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![]() Skewed kernel functions | ![]() sgWBTskew gradient Wall Boundary Treatment | ![]() Blast mitigationusing shock distruptors | ![]() Multimass Correction Procedurefor multi-component SPH simulations | ![]() Blast mitigation using foams |
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Research activities
free_surface_flows

3D dam break problem
Incompressible_multiphase

Multiphase dam break problem
BWM
Heat_transfer
4. Heat transfer

Pool boiling
skewed_kernel
4. Skewed kernel functions for one sided approximations in SPH



Distribution of skewed kernel function for different values of skewness parameter lamda

Skewed kernel approximation of a discontinuous function
sgWBT

Comparison of experimental Schlieren images (left column) of Chaudhuri et al. (2012) against the SPH simulations (right column) for the shock-wave propagation over a circular cylinder at time t= 46, 101, 157, and 212μs (top to bottom). Here, IS, incident shock; RS, reflected shock; TP, triple point; MS, Mach stem; SL, slip line; TRS, transverse reflected shock; V, vortex.
mmCorr

a)
b)
Simulation of Kelvin-Helmholtz instability a) without and b) with multimass correction
detonation

Spatio-temporal variation of the density for a sedov blast.
HIGH BUT NOT THE HIGHEST INTELLIGENCE,COMBINED WITH
THE GREATEST DEGREE OF PERSISTENCE
WILL ACHIEVE GREATER EMINENCE THAN THE HIGHEST DEGREE OF
INTELLIGENCE WITH SOMEWHAT LESS PERSISTENCE
- COX, 1926
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