TY - JOUR
T1 - The determination of explosion limits from a unified thermal and chain theory
AU - Yang, C. H.
AU - Gray, B. F.
PY - 1967
Y1 - 1967
N2 - A general equation for explosion limits (P-T relation) is derived from a unified thermal and chain theory. From this general equation, the criteria of explosion limits for either the pure chain or pure thermal theory can be deduced. For a purely thermal system (no chain reactions involved), the limits are shown to depend upon knowledge of the kinetics instead of the gross heat release rate alone. The result of the classical theory is obtained from the unified theory again when a single step reaction is assumed. It is also shown that explosions in a system which contains a branching chain in its kinetic scheme always go through a path of both energy and chain-carrier concentration divergence. In some cases, it may even go through a pure thermal mechanism without involving the divergence of the chain carrier at all (such as the third limit of the H2 and O2 system). In application of the theory to the H2 and O2 system, the general equation of explosion limits is shown to prescribe all three limits, lower, upper, and third. The discussion is extended to the CO and O2 system. It shows that the unified theory may be used to explain the previously unaccountably high activation energy deduced from the upper limit.
AB - A general equation for explosion limits (P-T relation) is derived from a unified thermal and chain theory. From this general equation, the criteria of explosion limits for either the pure chain or pure thermal theory can be deduced. For a purely thermal system (no chain reactions involved), the limits are shown to depend upon knowledge of the kinetics instead of the gross heat release rate alone. The result of the classical theory is obtained from the unified theory again when a single step reaction is assumed. It is also shown that explosions in a system which contains a branching chain in its kinetic scheme always go through a path of both energy and chain-carrier concentration divergence. In some cases, it may even go through a pure thermal mechanism without involving the divergence of the chain carrier at all (such as the third limit of the H2 and O2 system). In application of the theory to the H2 and O2 system, the general equation of explosion limits is shown to prescribe all three limits, lower, upper, and third. The discussion is extended to the CO and O2 system. It shows that the unified theory may be used to explain the previously unaccountably high activation energy deduced from the upper limit.
UR - http://www.scopus.com/inward/record.url?scp=29244436595&partnerID=8YFLogxK
U2 - 10.1016/S0082-0784(67)80237-6
DO - 10.1016/S0082-0784(67)80237-6
M3 - Article
AN - SCOPUS:29244436595
VL - 11
SP - 1099
EP - 1106
JO - Symposium (International) on Combustion
JF - Symposium (International) on Combustion
SN - 0082-0784
IS - 1
ER -