8
24
J.F. Roesler et al. / Chemosphere 42 (2001) 823±826
collected on a second pass with the trap at dry-ice
temperature ()70°C). All wetted surfaces (probe Te¯on
liner, soot ®lter and cold trap) are washed ultrasonically
The eect of changing the initial mixture composition
on the growth bath composition is only to alter methane
and acetylene concentrations. Methane is relatively slow
to oxidize and its addition yields a 70% self-increase in
BATH2 relative to BATH1. In contrast, the acetylene
concentration is reduced by 20% due to the reduction in
initial n-heptane. The global eect is therefore a substi-
2 2 2 2
with CH Cl . The detailed speciation of the CH Cl
soluble fraction is obtained by GC±FID and GC±MS
analysis. The total masses of condensable species (CS) of
molecular weight species greater than acenaphthylene
and the mass of soot (non-dichloromethane-soluble
condensable species) are determined gravimetrically.
tution of C
tions.
2 2
H with methane in equal carbon propor-
Based on the reaction systems described above one
would intuitively argue that, with less C and equal
concentrations, the formation of benzene, PAH and
soot should be reduced. Yet the experimental data in-
dicate just the opposite: the rate of formation of C
2
H
2
3
. Results and discussion
H
2
In order to bear some relation to a diesel fuel, the
initially injected hydrocarbon is n-heptane. Its purpose is
primarily to generate a C ±H (and now CH ) bath
6 6
H
increases by 60%. The concentrations of the PAH and
soot have been measured only at the 20 cm position and
increase in relative amounts that are species-dependent.
Naphthalene increases from 11 to 16 ppmv (45%),
acenaphthylene from 13 to 16 ppmv (23%), ¯uo-
ranthene from 1.3 to 1.5 ppmv (15%), pyrene from 2.1
to 3.2 ppmv (50%), CS from 0.29 to 0.33 mg/l in the
hot gases (15%), and soot from 0.048 to 0.084 mg/l of
soot (80%). The later increase is likely to be the cu-
mulated eect of a shortened induction period and faster
growth rate. Thus, globally the eect of the added
methane extends throughout the total chain of reactions
leading to soot.
2
H
2
2
4
for PAH and soot formation. Two mixtures are studied
at 1425 K with a bulk mean ¯ow velocity of 61 cm/s. The
®rst, BATH1 contains initial mole fractions of 0.49% n-
heptane and 0.6% O yielding an equivalence ratio of 9.0
2
and a C/O ratio of 2.85. BATH2 has the same total
carbon content and C/O ratio, but 10% of the carbon is
injected as methane instead of n-heptane.
Fig. 1 displays the measured species pro®les. The
decomposition of n-heptane is not observed in these
experiments because it occurs in the pre-heat region on a
time scale that is much shorter than that of PAH and
soot formation. The oxygen is also consumed rapidly in
These results concur with recent experiments that
showed a methane laminar pre-mixed ¯ame to produce
2 2
the pre-heat region. The pro®les of CO, H O and CO
are thus nearly ¯at. The molecular hydrogen content is
obtained by H-atom balancing on the measured species
and on the amount of injected n-heptane. Other species
would contribute negligibly. The rise in molecular hy-
drogen along the reactor tube results from the decay of
ethylene, methane and acetylene that are the three main
hydrocarbon species remaining at the end of the pre-
heat zone.
2 6
more PAH than an equivalent C H ¯ame (Senkan and
Castaldi, 1996). While the ¯ame data provide a global
dierence between the two fuel types in a complex re-
action system with large temperature gradient, the pre-
sent results isolate the speci®c role of methane by
imposing only a perturbation in an isothermal reaction
bath. Senkan and Castaldi (1996) suggested that the
presence of methyl radicals promotes the formation of
Fig. 1. Mole fraction pro®les measured along the reactor axis. Dashed lines and open symbols are curve ®ts and data for BATH1 (no
added methane). Solid lines and ®lled symbols are curve ®ts and data for BATH2 (added methane).