film coextrusion troubleshooting 7832

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  • 8/3/2019 Film Coextrusion Troubleshooting 7832

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    FILM COEXTRUSIONA Troubleshooting Guide

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    FILM COEXTRUSION:

    A TROUBLESHOOTING GUIDE

    Paul H. Jackson, Equistar Chemicals, LP

    (This article originally appeared inConverting Magazine, November 1994.)

    Successful production of coextruded products depends on several key factors,including polymer selections, hardware design (screw, feedblock/die, handling

    equipment, layer construction and optimal processing conditions). Proper selectionand adjustment of each factor will minimize difficulties and ensure high quality

    coextrusion results.Troubleshooting methods for coextrusion become increasingly complex as the

    number of layers in the structure increases, as the asymmetry of multi-layer con-struction grows, or as processing and rheological characteristics of coextrudedmaterials differ greatly from one another. Understanding the problems associated

    with nonuniform layer distribution and interfacial instability between layers or onfilm surfaces is very important when troubleshooting the coextrusion process.

    THE UNIFORMITY PROBLEM

    Nonuniform layer distribution is one of the more common problems encoun-

    tered in film coextrusion. This nonuniformity may appear in either the direction ofextrusion or tangential to the direction of film production.

    Layer uniformity in the machine direction can be influenced by die imperfec-

    tions, poor die design or adjustment, excessive extruder pressure variation, variablefilm tension, or film bubble or web instability.

    Layer uniformity tangential to machine direction can be influenced by poormelt temperature uniformity, viscosity mismatch between layers, poor hardware

    design, or viscoelastic f low characteristics induced by excessive shear stress.Poor layer uniformity tangential to machine direction is caused by nonuniform

    melt temperature across a melt pipe, feedblock and/or die, as well as poor melt-ing in an extruder. Melt temperature variance alters viscosity uniformity, whichexhibits a change in flow characteristics and layer distribution. Melt temperature

    of a single polymer stream can of ten vary by as much as 30F. A general rule ofthumb is to achieve 2F or less variation in melt temperature for each extruder.

    Homogenous melt temperatures can be achieved through installation of a staticmixer in the melt pipe, a dynamic mixer on the extrusion screw or a more efficient

    screw design, or through adjustment of pipe, feedblock and/or die temperatures.Variation in the thickness of a film, which eventually reaches a steady-state

    condition of nonuniformity (assuming homogenous melt temperature conditions

    for each polymer), can be caused by a viscosity mismatch between layers. In acoextrusion system, lower-viscosity polymers migrate to the region of highest

    shear stress (nearest the die wall) and tend to encapsulate higher-viscosity poly-mers. The amount of migration is dependent on the degree of viscosity mismatch,

    the length of the flow path, and the shear stress in the system.

    IMPROVING LAYER VARIATION

    Improvements in layer variations that are caused by viscosity-induced flow

    behavior can be achieved through adjustment of melt temperature, modification ofdistribution channels in the feedblock or die, or selection of a polymer with different

    viscosity characteristics which most commonly are measured by melt index. Also,annular dies typically are more tolerant of viscosity mismatch than flat-die systems.

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    Nonuniform layer distribution in the direction tangential to extrusion can also

    be caused by poor hardware design. Improperly designed flow channels of thefeedblock or die can cause poor steady-state layer distribution of materials, evenwith the most closely matched viscosities.

    Nonuniform distribution of layers, in the form of parabolic flow lines, inter-mixing of layers, roughness between polymer boundaries, melt fracture, or

    uncharacteristically high haze, can be caused by interfacial instability between

    layers or on film surfaces. The instabilities are believed to be a result of theviscoelastic behavior of polymers at the die land or region of highest shear stress.Improvements in layer instabilities can be achieved by reducing the shear

    stress between coextrusion layers and/or the die-land surfaces. Shear stress can be

    reduced by decreasing total output rate, increasing skin-layer melt temperature(decrease in viscosity), increasing the die gap, adding a process lubricant to the

    skin material, or selecting a lower viscosity material.An increase in the thickness of the skin layer can also reduce instability

    between polymer layers by moving the interface further from the high-shear-stressdie wall. This is especially significant for asymmetric coextrusion constructions.

    Finally, if coextrusion layers exhibit dramatic differences in melt elasticity, then

    choose materials that match more closely in extrudate elasticity as measured byextrudate swell.

    TROUBLESHOOTING AT A GLANCE

    Problem: Lines in the film surfacePossible cause: Die imperfections

    Solutions: Clean die buildup

    Remove contaminants from polymer melt channel Repair die nicks and burrs

    Problem: Gauge bands on film rollPossible cause: Poor die design

    Solutions:

    Install spiral-channel die design to eliminate weld lines Install rotating nip assembly in tower

    Possible cause: Poor die adjustment

    Solutions: Adjust concentricity of die gap Center air ring in relation to die gap

    Problem: Repeating pattern of variation in thickness of layer(s)

    Possible cause: Excessive extruder pressure variation (surging)Solutions:

    Achieve 1 percent or less variation in total head pressure for each extruder Adjust extruder temperature profile (feed and transition zones) Increase back pressure with restrictor f low plug

    Increase back pressure by installing f ine-mesh screen pack Change screw design of surging extruder(s)

    Check for worn screw(s) and replace if needed Check extruder feedthroat(s) for bridging and correct if needed

    Possible cause: Variable f ilm tensionSolution:

    Eliminate variability in drive speed

    Possible cause: Film bubble instability

    Solutions: Protect bubble from atmospheric air turbulence Correct pressure instability of air ring and/or internal air flow

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    Problem: Intermittent and somewhat random variation in thickness of layer(s)

    Possible cause: Poor melt temperature uniformitySolutions:

    Achieve 2F or less variation in melt temperature for each extruder

    Adjust extruder temperature profile to ensure complete melting ofextrudate

    Install new screw design with dynamic mixer for more eff icient melting

    capacity Reduce screw speed for increased residence time to complete meltingof the polymer(s)

    Adjust temperature of feed channels, die and/or feedblock

    Problem: Variation in thickness of layer(s) that reaches steady-state distribution

    Possible cause: Viscosity mismatch of polymer layersSolutions:

    Select polymers with matching viscosities Adjust temperature of polymers to aid in matching viscosities

    Possible cause: Poor hardware designSolution:

    Change die and/or feedblock design

    Problem: Uncharacteristically high film haze

    Possible cause: Viscoelastic flow characteristics induced by excessive shear stressbetween layers and/or feedblock/die surfaces

    Solutions: Select lower-viscosity skin layer(s) Increase melt temperature of skin-layer polymers

    Increase die temperatures Reduce total extrusion output

    Increase die-gap opening Add process lubricant to skin-layer polymer

    Increase thickness of skin layers Select polymer(s) that exhibit similar melt elasticity behavior

    (extrudate swell)

    Problem: Parabolic-shaped flow lines in direction of extrusionPossible cause: Same as for uncharacteristically high, film-haze problemSolution:

    Same as for uncharacteristically high, film-haze problem

    Problem: Intermixing of polymer layersPossible cause: Same as for uncharacteristically high, film-haze problem

    Solution: Same as for uncharacteristically high, film-haze problem

    Problem: Roughness between polymer-layer boundariesPossible cause: Same as for uncharacteristically high, film-haze problem

    Solution: Same as for uncharacteristically high, film-haze problem

    Problem: Melt fracture of film surfacePossible cause: Same as for uncharacteristically high, film-haze problem

    Solution: Same as for uncharacteristically high, film-haze problem

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    FILM COEXTRUSIONA Troubleshooting Guide

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    Coextrusion Processing Defined

    The conversion of mult iple thermoplast ics,

    f lowing through separate st reams, that are

    combined into a common primary passage and

    then shaped by a die. Multiple layers provide

    propert ies that cannot be provided by a single

    material for high barrier coextrusion processing.

    The main classes are: f ilm; sheet ; tubing;

    coat ing; and blowmolded shapes.

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    Successful Product ion of Coext rudedProducts Depends on Three Key Factors

    1.Polymer Selections

    2.Design of Hardware

    Screws, Feedblock/Die, Handling

    3.Coextrusion Layer Const ruct ion

    4.Opt imal Processing Condit ions

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    Layer Uniformity is Inf luenced by:

    Variations in ext rusion pressure

    Nominal ext rusion melt t emperature

    Viscosity-induced web f low

    Bubble or melt instability

    Variable f ilm tension

    Poor die design or improper adjustment

    Die imperfect ions or contaminants

    Interfacial Flow Instabilityis Caused by:

    Interfacial crit ical shear st ress

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    Extrusion Pressure Variations

    Variation in extrusion pressure, often referred

    to as surging, is directly related to feeding

    stability of an ext ruder.

    Improving layer uniformity caused by pressurevariat ion can be achieved through:

    Adjustment of back pressure

    Screenback

    Rest rictor f low plug

    Ext rusion screw design of feed and t ransit ionsections

    Adjustment of ext rusion screw-temperature

    profile

    Prevent polymer bridging in feedthroat

    Replace/repair worn ext rusion screw

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    Head Pressure Trace

    0 15 30 45 60 75 90 105 120

    TIME (seconds)

    1850

    1840

    1830

    1820

    1810

    1800

    1790

    1780

    1770

    1760

    1750

    HEAD

    PRESSURE

    1805

    1795

    1785

    1775

    1765

    1755

    1745

    1734

    1725

    1715

    1705

    HEAD

    PRESSURE

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    Layer Thickness InstabilityCaused by Pressure Variation

    FLOWDIRECTION

    STABLE FLOW

    Uniform thickness

    ONSET OF INSTABILITY

    Small gauge variat ion

    SEVERE INSTABILITY

    Large gauge variation

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    Extrusion FlangeBack Pressure Adjustment

    ADJUSTABLE VALVE

    INSTRUM ENT PORT

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    Typical Arrangement ofCoarse and Fine Screens Betw een

    the Screw and Breaker Plate

    BREAKERPLATE

    COARSE SCREEN

    FINE SCREENS

    COARSE SCREEN

    RESIN FLOW

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    M elt Temperature Variations

    Nonuniform melt temperature across a melt

    pipe, as well as poor polymer melt ing in an

    extruder, cause poor layer unif ormity.

    Homogenous polymer melt temperatures

    can be achieved through:

    Stat ic and/or dynamic mixers

    Adjustment of pipe and die temperatures

    Adjustment of ext rusion screw temperature

    profile

    Replace/repair worn ext rusion screw

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    414

    410

    406

    402

    398

    F 394

    390

    386

    382

    378

    374

    0 1/8 1/4 3/8 1/2 5/8 3/4 7/8 0

    BARRELWALL

    BARRELCENTER LINE

    BARRELWALL

    Typical Temperature Profileof Polymer M elt Stream in Pipe

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    Layer Thickness Instability Caused byNonuniform M elt Temperature

    FLOWDIRECTION

    STABLE FLOW

    Uniform thickness

    ONSET OF INSTABILITY

    Small gauge variat ion

    SEVERE INSTABILITY

    Large gauge variation

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    Adjustable Depth ProbeM elt Thermocouple

    EXPOSEDTHERMOCOUPLE

    JUNCTION

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    Distributive Mixing Sections

    Dulmadge mixing sect ion (Dow)

    Saxton mixing sect ion (DuPont)

    Pin mixing section (Barmag)

    Pineapple mixing sect ion

    Cavit y-t ransfer mixing sect ion

    (Davis-Standard)

    Slot ted-screw f light (Axon)

    Two types of stat ic mixers(Kenics and Ross ISG)

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    Viscosity Related Behavior

    Melt index select ion and the related viscosit y-

    induced f low behavior affect layer uniformity.

    Improvement of layer variations causedby viscosity-induced flow behavior can be

    achieved through:

    Adjustment of melt t emperature

    Modif icat ion of dist ribut ion channels

    Select polymer of dif ferent viscosity or

    viscoelast ic characterist ic

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    Viscosity-Induced Flow Behavior

    P1

    P2

    P1

    P2

    FLOW DIRECTIONTHROUGH A PIPE

    Migrat ion of low er viscosit y polymer

    to t he region of highest shear st ress.The effect is encapsulation of P2 by P1.

    The amount of migration or encapsulat ionis dependent on the degree of viscositymismatch, the length of the f low path andthe cri t ical shear st ress for the given system.

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    Viscosity vs. Shear Ratefor Various Polymers @ 230C

    100000

    10000

    1000

    100

    10 100 1000 10000SHEAR RATE (1/sec)

    VISCOSITY (poise)

    EVOH

    1.5 MI

    EVOH5.5 MI

    PPHIPS

    LDPE

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    Interfacial Flow Instability

    Excessive shear stress between layers, feedblock

    and/or die surfaces causes interfacial flow

    instability. Drag f low and dif ferences in polymer

    velocities of multiple layers create shear stresses.

    Reduction of interfacial shear stress near a die

    wall can be achieved through:

    Decreasing skin-layer viscosit y or increasing

    melt temperature

    Increasing die temperature

    Increasing skin-layer thickness

    Reducing total ext rusion output

    Increasing die-gap opening Adding process lubricant to skin layer

    Select ing polymers that exhibit similar

    melt elasticity

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    Critical Shear Stress of PolymersViscosity vs. Shear Rate

    Non-Newt onian Behaviorof Polymers

    LOG

    Viscosity(po

    ise)

    Newtonian Fluid Behavior

    Smooth Extrudate

    Irregular Distort ion Occursat Critical Shear Stress

    (Melt Fracture)

    LOG Shear Rate (1/sec)

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    Interfacial Instabilit y in CoextrusionCaused by Critical Shear Stress

    FLOWDIRECTION

    STABLE FLOW

    Smooth interface

    ONSET OF INSTABILITY

    Wavy interface develops

    SEVERE INSTABILITY

    Propagat ion of wavinessto surface

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    Polymer Interfaces and Critical ShearStresses Encountered in Coextrusion

    THEORETICALSHEAR STRESS

    Highest

    Intermediate

    Zero

    METAL

    METAL

    POLYMER 1

    POLYMER 2

    POLYMER 1

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    Coextrusion Melt-Flow Model

    Melt Velocit y

    Shear Rate

    POLYMER 1

    POLYMER 2

    POLYMER 3

    A

    B

    A = Stable Behavior

    B = Crit ical Behavior(Occurrence of Instability)

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    An Important Note

    Pressure variat ion, nonuniform melt

    temperatures, viscosity mismatch and the

    effects of critical shear rate instabilities seldom

    occur independently of one another. They

    most of ten occur simultaneously, wit h variance

    in the degree of severit y.

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    Polyolefins Sales Offices

    National and InternationalSales OfficeEquistar Chemicals, LP1221 McKinney Street, Suite 1600P.O. Box 2583

    Houston, TX 77252-2583Sales(800) 615-8999Customer Service(888) 777-0232

    Plexar is a registered trademark of Equistar Chemicals, LP.

    The information in this document is, to our knowledge, trueand accurate. However, since the particular uses and theactual conditions of use of our products are beyond ourcontrol, establishing satisfactory performance of ourproducts for the intended application is the customerssole responsibility. All uses of Equistar products and anywritten or oral information, suggestions or technical advicefrom Equistar is without warranty, express or implied, andis not an inducement to use any process or product inconflict with any patent.

    Responsible C