1
Advanced Modeling and Optimization of Diesel Engines Arbitrary Lagrangian Eulerian Approach Assess the fuel structure on emissions in diesel engine combustion and possible fuel optimization Develop a computational facility Large Eddy Simulation (LES) Reynolds Averaged Navier Stokes (RANS) approach Advanced combustion models Advanced soot models Advanced spray models Surrogate fuels Immersed Boundary (IB) method Verification and Validation Interfacing IB with STL files Coupling IB with ALE in the structured solver Towards realistic reciprocating engine simulations Shashank, Prahalled Iyengar, Liangyu Wang, Heinz Pitsch Uniformly accelerated piston Results Motivation Objective Immersed Boundary (IB) Technique GCEP LES RANS Challenges Complex geometry Moving parts Multiphysics interaction Chemistry Accuracy and efficiency Intake Manifold Strategy Based on the existing LES code Structured grid Accurate Navier Stokes solver Advanced numerical methods Multiphysics models New Techniques implemented Immersed boundary (IB) method Complex geometry like valves Arbitrary Lagrangian Eulerian (ALE) approach Moving piston Status of the Code ALE algorithm implemented in the structured grid solver IB technique implemented in the structured grid solver The computational nodes in this algorithm can be either • Fixed as in Eulerian description of motion • Following the material as in Lagrangian description of motion • Moving in an arbitrary manner depending the resolution required Verification Moving piston Fixed Wall Material particle Computational Node Particle motion …………. Mesh motion Flow in a simplified piston cylinder assembly Future work Maps complex geometry and moving parts onto structured grid Uses exact surface reconstruction technique on non-body conforming meshes Generate computational mesh easily even for complex geometry Complex geometry immersed in structured grid and the resulting grid Velocity field at three different time steps in an expansion compression cycle Channel flows: parallel and inclined For 32 x 32 Grid L= 5.00E-03 L2 = 1.41E-02 Walls, represented only by special reconstruction technique Intake open Piston Bottom Dead center Piston Intake closed Representation of immersed boundary

Shashank, Prahalled Iyengar, Liangyu Wang, Heinz …gcep.stanford.edu/pdfs/DJPwvV9uoqC8S02r45xP4Q/Shashank...Shashank, Prahalled Iyengar, Liangyu Wang, Heinz Pitsch Uniformly accelerated

  • Upload
    others

  • View
    13

  • Download
    0

Embed Size (px)

Citation preview

Page 1: Shashank, Prahalled Iyengar, Liangyu Wang, Heinz …gcep.stanford.edu/pdfs/DJPwvV9uoqC8S02r45xP4Q/Shashank...Shashank, Prahalled Iyengar, Liangyu Wang, Heinz Pitsch Uniformly accelerated

Advanced Modeling and Optimization of Diesel Engines

Arbitrary Lagrangian Eulerian Approach• Assess the fuel structure on emissions in diesel engine combustion

and possible fuel optimization

• Develop a computational facility • Large Eddy Simulation (LES)• Reynolds Averaged Navier Stokes (RANS) approach• Advanced combustion models• Advanced soot models• Advanced spray models• Surrogate fuels• Immersed Boundary (IB) method

Verification and Validation

• Interfacing IB with STL files• Coupling IB with ALE in the structured solver• Towards realistic reciprocating engine simulations

Shashank, Prahalled Iyengar, Liangyu Wang, Heinz Pitsch

Uniformly accelerated piston

Results

Motivation

Objective

Immersed Boundary (IB) Technique

GCEP

LES RANS

Challenges• Complex geometry• Moving parts• Multiphysics interaction• Chemistry• Accuracy and efficiency

Intake Manifold

Strategy

Based on the existing LES code• Structured grid• Accurate Navier Stokes solver• Advanced numerical methods• Multiphysics models

New Techniques implemented• Immersed boundary (IB) method

• Complex geometry like valves• Arbitrary Lagrangian Eulerian (ALE) approach

• Moving piston

Status of the Code• ALE algorithm implemented in the structured grid

solver• IB technique implemented in the structured grid

solver

The computational nodes in this algorithm can be either• Fixed as in Eulerian description of motion• Following the material as in Lagrangian description of motion• Moving in an arbitrary manner depending the resolution required

Verification

Mo

ving

pist

on

Fixed W

all

Material particle

Computational Node

Particle motion

…………. Mesh motion

Flow in a simplified piston cylinder assembly

Future work

• Maps complex geometry and moving parts onto structuredgrid

• Uses exact surface reconstruction technique on non-bodyconforming meshes

• Generate computational mesh easily even for complexgeometry

Complex geometry immersed in structured grid and the resulting grid

Velocity field at three different time steps in anexpansion compression cycle

Channel flows: parallel and inclined

For 32 x 32 Grid

L∞ = 5.00E-03

L2 = 1.41E-02

Walls, represented only byspecial reconstructiontechnique

Intake open

Piston

Bottom Dead center

Piston

Intake closed

Representation of immersed boundary