The kinetics of the reaction BrO + DMS --> products(1), were examined by us
e of pulsed-laser photolytic generation and time-resolved detection of the
BrO radical by absorption spectroscopy at total pressures of 60, 100, and 2
00 Torr N-2 (1 Torr = 133.322 Pa). A value of k(1) = (4.40 +/- 0.66) x 10(-
13) cm(3) s(-1) was obtained independent of pressure at 295 K. This value i
s significantly higher than that determined previously in low-pressure (<4
Ton He), discharge flow measurements (2.6 x 10(-13) cm(3) s(-1)). By observ
ing the formation of DMSO directly, we obtain a value of 1.17 +/- 0.34 for
its yield in reaction 1; the major uncertainty is the +/-30% in the DMSO cr
oss section. The impact of these results on the chemistry of the remote mar
ine boundary layer was assessed using a chemical box model. At daytime conc
entrations of 1-2 pmol/mol, the BrO radical was found to be an important si
nk for DMS and the dominant source of DMSO. In a second set of experiments,
pulsed-laser photolysis coupled with resonance fluorescence detection of B
r atoms was employed to study the equilibrium kinetics of Br + DMS + M <->
Br-DMS + M (4, -4) at 100 Torr N-2 and 295 K. Values of k(4) = (6.36 +/- 0.
43) x 10(-11) cm(3) s(-1) and k(-4) = (1.02 +/- 0.07) x 10(4) s(-1) were ob
tained, and were used to calculate the equilibrium constant K-4 = (6.24 +/-
0.56) x 10(-15) cm(3). The uncertainty is 2 sigma plus estimated systemati
c error. At high [Br] ((1-3) x 10(12) cm(-3)), Br atoms are lost from equil
ibrium via the fast reaction Br + Br-DMS --> Br-2 + DMS (5), and a value of
k(5) = (4.2(-1.2)(+2.3)) x 10(-10) cm(3) s(-1) was obtained. The uncertain
ty is 2 sigma plus the major systematic error incurred by estimating [Br](o
) from laser fluence measurements. Pulsed-laser photolysis combined with ti
me-resolved UV absorption at selected wavelengths and diode array measureme
nts in the wavelength range 300-450 nm showed a strong absorption centered
at 365 nm due to Br-DMS. A value of sigma(max)(365nm) = (2.74(-1.1)(+1.6))
x 10(-17) cm(2) was obtained by fitting to the time-resolved absorption sig
nal due to Br-DMS. The uncertainty is 2 sigma plus systematic error (as abo
ve).