Iodinated hydrocarbons are often used as precursors for hydrocarbon radicals in shock‐tube experiments. The radicals are produced by C─I bond fission reaction, and their formation can be followed through time‐resolved monitoring of the complementary I‐atom concentrations, for example, by I‐atom resonance absorption spectroscopy (I‐ARAS). This very sensitive technique requires, however, an independent calibration. As a very clean source of I atoms, CH3I is particularly well suited as calibration system for I‐ARAS presumed the yield of I atoms and the rate coefficient of I‐atom formation from CH3I are known with sufficient accuracy. But if the formation of I atoms from CH3I by I‐ARAS is to be characterized, an independent calibration system is required.
In this study, we propose a cross‐calibration approach for I‐ARAS based on the simultaneous time‐resolved monitoring of I and H atoms by ARAS in C2H5I pyrolysis experiments. For this reaction system, it can be shown that at sufficiently short reaction times very similar amounts of I and H atoms are formed (difference <1%). As calibration of H‐ARAS, with mixtures of N2O and H2, is a well‐established technique, we calibrated I‐atom absorption–time profiles with respect to simultaneously recorded H‐atom concentration–time profiles. Using this approach, we investigated the thermal decomposition of CH3I in the temperature range 950–2050 K behind reflected shock waves at two different nominal pressures (p ∼ 0.4 and 1.6 bar, bath gas: Ar). From the obtained absolute I‐atom concentration–time profiles at temperatures T < 1250 K, we inferred a second‐order rate coefficient k(T) = (1.7 ± 0.7) × 1015 exp(–20020 K/T) cm3 mol–1 s–1 for the reaction CH3I + Ar → CH3 + I + Ar. A small mechanism to describe the pyrolysis of CH3I under shock‐tube conditions is presented and discussed.