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Unintentionally expedited gas gettering
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I sealed this discharge tube with a fill pressure of about 5 mbar in order to get a nice air glow discharge using a 15 kV HV power supply for the plasma excitation. What I did not foresee, however, is that the discharge impedance would be low enough to draw a strong current and cause the electrodes (thin iron-nickel wires) to be heated to incandescence. The consequence is that the metal evaporation causes a particularly effective gettering of the gas fill (air), causing its pressure to drop significantly. The picture above shows that phase, while that below shows the tube state at the end of this process. By my estimate the pressure is now less than 1 mbar. The electrodes are now running cold since the discharge impedance has increased tremendously (note how the left electrode has melted), and the plasma is weaker and more diffuse (it appears a bit brighter in the picture because of the slower shutter time).

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Tuopeek - Despite its intrinsic challenges and difficulties I do find glass working to be a very rewarding activity, especially when combined with electricity and vacuum/gases. I can imagine the sense of wonder Crookes and Geissler must have felt when they made and ran their discharge tubes. I've also struggled with glass-metal seals and I agree with you that finding the right materials was not the biggest problem. What made the difference for me is the annealing step after I make a feedthrough (I use a broad oxygen-poor butane-propane mix flame for that). Adding that to my workflow changed everything (I work with soft soda-lime glass, which is particularly difficult given its high thermal expansion coefficient). The problem of gas cleanup is not so easily resolved though, especially with molecular gases... Daniel McFarland Moore certainly had to deal with that with his nitrogen and carbon dioxide tubes in the days before the fluorescent tube! If you don't want to (or can't) work at very low current, like in spectroscopic tubes, then there is no other way than to have a gas reservoir attached to the lamp if it is to be run for any extender period of time. This also applies to certain noble-gas lamps when an extremely long service life is needed, such as in this particular case.
I have an old Crookes type X-ray tube. These all had clever gas reservoirs to set pressures and hence the operating voltage for the tube. It’s also interesting to note the size and construction of CO2 laser tubes with only a thin central tube for the active discharge.
By the way, yesterday I managed to make my first vacuum incandescent lamp, but tungsten transport via the water cycle was particularly strong and resulted in severe blackening (despite that I baked and degassed the lamp thoroughly before I sealed it off). I'll look into gettering methods, including with the use of electrical discharges, maybe I can get rid of the residual water vapor and hydrogen via plasma molecular dissociation.
Tuopeek - Sealed CO2 lasers are certainly very interesting. If I remember correctly, those have some sort of catalytic regeneration of the carbon dioxide.
@Max - I think early CO2 lasers required a feed of fresh gas due to decomposition in the discharge. A catalyst would be a better cost option. I will have a look at the tube I have. Don’t remember seeing a catalyst but it has a large reservoir for gas and a convoluted route for it to circulate. Perhaps surprisingly CO2 is not the main gas, helium is and I think it job is mostly heat transport. Nitrogen is also part of the tube mixture.
Nice filament lamp by the way. I haven’t tried that, other than to form hot cathodes in other experiments. Is the vacuum not always going to be your enemy with filament evaporation? Have wondered if a simple getter and air filled would work with only a partial or minimum vacuum, although not efficiently.
Tuopeek - Tungsten evaporation will always be an issue in vacuum and at very low pressures. So, provided that I have everything else under control (i.e., oxygen and water vapor impurities), it's only a matter of operating the filament at the most suitable temperature. On the other hand, blackening from metallic evaporation (and sputtering) may not be that big of a problem in long discharge tubes if it's localized around the filament... will see, I need to do some tests to judge the severity of this issue.
About CO2 lasers, it's correct that the gas fill consists of a He-N2-CO2 mixture. Nitrogen and helium forms a Penning mixture which is useful to ensure a homogeneous discharge, especially at higher pressures such as in TEA lasers, while nitrogen stores energy from the discharge and transfers it to CO2 molecules via resonant collisions. That's a very well thought out system indeed!