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Numerical prediction of ice accretion based on LES and LPT
R. SZASZ, L. FUCHS, LUND UNIVERSITY, SWEDEN             WINTERWIND2013, ÖSTERSUND, 2013.02.12-13




                                              Goals                        Strategies
                                              • Develop tool to model      Ice shape     Flow
                                                simultaneously flow and
                                                ice accretion
                                                                              Flow      Ice shape
                                                   • Efficient
                                                   • Flexible
                                              • Validate                   Flow & Ice shape
                                              • Check sensitivity

Flow: LES + Im.Bound.


                                                           Droplets: LPT
                           Accretion: Impacting
                           droplets freeze
                           instantaneously
Numerical prediction of ice accretion based on LES and LPT
R. SZASZ, L. FUCHS, LUND UNIVERSITY, SWEDEN                   WINTERWIND2013, ÖSTERSUND, 2013.02.12-13


Flow                                     Droplet transport                       Ice accretion
•   Incompressible Navier Stokes         •   Lagrangian Particle Tracking        •   All droplets impacting on the
•   Finite Differences (3rd, 4th)        •   Typically low LWC                       surface freeze instantaneously
•   3D, time resolved                    •   Only drag force                             – Rime-ice conditions
        • LES (implicit)                 •   No collision                                – For other conditions heat
•   Efficient solver                     •   No break-up                                     transfer must be included
        • Equidistant Cartesian grid     •   Release: rectangular area, random   •   Distance from distance function
•   Complex geometries                       distribution                            used for IBM
        • Immersed Boundary              •   Removal: accretion or max streamwise        – Efficient but slightly lower
                                             position                                        accuracy
         Ut                                                                      •   Critical distance
                                         •   Impact parameters logged
                                                                                         – dcr=f∆
    Uc
          d


          ∆
          S i ≈ (uiT − uiL )e − Cd
                                     2
Numerical prediction of ice accretion based on LES and LPT
R. SZASZ, L. FUCHS, LUND UNIVERSITY, SWEDEN            WINTERWIND2013, ÖSTERSUND, 2013.02.12-13

                                              Problem set-up
                                              •    ’In-fog icing event 2’ [Hochart2008]
                                                  Parameter                     Value
                                                  Profile                       NACA 63415
                                                  Angle of attack               3̊
                                                  LWC                           0.37g/m3
                                                  MVD                           27.6 µm
                                                  Vrel                          18.7 m/s
                                                  Re                            2.49e5
                                                  Time                          10.6 min
 Case    f        ∆                               Mass of accreted ice          24±1.75 g
 B       1.0      7.81e-3                                   •   Nondimensional
                                                                     – Chord length 0.2 m
 G1      1.0      1.25e-2                                   •   Slightly smaller domain
 G2      1.0      2.08e-2                                            – 1.5x2.5 vs 2.5x3.0
                                                            •   Shorter time
 F1      0.75     7.81e-3                                   •   Extrapolated in time and space
 F2      0.50     7.81e-3                                   •   Top-hat velocity profile
                                                            •   Uniform droplet diameter
                                                            •   At least 20+10 TU
Numerical prediction of ice accretion based on LES and LPT
   R. SZASZ, L. FUCHS, LUND UNIVERSITY, SWEDEN   WINTERWIND2013, ÖSTERSUND, 2013.02.12-13

    Sample results
Not scaled




f=0.5




f=1.0
Numerical prediction of ice accretion based on LES and LPT
R. SZASZ, L. FUCHS, LUND UNIVERSITY, SWEDEN   WINTERWIND2013, ÖSTERSUND, 2013.02.12-13




    Future work
    •   Other icing regimes
           • Heat transfer                          •   Exaggerated testcase
                                                           • Coarse grid
    •   Combine with other existing
                                                           • Huge droplets
        models                                      •   Goal
           • FSI                                           • Illustrate methodology
           • Noise                                         • Test robustness

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Szasz robert

  • 1. Numerical prediction of ice accretion based on LES and LPT R. SZASZ, L. FUCHS, LUND UNIVERSITY, SWEDEN WINTERWIND2013, ÖSTERSUND, 2013.02.12-13 Goals Strategies • Develop tool to model Ice shape Flow simultaneously flow and ice accretion Flow Ice shape • Efficient • Flexible • Validate Flow & Ice shape • Check sensitivity Flow: LES + Im.Bound. Droplets: LPT Accretion: Impacting droplets freeze instantaneously
  • 2. Numerical prediction of ice accretion based on LES and LPT R. SZASZ, L. FUCHS, LUND UNIVERSITY, SWEDEN WINTERWIND2013, ÖSTERSUND, 2013.02.12-13 Flow Droplet transport Ice accretion • Incompressible Navier Stokes • Lagrangian Particle Tracking • All droplets impacting on the • Finite Differences (3rd, 4th) • Typically low LWC surface freeze instantaneously • 3D, time resolved • Only drag force – Rime-ice conditions • LES (implicit) • No collision – For other conditions heat • Efficient solver • No break-up transfer must be included • Equidistant Cartesian grid • Release: rectangular area, random • Distance from distance function • Complex geometries distribution used for IBM • Immersed Boundary • Removal: accretion or max streamwise – Efficient but slightly lower position accuracy Ut • Critical distance • Impact parameters logged – dcr=f∆ Uc d ∆ S i ≈ (uiT − uiL )e − Cd 2
  • 3. Numerical prediction of ice accretion based on LES and LPT R. SZASZ, L. FUCHS, LUND UNIVERSITY, SWEDEN WINTERWIND2013, ÖSTERSUND, 2013.02.12-13 Problem set-up • ’In-fog icing event 2’ [Hochart2008] Parameter Value Profile NACA 63415 Angle of attack 3̊ LWC 0.37g/m3 MVD 27.6 µm Vrel 18.7 m/s Re 2.49e5 Time 10.6 min Case f ∆ Mass of accreted ice 24±1.75 g B 1.0 7.81e-3 • Nondimensional – Chord length 0.2 m G1 1.0 1.25e-2 • Slightly smaller domain G2 1.0 2.08e-2 – 1.5x2.5 vs 2.5x3.0 • Shorter time F1 0.75 7.81e-3 • Extrapolated in time and space F2 0.50 7.81e-3 • Top-hat velocity profile • Uniform droplet diameter • At least 20+10 TU
  • 4. Numerical prediction of ice accretion based on LES and LPT R. SZASZ, L. FUCHS, LUND UNIVERSITY, SWEDEN WINTERWIND2013, ÖSTERSUND, 2013.02.12-13 Sample results Not scaled f=0.5 f=1.0
  • 5. Numerical prediction of ice accretion based on LES and LPT R. SZASZ, L. FUCHS, LUND UNIVERSITY, SWEDEN WINTERWIND2013, ÖSTERSUND, 2013.02.12-13 Future work • Other icing regimes • Heat transfer • Exaggerated testcase • Coarse grid • Combine with other existing • Huge droplets models • Goal • FSI • Illustrate methodology • Noise • Test robustness