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Point-implicit diffusion operator in a moving particle method ( MPPM ). Yao-Hsin Hwang Department of Marine Engineering National Kaohsiung Marine University. Diffusion operator. Time-step constraint for explicit scheme Implicit scheme: Iteration Numerically stable without iteration.
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Point-implicit diffusion operator in a moving particle method (MPPM) Yao-Hsin Hwang Department of Marine Engineering National Kaohsiung Marine University
Diffusion operator • Time-step constraint for explicit scheme • Implicit scheme: Iteration • Numerically stable without iteration
Features of existing particle methods • SPH, MPS, FVPM…. • Material particles (mass point, global mass conservation) • Operators realized with randomly particle cloud
Disadvantages of existing schemes • Inaccurate (inconsistent) operator realization (particle smoothing) —continuity constraint • Assignment of boundary condition • Particle management (impractically clustered or dispersive) • Computationally inefficient
Essentials of MPPM (1) • Inserted pressure mesh to realize pressure-related operators • Background mesh and length scale • Local mass conservation • Particle as observation point
Essentials of MPPM (2) • No particle management constraint • Feasible non-uniform distribution • No special boundary treatment • Constant and diagonally dominant coefficient matrix of pressure equation
Diffusion Procedure • Equation • Laplacian ,
Explicit Operator • Scheme • Time-step constraint
Implicit Operator • Scheme • Iteration required
Point-implicit Operator • Operator
Point-implicit Operator • Scheme A • Scheme B
Effective-Time Step • Scheme A • Scheme B
Stability Limits • Scheme A • Scheme B
Three-Point Analysis(1) • Boundary conditions: • Solution at • Results
Three-Point Analysis(2) Results
Pure Diffusion(1) • Particle distribution