Movies of 50kfps in 2011-12(under construction)

201202, ArHemix_150A50kfps


20120227_He(L)/Ar(R)150A50kfps, top=normal, btm=aTIG
He50kfps He1k_max He1kmean Ar50kfps Ar1k_max Ar1kmean


20111229, ArHe_mix, image and spct 150A50kfps
He20 H18A02 H17A03 H16A04 H15A05 H10A10 Ar20


20120227_ArHemix_R150A50kfps_noflux
He20 H18A02 H17A03 H16A04 H15A05 H10A10 H05A15 H02A18 Ar20
20120227_ArHe_R150A50kfps, 1kfps_max,mean


20120227, RHe150A50kfps
20120227_Ar150A50kfps



20120227_Ar20_R150A50kfps
n50kfps n2kmax n2kmean a50kfps a50kfps a1kmax a1kmean
781
Cathode angle is 90deg. This is unusual angle for stable arc ignition. The temperature increase of the top point is insufficient, because of less effect of joule heating passing through in the electrode. Cleaning action in helium shield is strong, however it is less compared to that for sharp angle.

20120227_Ar20_R150A50kfps
n50kfps n1kmax n1kmean a50kfps a50kfps a1kmax a1kmean
Cathode angle is 90deg. This is unusual angle for stable arc ignition. The temperature increase of the top point is insufficient, because of less effect of joule heating passing through in the electrode. However, cleaning action is much less compared to that for sharp angle.

image_20120227-28_He50A50kfps
spct_20120227-28_He50A50kfps
nHe nHe nHe aHe nAr


20111229, ArHemix150A50kfps


spct_20111229, ArHe_mix, 150A50kfps
He14Ar6 nHe50k nHe50k nH781 nA50k nA50k nA50k aA50k


20111230, 588nm, He150A50kfps(L3=normal,R4=aTIG)


Arc ignition movies on various base metal conditions
1)525kfps 2)He 100kfps 3)Ar 100kfps
(1)anode spot (2)oxide (3)Active flux (4)on Fe


2016.09.28쐬@2016.09.28