Chemistry Letters Vol.34, No.9 (2005)
1215
surface. Representative settings for trapping N2O5 were as fol-
lows: total flow rate F2 þ F3 ¼ 230 sccm (cm3ꢃminꢁ1 at STP);
initial diluted concentrations ½NOꢂ ¼ 0:17%, ½O3ꢂ ¼ 2:9%; re-
action volume Vr ¼ 300 cm3; trap temperature Tt ¼ 195 K
(dry-ice/methanol bath). Because of excess O3, >99% of NOx
can be rapidly converted to N2O5 in the reaction volume. NO2
impurity can be suppressed. The upper limit of N2O5 synthesis
rate was estimated as 5:3 ꢄ 10ꢁ2 gꢃhꢁ1 from the flow rates and
concentrations when complete trapping of N2O5 was assumed.
Note that practical collection efficiency of N2O5 is not 100%
because of heterogeneous loss and incomplete trapping. It is
remarkable that the reactions can be controlled easily only by
adjusting the flow rates and concentrations of initial NOx and
O3. After trapping N2O5, high-grade synthetic air was passed
through the trap and N2O5 was vaporized. N2O5 was diluted to
a suitable level by adding zero air, which was purified by a char-
coal filter. Then, NO2 and NO3 were monitored by the LIF in-
strument. Observed concentrations of NO2 were 209 and 398
ppbv before and after NO addition to the LIF cell, respectively.
Titrated NO3 was 94 ppbv and NO2 impurity in N2O5 was
115 ppbv, which was only 1.2 times higher than the formed
NO3. The LIF instrument can be calibrated for NO3 successfully
with less NO2 contamination. For calibration on N2O5, excess
NO was added just after the N2O5 source to convert N2O5 to
NO2 completely. From reactions (1) and (2), 1 molecule of N2O5
generates 3 NO2. Concentration of N2O5 can be determined
from the NO2 increment. When the heater tube with 1/2 inch di-
ameter and 50 cm length was heated to T ¼ 353 K, the conver-
sion yield of NO3 from N2O5 was 80%.4 The yield was limited
because of the NO3 loss on the wall. After the instrument is cali-
brated, N2O5 concentration can be quantified from the LIF signal
of converted NO3. As another experiment, the stability of the
N2O5 source was explored. After 3 h of reaction and proper di-
lution of N2O5, the averaged concentration of N2O5 was 143 ꢅ
5 ppbv as shown in Figure 2. N2O5 supply was stable for 3 h with
deviation of ꢅ4%. The deviation was mainly due to variation of
bath temperature and consumption of N2O5 powder in the trap.
Short-term variation of N2O5 was <1% as the standard deviation
of 1-min data for 10-min averaging. Consumption rate of N2O5
was estimated from flow rates and observed concentration as
1:2 ꢄ 10ꢁ4 gꢃhꢁ1, which was much smaller than N2O5 synthesis
rate. Thus, reaction period can be shortened in principle. For ex-
ample, it was confirmed that N2O5 was supplied for 7 h at least
after 3 h of reaction. Consequently, the procedure was establish-
ed to calibrate the LIF instrument accurately.
Figure 3. Relationships between calculated [NO3] and LIF
signals for the convenient source of NO3.
out solvent and dry ice. As shown in reactions (3) and (4),
NO3 can be generated when NOx is mixed with excess O3. As
indicated by the arrow C in Figure 1, the convenient supply of
NO3 was constructed. It consisted of a standard NO2 cylinder,
an O3 generator and a mixing system. No wet reagents were used
and the setup was easy and reproducible. The LIF instrument de-
tected the generated NO3 successfully. NO3 concentration can
be calculated theoretically from several parameters (e.g. initial
concentrations, temperature, reaction time, and rate constants),
with gas phase reactions considered.8 For example, ½NO3ꢂ ¼
23 ppbv for F4 ¼ 3000 sccm, F5 ¼ 300 sccm, F6 ¼ 80 sccm,
½NO2ꢂ ¼ 320 ppbv, ½O3ꢂ ¼ 71 ppmv, Vr ¼ 45 cm3, T ¼ 353 K,
and P ¼ 1 atm. The calculation has large uncertainties because
NO3 loss on the wall was not considered. However, the produc-
tion rate of NO3 is reasonable with the gas phase reactions con-
sidered. Thus, the relative response of NO3 on the material NO2
and O3 is proper. Figure 3 shows an example of the relationship
between the observed LIF signal and calculated NO3 concentra-
tion for the convenient source of NO3. As a result, excellent lin-
earity was observed between the signal and the relative concen-
tration (r2 ¼ 0:998). It was confirmed that the convenient source
is promising to prepare the ‘‘relative standard sample’’ of NO3.
From the slope of the regression line, the ‘‘preliminary sensitiv-
ity’’ can be determined in the field as 0.209 cps mWꢁ1 ppbvꢁ1. In
practical uses, after the relative variation of the preliminary
sensitivity is monitored frequently in the field campaign, the
comparison between the convenient source and the accurate
calibration should be explored to determine the correction factor
to acquire the absolute sensitivity. Note that the configurations
and settings of the convenient source should be preserved.
Finally, the secondary standard supply for NO3 was estab-
lished and validated by the LIF instrument. In field studies, it
is desirable to generate the standard sample conveniently with-
References
1
2
R. Atkinson, Atmos. Environ., 34, 2063 (2000).
A. Geyer, B. Alicke, S. Konrad, T. Schmitz, J. Stutz, and U. Platt,
J. Geophys. Res., 106, 8013 (2001).
3
S. S. Brown, H. Stark, T. B. Ryerson, E. J. Williams, D. K. Nicks, Jr.,
M. Trainer, F. C. Fehsenfeld, and A. R. Ravishankara, J. Geophys.
Res., 108, 4299 (2003).
4
5
J. Matsumoto, N. Kosugi, H. Imai, and Y. Kajii, Rev. Sci.
Instrum., 76, 064101 (2005).
R. P. Wayne, I. Barnes, P. Biggs, J. P. Burrows, C. E. Canosa-Mas, J.
Hjorth, G. L. Bras, G. K. Moortgat, D. Perner, G. Poulet, G. Restelli,
and H. Sidebottom, Atmos. Environ., 25A, 1 (1991).
W. R. Simpson, Rev. Sci. Instrum., 74, 3442 (2003).
T. Ishiwata, I. Fujiwara, and I. Tanaka, J. Phys. Chem., 87, 1349
(1983).
6
7
8
Figure 2. Long-term stability of N2O5 source.
Published on the web (Advance View) July 30, 2005; DOI 10.1246/cl.2005.1214