Cyclone - JK.pdf

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  • Hydrocyclones

  • Hydrocyclones

    Hydrocyclones

    O 1. Cyclone Operating VariablesO 2. Efficiency CurvesO 3. Nageswararao ModelO 4. Fish Hook EffectO 5. Density EffectsO 6. Fitting the ModelO 7. Limitations of the Model

  • Hydrocyclones

    Hydrocyclone Terminology

    Feed inlet

    Conical section

    Apex

    Cylindrical section

    Vortex finder

    Feed chamber

  • Hydrocyclones

    Hydrocyclone Flow Patterns

    Feed

    Overflow

    Underflow

    Inner flow spiral(upwards)

    Outer flow spiral(downwards)

  • Hydrocyclones

    Forces on Particles

    O CentrifugalO DragO Gravity

  • Hydrocyclones

    Separation VariablesParticle Properties

    O size O shape O s.g.

  • Hydrocyclones

    Separation VariablesFluid Properties

    O density O solids presentO viscosity

  • Hydrocyclones

    Separation VariablesMachine Properties

    O inlet area O diameterO cylinder lengthO cone angle O vortex finder diameter O spigot diameter O vortex finder lengthO angle of inclination

  • Hydrocyclones

    Efficiency Curves - I

    0.00.10.20.30.40.50.60.70.80.91.0

    0.01 0.10 1.00 10.00

    Size (mm)

    F

    r

    a

    c

    t

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    n

    t

    o

    C

    o

    a

    r

    s

    e

    ActualEfficiency

    Curve

  • Hydrocyclones

    Efficiency Curves - II

    0.00.10.20.30.40.50.60.70.80.91.0

    0.01 0.10 1.00 10.00

    Size (mm)

    F

    r

    a

    c

    t

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    n

    t

    o

    C

    o

    a

    r

    s

    e

    D50 Act

    Actual

    WaterSplit

  • Hydrocyclones

    Short Circuit Model

    Feed

    CoarseProduct

    FineProduct

    ShortCircuit

    TrueClassification

    Remainder

  • Hydrocyclones

    Efficiency Curves - III

    0.00.10.20.30.40.50.60.70.80.91.0

    0.01 0.10 1.00 10.00

    Size (mm)

    F

    r

    a

    c

    t

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    n

    t

    o

    C

    o

    a

    r

    s

    e

    D50 Act

    D50 Corr

    ActualCorrected

  • Hydrocyclones

    Efficiency Curves - IV

    0.00.10.20.30.40.50.60.70.80.91.0

    0.1 1 10

    D/D50c

    F

    r

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    c

    t

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    n

    t

    o

    C

    o

    a

    r

    s

    e

    ReducedEfficiencyCurve

  • Hydrocyclones

    Efficiency Curve Model - I

    2)(

    )1(C = E50

    )50o(

    +

    ee

    e

    cddcd

    d

  • Hydrocyclones

    Efficiency Curve - Varying

    0 .0

    0 .1

    0 .2

    0 .3

    0 .4

    0 .5

    0 .6

    0 .7

    0 .8

    0 .9

    1 .0

    1 1 0 1 0 0 1 0 0 0

    S iz e ( m )

    F

    r

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    t

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    t

    o

    F

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    n

    e

    0 .2 50 .512357 .51 0

  • Hydrocyclones

    Reduced Efficiency Constant for a Given Mineral

  • Hydrocyclones

    D50 Equation

    65.0 01

    15.02.05.0

    12

    )((93.0

    47.052.0

    250 22.0

    =

    =

    =

    DKK

    DL

    DDKK

    DDu

    DDK

    Dd

    DD

    c

    c

    c

    iDD

    gDP

    cc

    oD

    c

    c

    cp

  • Hydrocyclones

    Recovery to Underflow - I

    22.024.0

    50.0

    12

    27.053.040.219.1

    2 )(

    c

    c

    c

    iww

    cpc

    u

    c

    owf

    DL

    DDKK

    gDP

    DD

    DDKR

    =

    =

  • Hydrocyclones

    Recovery to Underflow - II

    22.024.0

    25.0

    12

    31.083.194.0

    2 )(

    c

    c

    c

    ivv

    cpc

    u

    c

    ovv

    DL

    DDKK

    gDP

    DD

    DDKR

    =

    =

  • Hydrocyclones

    Pressure-ThroughputEquation

    1.0 01

    2.01.045.012

    68.05.02

    )()(

    )()(2

    =

    =

    =

    cQQ

    c

    c

    cQQ

    c

    o

    pcQ

    DKK

    DL

    DDiKK

    DDPDKQ

  • Hydrocyclones

    Fish Hook Effect - I

    0

    0.2

    0.4

    0.6

    0.8

    1

    10 100 1000Size (m)

    F

    r

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    t

    o

    F

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    e

  • Hydrocyclones

    Fish Hook Effect - IIO Exaggerated in graphO Assumed originally to be caused by changing

    size measurement techniqueO With advent of wide size range measurement

    techniques (Laser etc) - phenomenon really occurs sometimes

    O Assumptions about short-circuiting of particles with water breaking down

    O High viscosity and large cyclones???

  • Hydrocyclones

    Efficiency Curve Model - II

    E = C(1+

    o( )d

    d cc

    dd c

    dd

    e

    e e50

    50

    50

    1

    2

    +

    *

    *

    )( )

    ( )

  • Hydrocyclones

    Efficiency Curve - Varying

    0 .0

    0 .2

    0 .4

    0 .6

    0 .8

    1 .0

    1 .2

    1 .4

    0 .1 0 1 .0 0 1 0 .0 0 1 0 0 .0 0 1 0 0 0 .0 0S ize (m )

    F

    r

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    c

    t

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    n

    t

    o

    F

    i

    n

    e

    0 .00 .20 .51 .02 .0

  • Hydrocyclones

    JKSimMet Cyclone Parameters - I

    Geometry Data

  • Hydrocyclones

    JKSimMet Cyclone Parameters - II

    Model Parameters

  • Hydrocyclones

    JKSimMet Cyclone Parameters - III

    Performance Data

  • Hydrocyclones

    SG Effects - 1

    0.00.10.20.30.40.50.60.70.80.91.0

    10 100 1000

    Size (m)

    F

    r

    a

    c

    t

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    o

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    t

    o

    F

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    e

    GalenaSphaleriteSilica

    d50c (Ga) d50c (Sp) d50c (Si)

  • Hydrocyclones

    SG Effects - 2

    0.00.10.20.30.40.50.60.70.80.91.0

    10 100 1000

    Size (m)

    F

    r

    a

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    t

    i

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    n

    t

    o

    F

    i

    n

    e

    GalenaSphaleriteSilicaAverage

    d50c (Ga) d50c (Sp) d50c (Si)

  • Hydrocyclones

    O KD0 depends on feed solids characteristics only -size & sg

    D50 Equation - II

    cc dmd 50mineral

    feed50

    1-sg1-sg =)(

  • Hydrocyclones

    Fitting the Cyclone Model - I

    O Use measured pressure wherever possibleO If in doubt about measured pressure, compare

    with manufacturers tablesO Make sure the Measured Pressure is available to

    Model Fitting by activating it on the Equipment Data Tab of the Model Fit Dialog window

    O Typical values of KQ0 are 300 - 600

  • Hydrocyclones

    Fitting the Cyclone Model - II

    O KD0 is typically 0.001 - 0.00001O Actual water split to O/F is fitted rather than

    KV1 and KW1 (both controlled by the water split)O You can calculate an estimate of the water split

    from the mass balanced water flow dataO Always fit the Water Split

  • Hydrocyclones

    Fitting the Cyclone Model - III

    O If the fit is poor at fine sizes, try setting to 0.1. If this improves the fit, then fit .

    O Plotting and inspecting the efficiency curve will help (Remember that you need data in the cyclone feed combiner port to plot efficiency curves)

  • Hydrocyclones

    Design Considerations - I

    O Cut Size Cyclone Diameter

    smaller > finer

    Operating Pressure higher > finer

    Feed Density lower > finer

    Inclination flatter > coarser

  • Hydrocyclones

    Design Considerations - II

    O Water split to overflow higher > more efficient90% not usually achievable

  • Hydrocyclones

    Design Considerations - III

    O Feed Size coarse feeds limit water split to O/F fine feeds increase viscosity cant create fine material in cyclone

    O Pressure controls wear in pump and cyclone trade-off between wear and operational flexibility

  • Hydrocyclones

    Design Considerations - IV

    O Operation at high overflow density capital v operating trade off

    capital thickeners are expensive

    operating higher operating pressure smaller cyclones larger mill

  • Hydrocyclones

    Cyclone Model Limitations I

    O Feed size effect As the feed becomes coarser, d50c tends to decrease

    even when all the other variables are kept constant.O Efficiency curve equation

    The analytic form used does not provide a perfect representation for the reduced efficiency curve.

  • Hydrocyclones

    Alternative Efficiency Curve Model

    d/d50(corrected)

    %

    o

    f

    F

    e

    e

    d

    t

    o

    O

    v

    e

    r

    f

    l

    o

    w

    (

    c

    o

    r

    r

    e

    c

    t

    e

    d

    )

    0

    20

    40

    60

    80

    100

    120

    140

    160

    180

    0.00 0.50 1.00 1.50 2.00 2.50

    Efficy. curve at 0.33xd50c

    Efficy. curve at d50c

    Efficy. curve at 0.66xd50c

  • Hydrocyclones

    Cyclone Model Limitations II

    O Viscosity Viscosity variations due to changes in pulp density

    are largely accounted for by the model. Viscosity variations caused by variable quantities of

    slimes affect the parameters in quite a systematic way.

  • Hydrocyclones

    Cyclone Model Limitations III

    O Increasing viscosity causes coarser cut size water split to overflow reduced pressure drop increased reduced efficiency curve constant till roping

  • Hydrocyclones

    Cyclone Model Limitations IV

    O Effect of roping cut size increased by 5 to 10 alpha value reduced to 0.1 - 0.2 water split not affected much pressure drop not affected much inclination allows operation at higher underflow

    density before roping

  • Hydrocyclones

    Cyclone Model Limitations V

    O Prediction of roping difficult SPOC constraint

    feed density

    Plitt constraint underflow size distribution

    O JKSimMet warns when either constraint is violated

  • Hydrocyclones

    Cyclone Model Limitations VI

    O SPOC Constraint

    at sg 2.7 at sg 4.0Feed

    DensityUnderflow

    DensityFeed

    DensityUnderflow

    DensityFeed

    DensityUnderflow

    Density% by Volume % by Weight % by Weight5 53 12.4 75.3 17.4 81.8

    10 54 23.1 76.0 30.8 82.415 55 32.3 76.7 41.4 83.020 56 40.3 77.5 50.0 83.625 57 47.4 78.2 57.1 84.130 58 53.6 78.8 63.1 84.735 59 59.2 79.5 68.3 85.2

  • Hydrocyclones

    Cyclone Model Limitations VI

    O SPOC Constraint

    at sg 2.7 at sg 4.0Feed

    DensityUnderflow

    DensityFeed

    DensityUnderflow

    DensityFeed

    DensityUnderflow

    Density% by Volume % by Weight % by Weight5 53 12.4 75.3 17.4 81.8

    10 54 23.1 76.0 30.8 82.415 55 32.3 76.7 41.4 83.020 56 40.3 77.5 50.0 83.625 57 47.4 78.2 57.1 84.130 58 53.6 78.8 63.1 84.735 59 59.2 79.5 68.3 85.2

  • Hydrocyclones

    Cyclone Model Limitations VI

    O SPOC Constraint

    at sg 2.7 at sg 4.0Feed

    DensityUnderflow

    DensityFeed

    DensityUnderflow

    DensityFeed

    DensityUnderflow

    Density% by Volume % by Weight % by Weight5 53 12.4 75.3 17.4 81.8

    10 54 23.1 76.0 30.8 82.415 55 32.3 76.7 41.4 83.020 56 40.3 77.5 50.0 83.625 57 47.4 78.2 57.1 84.130 58 53.6 78.8 63.1 84.735 59 59.2 79.5 68.3 85.2

  • Hydrocyclones

    Cyclone Model Limitations VII

    O Plitt constraint

    Roping onset% Solids by Vol.

    Underflow50% passing (m)

    % Solidsat sg 2.7

    % Solidsat sg 4.0

    35.2 50 59.4 68.539.0 60 63.3 71.945.9 80 69.6 77.250.5 100 73.4 80.353.9 120 75.9 82.458.6 170 79.3 85.060.0 200 80.2 85.761.3 250 81.0 86.4

  • Hydrocyclones

    Cyclone Model Limitations VII

    O Plitt constraint

    Roping onset% Solids by Vol.

    Underflow50% passing (m)

    % Solidsat sg 2.7

    % Solidsat sg 4.0

    35.2 50 59.4 68.539.0 60 63.3 71.945.9 80 69.6 77.250.5 100 73.4 80.353.9 120 75.9 82.458.6 170 79.3 85.060.0 200 80.2 85.761.3 250 81.0 86.4

  • Hydrocyclones

    Cyclone Model Limitations VII

    O Plitt constraint

    Roping onset% Solids by Vol.

    Underflow50% passing (m)

    % Solidsat sg 2.7

    % Solidsat sg 4.0

    35.2 50 59.4 68.539.0 60 63.3 71.945.9 80 69.6 77.250.5 100 73.4 80.353.9 120 75.9 82.458.6 170 79.3 85.060.0 200 80.2 85.761.3 250 81.0 86.4