Man-made debris from previous spacecraft missions poses a serious threat to spacecraft that are launched to operate in Earth orbit because it can strike such spacecraft at extremely high velocities and consequently damage mission-critical systems. Most satellites are constructed with honeycomb sandwich panels as their primary structural elements. To be able to perform a risk analysis, it is important to know, in the event of such a meteoroid or orbital debris particle impact, whether or not the impacting particle or parts thereof will exit the rear of the sandwich panel.A recently developed set of ballistic limit equations for two different types of honeycomb sandwich panels are studied to determine how well they perform when they are applied to systems that are outside of the database that was used to develop them. It was found that these ballistic limit equations are fairly conservative; they successfully predicted sandwich panel perforation in nearly all of the tests that resulted in perforation, while allowing approximately half of the nonperforating tests to be incorrectly labeled as tests with a perforation. This indicates the likelihood that use of these equations in design applications could result in overly robust shielding hardware.Nomenclature d c = critical projectile diameter for failure of rear wall, cm d p = projectile diameter, cm K MLI = adjustment factor for multilayer insulation K S2 = adjustment factor for scaling standoff distance S 2 in the hypervelocity regime K tw = adjustment factor for equipment cover plate thickness t w in the hypervelocity regime K 3D , K 3S = ESA triple-wall ballistic limit equation fit factors for the hyperballistic and ballistic velocity regimes, respectively S 1 , S 2 = standoff between first and second, and second and third bumper, where third bumper backwall, cm t b = thickness of the inner/second bumper (the rear face sheet in the case of a honeycomb sandwich panel), cm t ob = thickness of the outer bumper (the front face sheet in the case of a honeycomb sandwich panel), cm t w = thickness of third bumper/back wall/equipment cover plate, cm V, V n = impact velocity and its normal component (V cos ), respectively, km=s V t1 = transition velocity between ballistic and shatter velocity regimes, km=s V t2 = transition velocity between shatter and hypervelocity regimes, km=s V t1;n , V t2;n = normal component of V t1 cos and V t2 cos , respectively, km=s , , , , "= fit parameters for the Schäfer-Ryan-Lambert ballistic limit equation = impact angle (0 deg is a perpendicular impact on the target surface), deg ob , p = volumetric density of the outer bumper and the projectile, respectively, g=cm 3 y;ksi = yield stress of the equipment cover plate, ksi