Large Plasma Device: Difference between revisions

Content deleted Content added

Inline

Revision as of 19:16, 11 September 2018

The Large Plasma Device (often stylized as LArge Plasma Device or LAPD) is an experimental physics device housed at the Basic Plasma Science Facility at UCLA. It is designed as a general purpose laboratory for experimental plasma physics research. The device began operation in 1991^[1] and was upgraded twice in 2001 and 2016^[2] to its current version. The modern LAPD is operated as a national user facility, in which half the research time on the device is open to scientists at other institutions and facilities.

Machine overview

The LAPD is a linear pulsed-discharge device operated at a high (1 Hz) repetition rate, producing a strongly magnetized background plasma which is physically large enough to support Alfvén waves. Plasma is produced from a barium oxide (BaO) cathode-anode discharge at one end of a 20-meter long, 1 meter diameter cylindrical vacuum vessel (diagram). The resulting plasma column is roughly 16.5 meters long and 60 cm in diameter. The background magnetic field, produced by a series of large electromagnets surrounding the chamber, can be varied from 400 gauss to 2.5 kilogauss (40 to 250 mT).

Plasma parameters

Because the LAPD is a general-purpose research device, the plasma parameters are carefully selected to make diagnostics simple without the problems associated with hotter (e.g. fusion-level) plasmas, while still providing a useful environment in which to do research. The typical operational parameters are:

Density: n = 1–4 $\times$ 10¹² cm⁻³
Temperature: T_e = 6 eV, T_i = 1 eV
Background field: B = 400–2500 gauss (40–250 mT)

In principle, a plasma may be generated from any kind of gas, but inert gases are typically used to prevent the plasma from destroying the coating on the barium oxide cathode. Examples of gases used are helium, argon, nitrogen and neon. Hydrogen is sometimes used for short periods of time. Multiple gases can also be mixed in varying ratios within the chamber to produce multi-species plasmas.

At these parameters, the ion Larmor radius is a few millimeters, and the Debye length is tens of micrometres. Importantly, it also implies that the Alfvén wavelength is a few meters, and in fact shear Alfvén waves are routinely observed in the LAPD. This is the main reason for the 20-meter length of the device.

Plasma sources

The main source of plasma within the LAPD is produced via discharge from the barium oxide (BaO) coated cathode, which emits electrons via thermionic emission. The cathode is located near the end of the LAPD and is made from a thin nickel sheet, uniformly heated to roughly 900°C. The circuit is closed by a molybdenum mesh anode a short distance away. Typical discharge currents are in the range of 3-8 kiloamperes at 60-90 volts, supplied by a custom-designed transistor switch backed by a 4-farad capacitor bank.

A secondary cathode source made of lanthanum hexaboride (LaB₆) was developed in 2010^[3] to provide a hotter and denser plasma when required. It consists of four square tiles joined to form a 20 $\times$ 20 cm² area and is located at the other end of the LAPD. The circuit is also closed by a molybdenum mesh anode, which may be placed further down the machine, and is slightly smaller in size to the one used to close the BaO cathode source. The LaB₆ cathode is typically heated to temperatures above 1750°C by a graphite heater, and produces discharge currents of 2.2 kiloamperes at 150 volts.

The plasma in the LAPD is usually pulsed at 1 Hz, with the background BaO source on for 10-20 milliseconds at a time. If the LaB₆ source is being utilized, it typically discharges together BaO cathode, but for a shorter period of time (about 5–8 ms) nearing the end of each discharge cycle. The use of an oxide-cathode plasma source, along with a well-designed transistor switch for the discharge, allows for a plasma environment which is extremely reproducible shot-to-shot.

One interesting aspect of the BaO plasma source is its ability to act as an "Alfvén Maser", a source of large-amplitude, coherent shear Alfvén waves.^[4] The resonant cavity is formed by the highly reflective nickel cathode and the semitransparent grid anode. Since the source is located at the end of the solenoid which generates the main LAPD background field, there is a gradient in the magnetic field within the cavity. As shear waves do not propagate above the ion cyclotron frequency, the practical effect of this is to act as a filter on the modes which may be excited. Maser activity occurs spontaneously at certain combinations of magnetic field strength and discharge current, and in practice may be activated (or avoided) by the machine user.

Diagnostic access and probes

Probes

The main diagnostic is the movable probe. The relatively low electron temperature makes probe construction straightforward and does not require the use of exotic materials. Most probes are constructed in-house within the facility and include magnetic field probes^[5], Langmuir probes, Mach probes (to measure flow), electric dipole probes and many others. Standard probe design also allows external users to bring their own diagnostics with them, if they desire. Each probe is inserted through its own vacuum interlock, which allows probes to be added and removed while the device is in operation.

A 1 Hz rep-rate, coupled with the high reproducibility of the background plasma, allows the rapid collection of enormous datasets. An experiment on LAPD is typically designed to be repeated once per second, for as many hours or days as is necessary to assemble a complete set of observations. This makes it possible to diagnose experiments using a small number of movable probes, in contrast to the large probe arrays used in many other devices.

The entire length of the device is fitted with "ball joints," vacuum-tight angular couplings (invented by a LAPD staff member) which allow probes to be inserted and rotated, both vertically and horizontally. In practice, these are used in conjunction with computer-controlled motorized probe drives to sample "planes" (vertical cross-sections) of the background plasma with whatever probe is desired. Since the only limitation on the amount of data to be taken (number of points in the plane) is the amount of time spent recording shots at 1 Hz, it is possible to assemble large volumetric datasets consisting of many planes at different axial locations.

Visualizations composed from such volumetric measurements can be seen at the LAPD gallery.

Including the ball joints, there are a total of 450 access ports on the machine, some of which are fitted with windows for optical or microwave observation.

Other diagnostics

A variety of other diagnostics are also available at the LAPD to compliment probe measurements. These include photodiodes, microwave interferometers, a high speed camera (3 ns/frame) and laser-induced fluorescence.

References

^ Gekelman, W.; Pfister, H.; Lucky, Z.; Bamber, J.; Leneman, D.; Maggs, J. (Aug 1991). "Design, construction, and properties of the large plasma research device−The LAPD at UCLA". Review of Scientific Instruments. 62 (12): 2875–2883. Bibcode:1991RScI...62.2875G. doi:10.1063/1.1142175. ISSN 0034-6748.
^ Gekelman, W.; Pribyl, P.; Lucky, Z.; Drandell, M.; Leneman, D.; Maggs, J.; Vincena, S.; Van Compernolle, B.; Tripathi, S. K. P. (Feb 2016). "The upgraded Large Plasma Device, a machine for studying frontier basic plasma physics". Review of Scientific Instruments. 87 (2): 025105. Bibcode:2016RScI...87b5105G. doi:10.1063/1.4941079. ISSN 0034-6748. PMID 26931889.
^ Cooper, C. M.; Gekelman, W.; Pribyl, P.; Lucky, Z. (16 Aug 2010). "A new large area lanthanum hexaboride plasma source". Review of Scientific Instruments. 81 (8): 083503. Bibcode:2010RScI...81h3503C. doi:10.1063/1.3471917. ISSN 0034-6748. PMID 20815604.
^ Maggs, J. E.; Morales, G. J.; Carter, T. A. (14 Dec 2004). "An Alfvén wave maser in the laboratory". Physics of Plasmas. 12 (1): 013103. Bibcode:2005PhPl...12a3103M. doi:10.1063/1.1823413. ISSN 1070-664X.
^ Everson, E. T.; Pribyl, P.; Constantin, C. G.; Zylstra, A.; Schaeffer, D.; Kugland, N. L.; Niemann, C. (18 Nov 2009). "Design, construction, and calibration of a three-axis, high-frequency magnetic probe (B-dot probe) as a diagnostic for exploding plasmas". Review of Scientific Instruments. 80 (11): 113505. Bibcode:2009RScI...80k3505E. doi:10.1063/1.3246785. ISSN 0034-6748. PMID 19947729.

External links

Basic Plasma Science Facility website

[1] Gekelman, W.; Pfister, H.; Lucky, Z.; Bamber, J.; Leneman, D.; Maggs, J. (Aug 1991). "Design, construction, and properties of the large plasma research device−The LAPD at UCLA". Review of Scientific Instruments. 62 (12): 2875–2883. Bibcode:1991RScI...62.2875G. doi:10.1063/1.1142175. ISSN 0034-6748.

[2] Gekelman, W.; Pribyl, P.; Lucky, Z.; Drandell, M.; Leneman, D.; Maggs, J.; Vincena, S.; Van Compernolle, B.; Tripathi, S. K. P. (Feb 2016). "The upgraded Large Plasma Device, a machine for studying frontier basic plasma physics". Review of Scientific Instruments. 87 (2): 025105. Bibcode:2016RScI...87b5105G. doi:10.1063/1.4941079. ISSN 0034-6748. PMID 26931889.

[3] Cooper, C. M.; Gekelman, W.; Pribyl, P.; Lucky, Z. (16 Aug 2010). "A new large area lanthanum hexaboride plasma source". Review of Scientific Instruments. 81 (8): 083503. Bibcode:2010RScI...81h3503C. doi:10.1063/1.3471917. ISSN 0034-6748. PMID 20815604.

[4] Maggs, J. E.; Morales, G. J.; Carter, T. A. (14 Dec 2004). "An Alfvén wave maser in the laboratory". Physics of Plasmas. 12 (1): 013103. Bibcode:2005PhPl...12a3103M. doi:10.1063/1.1823413. ISSN 1070-664X.

[5] Everson, E. T.; Pribyl, P.; Constantin, C. G.; Zylstra, A.; Schaeffer, D.; Kugland, N. L.; Niemann, C. (18 Nov 2009). "Design, construction, and calibration of a three-axis, high-frequency magnetic probe (B-dot probe) as a diagnostic for exploding plasmas". Review of Scientific Instruments. 80 (11): 113505. Bibcode:2009RScI...80k3505E. doi:10.1063/1.3246785. ISSN 0034-6748. PMID 19947729.

[1]

[2]

[3]

[4]

[5]

@@ Line 1: / Line 1: @@
 [[Image:Lapd exterior.jpg|thumb|300px|right|The Large Plasma Device during an experiment.]]
-The '''Large Plasma Device''' (often stylized as '''LArge Plasma Device''' or '''LAPD''') is an experimental physics device housed at the Basic Plasma Science Facility at [[UCLA]].  It is designed as a general purpose laboratory for experimental [[plasma physics]] research.  The device began operation in 1991<ref>{{Cite journal|last=Gekelman|first=W.|last2=Pfister|first2=H.|last3=Lucky|first3=Z.|last4=Bamber|first4=J.|last5=Leneman|first5=D.|last6=Maggs|first6=J.|date=Aug 1991|title=Design, construction, and properties of the large plasma research device−The LAPD at UCLA|journal=Review of Scientific Instruments|language=en|volume=62|issue=12|pages=2875–2883|doi=10.1063/1.1142175|issn=0034-6748}}</ref> and was upgraded twice in 2001 and 2016<ref>{{Cite journal|last=Gekelman|first=W.|last2=Pribyl|first2=P.|last3=Lucky|first3=Z.|last4=Drandell|first4=M.|last5=Leneman|first5=D.|last6=Maggs|first6=J.|last7=Vincena|first7=S.|last8=Van Compernolle|first8=B.|last9=Tripathi|first9=S. K. P.|date=Feb 2016|title=The upgraded Large Plasma Device, a machine for studying frontier basic plasma physics|journal=Review of Scientific Instruments|language=en|volume=87|issue=2|pages=025105|doi=10.1063/1.4941079|pmid=26931889|issn=0034-6748}}</ref> to its current version. The modern LAPD is operated as a national user facility, in which half the research time on the device is open to scientists at other institutions and facilities.
+The '''Large Plasma Device''' (often stylized as '''LArge Plasma Device''' or '''LAPD''') is an experimental physics device housed at the Basic Plasma Science Facility at [[UCLA]].  It is designed as a general purpose laboratory for experimental [[plasma physics]] research.  The device began operation in 1991<ref>{{Cite journal|last=Gekelman|first=W.|last2=Pfister|first2=H.|last3=Lucky|first3=Z.|last4=Bamber|first4=J.|last5=Leneman|first5=D.|last6=Maggs|first6=J.|date=Aug 1991|title=Design, construction, and properties of the large plasma research device−The LAPD at UCLA|journal=Review of Scientific Instruments|language=en|volume=62|issue=12|pages=2875–2883|doi=10.1063/1.1142175|issn=0034-6748|bibcode=1991RScI...62.2875G}}</ref> and was upgraded twice in 2001 and 2016<ref>{{Cite journal|last=Gekelman|first=W.|last2=Pribyl|first2=P.|last3=Lucky|first3=Z.|last4=Drandell|first4=M.|last5=Leneman|first5=D.|last6=Maggs|first6=J.|last7=Vincena|first7=S.|last8=Van Compernolle|first8=B.|last9=Tripathi|first9=S. K. P.|date=Feb 2016|title=The upgraded Large Plasma Device, a machine for studying frontier basic plasma physics|journal=Review of Scientific Instruments|language=en|volume=87|issue=2|pages=025105|doi=10.1063/1.4941079|pmid=26931889|issn=0034-6748|bibcode=2016RScI...87b5105G}}</ref> to its current version. The modern LAPD is operated as a national user facility, in which half the research time on the device is open to scientists at other institutions and facilities.
 == Machine overview ==
@@ Line 23: / Line 23: @@
 The main source of plasma within the LAPD is produced via discharge from the barium oxide (BaO) coated cathode, which emits electrons via [[thermionic emission]].  The cathode is located near the end of the LAPD and is made from a thin nickel sheet, uniformly heated to roughly 900°C.  The circuit is closed by a molybdenum mesh anode a short distance away.  Typical discharge currents are in the range of 3-8 [[kiloampere]]s at 60-90 volts, supplied by a custom-designed transistor switch backed by a 4-[[farad]] capacitor bank.
-A secondary cathode source made of [[lanthanum hexaboride]] (LaB<sub>6</sub>) was developed in 2010<ref>{{Cite journal|last=Cooper|first=C. M.|last2=Gekelman|first2=W.|last3=Pribyl|first3=P.|last4=Lucky|first4=Z.|date=16 Aug 2010|title=A new large area lanthanum hexaboride plasma source|journal=Review of Scientific Instruments|language=en|volume=81|issue=8|pages=083503|doi=10.1063/1.3471917|pmid=20815604|issn=0034-6748}}</ref> to provide a hotter and denser plasma when required. It consists of four square tiles joined to form a 20 <math>\times</math>20 cm<sup>2</sup> area and is located at the other end of the LAPD.  The circuit is also closed by a molybdenum mesh anode, which may be placed further down the machine, and is slightly smaller in size to the one used to close the BaO cathode source.  The LaB<sub>6</sub> cathode is typically heated to temperatures above 1750°C by a graphite heater, and produces discharge currents of 2.2 kiloamperes at 150 volts.
+A secondary cathode source made of [[lanthanum hexaboride]] (LaB<sub>6</sub>) was developed in 2010<ref>{{Cite journal|last=Cooper|first=C. M.|last2=Gekelman|first2=W.|last3=Pribyl|first3=P.|last4=Lucky|first4=Z.|date=16 Aug 2010|title=A new large area lanthanum hexaboride plasma source|journal=Review of Scientific Instruments|language=en|volume=81|issue=8|pages=083503|doi=10.1063/1.3471917|pmid=20815604|issn=0034-6748|bibcode=2010RScI...81h3503C}}</ref> to provide a hotter and denser plasma when required. It consists of four square tiles joined to form a 20 <math>\times</math>20 cm<sup>2</sup> area and is located at the other end of the LAPD.  The circuit is also closed by a molybdenum mesh anode, which may be placed further down the machine, and is slightly smaller in size to the one used to close the BaO cathode source.  The LaB<sub>6</sub> cathode is typically heated to temperatures above 1750°C by a graphite heater, and produces discharge currents of 2.2 kiloamperes at 150 volts.
 The plasma in the LAPD is usually pulsed at 1&nbsp;Hz, with the background BaO source on for 10-20 milliseconds at a time.  If the LaB<sub>6</sub> source is being utilized, it typically discharges together BaO cathode, but for a shorter period of time (about 5–8 ms) nearing the end of each discharge cycle.  The use of an oxide-cathode plasma source, along with a well-designed transistor switch for the discharge, allows for a plasma environment which is extremely reproducible shot-to-shot.
-One interesting aspect of the BaO plasma source is its ability to act as an "Alfvén [[Maser]]", a source of large-amplitude, coherent shear Alfvén waves.<ref>{{Cite journal|last=Maggs|first=J. E.|last2=Morales|first2=G. J.|last3=Carter|first3=T. A.|date=14 Dec 2004|title=An Alfvén wave maser in the laboratory|journal=Physics of Plasmas|language=en|volume=12|issue=1|pages=013103|doi=10.1063/1.1823413|issn=1070-664X}}</ref>  The resonant cavity is formed by the highly reflective nickel cathode and the semitransparent grid anode.  Since the source is located at the end of the [[solenoid]] which generates the main LAPD background field, there is a gradient in the magnetic field within the cavity.  As shear waves do not propagate above the ion [[gyrofrequency|cyclotron frequency]], the practical effect of this is to act as a filter on the modes which may be excited.  Maser activity occurs spontaneously at certain combinations of magnetic field strength and discharge current, and in practice may be activated (or avoided) by the machine user.
+One interesting aspect of the BaO plasma source is its ability to act as an "Alfvén [[Maser]]", a source of large-amplitude, coherent shear Alfvén waves.<ref>{{Cite journal|last=Maggs|first=J. E.|last2=Morales|first2=G. J.|last3=Carter|first3=T. A.|date=14 Dec 2004|title=An Alfvén wave maser in the laboratory|journal=Physics of Plasmas|language=en|volume=12|issue=1|pages=013103|doi=10.1063/1.1823413|issn=1070-664X|bibcode=2005PhPl...12a3103M}}</ref>  The resonant cavity is formed by the highly reflective nickel cathode and the semitransparent grid anode.  Since the source is located at the end of the [[solenoid]] which generates the main LAPD background field, there is a gradient in the magnetic field within the cavity.  As shear waves do not propagate above the ion [[gyrofrequency|cyclotron frequency]], the practical effect of this is to act as a filter on the modes which may be excited.  Maser activity occurs spontaneously at certain combinations of magnetic field strength and discharge current, and in practice may be activated (or avoided) by the machine user.
 == Diagnostic access and probes ==
 === Probes ===
-The main diagnostic is the movable probe.  The relatively low electron temperature makes probe construction straightforward and does not require the use of exotic materials.  Most probes are constructed in-house within the facility and include magnetic field probes<ref>{{Cite journal|last=Everson|first=E. T.|last2=Pribyl|first2=P.|last3=Constantin|first3=C. G.|last4=Zylstra|first4=A.|last5=Schaeffer|first5=D.|last6=Kugland|first6=N. L.|last7=Niemann|first7=C.|date=18 Nov 2009|title=Design, construction, and calibration of a three-axis, high-frequency magnetic probe (B-dot probe) as a diagnostic for exploding plasmas|journal=Review of Scientific Instruments|language=en|volume=80|issue=11|pages=113505|doi=10.1063/1.3246785|pmid=19947729|issn=0034-6748}}</ref>, [[Langmuir probe]]s, Mach probes (to measure flow), electric dipole probes and many others.  Standard probe design also allows external users to bring their own diagnostics with them, if they desire.  Each probe is inserted through its own vacuum interlock, which allows probes to be added and removed while the device is in operation.
+The main diagnostic is the movable probe.  The relatively low electron temperature makes probe construction straightforward and does not require the use of exotic materials.  Most probes are constructed in-house within the facility and include magnetic field probes<ref>{{Cite journal|last=Everson|first=E. T.|last2=Pribyl|first2=P.|last3=Constantin|first3=C. G.|last4=Zylstra|first4=A.|last5=Schaeffer|first5=D.|last6=Kugland|first6=N. L.|last7=Niemann|first7=C.|date=18 Nov 2009|title=Design, construction, and calibration of a three-axis, high-frequency magnetic probe (B-dot probe) as a diagnostic for exploding plasmas|journal=Review of Scientific Instruments|language=en|volume=80|issue=11|pages=113505|doi=10.1063/1.3246785|pmid=19947729|issn=0034-6748|bibcode=2009RScI...80k3505E}}</ref>, [[Langmuir probe]]s, Mach probes (to measure flow), electric dipole probes and many others.  Standard probe design also allows external users to bring their own diagnostics with them, if they desire.  Each probe is inserted through its own vacuum interlock, which allows probes to be added and removed while the device is in operation.
 A 1&nbsp;Hz rep-rate, coupled with the high reproducibility of the background plasma, allows the rapid collection of enormous datasets.  An experiment on LAPD is typically designed to be repeated once per second, for as many hours or days as is necessary to assemble a complete set of observations.  This makes it possible to diagnose experiments using a small number of movable probes, in contrast to the large probe arrays used in many other devices.