This paper describes an analysis method for an inertial particle separator system modeled as a multi-element airfoil configuration. The analysis method is implemented in a numerical tool that is able to perform impingement analysis using spherical, nonspherical particles as well as water droplets for a range of Reynolds number (10 4 Re 5 10 5 ). A limitations of the analysis tool is that it lacks an appropriate particle rebound model for the treatment of particle-wall collisions. The usefulness of the analysis tool is its use in conjunction with a multipoint inverse design tool for the design of a multi-element airfoil based inertial particle separator system model in an inverse fashion as opposed to the direct design methods being employed currently for this task. With such a design and analysis tool at hand, the design space can be explored as well as tradeoff studies can be performed that can aid in the development of a more efficient design methodology for multi-element airfoil based inertial particle separator systems.= Runge-Kutta coefficients used to integrate the momentum equation l 0 ; n 0 = trajectory direction vector l 1 ; n 1 = airfoil panel plane direction vector m p = particle mass, p V p n = surface normal vector p = ambient pressure Re = Reynolds number based on particle diameter, a D eq U= a r p = particle position r p;i x p;i ; z p;i = particle current position during trajectory integration r p;i1 x p;i1 ; z p;i1 = particle new position during trajectory integration S = particle surface projection on the U * perpendicular plane S p = particle surface area s = airfoil panel surface arc length,= trajectory parametric equation parameter t 1 , t 2 = airfoil panel parametric equation parameters U = magnitude of particle relative velocity in body reference frame, jUj U = particle relative velocity in body reference frame, V a V p U 0 = initial particle relative velocity in body reference frame V a = freestream velocity in body reference frame, u a i w a k V i u i ; w i = current particle velocity during the trajectory integration V i1 u i1 ; w i1 = new particle velocity during the trajectory integration V p = particle volume V p = particle velocity in body reference frame, dr p =dt V 1 = unperturbed freestream velocity in wind reference frame, u 1 i w 1 k V 0 a = initial freestream velocity in body reference frame V 0 p = initial particle velocity in body reference frame u= axes in wind reference frame x p ; z p = axes in body reference frame x 0 ; z 0 = initial particle location in wind reference frame x 1 ; z 1 , x 2 ; z 2 = airfoil panel coordinates z = pressure head = geometric angle of attack with respect to airfoil chord line = impingement efficiency, dz 0 =ds x = step along the x axis z = step along the z axis = angle between the z p axis and z axis a = ambient air viscosity a = ambient air density p = particle mass density = time step in Runge-Kutta integration = shear stress = shape factor