2010
DOI: 10.1007/s00193-010-0287-6
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Mesoscale analysis of volumetric and surface dissipation in granular explosive induced by uniaxial deformation waves

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Cited by 43 publications
(21 citation statements)
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“…One reason for this discrepancy is that these simulations ignore damage in the microstructures and heat generation owing to frictional dissipation at crack surfaces and sliding interfaces. Panchadhara & Gonthier (2011) studied the compaction of granular explosives under uniaxial compression, using a Lagrangian finite and discrete element technique. Contact and friction across neighbouring grains are considered.…”
Section: Introductionmentioning
confidence: 99%
“…One reason for this discrepancy is that these simulations ignore damage in the microstructures and heat generation owing to frictional dissipation at crack surfaces and sliding interfaces. Panchadhara & Gonthier (2011) studied the compaction of granular explosives under uniaxial compression, using a Lagrangian finite and discrete element technique. Contact and friction across neighbouring grains are considered.…”
Section: Introductionmentioning
confidence: 99%
“…Additional details about the constitutive theory can be found in Ref. 3 Computations are performed using a combined finite and discrete element method that is well-suited for problems involving heterogeneity. This combined method uses the finite-element method (FEM), coupled with a radial return stress update algorithm, to numerically integrate the time-dependent, 2-D conservation principles and viscoplastic flow rule governing deformation of individual particles, and uses the discreteelement method (DEM) to account for interactions between particles.…”
Section: Computational Techniquementioning
confidence: 99%
“…Here, it is noted that although the underlying granular microstructure also depends on particle morphology, the only variable available in the multiphase model used to describe this microstructure is φ i . Efforts to include mesoscale physics within the continuum macroscale description have been attempted [5], but require additional submodeling such as mesoscale simulations [1,2,4,6,32], which is beyond the scope of this work. The gas internal energy is characterized by its thermal equation of state e g = e g (ρ g , P g ), while the solid equation of state includes a volume fraction contribution due to compaction, i.e., e i = e i (ρ i , P i , φ i ).…”
Section: Introductionmentioning
confidence: 99%