ror limits of k2 in a similar fashion to what was done for k1. The individual error sources were determined and calculated before they were combined using the root-sum-square method to obtain ±20% uncertainty for k2 at 1209 K.
ror limits of k2 in a similar fashion to what was done for k1. Theindividual error sources were determined and calculated beforethey were combined using the root-sum-square method to obtain±20% uncertainty for k2 at 1209 K.