The breakup, penetration, droplet size, and size distribution of a Jet A-l fuel in air crossflow has been investigated with focus given to the impact of surrounding air pressure. Data have been collected by particle Doppler phased analyzer (PDPA), Mie-scattering with high speed photography augmented by laser sheet, and Mie-scattering with intensified chargecoupled device (ICCD) camera augmented by nanopulse lamp. Nozzle orifice diameter, d," was 0.508 mm and nozzle orifice length to diameter ratio, l,Jd0, was 5.5. Air crossflow velocities ranged from 29.57 to 137.15 mis, air pressures from 2.07 to 9.65 bar, and temper ature held constant at 294.26 K. Fuel flow provides a range offuellair momentum flux ratio (q) from 5 to 25 and Weber number from 250 to 1000. From the results, adjusted correlation of the mean drop size has been proposed using drop size data measured by PDPA as follows: (Do/Di2) = 0.267We"Mqom(pl/p a)OM(pi/pay° >b. This correlation agrees well and shows roles of aerodynamic Weber number, Wea, momentum flux ratio, q, and density ratio, ptlpa. Change of the breakup regime map with respect to surrounding air pressure has been obsen ed and revealed that the boundary betw een each breakup modes can be predicted by a transformed correlation obtained from above correlation. In addi tion, the spray trajectory for the maximum Mie-scattering intensity at each axial location downstream of injector is extracted from averaged Mie-scattering images. From these results, correlations with the relevant parameters including q, xld," density ratio, viscosity ratio, and Weber number are made over a range of conditions. According to spray trajec tory at the maximum Mie-scattering intensity, the effect of surrounding air pressure becomes more important in the farfield. On the other hand, effect of aerodynamic Weber number is more important in the neaifield.