Numerical simulations of the flow past a multi-element airfoil in plunging motion are performed. The present research study investigates the physics, the integrated load performance and the propulsive efficiency of the plunging three-element McDonnell Douglas airfoil MDA 30P-30N at Re=6.5x10 5 . Effects of the geometric angle of attack and amplitude of the plunging motion are examined. The flow field downstream of the high-lift configuration is found to be similar to the single-element airfoil flow regimes at the same reduced frequency. In the present study, the latter parameter is kept constant and equal to k=0.63 revealing classical vortex streets with no recirculating regions far from the airfoil. The vorticity magnitude of the vortex patterns is significantly influenced by the plunging amplitude and weakly influenced from the geometric angle of attack. Plunging amplitude affects the time variation of the loads and the flow-field in the vicinity of the high-lift device. At St=0.1, the loads reach their peaks at the middle of the up-stroke or down-stroke phase, exhibiting sinusoidal variation. At higher St numbers, large regions of detached flow are observed and the loads variation alters significantly. Attachment of the flow during the upstroke and down-stroke phase increases the propulsive performance. During the upstroke, at high geometric angles of attack, the flow is well attached. However, at lower angles, the flow detaches from the slat surface, forming small vortical structures in the leading part of the device. The opposite trend is observed during the down-stroke. Hence, at high geometric angles of attack, the flow is significantly detached. At a=22 o , vast flow detachment, is found to be the main reason for not generating mean thrust at all St numbers. Maximum propulsive performance is found at a=0 o and St=0.3 with mean Cd=-0.83. Lift performance is degraded as the amplitude of the oscillations increases. This result is revealed at all angles of attack. The mean lift coefficient could drop at 60% of its steady flight value. Nomenclature α geometrical angle of attack ( o ) D axial force (N) L lift force (N) C d C p drag coefficient, C d =D/(0.5cρU 2 ) power coefficient, ( ) ( ) l C t y t U