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Ananth Ramaswamy

Publications and source records attributed to Ananth Ramaswamy.

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FeynKrack: A continuum model for quasi-brittle damage through Feynman-Kac killed diffusion

Continuum damage mechanics (CDM) is a popular framework for modelling crack propagation in solids. The CDM uses a damage parameter to quantitatively assess what one loosely calls `material degradation'. While this parameter is sometimes given a physical meaning, the mathematical equations for its evolution are generally not consistent with such physical interpretations. Curiously, degradation in the CDM may be viewed as a change of measures, wherein the damage variable appears as the Radon-Nikodym derivative. We adopt this point of view and use a probabilistic measure-valued description for the random microcracks underlying quasi-brittle damage. We show that the evolution of the underlying density may be described via killed diffusion as in the Feynman-Kac theory. Damage growth is then interpreted as the reduction in this measure over a region, which in turn quantifies the disruption of bonds through a loss of force-transmitting mechanisms between nearby material points. Remarkably, the evolution of damage admits an approximate closed-form solution. This brings forth substantive computational ease, facilitating fast yet accurate simulations of large dimensional problems. By selecting an appropriate killing rate, one accounts for the irreversibility of damage and thus eliminates the need for ad-hoc history-dependent routes typically employed, say, in phase field modelling of damage. Our proposal FeynKrack (a short form for Feynman-Kac crack propagator) is validated and demonstrated for its efficacy through several simulations on quasi-brittle damage. It also offers a promising stochastic route for future explorations of non-equilibrium thermodynamic aspects of damage.

physics.comp-ph

A discrete cohesive zone model for beam element: Application to adhesively bonded laminates and sandwich panels

A new discrete cohesive zone model (DCZM) is presented for modeling the interface behavior of adhesive-bonded thin laminates and sandwich panels. The proposed model treats the interface as a spring element and the adherent as a beam element. The use of the preceding assumptions facilitates the simplification of the computational framework reducing the problem from a 2D to 1D, thereby relaxing the requirements of maintaining the aspect ratio of elements in the finite element mesh. For thin laminates, the constitutive relation of the adhesive is represented by a bi-linear traction-separation law, whereas for sandwich panels, an exponential law is employed to model the adhesive behavior. In order to validate the proposed model for thin laminates, simulations of three established fracture tests: DCB, ENF, and MMB have been undertaken. Additionally, for the sandwich panel, two experiments documented in the literature have been simulated for assessing the efficacy of the modelling. One experiment has a mode-I interface failure and the other one a mode-II interface failure between the core and skin. It has been observed that the model is not sensitive to either the element size or the load step size. The results have been compared with reported (benchmark) numerical, analytical, and experimental findings. The proposed methodology for thin laminates offers a significant reduction in the computational effort (reduced number of unknown degrees of freedom compared to existing methods) with no compromise on the accuracy of the predictions. Specifically, it reduces the unknown degrees of freedom by more than 25\% compared to the corresponding mesh used in existing continuum cohesive zone model (CCZM) approaches. The Newton-Raphson solver can achieve quick convergence and no line search feature is required. The proposed algorithm is easy to implement on any computational platform.

physics.comp-ph