Rate dependence of poly(vinyl chloride), the effects of plasticizer and time–temperature...

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Rate dependence of poly(vinyl chloride), the effects of plasticizer and time–temperature superposition by Michael J. Kendall, and Clive R. Siviour Proceedings A Volume 470(2167):20140012 July 8, 2014 ©2014 by The Royal Society

Transcript of Rate dependence of poly(vinyl chloride), the effects of plasticizer and time–temperature...

Rate dependence of poly(vinyl chloride), the effects of plasticizer and time–temperature superposition

by Michael J. Kendall, and Clive R. Siviour

Proceedings AVolume 470(2167):20140012

July 8, 2014

©2014 by The Royal Society

Yield stress dependence on absolute temperature of an arbitrary polymer, with multiple strain rates shown to obey a linear time–temperature superposition.

Michael J. Kendall, and Clive R. Siviour Proc. R. Soc. A 2014;470:20140012

©2014 by The Royal Society

PMMA yield data as a function of temperature mapped onto strain rate yield data to create master curves at 100°C in uniaxial compression.

Michael J. Kendall, and Clive R. Siviour Proc. R. Soc. A 2014;470:20140012

©2014 by The Royal Society

Comparison of the PC variation of peak stress with temperature, and the variation of peak stress with strain rate mapped onto temperature. [8].

Michael J. Kendall, and Clive R. Siviour Proc. R. Soc. A 2014;470:20140012

©2014 by The Royal Society

Representative behaviour of PVC. (a) True stress–true strain response in uniaxial compression over all rates tested at 20°C and (b) the true yield stress as a function of strain rate over a

logarithmic scale.

Michael J. Kendall, and Clive R. Siviour Proc. R. Soc. A 2014;470:20140012

©2014 by The Royal Society

Representative behaviour of PVC. (a) True stress–true strain response in uniaxial compression over all temperatures tested at 10−2 s−1 and (b) the true yield stress as a function of temperature

over a linear scale in °C.

Michael J. Kendall, and Clive R. Siviour Proc. R. Soc. A 2014;470:20140012

©2014 by The Royal Society

Representative behaviour of PPVC-2.

Michael J. Kendall, and Clive R. Siviour Proc. R. Soc. A 2014;470:20140012

©2014 by The Royal Society

Representative behaviour of PPVC-2.

Michael J. Kendall, and Clive R. Siviour Proc. R. Soc. A 2014;470:20140012

©2014 by The Royal Society

True yield stress of PPVC-2 as a function of strain rate over a logarithmic scale presenting the influences of two different rate-activated processes (α and β).

Michael J. Kendall, and Clive R. Siviour Proc. R. Soc. A 2014;470:20140012

©2014 by The Royal Society

Representative behaviour of PPVC-4.

Michael J. Kendall, and Clive R. Siviour Proc. R. Soc. A 2014;470:20140012

©2014 by The Royal Society

Representative behaviour of PPVC-4.

Michael J. Kendall, and Clive R. Siviour Proc. R. Soc. A 2014;470:20140012

©2014 by The Royal Society

Representative behaviour of PPVC-6.

Michael J. Kendall, and Clive R. Siviour Proc. R. Soc. A 2014;470:20140012

©2014 by The Royal Society

Representative behaviour of PPVC-6.

Michael J. Kendall, and Clive R. Siviour Proc. R. Soc. A 2014;470:20140012

©2014 by The Royal Society

PVC elastic modulus (solid lines) and loss modulus (dashed lines) curves at 0.035 s−1 (1 Hz, light grey), 0.35 s−1 (10 Hz, dark grey) and 3.5 s−1 (100 Hz, black). β- and α-transitions are centred,

respectively, at approximately (i) −45°C and (ii) 82°C.

Michael J. Kendall, and Clive R. Siviour Proc. R. Soc. A 2014;470:20140012

©2014 by The Royal Society

PPVC-2 elastic modulus and loss modulus curves at 0.035 s−1 (1 Hz, light grey), 0.35 s−1 (10 Hz, dark grey) and 3.5 s−1 (100 Hz, black) starting at (a) −100°C and (b) −150°C. β- and α-transitions

are centred, respectively, at approximately −150 and 45°C.

Michael J. Kendall, and Clive R. Siviour Proc. R. Soc. A 2014;470:20140012

©2014 by The Royal Society

PPVC-4 elastic modulus and loss modulus curves at 0.035 s−1 (1 Hz, light grey), 0.35 s−1 (10 Hz, dark grey) and 3.5 s−1 (100 Hz, black). β- and α-transitions are centred, respectively, at

approximately −150 and 0°C.

Michael J. Kendall, and Clive R. Siviour Proc. R. Soc. A 2014;470:20140012

©2014 by The Royal Society

PPVC-6 elastic modulus and loss modulus curves at 0.035 s−1 (1 Hz, light grey), 0.35 s−1 (10 Hz, dark grey) and 3.5 s−1 (100 Hz, black). β- and α-transitions are centred, respectively, at

approximately −150 and −20°C.

Michael J. Kendall, and Clive R. Siviour Proc. R. Soc. A 2014;470:20140012

©2014 by The Royal Society

PVC yield stresses where (a) temperature data (squares) are mapped onto strain rate data (triangles) and (b) strain rate data are mapped onto temperature data using D=13.5°C/decade ε˙.

Michael J. Kendall, and Clive R. Siviour Proc. R. Soc. A 2014;470:20140012

©2014 by The Royal Society

PPVC-2 yield stresses where (a) temperature data (squares) are mapped onto strain rate data (triangles) and (b) strain rate data are mapped onto temperature data using D=11°C/decade ε˙.

Michael J. Kendall, and Clive R. Siviour Proc. R. Soc. A 2014;470:20140012

©2014 by The Royal Society

PPVC-4 yield stresses where (a) temperature data (squares) are mapped onto strain rate data (triangles) and (b) strain rate data are mapped onto temperature data using D=8.5°C/decade ε˙.

Michael J. Kendall, and Clive R. Siviour Proc. R. Soc. A 2014;470:20140012

©2014 by The Royal Society

PPVC-6 yield stresses where (a) temperature data (squares) are mapped onto strain rate data (triangles) and (b) strain rate data are mapped onto temperature data using D=7.5°C/decade ε˙.

Michael J. Kendall, and Clive R. Siviour Proc. R. Soc. A 2014;470:20140012

©2014 by The Royal Society

PVC (a), PPVC-2 (b), PPVC-4 (c) and PPVC-6 (d) with yield stress data at 10−2 s−1 superimposed onto elastic modulus data at 0.035 s−1 (1 Hz, light grey), 0.35 s−1 (10 Hz, dark grey) and 3.5 s−1

(100 Hz, black).

Michael J. Kendall, and Clive R. Siviour Proc. R. Soc. A 2014;470:20140012

©2014 by The Royal Society

PPVC-2 yield stresses where (a) strain rate data (triangles) are mapped onto temperature-dependent data (squares) and (b) temperature data (squares) are mapped onto strain rate

(triangles) data using D=6°C/decade ε˙.

Michael J. Kendall, and Clive R. Siviour Proc. R. Soc. A 2014;470:20140012

©2014 by The Royal Society

PPVC-2 (a) strain rate data (triangles and circles) mapped onto temperature data (squares), and (b) PPVC-2 temperature data (squares and circles) mapped onto strain rate data (triangles).

Michael J. Kendall, and Clive R. Siviour Proc. R. Soc. A 2014;470:20140012

©2014 by The Royal Society

PVC (a) strain rate data (triangles and circles) mapped onto temperature data (squares) and (b) temperature data (squares and circles) mapped onto strain rate data (triangles).

Michael J. Kendall, and Clive R. Siviour Proc. R. Soc. A 2014;470:20140012

©2014 by The Royal Society