A bimolecular chemical reaction (reactant1 + reactant2 --> products) i
n laminar Poiseuille flow is experimentally observed using a spectroph
otometer. The reaction rate (r(m)) follows the second-order rate law;
that is, r(m) = kappa c(1)c(2), where c(m) (m = 1, 2) are the reactant
concentrations. The reaction rate constant kappa is independently est
imated by monitoring the reaction kinetics in a completely mixed batch
reactor using the stopped-flow technique. In the reactive transport e
xperiments, the reactants are introduced in a tube and are initially s
eparated by a sharp interface. The variation of the fluid velocity ove
r the cross section of the tube causes the concentrations of the react
ants to vary around their cross-sectional average values ((c) over bar
(m)). These spatial variations in the concentrations (c(m)') influence
the overall reaction rate. The cross-sectional average reaction rate
is given by (r) over bar(m) = kappa<(c(1)c(2))over bar> = kappa((c) ov
er bar(1)(c) over bar(2) + <(c(1)c(2))over bar>) = kappa(1 + s)(c) ove
r bar(1)(c) over bar(2) where s = <(c(1)'c(2)')over bar>/((c) over bar
(1)(c) over bar(2)) is the segregation intensity. The experimentally o
bserved breakthrough concentration of the product is in agreement with
a numerical model that accounts for the effects of the segregation in
tensity. On ignoring the influence of the segregation intensity, the p
redicted product concentration substantially exceeds the experimental
observations. This shows that for initially non-overlapping reactants
the segregation intensity is negative (s < 0) and that the overall che
mical transformation rate in flowing systems can be significantly diff
erent from that implied by substituting the mean concentrations in the
expression for the reaction rate.