Plasticating single-screw extrusion of amorphous polymers: Development of a mathematical model and comparison with experiment

A mathematical model was developed for plasticating single‐screw extrusion of amorphous polymers. We considered a standard metering screw design. By introducing a ‘critical flow temperature’ (Tcf), below which an amorphous polymer may be regarded as a ‘rubber‐like’ solid, we modified the Lee‐Han mel...

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Published inPolymer engineering and science Vol. 36; no. 10; pp. 1360 - 1376
Main Authors Han, Chang Dae, Lee, Kee Yoon, Wheeler, Norton C.
Format Journal Article
LanguageEnglish
Published Hoboken Wiley Subscription Services, Inc., A Wiley Company 01.05.1996
Wiley Subscription Services
Society of Plastics Engineers, Inc
Blackwell Publishing Ltd
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Abstract A mathematical model was developed for plasticating single‐screw extrusion of amorphous polymers. We considered a standard metering screw design. By introducing a ‘critical flow temperature’ (Tcf), below which an amorphous polymer may be regarded as a ‘rubber‐like’ solid, we modified the Lee‐Han melting model, which had been developed earlier for the extrusion of crystalline polymers, to model the flow of an amorphous polymer in the screw channel. Tcf is de facto a temperature equivalent to the melting point of a crystalline polymer. The introduction of Tcf was necessary for defining the interface between the solid bed and the melt pool, and between the solid bed and thin melt films surrounding the solid bed. We found from numerical simulations that (1) when the Tcf was assumed to be close to its glass transition temperature (Tg), the viscosity of the polymer became so high that no numerical solutions of the system of equations could be obtained, and (2) when the value of Tcf was assumed to be much higher than Tg, the extrusion pressure did not develop inside the screw channel. Thus, an optimum modeling value of Tcf appears to exist, enabling us to predict pressure profiles along the extruder axis. We found that for both polystyrene and polycarbonate, Tcf lies about 55°C above their respective Tgs. In carrying out the numerical simulation we employed (1) the WLF equation to describe the temperature dependence of the shear modulus of the bulk solid bed at temperatures between Tg and Tcf, (2) the WLF equation to describe the temperature dependence of the viscosity of molten polymer at temperatures between Tcf and Tg + 100°C, (3) the Arrhenius relationship to describe the temperature dependence of the viscosity of molten polymer at temperatures above Tg + 100°C, and (4) the truncated power‐law model to describe the shear‐rate dependence of the viscosity of molten polymer. We have shown that the Tg of an amorphous polymer cannot be regarded as being equal to the Tm of a crystalline polymer, because the viscosities of an amorphous polymer at or near its Tg are too large to flow like a crystalline polymer above its Tm. Also conducted was an experimental study for polystyrene and polycarbonate, using both a standard metering screw and a barrier screw design having a length‐to‐diameter ratio of 24. For the study, nine pressure transducers were mounted on the barrel along the extruder axis, and the pressure signal patterns and axial pressure profiles were measured at various screw speeds, throughputs, and head pressures. In addition to significantly higher rates, we found that the barrier screw design gives rise to much more stable pressure signals, thus minimizing surging, than the metering screw design. The experimentally measured axial pressure profiles were compared with prediction.
AbstractList A mathematical model was developed for plasticating single-screw extrusion of amorphous polymers. We considered a standard metering screw design. By introducing a "critical flow temperature (T sub cf ), below which an amorphous polymer may be regarded as a "rubber-like" solid, we modified the Lee-Han melting model, which had been develoepd earlier for the extrusion of crystalline polymers, to model the flow of an amorphous polymer in the screw channel. T sub cf is de facto a temperature equivalent to the melting point of a crystalline polymer. The introduction of T sub cf was necessary for defining the interface between the solid bed and the melt pool, and between the solid bed and thin melt films surrounding the solid bed. We found from numerical simulations that (1) when the T sub cf was assumed to be close to its glass transition temperature (T sub g ), the viscosity of the polymer became so high that no numerical solutions of the system of equations could be obtained, and (2) when the value of T sub cf was assumed to be much higher than T sub g , the extrusion pressure did not develop inside the screw channel. Thus, an optimum modeling value of t sub cf appears to exist, enabling us to predict pressure profiles along the extruder axis. We found that for both polystyrene and polycarbonate, T sub cf lies approx55 deg C above their respective T sub g s. In carrying out the numerical simulation we employed (1) the WLF equation to describe the temperature dependence of the shear modulus of the bulk solid bed at temperatures between T sub g and T sub cf , (2) the WLF equation to describe the temperature dependence of the viscosity of molten polymer at temperatures between T sub cf-T sub g +100 deg C, (3) the Arrhenius relationship to describe the temperature dependence of the viscosity of molten polymer at temperatures > T sub g +100 deg C, and (4) the truncated power-law model to describe the shear-rate dependence of the viscosity of molten polymer. We have shown that the T sub g of an amorphous polymer cannot be regarded as being equal to the T sub m of a crystalline polymer, because the viscosities of an amorphous polymer at or near its T sub g are too large to flow like a crystalline polymer above its T sub m . Also conducted was an experimental study for polystyrene and polycarbonate, using both a standard metering screw and a barrier screw design having a length-to-diameter ratio of 24. For the study, nine pressure transducers were mounted on the barrel along the extruder axis, and the pressure signal patterns and axial pressures profiles were measured at various screw speeds, throughputs, and head pressures. In addition to significantly higher rates, we found that the barrier screw design gives rise to much more stable pressure signals, thus minimizing surging, than the metering screw design. The experimentally measured axial pressure profiles were compared with prediction.
Abstract A mathematical model was developed for plasticating single‐screw extrusion of amorphous polymers. We considered a standard metering screw design. By introducing a ‘critical flow temperature’ ( T cf ), below which an amorphous polymer may be regarded as a ‘rubber‐like’ solid, we modified the Lee‐Han melting model, which had been developed earlier for the extrusion of crystalline polymers, to model the flow of an amorphous polymer in the screw channel. T cf is de facto a temperature equivalent to the melting point of a crystalline polymer. The introduction of T cf was necessary for defining the interface between the solid bed and the melt pool, and between the solid bed and thin melt films surrounding the solid bed. We found from numerical simulations that (1) when the T cf was assumed to be close to its glass transition temperature ( T g ), the viscosity of the polymer became so high that no numerical solutions of the system of equations could be obtained, and (2) when the value of T cf was assumed to be much higher than T g , the extrusion pressure did not develop inside the screw channel. Thus, an optimum modeling value of T cf appears to exist, enabling us to predict pressure profiles along the extruder axis. We found that for both polystyrene and polycarbonate, T cf lies about 55°C above their respective T g s. In carrying out the numerical simulation we employed (1) the WLF equation to describe the temperature dependence of the shear modulus of the bulk solid bed at temperatures between T g and T cf , (2) the WLF equation to describe the temperature dependence of the viscosity of molten polymer at temperatures between T cf and T g + 100°C, (3) the Arrhenius relationship to describe the temperature dependence of the viscosity of molten polymer at temperatures above T g + 100°C, and (4) the truncated power‐law model to describe the shear‐rate dependence of the viscosity of molten polymer. We have shown that the T g of an amorphous polymer cannot be regarded as being equal to the T m of a crystalline polymer, because the viscosities of an amorphous polymer at or near its T g are too large to flow like a crystalline polymer above its T m . Also conducted was an experimental study for polystyrene and polycarbonate, using both a standard metering screw and a barrier screw design having a length‐to‐diameter ratio of 24. For the study, nine pressure transducers were mounted on the barrel along the extruder axis, and the pressure signal patterns and axial pressure profiles were measured at various screw speeds, throughputs, and head pressures. In addition to significantly higher rates, we found that the barrier screw design gives rise to much more stable pressure signals, thus minimizing surging, than the metering screw design. The experimentally measured axial pressure profiles were compared with prediction.
A mathematical model was developed for plasticating single‐screw extrusion of amorphous polymers. We considered a standard metering screw design. By introducing a ‘critical flow temperature’ (Tcf), below which an amorphous polymer may be regarded as a ‘rubber‐like’ solid, we modified the Lee‐Han melting model, which had been developed earlier for the extrusion of crystalline polymers, to model the flow of an amorphous polymer in the screw channel. Tcf is de facto a temperature equivalent to the melting point of a crystalline polymer. The introduction of Tcf was necessary for defining the interface between the solid bed and the melt pool, and between the solid bed and thin melt films surrounding the solid bed. We found from numerical simulations that (1) when the Tcf was assumed to be close to its glass transition temperature (Tg), the viscosity of the polymer became so high that no numerical solutions of the system of equations could be obtained, and (2) when the value of Tcf was assumed to be much higher than Tg, the extrusion pressure did not develop inside the screw channel. Thus, an optimum modeling value of Tcf appears to exist, enabling us to predict pressure profiles along the extruder axis. We found that for both polystyrene and polycarbonate, Tcf lies about 55°C above their respective Tgs. In carrying out the numerical simulation we employed (1) the WLF equation to describe the temperature dependence of the shear modulus of the bulk solid bed at temperatures between Tg and Tcf, (2) the WLF equation to describe the temperature dependence of the viscosity of molten polymer at temperatures between Tcf and Tg + 100°C, (3) the Arrhenius relationship to describe the temperature dependence of the viscosity of molten polymer at temperatures above Tg + 100°C, and (4) the truncated power‐law model to describe the shear‐rate dependence of the viscosity of molten polymer. We have shown that the Tg of an amorphous polymer cannot be regarded as being equal to the Tm of a crystalline polymer, because the viscosities of an amorphous polymer at or near its Tg are too large to flow like a crystalline polymer above its Tm. Also conducted was an experimental study for polystyrene and polycarbonate, using both a standard metering screw and a barrier screw design having a length‐to‐diameter ratio of 24. For the study, nine pressure transducers were mounted on the barrel along the extruder axis, and the pressure signal patterns and axial pressure profiles were measured at various screw speeds, throughputs, and head pressures. In addition to significantly higher rates, we found that the barrier screw design gives rise to much more stable pressure signals, thus minimizing surging, than the metering screw design. The experimentally measured axial pressure profiles were compared with prediction.
Audience Academic
Author Lee, Kee Yoon
Han, Chang Dae
Wheeler, Norton C.
Author_xml – sequence: 1
  givenname: Chang Dae
  surname: Han
  fullname: Han, Chang Dae
  organization: Department of Polymer Engineering, The University of Akron, Akron, Ohio 44325-0301
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  givenname: Kee Yoon
  surname: Lee
  fullname: Lee, Kee Yoon
  organization: Department of Polymer Science and Engineering, Chung Nam National University, Taejeon, Chung Nam, Republic of Korea
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  givenname: Norton C.
  surname: Wheeler
  fullname: Wheeler, Norton C.
  organization: Davis-Standard Division, Crompton & Knowles Corporation, Pawcatuck, Connecticut 06379
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Issue 10
Keywords Amorphous polymer
Single screw extruder
Experimental study
Mathematical model
Modeling
Extrusion molding
Plasticization
Comparative study
Language English
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  doi: 10.1002/pen.760301003
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  doi: 10.1002/pen.760311109
– volume: 27
  start-page: 1199
  year: 1976
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  publication-title: Polymer
  contributor:
    fullname: Shapiro J.
– volume-title: Viscoelastic Properties of Polymers
  year: 1980
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  contributor:
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– start-page: 277
  volume-title: Properties of Polymers
  year: 1976
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  doi: 10.1002/pen.760241208
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  doi: 10.1002/pen.760250706
– volume-title: Engineering Principles of Plasticating Extrusion
  year: 1970
  ident: e_1_2_1_2_2
  contributor:
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Snippet A mathematical model was developed for plasticating single‐screw extrusion of amorphous polymers. We considered a standard metering screw design. By...
Abstract A mathematical model was developed for plasticating single‐screw extrusion of amorphous polymers. We considered a standard metering screw design. By...
A mathematical model was developed for plasticating single-screw extrusion of amorphous polymers. We considered a standard metering screw design. By...
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SubjectTerms Applied sciences
Crystalline polymers
Exact sciences and technology
Extrusion
Extrusion moulding
Machinery and processing
Mathematical models
Moulding
Plastics
Polymer industry, paints, wood
Technology of polymers
Title Plasticating single-screw extrusion of amorphous polymers: Development of a mathematical model and comparison with experiment
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Volume 36
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