Heat Transfer in Solid and Fluids

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    Heat Transfer in Solid and Fluids

    John Dunec

    COMSOL 

    © 2013 COMSOL. COMSOL, COMSOL Multiphysics, Capture the Concept and COMSOL Desktop are registered trademarks ofCOMSOL AB. LiveLink is a trademark of COMSOL AB. Other product or brand names are trademarks or

    registered trademarks of their respective holders.

    Jon Ebert

    SC Solutions 

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    Agenda

    • Multiphysics and the Power of COMSOL

    • An Overview of Heat Transfer with COMSOL

     –

    Conduction / Convection / Radiation – Coupling Heat Transfer with other Physics

    • Thermal Modeling of a CVD Reactor

     –

    Video Demo

    • Q&A Session

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    Multiphysics: Multiple Interacting Phenomena

    Could be simple

    • Heat convected by Flow

    Could be complex

    • Local temperature sets

    reaction rates

    • Multiple exothermic reactions

    • Convected by flow in pipes

    and porous media

    • Viscosity strongly temperature

    dependent

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    COMSOL Multiphysics® Solves These!

    • Multiphysics  – Everything can link to everything

    • Flexible  – You can model just about anything

    • Usable  – You can keep your sanity doing it

    • Extensible  – If its not specifically there…add it! 

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    All Inclusive Interactive Modeling Environment

    Model Builder

    Provides instant

    access to any part of

    the model settings

    • CAD/Geometry• Materials

    • Physics

    • Mesh

    • Solve

    • Results

    Graphics

    Ultrafast graphic presentation, stunning

    visualization, and multiple plots

    COMSOL Desktop®Straightforward to

    use, it gives full

    insight and control

    over the modeling

    process

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    Product Suite

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    Anywhere you can type a number or an equation

    • …Or an interpolation function 

    • And it can depend on anything known in your problem

    Example: Concentration-dependant viscosity

    221001.0   c 

    Low concentration,

    High velocity

    High concentration,

    Low velocity

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    Add Your Own Equations to COMSOL’s 

    Don’t see what you need? 

    Add your own equation

    ODE’s • PDE’s 

    • Weak form PDE’s 

    Just type them in

    • No Recompiling

    • No Programming

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    Interface with CAD, Excel and MATLAB

    • CAD import

    • LiveLink for CAD softwares

    • LiveLink for  Excel

    LiveLink for  MATLAB

    Pacemaker Electrode Modeled with LiveLink™  for  SolidWorks®

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    Support for High-Performance Computing

    Multi-Core Parallel Computing

    • No Extra Charge

    • Fully Supported on all Licenses

    Cluster Parallel Computing

    • No Extra Charge

    • Requires Floating Network License

    • Freq Sweep / Parametric Sweep

    • Distributed Single Large Problem

    Solvers

    • Direct / Iterative - Fully Coupled / Segregated

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    Conjugate heat transfer around an

    aluminum heat sink

    Heat Transfer in COMSOL Multiphysics

    Used on its Own

    • Conduction

    • Thermal Radiation

    • Thin Conductive Media and Resistive Layers

    Linked to Flow• Conduction-Convection

    • Laminar / Turbulent

    • Porous Media

    • Bioheat Equation

    Linked to Other Physics

    • Structural mechanics

    • Electromagnetics

    • … 

    Temperature of a disc brake of a car in brake-

    and-release sequence

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    Light Bulb: All Forms of Heat Transfer

    • 60 W filament heats rapidly over the first seconds

    • Induces a flow driven by natural convection

    • Conduction / Convection / Radiation

    t=0.1 sec t=6 sec t=60 s

    Temperature Velocity Temperature Velocity Temperature Velocity

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    Laser Heating: Surface Heating

    • Define Surface Flux hf(x,y)

    • Multiply by emissivity

    Laser Intensity - Gaussian

    Wafer spinning,

    Laser moving back

    and forth

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    Phase Change:

    Boiling

    • Two Phase Flow with Heat Transfer

    • Use Phase Field for 2-Phase Flow

    Heat: 105 W/m3

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    Heat Transfer Linked to Other Physics

    • Electrical, Mechanical, Fluid, Chemical, Acoustic

    • Anything can link to anything!

    Microwave heating in a waveguide – Skin depth heating of copper plated waveguide

     – Volumetric heating of dielectric block

     – Properties of block are temperature dependent

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    Joule Heating

    • Volts x Amps = Power

    • Power goes to heat

    • Heat expands metal

    Current Direction, Isotherms

    Temperature [C], Deformation (10x)Current Density from 0.2 volts across resistor

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    Magnetic Induction Heating

    • Furnace reactor that heats a susceptor of graphite, using an 8

    kW RF signal at 20 kHz

    • Used in the fabrication of semiconductors to grow layers on

    wafers

    Surface Plot

    • Temperature

    Contours

    • Temperature

    Arrow Plot

    • B-field

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    Exothermic / Endothermic Reactions

    Three Physics: Flow / Heat / Convection-Diffusion with Reactions

    • Flow

    • Temperature WITHOUT exothermic reaction

    •Temperature WITH exothermic reaction

    Heater lifts T over activation energy Higher Temperature speeds reaction

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    Chemical Heating

    Heat from Curing Reaction After 700 sec

    Temperature Profile After 750 sec

     P  M M A  C  e m e

     n t  

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    SC SOLUTIONS

    Thermal Modeling of a CVD Reactor

    Case Study: Temperature Control of a Cold-wall Vertical

    CVD Reactor with Rotating Susceptor

     Jon Ebert

    SC Solutions, Inc.

    1261 Oakmead Pkwy., Sunnyvale, CA 94085

    Email: [email protected] 

    COMSOL Webinar

    March 7, 2013

    Copyright© 2013, SC Solutions, Inc. All Rights Reserved  20

    SC S l ti

    mailto:[email protected]:[email protected]

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    SC SOLUTIONS

    SC Solutions

    Engineering firm in Silicon Valley – 40 employees

    Structural Division Founded in 1989

    Control Division Founded in 1996

    o Engineering Consulting

    Using models for equipment design

    o Feedback Control Software for Semiconductor Industry

    Using models for equipment control

    o Contract Research

    COMSOL® Certified Consultant, MathWorks® Partner.

    Copyright© 2013, SC Solutions, Inc. All Rights Reserved  21

    MATLAB is a registered trademark of The MathWorks, Inc.

    O i

    http://www.mathworks.com/products/connections/product_detail/service_35810.html

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    SC SOLUTIONS

    Overview

    Overview of Chemical Vapor Deposition (CVD)

    o Chemical process for growing thin solid films

    Metal-organic Chemical Vapor Deposition (MOCVD)

    o CVD with metal-organic precursors (e.g., tri-methyl Gallium)

    o Used to manufacture Light Emitting Diodes (LEDs)

    A Case Study of Temperature Control of a Rotating Susceptor CVD Reactoro Show how we use COMSOL and Livelink for Matlab in concert with optimization and

    control tools.

    o Evaluate design limits for a range of operating conditions.

    Summary

    Copyright© 2013, SC Solutions, Inc. All Rights Reserved  22

    Ch i l V D iti

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    SC SOLUTIONS

    Chemical Vapor Deposition

    Process by which a thin solid film is formed on a surface (e.g., wafer) from gas-

    phase precursors via chemical reactions.

    Used for growing high-purity crystalline layers, typically semiconductor

    multilayers.

    Copyright© 2013, SC Solutions, Inc. All Rights Reserved  23

    Susceptor 

    Wafer Wafer 

    Wafer 

    Heater Coils

    Heater Coils

    Gas flow

    Wafer  Wafer 

    Wafer Wafer 

    Process Gas Entry

    Rotating HeatedSusceptor 

    Process Gas Entry

    Wafer 

    Rotating HeatedSusceptor 

    Gas Exit

    Horizontal Reactor

    Vertical Reactor

    Pancake Reactor

    MOCVD for LEDs

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    SC SOLUTIONS

    MOCVD for LEDs

    MOCVD is used to produce Light Emitting Diodes (LEDs) by

    reacting metal-organic precursors (e.g.,tri-methyl Gallium, tri-

    methyl Indium, etc.).

    Increasingly important for many applications (LED TV’s,

    Lighting, etc.) due to potential for high efficiency.

    InGaN/GaN multiple quantum well (MQW) structures are

    grown on sapphire substrates for green, blue, and white LEDs.

    Copyright© 2013, SC Solutions, Inc. All Rights Reserved  24

    Studies* have shown that LED properties such as photoluminescence and

    electroluminescence can vary by a factor of two if the substrate temperature is

    changed from 1000°C to 1030°C.

    Involves many process steps over a wide temperature range (500-1100°C).

    As a result, real-time control  of substrate temperature to within 1°C or less is

    essential for repeatable manufacturing of LEDs with desired color .

    * For example, see J. W. Ju, et al., “Effects of p-GaN Growth Temperature on a Green InGaN/GaN Multiple Quantum

    Well,” Journal of the Korean Physical Society, Vol. 50, No. 3, March 2007, pp. 810-813.

    Wikipedia

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    SC SOLUTIONS

    A Case Study

    Temperature Control of a Rotating Susceptor, Cold-wall

    MOCVD System

    Copyright© 2013, SC Solutions, Inc. All Rights Reserved  25

    COMSOL Model

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    SC SOLUTIONS

    COMSOL Model

    Copyright© 2013, SC Solutions, Inc. All Rights Reserved  26

    CVD Surface

    A vertical reactor with top-side showerhead and rotating susceptor.

    The temperature on the CVD Surface is critically important

    Cold walls

    “Showerhead” 

    2D Axisymmetric COMSOL model –  Non-isothermal flow, with swirl and buoyancy.

    Example Operating Conditions

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    SC SOLUTIONS

    Example Operating Conditions

    Copyright© 2013, SC Solutions, Inc. All Rights Reserved  27

    Hydrogen is the main carrier gas (no reactions, only heat transfer).

    Nominal operating temperature is 1100°C.

    Susceptor rotation rate = 100 RPM

    Operating pressure range is 100 Torr ≤ p ≤ 500 Torr (1 Atm = 760 Torr)

    Operating flow rate range is 5 slm ≤ Q ≤ 50 slm (slm = standard liters per minute)

    Required temperature uniformity of ± 0.5°C (over widest possible area of susceptor)

    The goal is to adjust the control flux, q(r), to get good temperature

    uniformity on the CVD Surface.

    Pressure (Torr)

       F    l   o   w   r   a   t   e    (   S   L   M    )

    5

    50

    100 500

    Process

    Window

    Heat Transfer

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    SC SOLUTIONS

    Heat Transfer

    Gas Convection and Conduction

    o The cold gas (27°C) is injected at the showerhead

    o Convective cooling flux of the susceptor is of order 10 4 W/m2 

    o qc  = h(T sus-T wall  ), h is of order 10-100 W/m2°C

    Radiation

    o qr  = (T sus4 –  T wall 

    4 ), = effective emissivity, = Stefan-Boltzmann constant.

    o Radiation losses are of order 10 5 W/m2 

    o Radiation does not vary with flow rate or pressure.

    Conduction

    o Gas conduction is fairly high for Hydrogen (compared to other gases)

    o Solid conduction in susceptor is important, especially if we heat from backside.

    The distribution of heat transfer at the CVD surface varies with flow rate and

    pressure due to changes in convection heat transfer.

    Copyright© 2013, SC Solutions, Inc. All Rights Reserved  28

    Heater Zone Definition

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    SC SOLUTIONS

    Heater Zone Definition

    It is common to divide the control flux into a number of independently controlled

    “zones”. 

    Here we divide the control flux into six independent zones.

    o Uniformly divided along the radius

    o Heaters can be made in many ways

    Resistive films

    Lamp arrays

    Hot filaments

    RF Inductive elements

    Copyright© 2013, SC Solutions, Inc. All Rights Reserved  29

    This is the system to be controlled

    Surface temperature

    Heater zones

    Gas inflow

       A   x

       i   s   o    f   R   o   t   a   t   i   o   n

    CVD Surface

    The Control Problem

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    SC SOLUTIONS

    The Control Problem

    The controller, C, adjusts the flux, q, to make the temperature T on the CVD

    surface uniform at the reference temperature, Tref .

    This is a form of the “inverse problem”. 

    (What inputs do I need to produce a given output?)

    Real-time feedback is a common method of dynamically solving this problem.

    Copyright© 2013, SC Solutions, Inc. All Rights Reserved  30

    Controller CVD System

    Feedback

    (1100°C)

    For this demo, we will focus on steady-state, but the same methods are used to solve the time-

    varying dynamic control problem (e.g., uniformity during temperature ramp, stabilization, etc).

    COMSOL®Matlab®LiveLink for Matlab

    Baseline System Performance

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    SC SOLUTIONS

    Baseline System Performance

    Copyright© 2013, SC Solutions, Inc. All Rights Reserved  31

    Normalized power commands

    100 Torr, 50 slm 32 degC

     5  x  p o w e r  o

     nz  o n e 6 

    Temperature on CVD Surface

    Edge cold, can

    we do better?

    Optimal Control

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    SC SOLUTIONS

    Optimal Control

    Copyright© 2013, SC Solutions, Inc. All Rights Reserved  32

    In words:

    Find the input control flux, q, for each heater that produces the besttemperature uniformity.

    subject to the constraint that q ≥ 0 

    the uniformity is optimized over limited radius (r < Rmax).

    Mathematically:

    How Many Independent Heaters do we Need?

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    SC SOLUTIONS

    How Many Independent Heaters do we Need?

    In practice, for each independent heater we need an another power supply and

    an another temperature sensor – adding heaters is expensive.

    We want as few as possible.

    We also want uniformity over the largest possible radius (Rmax).

    Can we make ONE heater work for the entire operating range of pressure andflow rate?

    Strategy: fix the ratio of each heater power from baseline optimal result (100Torr,

    50slm) and scale this power distribution up and down with one input scaling.

    o This ratio can be done in hardware (e.g., filament density distribution, or resistancevariation, etc.)

    o One zone control requires only one temperature sensor.

    Copyright© 2013, SC Solutions, Inc. All Rights Reserved  33

    Optimizing Rmax (6-zone control)

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    SC SOLUTIONS

    Optimizing Rmax (6 zone control)

    Copyright© 2013, SC Solutions, Inc. All Rights Reserved  34

    It is only possible to get

    the inner 0.13m radius

    within the design limits.

    Rmax = 0.13 m

    Rmax = 0.15m

    If we try to optimize T for the

    whole radius (0

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    SC SOLUTIONS

    One zone Control

    We found the “optimal” Rmax to produce the largest area of temperature within

    design limits.

    Next we want to optimize the input flux distribution for different operating

    conditions.

    First we look at 1-zone control, then look at the improvement of increasing the

    number of independent control zones.

    Copyright© 2013, SC Solutions, Inc. All Rights Reserved  35

    One Zone Control

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    SC SOLUTIONS

    One Zone Control

    Copyright© 2013, SC Solutions, Inc. All Rights Reserved  36

    In all cases the mean

    temperature optimized for

    r

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    SC SOLUTIONS

    Lower Pressure Flow fields (100 Torr)

    Copyright© 2013, SC Solutions, Inc. All Rights Reserved  37

    100 Torr, 50 slm

    Baseline case.

    100 Torr, 5 slm

    For slower flow we start to see

    some “lift” of the streamlines

    at larger radius.

    Higher Pressure Flow fields (500 Torr)

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    SC SOLUTIONS

    Higher Pressure Flow fields (500 Torr)

    Copyright© 2013, SC Solutions, Inc. All Rights Reserved  38

    500 Torr, 50slm

    Buoyancy driven recirculation is

    causing a significant

    redistribution of the convective

    losses.

    500 Torr, 5slm

    Buoyancy driven recirculation

    even more complex here.

    1-zone control cannot work

    for this range of operating

    conditions.

    Two-zone Control

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    SC SOLUTIONS

    Two zone Control

    Copyright© 2013, SC Solutions, Inc. All Rights Reserved  39

    Group q1-q5 as one zoneq6 is second zone

    Much better, but still

    not within design

    limits.

    Both 100 Torr

    processes are close to

    being within the design

    limits.

    Temperature 2-zone Control

    Six-zone Control

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    SC SOLUTIONS

    Six zone Control

    Copyright© 2013, SC Solutions, Inc. All Rights Reserved  40

    Temperature Uniformity vs Number of Control Zones

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    SC SOLUTIONS

    e pe atu e U o ty s u be o Co t o o es

    Copyright© 2013, SC Solutions, Inc. All Rights Reserved  41

    Summary

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    SC SOLUTIONS

    y

    This case study illustrates how COMSOL can be used in concert with SC control

    tools to evaluate optimal closed-loop performance of a system.

    In this particular case study, the results point to a need to eliminate “roll cells” in

    the flow, either by changing the geometry, increasing the flow rate, or increasing

    the rotation rate.

    Demo will show:

    o Livelink for Matlab is a very powerful feature of COMSOL, allowing use of control tools

    that have been developed over many years.

    o The “swirl” feature in COMSOL is very important for these types of problems where

    models must be run many times.

    Copyright© 2013, SC Solutions, Inc. All Rights Reserved  42

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    Video Demo

    • Please wait while the content is

    loading… 

    • Applications shown in the demo

     – 3D swirling flow over a hot susceptor

     – 2D swirling flow over a hot susceptor

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    SC SOLUTIONS

    Thermal Modeling of a CVD Reactor

    Case Study: Temperature Control of a Cold-wall Vertical

    CVD Reactor with Rotating Susceptor

     Jon Ebert

    SC Solutions, Inc.

    1261 Oakmead Pkwy., Sunnyvale, CA 94085

    Email: [email protected] 

    COMSOL Webinar

    March 7, 2013

    Copyright© 2013, SC Solutions, Inc. All Rights Reserved  44

    mailto:[email protected]:[email protected]

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    Product Suite

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    • Register to our free hands-onworkshops at

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    Try COMSOL Multiphysics®

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     – Toronto, ON

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     – Richardson, TX

    • Europe – Nürnberg-Erlangen, Germany – Saint Martin d'Hères, France – Brno, Czech Republic – Uppsala, Sweden – Helsinki, Finland – London, United Kingdom – Wien, Austria – Trondheim, Norway – Cranfield, United Kingdom – Zilina, Slovakia

    • Register to our free hands-onworkshops at

    www.comsol.com/events 

    http://www.comsol.com/eventshttp://www.comsol.com/events

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    Contact Us

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    Q&A Session