52 17 # first data record, number of data records Reference: JPL Publication 97-4 Chemical Kinetics and Photochemical Data for Use in Stratospheric Modeling Evaluation Number 12 January 15, 1997 page 165 N2O5 + hv -> Products "The absorption cross sections of dinitrogen pentoxide, N2O5, have been measured at room temperature by Jones and Wulf [146] between 285 and 380 nm, by Johnston and Graham [142] between 210 and 290 nm, by Graham [108] between 205 and 380 nm, and for temperatures in the 223 to 300K range by Yao et al. [332], between 200 and 380 nm. The agreement is good, particularly considering the difficulties in handling N2O5. The recommended cross section values, listed in Table 18, are taken from Yao et al. [332]. For wavelenghts shorter than 280 nm there is little or no temperature dependence, and between 285 and 380 nm the temperature effect is best computed with the expression listec at the bottom of Table 18. Recent measurements of the cross sections and their temperature dependence by Harwood et al. [116] yield values in excellent agreement with this recommendation except at the longest wavelengths (380 nm) and lowest temperatures (233K), where the new values are about 30% lower. However, the contribution to solar photodissociation from these longer wavelengths is negligible, and the differences between the predicted photolysis rates from the two stes of data are small than 3% (Harwood et al. [116]). There are several studies on the primary photolysis products of N2O5: Swanson et al. [297] have measured the quantum yeild for NO3 production at 249 and at 350 nm, obtaining a value close to unity, which is consistent with the observations of Burrows et al. [42] for photolysis at 254 nm. Barker et al. [15] report a quantum yield for O(3P) production at 290 nm of less than 0.1, and near unity for NO3. For O-atom production margitan (private communication, 1985) measured a quantum yield value of 0.35 at 266 nm, and RAvishankara et al. [252] report values of 0.72, 0.38, 0.21 and 0.15 at 248, 266, 287, and 289 nm, respectively, with a quantum yield near unity for NO3 production at all these wavelengths. It appears, then, that NO3 is produced with unit quantum yield while the O-atom, and hence the NO yield, increases at shorter wavelenghts, with a consequent decrease in the NO2 yield. The study of Oh et al. [233] indicates that, besides NO3, the promary photolysis products are a wavelenght-dependent mixture of NO2, NO2* and NO+O, where NO2* represents one or more excited electronic states, most likely the 2_B1 state." "For 285 nm < lambda < 380 nm; 300 K > T > 225K: 1E20 sigma = exp[2.735 + ((4728.5 - 17.127 lambda)/T)] where sigma is in cm^2/molecule; lambda is in nm; and T in K." "Table 18. Absorption Cross Sections of N2O5 ========================== lambda 1E20 sigma (nm) (cm^2) ========================== 200 920 205 820 210 560 215 370 220 220 225 144 230 99 235 77 240 62 245 52 250 40 255 32 260 26 265 20 270 16.1 275 13.0 280 11.7