1'0DC129 Vlcm Torr %TIC 3 0 30 (155.,,,,,'" 0 1 0 3 Torr % T I C 2 0 '0 4 0 60 8 3 803 2 0 ETHYL BUTYRATE 2 o L _ _ . d 1 0 43 60 8 0 1 0 3 1 2 0 "ROPYL PRCP OluA-E Flgure 3.Water CI spectra of ethyl butyrate and propyl propionate obtained in the drift-tube CI source with water reagent gas at 110 OC and 0.103 Torr. The drift field strength was 129 Vkm-Torr, sufficient to produce substantial amounts of fragmentation characteristic of these two structural isomers preferential solvation of the product ion favors formation of RCOOH2+-OH2 from (RCOOR')H+.OH, over formation of RCOOH2+ from (RCOOH')H+. Inasmuch as the origins and analytical utility of all of the various ions observed in the CI spectra of esters have been discussed extensively in previous work (6,8,14), there is no ease of identifying esters from their water CI spectra at high E / P in the drift tube source, Figure 3 compares the spectra of ethyl butyrate and propyl propionate at 129 V/cm-Torr. The MH+ ions at m / e 117 are present for both esters, but none of the other peaks are identical. The fragment ions in ethyl butyrate are R+ ( m / e 43), RCO' ( m / e 711, RCOOH2+ ( m / e 89), and RCOOH2+.0H2 ( m / e 107), while the fragment ions \ need to repeat that information here. As an example of the The use of "in-beam" sample introduction to obtain chemical ionization (CI) mass spectra of thermally labile compounds and salts of low volatilHy is descrlbed. Samples are introduced on the surface of Teflon tubing and the effects of changing the sample position in the source are shown. The time and temperature dependence of some CI mass spectra are shown.