  Experimental and computational investigations are carried out to elucidate
the influence of ethanol addition on n-heptane auto-ignition in counterflows.
An axisymmetric stream of air, temperature gradually increased, is directed
onto the surface of an evaporating pool of a liquid fuel. The air-stream
temperature at auto-ignition is measured at various strain rates for n-heptane,
ethanol, and various n-heptane/ethanol mixtures. Critical conditions for
auto-ignition are predicted employing San Diego Mechanism for both fuels and
fuel mixtures, and the results are compared with measurements. Measurements and
predictions show that low-temperature chemistry (LTC) plays a significant role
in promoting auto-ignition of n-heptane at low strain rates, but there is
insufficient residence time at high strain rates for LTC to take place, so
auto-ignition is promoted by high-temperature chemistry. Experimental and
computational results show addition of ethanol inhibits LTC of n-heptane. To
identify the responsible elementary steps, computations are performed to
identify those dominate O2 consumption and contribute to the temperature rise
in the reaction zone for n-heptane and n-heptane/ethanol mixtures at low strain
rates. For n-heptane, O2 is consumed primarily by the low-temperature steps
that result in ketohydroperoxide; the temperature rise is produced by
subsequent LTC steps. For the mixtures, a key step consuming O2 is O2 + CH3CHOH
= HO2 + CH3CHO, and the heat release occurs through the classical
high-temperature reaction mechanism. Thus, the inhibition of auto-ignition that
is observed to occur when ethanol is added to n-heptane arises from the
competition for O2 between this step and the LTC addition of O2 to the heptyl
radical and to the radical arising from the subsequent isomerization, for
n-heptane.
