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Beitrag zur Physik der Fette - Über ein neues verbessertes Meßverfahren zur Erfassung und Bewertung der Erstarrungseigenschaften von Fetten

✍ Scribed by Baenitz, W.


Publisher
John Wiley and Sons
Year
1984
Weight
242 KB
Volume
86
Category
Article
ISSN
0931-5985

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✦ Synopsis


0-R' resulting from the P-cleavage and also C,H,+ radical. The corresponding 0-cleavage ion CH,-0-R' in ASE appears at m/e 71.

Series ofpeaks at m/e 41, 55,69,83,97,111,125,139 etc., are present in both the spectra are due to R-2H ions of stearyl radical. The peak at m/e 281 in ASE and VSE spectra is due to the loss of methyl and ethyl ra&cals from the molecular ions respectively.

Contrast features:

Essentially the spectra belonging to ASE and VSE are identical in many respects except for the peak m/e 2.50 which is in higher abundance in VSE than in ASE. This is due to the fact that the loss of ethanol (M-46) occurs in VSE more predominantly when the alkyl chain R has more than 5 carbon atoms '. Similar phenomenon is also observed in ASE due to the loss of propyl alcohol (M-60).

In the 15 eV spectra of these two monomers (Figures 5b andSb) hydrocarbon ions produced via secondary decomposition were depressed and the molecular ion M, M-15 and oxygen containing peaks are enhanced. Thus the base peak at m/e 58 in M E (Fig. 5b) is due to the rearrangement ion from the a-cleavage. Otherwise the spectra are identical.

The major six peaks of mass spectra at 70 eV and 15 eV of six vinyl monomers under the study are tabulated in the Table 1 as per ASTM Mass Spectral Data Book I.