The concentration of the product nitric oxide, [NO(X 2 Π r )] product , formed in the title reactions is measured as a function of the vibrational energy distribution in the N 2 (A 3 Σ u + ) for V′ e 6 in a rapidly pumped dischargeflow reactor at ∼298 K and a total pressure of ∼2 Torr using laser-excited fluorescence techniques. For the reaction N 2 (A 3 Σ u + ,V′ e 2) + O( 3 P) there is no [NO(X 2 Π r )] observed detected above the noise in the background emission signal. Correcting this null measurement for competing reactions, the NO(X 2 Π r ) + N( 4 S, 2 D) product yield accounts for e2% (signal-to-background noise ) 1, 1σ) of the [N 2 (A 3 Σ u + ,V′)] total . For the reaction N 2 (A 3 Σ u + ,V′ e 6) + O( 3 P) the [NO(X 2 Π r )] observed is seen to increase slightly relative to the reaction N 2 (A-3 Σ u + ,V′ e 2) + O( 3 P). Correcting the [NO(X 2 Π r )] observed for competing reactions, the NO(X 2 Π r ) + N( 4 S, 2 D) product yield accounts for 5.7 ( 1.1% of the [N 2 (A 3 Σ u + )] total and as much as 57 ( 14% of the [N 2 -(A 3 Σ u + ,3 e V′ e 6)]. For the reaction N 2 (A 3 Σ u + ,V′ e 6) + O 2 (X 3 Σ g -) no [NO(X 2 Π r )] observed is detected above the noise in the background emission signal. Correcting this null measurement for competing reactions, the NO(X 2 Π r ) + NO(X 2 Π r ) product yield represents <0.1% of the [N 2 (A 3 Σ u + ,V′)] total . Possible implications of these observations are discussed.