=https://web.archive.org/web/20121004233022/http://www.pescadoo.net/malc/art-6.htm |archive-date=4 October 2012 |url-status=dead}}</ref>

==Physics of the Z machine==
[[File:MagLIF cartoon.svg|thumb|400px|The stages of a typical MagLIF implosion at Z.{{ordered list
| A laser preheats the fuel.
| An axial current is driven through the liner.
| The current induces an azimuthal magnetic field.
| The magnetic force implodes the liner, compressing and further heating the fuel.}}]]

The Z machine uses the well known principle of [[Z-pinch]] to produce hot short-lived plasmas. The plasma can be used as a source of x-rays, as a surrogate for the inside of a thermonuclear weapon, or as a surrogate for the core of a fusion power plant.

In a Z-pinch, the fast discharge of current through a column of plasma causes it to be compressed towards its axis by the resulting [[Lorentz force]]s, thus heating it. [[Willard Harrison Bennett]] successfully researched the application of Z-pinches to plasma compression. The Z machine layout is cylindrical. On the outside it houses huge [[capacitor]]s discharging through [[Marx generator]]s which generate a one microsecond high-voltage pulse. This pulse is then compressed by a factor of 10 to enable the creation of 100&nbsp;ns discharges.

Most experiments on the Z machine run the current discharge through a conductive tube (called a ''liner'') filled with gas. This approach is known as [[magnetized liner inertial fusion]], or MagLIF. The compression of a MagLIF Z-pinch is limited because the current flow is highly unstable and rotates along the cylinder which causes twisting of the imploding tube therefore decreasing the quality of the compression.

The Z machine has also conducted experiments with arrays of tungsten wires rather than liners. The space inside the wire array was filled with polystyrene, which helps homogenize the X-ray flux. By removing the polystyrene core, Sandia was able to obtain a thin 1.5&nbsp;mm plasma cord in which 10 million amperes flowed with 90 megabars of pressure.{{citation needed|date=December 2018}}

==Early operation 1996–2006==
The key attributes of Sandia's Z machine<ref>{{cite web |url=http://www.sandia.gov/media/zmachine.htm |title=Sandia National Laboratories - News Releases |publisher=Sandia.gov |access-date=2015-06-20 |archive-url=https://web.archive.org/web/20150609044423/http://www.sandia.gov/media/zmachine.htm |archive-date=2015-06-09 |url-status=live }}</ref> are its 18 million amperes of current and a discharge time of less than 100 [[second|nanoseconds]]. This current discharge was initially run through an array of [[tungsten]] wires.<ref>{{cite web |url=http://www.sandia.gov/media/z290.htm |title=Sandia Z accelerator |publisher=Sandia.gov |access-date=2015-06-20 |archive-url=https://web.archive.org/web/20150428231250/http://www.sandia.gov/media/z290.htm |archive-date=2015-04-28 |url-status=live }}</ref>
In 1999, Sandia tested the idea of nested wire arrays;<ref>{{cite web |url=http://www.sandia.gov/media/NewsRel/NR1999/zmach.htm |title=News Release - Z machine |publisher=Sandia.gov |access-date=2015-06-20 |archive-url=https://web.archive.org/web/20150607033045/http://www.sandia.gov/media/NewsRel/NR1999/zmach.htm |archive-date=2015-06-07 |url-status=live }}</ref> the second array, out of phase with the first, compensates for [[Rayleigh-Taylor instabilities]].
In 2001, Sandia introduced the Z-Beamlet laser (from surplus equipment of the [[National Ignition Facility]]) as a tool to better image the compressing pellet.<ref>{{cite web |author=Neal Singer |url=http://www.sandia.gov/media/NewsRel/NR2001/Zbeam.htm |title=News Release - Z-Beamlet |publisher=Sandia.gov |access-date=2015-06-20 |archive-url=https://web.archive.org/web/20150924094139/http://www.sandia.gov/media/NewsRel/NR2001/Zbeam.htm |archive-date=2015-09-24 |url-status=live }}</ref>  This confirmed the shaping uniformity of pellets compressed by the Z machine.

In 1999, Sandia started the Z-IFE project,<ref>{{cite web |url=http://fire.pppl.gov/fpa05_olson.pdf |title=Z-Pinch Inertial Fusion Energy |publisher=Fire.pppl.gov |access-date=2015-06-20 |archive-url=https://web.archive.org/web/20160303195515/http://fire.pppl.gov/fpa05_olson.pdf |archive-date=2016-03-03 |url-status=live }}</ref> which aimed to solve the practical difficulties in harnessing fusion power. Major problems included producing energy in a single Z-pinch shot, and quickly reloading the reactor after each shot. By their early estimates, an implosion of a fuel capsule every 10 seconds could economically produce 300&nbsp;MW of fusion energy.

Sandia announced the fusing of small amounts of [[deuterium]] in the Z machine on April 7, 2003.<ref>{{cite web |url=http://www.sandia.gov/news-center/news-releases/2003/nuclear-power/Zneutrons.html |title=Sandia National Laboratories — News Release — Z produces fusion neutrons |website=www.sandia.gov |access-date=17 January 2022 |archive-url=https://web.archive.org/web/20030603190249/http://www.sandia.gov/news-center/news-releases/2003/nuclear-power/Zneutrons.html |archive-date=3 June 2003 |url-status=dead}}</ref>

Besides being used as an X-ray generator, the Z machine propelled small plates at 34 kilometers a second, faster than the 30 kilometers per second that Earth travels in its orbit around the [[Sun]], and four times [[escape velocity|Earth's escape velocity]] (3 times it at sea level).<ref>{{cite web |url=https://share.sandia.gov/news/resources/releases/2005/nuclear-power/z-saturn.html |title=Sandia National Labs: News: Title |publisher=Share.sandia.gov |date=2005-06-06 |access-date=2015-06-20 |archive-url=https://web.archive.org/web/20160304040225/https://share.sandia.gov/news/resources/releases/2005/nuclear-power/z-saturn.html |archive-date=2016-03-04 |url-status=live }}</ref> It also successfully created a special, hyperdense "hot ice" known as [[ice VII]], by quickly compressing water to pressures of 70,000 to 120,000 [[Atmosphere (unit)|atmospheres]] (7 to 12 [[gigapascal|GPa]]).<ref>{{cite web |url=http://www.sandia.gov/news/resources/releases/2007/z-ice.html |title=Ice created in nanoseconds by Sandia's Z machine - March 15, 2007 |publisher=Sandia.gov |date=2007-03-15 |access-date=2015-06-20 |archive-url=https://web.archive.org/web/20111017135615/http://sandia.gov/news/resources/releases/2007/z-ice.html |archive-date=2011-10-17 |url-status=live }}</ref> Mechanical shock from impacting Z-machine accelerated projectiles is able to melt diamonds.<ref>{{cite web |url=https://share.sandia.gov/news/resources/releases/2006/diamonds.html |title=Z machine melts diamond to puddle |publisher=Share.sandia.gov |date=2006-11-02 |access-date=2015-06-20 |archive-url=https://web.archive.org/web/20160304031129/https://share.sandia.gov/news/resources/releases/2006/diamonds.html |archive-date=2016-03-04 |url-status=live }}</ref>

During this period the power of X-ray produced jumped from 10 to 300TW.<ref>{{cite web |url=http://www.sandia.gov/media/images/jpg/Z03.jpg |format=PDF |title=Pulsed Power Graph |publisher=Sandia.gov |access-date=2015-06-20 |archive-url=https://web.archive.org/web/20150924094156/http://www.sandia.gov/media/images/jpg/Z03.jpg |archive-date=2015-09-24 |url-status=live }}</ref> In order to target the next milestone of fusion breakeven, another upgrade was then necessary<ref>{{cite web |url=https://share.sandia.gov/news/resources/releases/2004/physics-astron/Z-R.html |title=Z's $61.7 million refurbishment to advance fusion machine's capabilities |publisher=Share.sandia.gov |access-date=2015-06-20 |archive-url=https://web.archive.org/web/20160304083952/https://share.sandia.gov/news/resources/releases/2004/physics-astron/Z-R.html |archive-date=2016-03-04 |url-status=live }}</ref>

== After refurbishment (2007–) ==
[[Image:Petawatt LTD z pinch.png|thumb|right|Proposed model of a 1 petawatt LTD-based z-pinch accelerator.<br /> 104 m diameter, 70 megaamperes, 24 megavolts.]]
A $60 million (raised to $90 million) retrofit program called ZR (Z Refurbished) was announced in 2004 to increase its power by 50%. The Z machine was dismantled in July 2006 for this upgrade, including the installation of newly designed hardware and components and more powerful [[Marx generator]]s. The deionized water section of the machine has been reduced to about half the previous size while the oil section has been expanded significantly in order to house larger intermediate storage lines (i-stores) and new laser towers, which used to sit in the water section. The refurbishment was completed in October 2007.<ref>{{cite web |url=http://www.sandia.gov/news/resources/releases/2007/zaccelerator.html |title=Successful 'shots' signal re-opening of Sandia's giant Z accelerator - October 17, 2007 |publisher=Sandia.gov |date=2007-10-17 |access-date=2015-06-20 |archive-url=https://web.archive.org/web/20100402210006/http://www.sandia.gov/news/resources/releases/2007/zaccelerator.html |archive-date=2010-04-02 |url-status=live }}</ref>
The newer Z machine can now shoot around 26 million amperes<ref name="sandia">{{cite web|url=http://www.sandia.gov/z-machine/about_z/index.html|title=About Z|publisher=Sandia National Laboratories|access-date=30 October 2016|archive-url=https://web.archive.org/web/20161030142206/http://www.sandia.gov/z-machine/about_z/index.html|archive-date=2016-10-30|url-status=live}}</ref> (instead of 18 million amperes previously) in 95 nanoseconds. The radiated power has been raised to 350 terawatts and the X-ray energy output to 2.7 [[megajoule]]s. In 2006 wire array experiments reach ultra-high temperatures (2.66 to 3.7 billion kelvins).<ref>{{cite journal |first1=M. G. |last1=Haines |first2=P. D. |last2=LePell |first3=C. A. |last3=Coverdale |first4=B. |last4=Jones |first5=C. |last5=Deeney |first6=J. P. |last6=Apruzese |title=Ion viscous heating in a magnetohydrodynamically unstable Z pinch at over 2×10^9 Kelvin |journal=Physical Review Letters |date=2006-03-23 |volume=96 |page=075003 |doi=10.1103/PhysRevLett.96.075003 |url=https://journals.aps.org/prl/abstract/10.1103/PhysRevLett.96.075003 |access-date=18 October 2024}}</ref>

Sandia's roadmap for the future includes another Z machine version called ZN (Z Neutron) to test higher yields in fusion power and automation systems. ZN is planned to give between 20 and 30 MJ of hydrogen fusion power with a shot per hour using a Russian [[Linear Transformer Driver]] (LTD) replacing the current Marx generators.<ref>{{cite web |url=http://www.sandia.gov/LabNews/070427.html |title=Sandia National Labs: News: Publications: Sandia Lab News: April 27, 2007 |publisher=Sandia.gov |date=2007-04-27 |access-date=2015-06-20 |archive-url=https://web.archive.org/web/20150924093956/http://www.sandia.gov/LabNews/070427.html |archive-date=2015-09-24 |url-status=live }}</ref> After 8 to 10 years of operation, ZN would become a transmutation pilot plant capable of a fusion shot every 100 seconds.<ref>{{cite web |url=https://prod-ng.sandia.gov/techlib-noauth/access-control.cgi/2006/067148.pdf |title=Z-Inertial Fusion Energy : Power Plant Final Report FY 2006 |publisher=Sandia National Laboratories |access-date=2020-11-22 }}</ref>

The next step planned would be the Z-IFE (Z-inertial fusion energy) test facility, the first true z-pinch driven prototype fusion power plant. It is suggested it would integrate Sandia's latest designs using LTDs. Sandia Labs recently proposed a conceptual 1 petawatt (10<sup>15</sup> watts) LTD Z-pinch power plant, where the electric discharge would reach 70 million amperes.<ref>{{cite web |url=http://www.sandia.gov/pulsedpower/prog_cap/pub_papers/accelerator_architecture_PRSTAB_2007.pdf |title=Architecture of petawatt-class z-pinch accelerators |publisher=Sandia.gov |access-date=2015-06-20 |url-status=dead |archive-url=https://web.archive.org/web/20160303192309/http://www.sandia.gov/pulsedpower/prog_cap/pub_papers/accelerator_architecture_PRSTAB_2007.pdf |archive-date=2016-03-03 }}</ref> As of 2012, fusion shot simulations at 60 to 70 million amperes are showing a 100 to 1000 fold return on input energy. Tests at the Z machine's current design maximum of 26-27 million amperes were set to begin in 2013.<ref>{{cite web |url=https://share.sandia.gov/news/resources/news_releases/z-fusion-energy-output/ |title=Sandia National Laboratories: News Releases : Nuclear fusion simulation shows high-gain energy output |publisher=Share.sandia.gov |date=2012-03-20 |access-date=2015-06-20 |archive-url=https://web.archive.org/web/20150714180811/https://share.sandia.gov/news/resources/news_releases/z-fusion-energy-output/ |archive-date=2015-07-14 |url-status=live }}</ref><ref>{{cite journal
 |title        = Triple-threat method sparks hope for fusion; The secrets to its success are lasers, magnets and a big pinch.
 |author       = W Wayt Gibbs
 |journal      = Nature
 |volume = 505
 |issue = 7481
 |pages = 9–10
 |date         = 30 December 2013
 |doi = 10.1038/505009a
 |pmid = 24380935
 |doi-access = free
 |bibcode = 2014Natur.505....9G
 }}</ref>{{Clarify |date=August 2019 |reason=See 2019-08-22 in edit history}}

==See also==
*[[Stockpile stewardship]]
*[[Pulsed power]]
*[[Inertial fusion power plant]]

==References==
{{Reflist|colwidth=30em}}

==External links==
*[http://www.sandia.gov/z-machine/ Home Page Z Pulsed Power Facility]
*[http://observer.guardian.co.uk/life/story/0,6903,416412,00.html "A machine called Z"], an article from ''The Observer''
*[https://web.archive.org/web/20060715001220/http://www.aip.org/enews/physnews/2006/split/767-3.html ''Physics News Update''], February 28, 2006

{{fusion power}}

{{authority control}}

[[Category:Inertial confinement fusion]]
[[Category:Nuclear research institutes]]
[[Category:Nuclear stockpile stewardship]]
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