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Diploma thesis in Physics submitted by Florian Freundt born in ...

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Chapter 4<br />

Measur<strong>in</strong>g methods<br />

4.1 Mass spectrometry of He, Ne, Ar, Kr and Xe<br />

Measurements of He, Ne, Ar, Kr and Xe were conducted us<strong>in</strong>g a GV Instruments MM5400<br />

mass spectrometer and a preparation l<strong>in</strong>e built and set up <strong>by</strong> Friedrich [2007]. The samples<br />

were measured <strong>in</strong> four dist<strong>in</strong>ct runs, the first three dur<strong>in</strong>g September to November 2010 and the<br />

last one <strong>in</strong> May 2011. The first three runs utilized the same setup and sample size, while some<br />

changes were made for the fourth run, <strong>in</strong>clud<strong>in</strong>g a slightly different <strong>in</strong>let setup, different sample<br />

size and modified measur<strong>in</strong>g processes for He, Ar, Kr and Xe.<br />

4.1.1 Sample preparation and measur<strong>in</strong>g procedure<br />

The copper sample tubes were <strong>in</strong>stalled <strong>in</strong> an <strong>in</strong>let volume of known size which was evacuated<br />

to less than 5.0 × 10 −6 mbar. The process of <strong>in</strong>stall<strong>in</strong>g the sample tubes <strong>in</strong>side the <strong>in</strong>let was<br />

responsible for most sample losses s<strong>in</strong>ce mechanical stress had to be exerted on the fragile seal<strong>in</strong>g<br />

before the surround<strong>in</strong>g volume was evacuated. The sample was vented <strong>in</strong>to the evacuated <strong>in</strong>let<br />

volume <strong>by</strong> apply<strong>in</strong>g pressure perpendicular to one of the p<strong>in</strong>ch po<strong>in</strong>ts us<strong>in</strong>g a modified valve,<br />

there<strong>by</strong> crack<strong>in</strong>g the seal<strong>in</strong>g and releas<strong>in</strong>g the gas <strong>in</strong>to the <strong>in</strong>let volume almost <strong>in</strong>stantaneously.<br />

In rare cases the crack<strong>in</strong>g was so m<strong>in</strong>ute that the vent<strong>in</strong>g happened slowly over a timespan of 3<br />

to 10 m<strong>in</strong>utes.<br />

After tak<strong>in</strong>g a pressure read<strong>in</strong>g of the gas <strong>in</strong>side the <strong>in</strong>let volume, the gas was transferred to<br />

the preparation l<strong>in</strong>e where gas separation was done: The different noble gases cannot be measured<br />

side <strong>by</strong> side <strong>in</strong> a s<strong>in</strong>gle step but have to be separated. This is due to the differences<br />

<strong>in</strong> concentration magnitudes as well as to prevent <strong>in</strong>terference effects: The mass spectrometer<br />

discrim<strong>in</strong>ates mass-to-charge ratios, therefore a twice ionized 40 Ar atom will provide the same<br />

result as a s<strong>in</strong>gle-ionized 20 Ne atom. The gas separation was realized <strong>by</strong> an adsorption refrigeration<br />

system, adsorb<strong>in</strong>g the noble gases Ar, Kr and Xe, as well as all other permanent gases, at<br />

25 K <strong>in</strong> a permanent gas trap while He and Ne were adsorbed at temperatures below 12 K <strong>in</strong> an<br />

activated carbon reservoir. The gases were then released separately through <strong>in</strong>cremental heat<strong>in</strong>g<br />

43

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