2005 grey cast iron cylinder presentation

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    Grey Iron Cylinder InoculantFloat

    Joe Licavoli Aaron Lueker

    Dan SeguinPaul NelsonTerri Mullen

    Andrew Zeagler

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    Process Grey Iron was cast into many

    different cylindrical moldswith varying height; 6,12, and20in

    Inoculant was added to themelt to initiate nucleationsites for graphite flakes toform in the solid

    The uniformity of flakesaffects the mechanicalproperties of the material

    Type D/E Flakes 20 m Scale Bar

    Type A/B Flakes 20 m Scale Bar

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    Initial Defective Iron Sample

    The hollow areainside of the solidifiediron sample is where

    the Ferro-Silicateinoculant coagulated,leaving it un-reactedwith the iron.

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    Considerations for the Grey IronCasting Process

    Solidification - The cylinder may take too long tosolidify, giving the inoculant the opportunity tofloat

    Flotation - The inoculant may flow almostcompletely to the surface before reacting withthe melt

    Dissolution - The radius of the inoculant affectsits flotation. Since dissolution affects radius,dissolution may, in turn, affect flotation

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    Our Groups Problems to solve

    Grey Iron Cylinderproblems

    Solidification Flotation Dissolution

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    Solidification

    Chvorinovs rule used to determinesolidification time.

    Solidification from top determined usingNewtons Law of cooling. Inconsistencies in calculation with reality. Did not account heat flow from sides through

    top.

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    Solidification from Mold Walls

    Calculate energy conducted away from themetal to the mold during solidification

    Excess energy had two sources From the phase transformation From superheating

    This energy had to be conducted away fromthe metal through mold surfaces

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    Solidification from the Mold Wall

    Chvorinovs rule yields the following equationfor time through Fouriers Law of Conduction:

    Time comes out to be 8.9 minutes

    t s T p M Q t T p 2

    T m T o 2

    22 A

    2 M2

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    Effect of Pour Temperature

    1400 1600 1800520

    530

    540

    ts T p

    T

    Notice: Not very temperature dependent

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    Solidification from Top

    Heat dissipated by convection through top of mold Modeled using Newtons Law of Cooling

    Heat flux found, multiplied by solidification time and

    energy liberated to find depth of solidification as afunction of pour temperature

    D sol T p qV m

    C Metal T p T m A m1

    H f Metal t im

    D sol 1773K ( ) .529

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    Inconsistencies

    The calculated solidification distance fromthe top was inconsistent with actual results 1.5- 2.5 in reality

    Rough estimate from casting

    Did not account for heat flow from sides

    through top Limited models for heat transfer coefficient in

    calculating heat flux

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    Magmasoft Simulations Modeled solidification to

    understand where inoculantswould have the most time to float

    Limitations of the universitiesversion of Magmasoft did not

    allow for the modeling of the Ironcontaining inoculant particles

    Knowing the temperature andgeometries of the un-solidifiedsections as time passes could

    allow for a more accuratecalculation of final inoculantdistribution

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    Cooling Rate Control of Flake Spacing

    Flake spacing is controlled bycooling rate

    Since the cylinder has a constant

    cooling rate, there is uniform flakespacing throughout the cylinder

    This would be a good medium toattempt an experiment todetermine the relationship ofinoculant mixing time vs. flakespacing (i.e. fade)

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    Simulated Inoculant Mixing

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    Flotation

    The inoculant is mixed in with the liquidgrey iron as it is poured into the transfercrucible

    From here it is poured into the desiredmold

    As the mold solidifies, the particles ofinoculant begin to float because they areless dense than the grey iron

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    Flotation contd.

    The following calculations were used fromexample 3.3 (Gaskell)

    Terminal Velocity-

    Also the critical radius for flotation can be

    found by

    R T p L x 9 v t T p L x

    2 Metal Inoculent g.

    v t T p L x L xt s T p L

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    Flotation contd. With this data we can also find the Reynolds

    number which will show whether the flow islaminar or turbulent

    The Reynolds number will be less than 0.1,exhibiting laminar flow. (This confirms that ourequation for terminal velocity is valid)

    R e T p L x 2 R T

    p L x

    v

    t T

    p L x

    Metal

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    Flotation cont.

    Figure F.1 In this figure the

    critical particle

    radius is found asthe length of thecylinder isincreased 0 0.1 0.2 0.3 0.4 0.55 10

    6

    1 10 5

    1.510 5

    2 10 5

    2.510 5

    2.325 10 5

    9.181 10 6

    R T p

    L x

    0.60.015 L

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    Flotation Results

    Flotation problems -Most of the particles

    floated to the

    surface withoutreacting with thegrey iron melt

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    Dissolution

    Changes in particle diameter may influenceflotation time

    Dissolution equation derived from analogous

    heat transfer equations in Gaskell

    R t

    h D Isi Lsi atSI

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    Dissolution contd.

    Equations derived from Gaskell lead tosolution for mass transfer coefficient h D

    hD

    2 .4 R e T p L x 0.5

    .06R e T p L x 2

    3

    1

    poise

    2.410 9

    .4

    s

    .25

    2 R T p L x DSi

    s

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    Problems with Result

    Calculations do not agree with experiment Unavailable ternary phase diagram forced

    approximation from binary phase diagram

    Viscosity difference is unknown

    hD

    2 .4 R e T p L x 0.5

    .06R e T p L x 2

    3

    1

    poise

    2.410 9

    .4

    1

    1

    .25

    2 R T p L x DSi

    R th D Isi Lsi

    atSI

    Particle radius ~tenths of mm

    R = .2363 mm/s

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    A More Likely Explanation

    Interfacial resistance may account fordifferences

    Solidification at inoculant surface mayserve as a barrier to further atomicdiffusion

    Conclusion: Better numbers andconsideration of interfacial resistancecould accurately model dissolution.

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    Conclusions Based on solidification model in conjunction withflotation model, inoculant particles in our

    particular application would have ample time tofloat.

    The flotation of incoculant did in fact lead to thenumerous pores located on the surface of thecylinder.

    Dissolution could be a huge factor in removing

    inoculant from the molten iron before it floated,but interfacial considerations need to be taken tounderstand the complete dynamics.

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    References

    Metal Casting Handbook For MY4130 byKarl B. RundmanDavid R. Gaskell An Introduction to

    Transport Phenomena in MaterialsEngineering

    SAH Free Consulting Firm Bring all yourproblems to me, Ill help ya out. unless

    yer a union guy The offices of Lord Chadwick Boyle III & Sir

    Chester Fairfax.

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    Questions

    ?????