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CCC Annual Report UIUC, August 20, 2014 Yonghui Li Department of Mechanical Science & Engineering University of Illinois at Urbana-Champaign Modeling SEN Preheating University of Illinois at Urbana-Champaign Metals Processing Simulation Lab Yonghui Li 2 Objectives Develop an accurate preheating model to optimize preheating process: Fuel composition; Preheating time; Torch configuration; – Insulation; Refractory conductivity. Obtain air entrainment, flow and temperature distributions from combustion model. Evaluate Flame Temperature Model (in spread-sheet).

Modeling SEN Preheatingccc.illinois.edu/s/2014_Presentations/16_Li-Y... · 2014. 8. 18. · Modeling SEN Preheating ... a chemical equilibrium program which can predict adiabatic

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  • CCC Annual ReportUIUC, August 20, 2014

    Yonghui Li

    Department of Mechanical Science & EngineeringUniversity of Illinois at Urbana-Champaign

    Modeling SEN Preheating

    University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Yonghui Li • 2

    Objectives

    • Develop an accurate preheating model to optimize preheating process:– Fuel composition;– Preheating time;– Torch configuration;– Insulation;– Refractory conductivity.

    • Obtain air entrainment, flow and temperature distributions from combustion model.

    • Evaluate Flame Temperature Model (in spread-sheet).

  • University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Yonghui Li • 3

    Burner tip

    TC 1 SEN

    TC 5TC 3

    TC 4 TC 6

    Gas temperature

    Wall temperature

    Premixed natural gas(mainly CH4)/ O2

    Two-port SEN

    Preheating experiment setup[1]

    Stand-off distance

    97

    197

    341

    Unit: mm

    324oC

    249oC

    174oC

    23oC

    91oC

    Infra-red photo of SEN outside wall

    University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Yonghui Li • 4

    Measurements[2] (for model validation)2. Wall temperature (transient are not listed here. )

    1. Gas temperature 197mm below SEN top

    3. The shape of flame

    4. SEN outside wall temperature

    324oC

    249oC

    174oC

    23oC

    91oC

    Thermocouple

    TC3 TC4 TC5 TC6

    X* (mm) 394 538 394 538

    Y* (mm) 48 48 69 69

    Temp. (oC) 584 554 453 397

    X: Distance from top air inlet;Y: Distance from SEN centerline.

  • University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Yonghui Li • 5

    Thermal – Flow Model

    • FLUENT simulation is 2D axisymmetric. – The two-port SEN is simplified as a ring shaped port with the

    same exit area.• The burner tip is assumed as annular shape with 3× bigger area.

    – To avoid supersonic and mesh refinement at burner tip, accounting for gas expansion.

    24*1.6mm diameter

    1*0.8mmdiameter

    Simplified as

    Mixture inlet

    17.4mm diameter of outer ring of holes

    Rosebud tip surface

    University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Yonghui Li • 6

    Model geometry and mesh97mm Validation Case 147mm Case

    1-mm coating layer with 4 cells through thickness

    Stand-off distance

    88843 quadrilateral cells total

    14797

    Insulation Case

  • University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Yonghui Li • 7

    Material Properties

    • Flow • SEN [1,4,5]

    0

    5

    10

    0 200 400 600 800 1000 1200

    Ther

    mal

    Con

    duct

    ivity

    (W

    /m-K

    )

    Temperature (°C)

    50010001500200025003000

    0 200 400 600 800 1000 1200Spe

    cific

    Hea

    t (J/

    kg-K

    )

    Temperature (°C)

    16% Porosity Doloma-Graphite

    Glaze

    Glaze

    16% Porosity DG

    Gas average [3]thermal conductivity2.7006 W/mK viscosity 9.32×10-5 kg/m

    Species thermodynamic properties: thermo.db

    University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Yonghui Li • 8

    Key features--combustion

    • Non-premixed species model. • Fuel inlet: perfectly mixed CH4 and O2 in

    1:2 mole ratio in a total mass flow rate of 3.8 g/s[2].

    • Ambient air entrainment.• Non-adiabatic energy treatment.• GRI-Mech 3.0[6] natural gas combustion

    mechanism, contains 325 reactions and 53 species.

    8

  • University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Yonghui Li • 9

    Model validation

    9

    University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Yonghui Li • 10

    Temperature across SEN: 97mm Validation Case

  • University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Yonghui Li • 11

    Temperature across SEN: High-k Refractory Case

    Outer glaze

    SEN outer wall

    SEN refractory wall

    Nozzle inner bore with gasInner glaze

    SEN inner wall

    Measured TC3

    TC 3-5line at 5min

    TC5TC6TC4

    TC 3-5line at 10min

    TC 3-5& 4-6 line at SS

    University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Yonghui Li • 12

    Temperature across SEN: Insulation Case

  • University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Yonghui Li • 13

    Transient temperature validation

    TC 3 error= 25oCTC 4 error= 45oC

    TC 5 error= 32oC

    TC 6 error= 83oC

    Error causes:

    • Excessive thermal conductivity/diffusivity due to uncertain refractory properties

    • Neglect of Zirconia sleeve at lower part of SEN

    • Neglect of contact resistance at TC tip0 10 20 30 40 50 60 70 80 90 100 110

    0

    100

    200

    300

    400

    500

    600

    700

    S

    EN

    wal

    l tem

    pera

    ture

    (°C

    )

    Time (min)

    TC3 MEASURE TC4 MEASURE TC5 MEASURE TC6 MEASURE TC3 FLUENT TC4 FLUENT TC5 FLUENT TC6 FLUENT

    University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Yonghui Li • 14

    Flame shape & Outer wall temperature contour validation

    Flame shape comparisons of predicted temperature contours and close-up

    photographSEN outer wall temperature comparison

  • University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Yonghui Li • 15

    Model Parametric study

    15

    University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Yonghui Li • 16

    Inputs of 4 cases

    Model Inputs97mm

    Validation Case

    147mm Case

    Insulated Case

    High-kCase

    Thermal conductivity DG, Glaze DG, Glaze

    DG, Glaze, Insulation DG, Glaze

    Specific heat DG, Glaze DG, Glaze DG, Glaze, Insulation DG, Glaze

    Stand-off distance 97mm 147mm 97mm 97mm

    Insulation layer No No Yes No

  • University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Yonghui Li • 17

    Flow distribution

    Velocity (m/s)

    (a) Direction arrows in the whole domain (b) Velocity vector inside SEN

    (c) Zoom-in vector near SEN top

    60 m/s

    5 m/s

    147mm Case

    97mm Case 147mm Case

    Air entrainment154% 135%

    Stand-off distance

    Flame spreads

    Air entrainment

    Flame temperature97mm Validation Case

    University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Yonghui Li • 18

    Temperature distribution

    (d)

    (a) 97mm Validation Case(b) 147mm Case

    (c) Insulation Case(d) High-k Refractory Case

    (c)(b)(a)

    Temperature (oC)

  • University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Yonghui Li • 19

    Transient temperature comparisons among 4 cases

    0 10 20 30 40 50 60 70 80 90 100 1100

    200

    400

    600

    800

    1000

    1200

    SE

    N w

    all t

    empe

    ratu

    re (°

    C)

    Time (min)

    Measure TC3 Measure TC5 97mm Case TC3 97mm Case TC5 147mm Case TC3 147mm Case TC5 High-k Refractory Case TC3 High-k Refractory Case TC5 Insulation Case TC3Insulation Case TC5

    University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Yonghui Li • 20

    Flame Temperature Modelin Excel VBA

    20

  • University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Yonghui Li • 21

    Flame Temperature Model(VBA)

    InputsFuel typeOxygen sourceOxygen source fractionAir entrainmentReactants temperatureReactants pressure

    OutputsFlame/Products temperatureProducts pressureSpecies componentProducts propertiesForce convection coefficient Free convection coefficient

    Gaseq[7]

    • Gaseq[7]: a chemical equilibrium program which can predict adiabatic temperature and composition at constant pressure.

    • Oxygen Source Fraction = mole of oxygen inputmole of oxygen required for stoichiometric reaction

    • Air Entrainment = mole of entrained airmole of air needed for stoichimetric reaction

    University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Yonghui Li • 22

    Flame Temperature Model Results

    Simple spread-sheet model can predict flame temperature approximately without sophisticated chemical reactions and thermal hydraulic models.

    Air entrainment

    Oxygen sourcefraction

    Reactants Temp.

    Flame Temp.

    Flametemp.

    97mm Validation Case 154% 100% 19 oC 1328 oC 1343oC

    147mm Case 135% 100% 19 oC 1451 oC 1587oC

    MeasurementCombustion

    Model ResultComb.Model

    Reactants, products pressure is 1atm.

  • University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Yonghui Li • 23

    Conclusions• A 2D axisymmetric model of nozzle preheating is developed, including

    325 chemical reactions with 53 species of methane combustion.• Steady-state fluid flow, heat transfer and gas combustion, and transient

    heat conduction in the SEN walls are simulated. • The model predictions were validated with a preheating experiment,

    including the gas temperature across the flame, SEN wall temperature histories, flame shape, and SEN outer wall temperature distribution.

    • Moving the burner further away from the SEN top leads to higher SEN temperature, due to flame expansion causing less air entrainment.

    • Adding an insulation layer causes higher SEN wall temperatures and milder temperature gradients.

    • Increasing refractory conductivity causes milder temperature gradient at SEN.

    • To optimize preheating, a proper stand-off distance, stoichiometric fuel composition, proper refractory thermal properties , and insulation layers are recommended.

    • A simple spread-sheet model of the adiabatic flame temperature predicts gas temperature approximately, based on knowing the air entrainment.

    University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Yonghui Li • 24

    Acknowledgements

    • The authors are grateful to R. Nunningtonand other personnel at Magnesita Refractories for providing the measurement data.

    • The authors appreciate the support from the Continuous Casting Consortium at the University of Illinois.

  • University of Illinois at Urbana-Champaign • Metals Processing Simulation Lab • Yonghui Li • 25

    References[1] R. Nunnington, Magnesita Refractories, private communication, Jun, Aug 2012 [2] Magnesita Refractories, PB10 SEN Temperature Data for CCC Heat Flow Model, Report, York, March 31st, 2010[3] FLUENT 13.0[3] Charles E. Heat Transfer in Industrial combustion, p469[4] T. Shimizu, Thermal conductivity of high porosity alumina refractory bricks made by a slurry gelation and foaming method, Journal of the European Ceramic Society, 2013[5] Hayashi K, Fujino Y, Nishikawa T. Thermal conductivity of Aluminiumand Zirconia fiber insulators at high temperature. Yogyo Kyokai Shi 1983;91:450–6.[6] Gregory P. Smith, David M. Golden, Michael Frenklach, Nigel W. Moriarty, Boris Eiteneer, Mikhail Goldenberg, C. Thomas Bowman, Ronald K. Hanson, Soonho Song, William C. Gardiner, Jr., Vitali V. Lissianski, and Zhiwei Qin http://www.me.berkeley.edu/gri_mech/[7] Gaseq, Chemical equilibrium program, available at http://www.gaseq.co.uk/[8] Y. Li, MS Thesis, Transient Model of Preheating a Submerged Entry Nozzle, 2014