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This study examines the effects of various surface treatments on Cu samples and analyzes the evolution of breakdown voltage (b) during conditioning and breakdown resistance (BDR) measurements. The results indicate that surface treatments primarily affect the initial breakdowns, while subsequent sparks show consistent behavior across all samples. Furthermore, the correlation between b and the next breakdown field suggests potential field-induced effects on small tips.
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Recent DC spark results Antoine Descoeudres, Yngve Levinsen, Sergio Calatroni, Mauro Taborelli
Outline • Surface treatments of Cu samples • Evolution of b during conditioning and BDR measurements
Outline • Surface treatments of Cu samples • rolled sheet (reference) • heat treatment • milling • Subu • Electro-polishing
‘‘de-conditioning’’ due to spark damages (observed only with Cu) Cu standard sample (rolled sheet) • First 2 – 3 sparks : Eb = 350 – 400 MV/m, b = 15 – 20 • After a few sparks: ~ 170 MV/m, b ~ 50 • The delay before the first spark is usually very long (ms)
Quantity of gas released during a spark : slightly less, but within error bars Cu + heat treatment at 875°C • Both electrodes treated in a brazing cycle (2h) • Same results as non-heated Cu (Eb, b, BDR…)
good surface state at the start, like rolled sheet Cu + milling • Sample milled in the CERN workshop (no idea what the roughness may be…) • Standard behaviour :
Eb = 200 MV/m, b = 20 – 35 Cu (milled) + Subu treatment • Subu : ~ 20 mm removed • The surface state at the start is not as good :
Also a good surface state, comparable to standard Cu Cu (milled) + Electro-polishing • Electro-polishing: ~ 20 mm removed
The first sparks destroy rapidly the benefit of a good surface preparation Surface treatments of Cu : summary • Surface treatments on Cu only affects the very first breakdowns • After a few sparks: ~ 170 MV/m, b ~ 50 for every samples And in RF ? Sparks are distributed over a much larger surface… Treatments are maybe still useful
Outline • Surface treatments of Cu samples • Evolution of b during conditioning and BDR measurements
Evolution of b during conditioning measurements • In the 2nd DC spark setup: automatization of b measurements between each spark
Evolution of b during conditioning measurements • Correlation between b and the next breakdown field • No correlation between b and the previous breakdown field b · Eb = cst
Evolution of b during conditioning measurements • b · Eb is much less dispersed than Eb Local field : b · Eb = cst = 9.8 GV/m (± 0.2) for Cu
Are small tips pulled by the field? (we need more data) Evolution of b during BDR measurements spark • ‘calm’ period low b • b seems to increase (a few %) during a calm period if E is sufficiently high