FIDAP Numerical Modeling

30
FIDAP Numerical Modeling Scott Taylor

description

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. - PowerPoint PPT Presentation

Transcript of FIDAP Numerical Modeling

Page 1: FIDAP Numerical Modeling

FIDAP Numerical Modeling

Scott Taylor

Page 2: FIDAP Numerical Modeling

List of Topics

1. Fixed Gap – Rigid Pad2. Fixed Gap – Deformable Pad3. Modified Step4. Free Surface Integration

Page 3: FIDAP Numerical Modeling

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

Page 4: FIDAP Numerical Modeling

Boundary Conditions

Velocity (x,y) 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

Page 5: FIDAP Numerical Modeling

Fixed Gap Width: 10 μm step

Pad

Wafer

Page 6: FIDAP Numerical Modeling

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.

Page 7: FIDAP Numerical Modeling
Page 8: FIDAP Numerical Modeling

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

Page 9: FIDAP Numerical Modeling

Step Sensitivity

Step height increased to 30 μm.

All other conditions the same

Page 10: FIDAP Numerical Modeling

Step Sensitivity

Step height decreased to 3 μm.

All other conditions the same

Page 11: FIDAP Numerical Modeling

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.

Page 12: FIDAP Numerical Modeling

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

Page 13: FIDAP Numerical Modeling

Model

SLURRY

WAFER

INLET OUTLET

PAD

• Model is NOT to scale

Page 14: FIDAP Numerical Modeling

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.

Page 15: FIDAP Numerical Modeling
Page 16: FIDAP Numerical Modeling

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

Page 17: FIDAP Numerical Modeling

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

Page 18: FIDAP Numerical Modeling

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

Page 19: FIDAP Numerical Modeling

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.

Page 20: FIDAP Numerical Modeling

Pressure contour now located around step.

Page 21: FIDAP Numerical Modeling

Deflection in Ydirection is very similar to 90 deg. step.

Other results are as expected.

Page 22: FIDAP Numerical Modeling

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

Page 23: FIDAP Numerical Modeling

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.

Page 24: FIDAP Numerical Modeling

USRBCN Problems Not robust

Model locked Nodes Geometry

Parameter changes difficult Substantial computational time Error prone

Potential to inadvertently modify solution arrays

Page 25: FIDAP Numerical Modeling

To Do

Finish writing subroutine for models.

Determine grid dependence. Gather results for variety of

conditions. Complete thesis/manual

Page 26: FIDAP Numerical Modeling

Backup Slides

Page 27: FIDAP Numerical Modeling
Page 28: FIDAP Numerical Modeling
Page 29: FIDAP Numerical Modeling
Page 30: FIDAP Numerical Modeling