1IntroductionAs ak ey component of as olid rocket motor( SRM), the structural integrity of solid propellantsp lays ac rucial role in its service life evaluation. During shipment, storagea nd ignition,t he solid propellants inside aS RM generally suffer from diverse loadings [1,2].T od etermine the integrity and service life of the SRM, it is necessary to evaluatet he stress and strain distributionsa sw ell as the aging and damage of the solid propellant grainsb ased on viscoelastic constitutive theory and computational modeling [1][2][3][4].N umerical analyses performed by various researchers clearly demonstrated that the Poisson's ratio variation in solid propellant grains has as ignificant effect on the resulting stress and strain response. Despite the Poisson's ratio is generally treated as ac onstant for simplicity,m odels that assume ac onstantP oisson ratio usually cannot achieve good results, especially for short-duration loading cases. In fact, the Poisson'sr atio of solid propellants, known as at ime-temperature dependent viscoelastic property,i sacomplex function dependent on both time and load histories [5]. Thus, to feed the numerical techniques, experimental determination of time-varying Poisson's ratio of the propellant grains is of practical importance. However,s ince solid propellant grains are very flexible and soft in nature, it is extremely challenging to use existing experimental techniques to accurate measure its time-dependent Poisson's ratio, whichi se xpected to vary from compressible (v < 0.5) to incompressible (v % 0.5) and thusd emanding very high accuracyo ns train measurements.To determine the Poisson's ratio of solid propellants, both indirect and direct measurementt echniquesc an be used [6][7][8].T he indirect measurement methods first measure other material parameters, such as tensile/compressive modulus ands hear modulus, Poisson's ratio is then numerically computed based on the transversal relationship among these material parameters. Becauset he indirect techniques involve multiple measurement and fitting of several mechanical parameters, their practical implementation is not only troublesome, but also prone to induce large measuremente rrors due to the error accumulation involved in various steps.I nc ontrast, the direct measurement