A detachable missile nose was designed, tested, and implemented in a new missile. This design enables the use of lowdrag supersonic configurations for the major part of the flight, with the application of blunt seekers that are active during the end game. The configuration of the ejected shroud was designed using a novel approach, which included only a small amount of wind-tunnel experiments, coupled with an aerodynamic model produced by computational fluid dynamics. A simulation of flow dynamics, coupled with rigid-body dynamics, was developed and tested. Databases of aerodynamic forces and moments were produced using quasi-steady computations, for hinged and free flight of the shroud, at very demanding conditions of supersonic flight and large angles of attack. These databases were used by rigid-body dynamic simulations, in one-and six-degree-of-freedom modes, in order to predict the shroud's trajectories. Very good agreement with experimental data has been achieved. The present methodology enabled the analysis of hundreds of trajectories at a reasonable computation effort.Nomenclature CD 0 = zero-lift drag coefficient Cm x , Cm y , Cm z = roll, pitch, and yaw-moment coefficients C x , C y , C z = axial, side, and normal force coefficients D = missile base diameter, m F x , F y , F z = axial, side, and normal forces, N I b = moment of inertia with respect to center of gravity, N · m 2 L, M, N = roll, pitch, and yaw moment about the center of gravity, N · m L∕D = projectile length to diameter ratio l = shroud length, m m = total mass of a shroud half, kg p, q, r = angular velocity in roll, pitch, and yaw, rad∕s t ref = reference time scale, s V b = velocity vector of the shroud in a coordinates system attached to the missile, m∕s w = induced wind velocity, m∕s x, z = axial and normal coordinate, m X cg , Z cg = center of gravity location measured from the nose tip, m X NP = center of pressure location measured from the nose tip, m α, β = angle of attack and side-slip angle, deg θ = deflection angle, deg _ θ 0 = initial angular deflection velocity, rad∕s ω = angular velocity vector in a missile's attached coordinate system, rad∕s