Abstract:Cascaded arc plasma sources with channel diameters between 4 and 8 mm were experimentally investigated at discharge currents up to 900 A and hydrogen (H 2 ) flow rates up to 10 slm. Pressure measurements at the arc exit showed that the heavy particle temperature in the discharge channel was about 0.8 eV. The electron temperature was calculated from the electron mass balance, taking into account electron losses due to ambipolar diffusion and convection out of the source channel. This calculation showed that the… Show more
“…The temperature decreases with the gas flow rate, while increases with the arc current, and these trends have a good agreement with Vijers's results. 17,18 As higher gas flow rate will lead to increase of inlet pressure, according to Ref. 27, electron temperature will decrease as increasing the pressure in the discharge channel.…”
Section: A Plasma Parameters Measurementsmentioning
confidence: 99%
“…16 Vijers completed a lot of experimental and theoretical characterization work with a similar device, which functioned as a plasma source. 17,18 In this paper, we will first present a typical design of plasma window in Sec. II.…”
An arc discharge with channel diameters of 3 mm and 6 mm and lengths between 30 mm and 60 mm was experimentally investigated for its potential to function as plasma window, i.e., interface vacuum regions of different pressures. Electron temperature of the plasma channel measured spectroscopically varied in the range of 7000 K to 15 000 K, increasing with discharge current while decreasing with gas flow rate. That plasma window had a slightly positive I-V characteristics over the whole range of investigated current 30 A-70 A. Measurements of pressure separation capability, which were determined by input current, gas flow rate, discharge channel diameter, and length, were well explained by viscosity effect and "thermal-block" effect. The experimental results of global parameters including temperature, gas flow rate, and voltage had a good agreement with the simulation results calculated by an axis-symmetry Fluent-based magneto-hydrodynamic model. V C 2014 AIP Publishing LLC. [http://dx.
“…The temperature decreases with the gas flow rate, while increases with the arc current, and these trends have a good agreement with Vijers's results. 17,18 As higher gas flow rate will lead to increase of inlet pressure, according to Ref. 27, electron temperature will decrease as increasing the pressure in the discharge channel.…”
Section: A Plasma Parameters Measurementsmentioning
confidence: 99%
“…16 Vijers completed a lot of experimental and theoretical characterization work with a similar device, which functioned as a plasma source. 17,18 In this paper, we will first present a typical design of plasma window in Sec. II.…”
An arc discharge with channel diameters of 3 mm and 6 mm and lengths between 30 mm and 60 mm was experimentally investigated for its potential to function as plasma window, i.e., interface vacuum regions of different pressures. Electron temperature of the plasma channel measured spectroscopically varied in the range of 7000 K to 15 000 K, increasing with discharge current while decreasing with gas flow rate. That plasma window had a slightly positive I-V characteristics over the whole range of investigated current 30 A-70 A. Measurements of pressure separation capability, which were determined by input current, gas flow rate, discharge channel diameter, and length, were well explained by viscosity effect and "thermal-block" effect. The experimental results of global parameters including temperature, gas flow rate, and voltage had a good agreement with the simulation results calculated by an axis-symmetry Fluent-based magneto-hydrodynamic model. V C 2014 AIP Publishing LLC. [http://dx.
“…On the source manipulator water cooled cascaded arc sources [3] of different configurations can be installed depending on the requirements for plasma density and plasma temperature ranges. During plasma operation, the gas flows (up to 66.7 Pa m 3 /s per gas), gas types and cathode to anode current can be changed.…”
h i g h l i g h t s• High heat flux, high density plasmas in a highly accessible linear plasma device.• Plasma exposure of targets of different sizes under selectable plasma beam angles.• Dedicated plasma and surface diagnostics.• Differential vacuum pumping system. a r t i c l e i n f o
b s t r a c tThe construction phase of the linear plasma generator Magnum-PSI at the FOM institute DIFFER has been completed and the facility has been officially opened in March 2012. The scientific program to gain more insight in the plasma-wall interactions relevant for ITER and future fusion reactors has started.In Magnum-PSI, targets of a wide range of materials and shapes can be exposed to high particle, high heat flux plasmas (>10 24 ions m −2 s −1 ; >10 MW/m 2 ). For magnetization of the plasma, oil-cooled electromagnets are temporarily installed to enable pulsed operation until the device is upgraded with a superconducting magnet. The magnets generate a field of up to 1.9 T close to the plasma source for a duration of 6 s. Longer exposure times are available for lower field settings.Plasma characterizations were done with a variety of gases (H, D, He, Ne and Ar) to determine the machine performance and prepare for subsequent scientific experiments. Thomson scattering and optical emission spectroscopy were used to determine the plasma parameters while infrared thermography and target calorimetry were used to determine the power loads to the surface. This paper reports on the status of Magnum-PSI and its diagnostic systems. In addition, an overview of the plasma parameters that can be achieved in the present state will be given.
“…This is an unprecedented high value for a steady-state cascaded arc source and more than a factor of two higher than achieved in Pilot-PSI. 20 We attribute this high efficiency to low transport losses due to the low background pressure.…”
Intense magnetized hydrogen and deuterium plasmas have been produced with electron densities up to 3.6 × 1020 m−3 and electron temperatures up to 3.7 eV with a linear plasma generator. Exposure of a W target has led to average heat and particle flux densities well in excess of 4 MW m−2 and 1024 m−2 s−1, respectively. We have shown that the plasma surface interactions are dominated by the incoming ions. The achieved conditions correspond very well to the projected conditions at the divertor strike zones of fusion reactors such as ITER. In addition, the machine has an unprecedented high gas efficiency.
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