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          FLOTHERM Advanced Training Course7-12

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          AdvancedTraining_11_Compact_Models.pdf
          Compact Models,Advanced Resistances

          Compact Representation
          of Heat Sinks
          -Why Compact Representation in System Level Model?
          – Faster Solution
          – Less Grid
          – Fewer Iterations - Simplified Conjugate Heat Transfer Problem
          – Much Easier to Work With and Debug Compact Representation of Heat Sinks
          -Attributes of a Good Heat Sink Compact Model:
          – Preserve the Flow Characteristics Through and Around the Heat Sink
          – Correct Pressure Drop (Contraction, Expansion, Friction)
          – Correct Bypass to Sides and Top
          – Preserve the Conduction Characteristics in the Heat Sink Base and Fins (Heat Sink Efficiency)
          – Preserve the Convection Effects of the Base and Fins. (Forced or Natural Convection)
          - The Heat Sink SP Compact Model Provides a Good representation of these attributes and saves modeling and solve time for System Level Modeling

          -The Pressure Drop Terms Include:
          – Sudden Contraction Entrance Collapsed Resistance.
          – Sudden Expansion Collapsed Resistance for Exit and Top.
          – Volume Resistance for the Laminar or Turbulent Frictional Flow in the Heat Sink Channels
          - Heat Transfer is Treated Using a Volumetric Based Heat Transfer Coefficient. This Coefficient is a Function of Flow Rate for Turbulent Flow and Constant for Laminar.
          - The Heat Transfer Model Does Not Account For Fin Efficiency. Under Predicts Base Temperature for Highly Convective Cases Where Fins Are Thin.

          Compact Representation of
          Heat Sinks
          - Option 2: Approximation Based on Computational or Physical Wind Tunnel Characterization
          – Represent Heat Sink Base As a Conducting Cuboid
          – Perform(Separate) Computational/Physical Wind Tunnel Analysis to Determine Flow Impedance Characteristics of Fins
          – Account for Impedance of Heat Sink Fins With Volume Resistance in System Level Model
          – Account for Heat Dissipation of Fins with Volume Heat Transfer Coefficient in System Level Model
          Resistance and

          -Option 2: Approximation Based on Computational Wind Tunnel Characterization (Cont.)
          – Duct Detailed Fins (Only) of Heat Sink With Computational Domain: Use Symmetry Faces on 4 Long Sides and Open Faces on Ends
          – Extend the Computational Domain as Shown
          – Use Fixed Flow Device and Collapsed Resistance (or Nothing) for Ends

          Wind Tunnel Characterization (Cont.)
          – Use ΔP vs. V Data to Define Equivalent Non-Collapsed Resistance
          – Can Use Advanced Resistance Attribute (When ΔP Is Not α V2
          – Refer to Resistance Calculation Slides Later in this Lecture)
          – Typically Use Standard Resistance Attribute (Iteratively If ΔP Is Not α V2)

          – Replace Detailed Fins (Cuboids) With Non-Collapsed Resistance
          – Re-Run One Case to Ensure that Computed ΔP’s for Detailed and Compact Models Agree

          Modeling Grilles, Filters and
          Other Flow Resistances
          - Use a (Collapsed or Non-Collapsed) Resistance With Appropriate
          Loss Coefficient
          - Recall, Definition of Loss Coefficient
          Δp = f (ρv2/2) (Collapsed)
          Δp/Δx = fx (ρv2/2) (Non-Collapsed)
          Δp/Δy = fy (ρv2/2) (Non-Collapsed)
          Δp/Δz = fz (ρv2/2) (Non-Collapsed)
          where:
          v = velocity (device or approach)
          f = loss coefficient

          Modeling Flow Resistances
          - Available Loss Coefficient Options
          – Standard
          – Assumes Δp α v2
          – Constant Loss Coefficient f
          – Advanced
          – Allows complicated Δp dependence on v
          – Loss Coefficient f not Constant
          f = a/Re + b/Reα
          in which,
          f = loss factor (as before)
          Re = ρUL/μ = Reynolds No. based on
          a user specified length scale
          a,b,α = constants specified by the user

          Modeling Flow Resistances
          - Where Do I Get Loss Coefficients?
          – Reference Texts, e.g., Fried and Idelchick
          – Manufacturer Data
          – Perform Computational Wind Tunnel Analysis on Device
          - Advice on Loss Coefficients
          – Use Standard Model If You Have ΔP~V2
          – Most Turbulent, High Re Flows
          – Use Advanced Model If You Have ΔP~V, ΔP~V1.7, etc.
          – Laminar and Transitional, Lower Re Flows
          – Can Always Use Standard Model If You’re Willing to Iterate

          Example: Given ΔP=kV
          -This Case is Typical for Laminar Flow
          - If Resistance Can Be Modeled As “Thin”:
          – Resistance Type: Planar
          – Loss Coefficients Based On: Approach Velocity
          – Resistance Formula: Advanced
          – Length Scale (L): 1 m
          – A Coefficient: (2 L k)/μ
          – B Coefficient: 0
          – Index: 0

          Other Compact Models
          The Flow Losses and Heat Addition of All Components/Modules in the Analysis Need to be Accounted For.
          - In Cases Where the Details of those Components Are Not Important, the Above is Still True.
          - Create Compact Models for These:
          – Guess the Losses and Heat (Typically Early in Concept Design and Optimization)
          – Use a Combination of Collapsed or Volumetric Resistances With Associated Sources.
          – Create Detailed Windtunnel Models of Modules, Characterize for Losses and Create Good Compact Models. (Later when more information is available).
          – This Process is Similar to the Manual Heat Sink Compact Model

          Angled Resistances
          -There are 2 Ways to Create this Angled
          Resistance In Flotherm.
          – Use flotherm.com and go to the User Support Center. Choose [Support], Then [Web Parts].
          – Do it Yourself Using the Instructions on the Following Page.

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