242 Bull. Chem. Soc. Jpn., 75, No. 2 (2002)
Chemical Ionization of Alkylbenzenes
distributions on the reaction time was measured in order to ex-
amine the effects of collisional stabilization. The reactivity of
CH5 , C2H5 , and C3H5 for alkylbenzenes was discussed
from the initial product-ion distributions and from thermo-
chemical calculations of heats of reactions.
an excess energy will be partly relaxed by collisions with CH4
and He gases. Therefore, fragmentation will be suppressed in
CI mass spectra obtained at long reaction times. In order to
examine the contribution of collisional stabilization in our CI
conditions, the dependence of product-ion distributions on the
reaction time was measured.
+
+
+
Experimental
For examples, Figs. 1 and 2 show product-ion distributions
of CyH2y + 1+ (y = 3–10) and PhCyH2y+ (y = 1–13) in the reac-
CI mass spectra were obtained using an ion-trap type of Hitachi
M7200 GC/MS under a reactant-ion selective mode. The CI CH4
gas was introduced directly in an ion-trap cell. The electron-im-
+
+
+
tions of CH5 , C2H5 , and C3H5 with typical reagents
(PhCxH2x + 1: x = 8 and 13) at five different reaction times: 0.5,
+
+
2, 10, 20, and 40 ms. The CyH2y + 1+ (y = 3–10) and PhCyH2y
pact ionization on CH4 provides primary CHn (n = 2–4) ions.
One of the reactant CH5+, C2H5+, and C3H5+ ions produced from
(y = 1–13) distributions exhibit single peaks in most cases. It
+
+
+
the subsequent fast ion-molecule reactions of CHn (n = 2–4)
is clear from Figs. 1 and 2 that the CyH2y + 1 and PhCyH2y
with CH4 was selectively trapped as a reactant ion in an ion-trap
cell. The maximum and average kinetic energies of the reactant
ions in our apparatus were evaluated to be 10 and 4.2 eV (1 eV =
96.485 kJ mol−1) for CH5+, 6.0 and 2.4 eV for C2H5+, and 4.3 and
1.7 eV for C3H5+, respectively, using a pseudo-potential well
method.14 These energies are higher than that in the medium-pres-
sure CI experiments, which was estimated to be less than 1 eV.16
The time for storing a reactant ion was kept at a constant time of 5
ms. If reactant ions in vibrationally excited levels are formed,
they will be thermalized by collisions with CH4 and He during
their trapping time in the cell. The ion-trap cell was kept at ꢁ 170
°C. The reagents were diluted in hexane and injected into the GC
with a high-purity carrier He gas. The partial pressures of CH4
and He and in an ion-trap cell were 9 × 10−3 and 7 × 10−3 Pa, re-
spectively. The reaction time corresponding to the residence time
in the ion-trap was varied from 0.5 to 40 ms. The mass spectra
were measured at low reagent concentrations of about 1000–
10000 pg cm−3 in order to reduce secondary ion-molecule reac-
tions. It is known that the number of ions stored in the ion trap de-
pends on the radio frequency voltage.17 Thus, the CI mass spectra
obtained in this study were calibrated against NIST standard da-
ta.18
The operating conditions in the ion-trap cell used in this work
were significantly different from those of the conventional medi-
um-pressure CI mass spectrometer developed by Field et al.1–4 In
the medium-pressure CI measurements, the typical CH4 gas pres-
sure was 133 Pa and the residence time of reactant ions in the ion-
ization-reaction chamber was about 10 µs. Field4 evaluated the to-
tal number of collisions of reactant ions with CH4 during this resi-
dence time to be about 200. In the present low-pressure CI mea-
surements, the total number of collisions of a product ion with
CH4 was estimated to be about 1–100 times within the reaction
time of 0.5–40 ms from a simple gas-kinetic hard-sphere collision
model.
distributions depend on the reaction time in most cases, though
+
the changes in the PhCyH2y distributions are smaller than
those in the CyH2y + 1+ ones. The decreases or increases in the
product-ion distributions with increasing the reaction time are
+
+
shown by arrows in Figs. 1 and 2. In all the six CH5 , C2H5 ,
+
and C3H5 reactions shown in Fig. 1, the branching ratios of
+
CyH2y + 1 decrease with increasing the reaction time, except
+
for the branching ratios of CyH2y + 1+ (y = 9, 10) in the CH5 /
PhC13H27 reaction, for which an inverse relation is observed.
+
The branching ratios of PhCyH2y having small y values de-
crease, while those having large y values increase in many cas-
es.
+
+
In addition to major CyH2y + 1 and PhCyH2y ions, [M +
H]+, [PhH + H]+, [PhC2H5 + H]+, [M + C3H5]+, and [M +
C3H5 − C2H4]+ ions were observed in many reactions. With
increasing reaction time, the branching ratios of [M + H]+,
[M+C3H5]+, and [M + C3H5 − C2H4]+ ions increase, while
those of [PhH + H]+ and [PhC2H5 + H]+ either slightly de-
crease or are nearly constant. These findings indicate that col-
lisonal stabilization with CH4 and He participates in the forma-
tion of the former ions. We found here that collisional stabili-
zation take part in most of all reactions. Thus, the initial prod-
uct distributions were determined by extrapolating the depen-
dence of branching ratios of product ions on the reaction time
to zero reaction time. The results obtained are summarized in
Tables 1–3. The uncertainties of the initial branching-ratios
were estimated to be within 8%. Two major product ions are
+
+
alkyl CyH2y + 1 (y ꢁ x) and PhCyH2y (y ꢁ x) ions. The de-
pendence of their intensity distributions on the chain length x
is shown below for the three reactions.
+
Distribution of Alkyl CyH2y + 1 (y = 3–10: y ꢁ x) Ions:
Figures 3(a)–3(i) show initial product-ion distributions of
CyH2y + 1+ (y = 3–10: y ꢁ x) obtained for short (x = 3–5), me-
dium (x = 6–9), and long (x = 10–13) chain reagents. The
Results and Discussion
+
+
+
CyH2y + 1 (y = 3–10) ions are observed in the CH5 , C2H5 ,
+
Contribution of Collisional Stabilization and Initial
and C3H5 reactions; differences in the intensity distributions
Product-Ion Distributions: When CI mass spectra resulting
are relatively small among the three reactions. Figures 3(a)–
3(i) show that the CyH2y + 1 distributions depend strongly on
+
+
from ion-molecule reactions of CH5 , C2H5 , and C3H5+ with
+
alkylbenzenes (PhCxH2x + 1: x = 3–13) were measured, [M +
the chain length x for short reagents below x < 7, where the
dominant alkyl ions are CxH2x + 1+. On the other hand, the dis-
tributions become similar for long-chain reagents x ꢀ 7, where
+
+
H]+, CyH2y + 1 (y = 3–10), and PhCyH2y (y = 1–13) ions
were observed. Here, x represents the number of carbons of
alkyl groups in a reagent, while y stands for the number of car-
bons of fragment alkyl groups. In addition, the [PhC2H5 +
H]+ ion was observed in the C2H5+ reaction, and adduct [M +
C3H5]+ ions were observed in the C3H5+ reaction. If the colli-
sional stabilization takes part in the formation of product ions,
+
the dominant alkyl ions are CyH2y + 1+ (y = 4–6). In the CH5
+
+
and C2H5 reactions, the CyH2y + 1 distributions peak at y =
3–6 for short (x = 3–6) chain reagents, and at y = 4, 5 for
+
longer (x > 6) chain reagents. In the C3H5 reactions, the
+
CyH2y + 1 distributions peak at y = 3, 4 for short (x = 3–6)