Abstract. -Granular materials are inherently heterogeneous, leading to challenges in formulating accurate models of sound propagation. In order to quantify acoustic responses in space and time, we perform experiments in a photoelastic granular material in which the internal stress pattern (in the form of force chains) is visible. We utilize two complementary methods, high-speed imaging and piezoelectric transduction, to provide particle-scale measurements of both the amplitude and speed of an acoustic wave in the near-field regime. We observe that the wave amplitude is on average largest within particles experiencing the largest forces, particularly in those chains radiating away from the source, with the force-dependence of this amplitude in qualitative agreement with a simple Hertzian-like model of particle contact area. In addition, we are able to directly observe rare transient force chains formed by the opening and closing of contacts during propagation. The speed of the leading edge of the pulse is in quantitative agreement with predictions for onedimensional chains, while the slower speed of the peak response suggests that it contains waves which have travelled over multiple paths even within just this near-field region. These effects highlight the importance of particle-scale behaviors in determining the acoustical properties of granular materials.Introduction. -Sound propagation in granular materials differs from propagation in ordinary elastic materials in that there is a poor separation of length scales, particularly manifest in the branching networks of force chains which transmit stresses between particles. Continuum models [1][2][3], including effective medium theory (EMT), have failed to quantitatively describe important features such as the dependence of the sound speed on pressure [4][5][6]. Particle-scale changes in the coordination number and force chains are likely responsible for important deviations from these models, and have been the focus of numerical simulations on model amorphous systems near jamming, where soft modes are important [7][8][9].Hertzian contact theory underlines models of sound propagation, whether as the interaction potential between particles in discrete element simulations [10] or in the calculation of an effective bulk modulus in EMT [1]. The contact force f between two particles is given by an equation of the form f ∝ δ β , where δ is the distance each particle is compressed and the exponent β depends on the particle geometry. Two common idealized situations are β = 3/2 for spheres and β = 1 for cylinders. The contact area a between the particles, which in EMT are permanently bonded, has a force dependence given by a ∝ f