INP

Leibniz Institute for Plasma Science and Technology
Felix-Hausdorff-Str. 2
17489 Greifswald
GERMANY

https://www.inp-greifswald.de/en/
welcomeatinp-greifswald [punkt] de

The Leibniz Institute for Plasma Science and Technology (INP) is the largest non-university institute in the field of low temperature plasmas, their basics and technical applications in Europe. The institute carries out research and development from idea to prototype. The topics focus on the needs of the market. At present, plasmas for materials and energy as well as for environment and health are the focus of interest.

Cite Dataset

Advanced temporal analysis of anode activity during mode transitions in high current vacuum arcs - dataset

Anode activity in high current vacuum arcs leads to the formation of various high current modes and transitions between them. Intense material evaporation during the anode spot mode and formation of a neutral vapour cloud during the anode plume mode modify the arc plasma properties and, hence, can have a crucial impact in applications, like e.g. reduction of interruption performance of switching devices. The influence of anode mode appearance on arc plasma parameters and on anode surface temperature was studied in detail by a novel optical diagnostic technique—intensified video optical emission spectroscopy. Employing advanced diagnostic methods, the ground state density, excitation temperature and pressure profiles close to the anode surface have been determined. For the anode plume mode, higher copper vapour pressure was found in the plume shell compared to its core. The copper ion density distribution shows a maximum outside of the plume shell. Consequently, a higher electrical conductivity in the surrounding area of the plume might be expected, i.e. the arc current flows around the plume rather than through it. Analysis of the temporal evolution of electrical and optical signals reveals that voltage jumps and drops during the mode transitions are accompanied by noticeable changes in the anode surface temperature. Thus, the formation of the anode plume leads to temperature lowering while the transition to the anode spot mode is accompanied by a temperature increase. In general, a clear correlation between electrode surface temperature and arc voltage in the case of constricted anode attachment is found. The results of this study give new insights into anode plume properties and consequences of anode mode transitions. Reversible mode transitions and correlations between arc voltage and anode surface temperature, as well as changes in the current path during anode plume mode, have to be considered as factors for optimization of electrode design and choice of materials for switching applications.

FieldValue
Group
Authors
Release Date
2025-09-16
Identifier
3430ff37-1c98-4482-a8a5-8d04aea4c924
Permanent Identifier (DOI)
Permanent Identifier (URI)
Is supplementing
Plasma Source Name
Plasma Source Application
Plasma Source Specification
Plasma Source Properties

Model vacuum circuit breaker with a contact system in a vacuum chamber with optical access (four glass windows), with a pneumatic drive to move the lower electrode (grounded cathode) with an averaged velocity of 1.25 m/s, with a pumping system (roughing pump and turbomolecular pump) to evacuate the chamber down to 10^-7 mbar pressure, and with an AC pulse current source based on a capacitor bank. The fixed anode and the movable cathode are disc-shaped electrodes of CuCr (60/40) with a diameter of 30 mm.

Plasma Source Procedure

The vacuum arc is ignited by contact separation. 50 Hz sinosoidal currents with peak values from 1 to 7.5 kA have been studied.

Plasma Medium Name
Plasma Medium Properties

Cu-Cr metal vapour from electrode erosion with time dependent and inhonogeneous distribution strongly dependent on the cathode and anode evaporation by cathode and anode spots.

Plasma Target Name
Plasma Target Properties
No target (electrodes can be considered as the target)
Plasma Diagnostics Name
Plasma Diagnostics Properties

Electric measurements:
Arc current measured with Rogowski coil (PEM CWT 1500), arc voltage measured with voltage probe (Tektronix P6015A, bandwidth 75 MHz), recording with an oscilloscope.

High-speed imaging of the arc:
High-speed camera Photron Nova S12 (HSC 1) with frame rate 20000 fps and exposure time of 0.7 – 1.7 µs.

Optical emission spectroscopy (OES) of the arc:
intensified video OES with spectrograph Andor Shamrock SR-750i and camera Photron Nova S16 (HSC 2) combined with image intensifier Hamamatsu C10880 with frame rate 200 000 fps and exposure time of 0.7 – 1.7 µs.

Measurement of anode surface temperature:
a) high-speed camera Photron Nova S6 (HSC 3) with narro band filter (MIF) with central wavelength 891 nm and FWHM 10 nm with frame rate 22 500 fps and exposure time 5 µs.
b) NIR fiber spectrometer Hamamatsu C114GA with temporal resolution of 1,25 ms and exposure teime of 50 - 200 µs adapted by an optics to the measurement of an area of 3 mm^2 at the anode centre (starting of the measurements 1 ms before current zero).

Plasma Diagnostics Procedure

Optical emission spectroscopy (OES) of the arc:
Recording of the spectra over the arc cross section at the position of 1 mm below the anode surface.

Measurement of anode surface temperature:
Anode surface temperature distribution was deduced from records of Nova S6 by correction of the arc radiation and comparison with NIR measurements.

Language
English
License
Public Access Level
Public
Contact Name
Uhrlandt, Dirk
Contact Email

Data and Resources