FIDAP Numerical Modeling

Slides:



Advertisements
Similar presentations
Fluid Mechanics Research Group Two phase modelling for industrial applications Prof A.E.Holdø & R.K.Calay.
Advertisements

Instructor: André Bakker
Hongjie Zhang Purge gas flow impact on tritium permeation Integrated simulation on tritium permeation in the solid breeder unit FNST, August 18-20, 2009.
University of Western Ontario
Beams and Frames.
Pharos University ME 352 Fluid Mechanics II
UNICAMP THE HEIGHT OF LIQUID METHOD FOR FREE SURFACE FLOWS Flow simulations of real processes often involve fluids that are separated by a sharp interface.
PREPARED BY: JANAK GAJJAR SD1909.  Introduction  Wind calculation  Pressure distribution on Antenna  Conclusion  References.
University of South Carolina FCR Laboratory Dept. of Chemical Engineering By W. K. Lee, S. Shimpalee, J. Glandt and J. W. Van Zee Fuel Cell Research Laboratory.
Quanitification of BL Effects in Engineering Utilitites… P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Engineering Parameters.
1 Design and drawing of RC Structures CV61 Dr. G.S.Suresh Civil Engineering Department The National Institute of Engineering Mysore Mob:
Rotation and angular momentum
Flow rate across a fluid element with top and bottom faces moving Fluid element h dx dy Consider the fluid element with dimensions dx, dy, and h (film.
1 CREL meeting 2004 CFD Simulation of Fisher-Tropsch Synthesis in Slurry Bubble Column By Andrey Troshko Prepared by Peter Spicka Fluent Inc. 10 Cavendish.
Practise questions Answers later.
CP502 Advanced Fluid Mechanics
1 Tutorial 5-1: Part Sketch / Geometric Constraints.
Pure Elastic 2D Beam Bending Using Numerical Methods
CMP Modeling – Current Status Goal is to develop a comprehensive CMP model that complements experimental program Begin with hydrodynamic slurry flow model.
HEAT TRANSFER FINITE ELEMENT FORMULATION
BUDAPEST UNIVERSITY OF TECHNOLOGY AND ECONOMICS ELECTRONICS TECHNOLOGY DEPARTMENT Final Report Rev.: Dr. László Jakab, László Milán.
1 Challenge the future The Lateral Motion of Wafer under the Influence of Thin-film Flow Leilei Hu Solid and Fluid Mechanics
Aaron Aoyama 1, J. Blanchard 2, N. Ghoniem 1, S. Sharafat 1* 1 University of California Los Angeles 2 University of Wisconsin Madison With Contributions.
Numerical simulation of droplet motion and two-phase flow field in an oscillating container Tadashi Watanabe Center for Computational Science and e-Systems.
DCLL ½ port Test Blanket Module thermal-hydraulic analysis Presented by P. Calderoni March 3, 2004 UCLA.
CFD Study of the Development of Vortices on a Ring Wing
Some slides on UCLA LM-MHD capabilities and Preliminary Incompressible LM Jet Simulations in Muon Collider Fields Neil Morley and Manmeet Narula Fusion.
MOTION OF ERYTHROCYTES ALONG THE CAPILLARIES Alexander V. Kopyltsov.
Workshop 2 Steel Bracket Modified by (2008): Dr. Vijay K. Goyal Associate Professor, Department of Mechanical Engineering University of Puerto Rico at.
APPLICATION TO EXTERNAL FLOW
Appendix A.
Optimization of planar pixel detector. T. Habermann Planar pixel detectors L W H ground U.
Universität Dortmund Fakultät für Mathematik IAM technische universität dortmund A numerical set-up for benchmarking and optimization of fluid-structure.
Tony Arts Carlo Benocci Patrick Rambaud
Mesh Refinement: Aiding Research in Synthetic Jet Actuation By: Brian Cowley.
Date of download: 6/23/2016 Copyright © ASME. All rights reserved. From: Computational Fluid Dynamics Investigation of Turbulent Flow Inside a Rotary Double.
AERODYNAMIC OPTIMIZATION OF REAR AND FRONT FLAPS ON A CAR UNIVERSITY OF GENOVA – POLYTECHNIC SCHOOL ADVANCED FLUID DYNAMICS COURSE 2015/2016 Student: Giannoni.
Date of download: 9/19/2016 Copyright © ASME. All rights reserved. From: Numerical Analysis for Elucidation of Nonlinear Frictional Characteristics of.
Qs. 1 on VI The coefficient of dynamic viscosity values for a high grade oil and a low grade oil at 40 oC are 15 cp and 60 cp respectively. It is required.

WORKSHOP 7 LINEAR CONTACT
Numerical Modeling for Hydraulic Fracture Prediction on Fused Silica Surrogate Cylindrical Samples Varun Gupta.
Hamdache Abderrazaq 1*, Belkacem Mohamed 1, Hannoun Nourredine 2
Continuum Mechanics (MTH487)
Date of download: 10/14/2017 Copyright © ASME. All rights reserved.
Date of download: 10/22/2017 Copyright © ASME. All rights reserved.
Shear in Straight Members Shear Formula Shear Stresses in Beams
Poisson’s Ratio For a slender bar subjected to axial loading:
Mechanical Properties
FEA Analysis of the LHCB Velo RF foil
Outer Shell (fuel grain housing) Inner Shell (NOS/rocket housing)
FLAT PLATE COLUMN BUCKLING
Linear Kinematics of Human Movement
Multi-physics Simulation of a Wind Piezoelectric Energy Harvester Validated by Experimental Results Giuseppe Acciani, Filomena Di Modugno, Ernesto Mininno,
ENFORCED MOTION IN TRANSIENT ANALYSIS
Panel Methods.
Fluent Overview Ahmadi/Nazridoust ME 437/537/637.
MAE 5130: VISCOUS FLOWS Examples Utilizing The Navier-Stokes Equations
BDA30303 Solid Mechanics II.
Poisson’s Ratio For a slender bar subjected to axial loading:
Chrono::FEA Validation.
Ch. 2: Fundamental of Structure
Current Model Model is 2D. FIDAP equates force and moment on the wafer surface and rotates the wafer into equilibrium.
Phoebus 2A, Nuclear Thermal Element
Mesh Control using Size Functions and Boundary Layers
OVERVIEW OF FINITE ELEMENT METHOD
Poisson’s Ratio For a slender bar subjected to axial loading:
Subject Name: FLUID MECHANICS
National Chung Cheng University
Finite Element Modelling in Geosciences FEM in 2D for viscous materials Introduction to Finite Element Modelling in Geosciences Summer 2018.
Presentation transcript:

FIDAP Numerical Modeling Scott Taylor

List of Topics Fixed Gap – Rigid Pad Fixed Gap – Deformable Pad Modified Step Free Surface Integration

1. Fixed Gap – Rigid Pad Model Length = 10 mm Rigid Pad no deformation Step dimensions 10 μm high 1 mm long Gap thickness = 20 μm

Boundary Conditions Velocity (x,y) Slurry Properties Pad = (0.278, 0) m/s or --- 70 RPM Wafer = (0) m/s Inlet/Outlet = (--, 0) m/s Slurry Properties Density = 1164 kg/m^3 Viscosity = 2 cp

Fixed Gap Width: 10 μm step Wafer Pad Fixed Gap Width: 10 μm step

Results Results for streamline, UX, UY are as expected. A change in magnitude of velocity only results in magnitude change of solution. Pressure contours need to be investigated.

Pressure Contour Large pressure variation at step face High (Low) pressure ‘pocket’ offset from corner Couette flow (no step) run as validation. No abnormal results Step sensitivity study

Step Sensitivity Step height increased to 30 μm. All other conditions the same

Step Sensitivity Step height decreased to 3 μm. All other conditions the same

Step Sensitivity Unexpected pressure contour most likely the result of sharp geometric discontinuity and not a genuine solution. Possible way to reduce is to introduce sloping sides, rather than sharp corner.

2. Fixed Gap – Deformable Pad Pad now modeled as a continuum instead of a line boundary. Pad Properties – Homogeneous & Isotropic Density = 630 kg/m^3 Young’s Modulus = 20 - 40E6 Mpa Poisson’s ratio = 0.3

Model WAFER SLURRY INLET OUTLET PAD Model is NOT to scale

Boundary Conditions Old method – Minimal BC UX wafer = 0.84 m/s UY inlet/outlet = 0 m/s DX/DY bottom of pad = 0 m Lack of BC’s allow FIDAP to get smoother results. Create ‘edge effects’ that are undesirable.

Boundary Conditions – New Method Pad given velocity Model ‘attachment’ of pad boundary to continuum help attain convergence. BC additions: UX pad = 0.278 m/s DY/DX pad bottom = 0 m: DY pad sides (left & right) = 0 m UX/UY wafer = 0 m

Discontinuity more apparent, but edge effects are eliminated, which will help with free surface integration.

General Results Deformation in X, Y directions small Order of nanometers Depends on E, υ, velocity Pressure Contours similar to rigid pad Deflections don’t appear to affect pressure distribution

3. Modified Step Slope given to step to reduce any errors due to discontinuity. Old New Angle reduced to 45 degrees from 90. NOTE: Currently, any model with the modified step has more nodes than the older model, but resolution near the step is decreased.

Pressure contour now located around step.

Deflection in Ydirection is very similar to 90 deg. step. Other results are as expected.

4. Free Surface FIDAP capable of coupling pad deformation with a movable wafer Force balance Moment balance Attempts to use ‘standard’ free surface rigid body motion unsuccessful. Solution diverges Model database related

Free Surface - Subroutine Using USRBCN user subroutine, surface position can be modified explicitly. Subroutine currently being written to work with wafer ‘step’. Subroutine successful for a flat wafer.

USRBCN Problems Not robust Substantial computational time Error prone Model locked Nodes Geometry Parameter changes difficult Substantial computational time Error prone Potential to inadvertently modify solution arrays

To Do Finish writing subroutine for models. Determine grid dependence. Gather results for variety of conditions. Complete thesis/manual

Backup Slides