“…For both flame geometries, the potential flow assumption, which is commonly used in the large activation energy asymptotic analysis [3,10,20], is employed here. By introducing a geometry factor N with N ¼ 0 for the counterflow flame and N ¼ 1 for the tubular flame (with e R I and e R O being the inner and outer tube radius, respectively), the potential flow field for both configurations can be written as…”