A Theoretical and Experimental Investigation on Short-Time Stretch Relaxation of Entangled Polymer Solutions Y. H. Wen (溫玉合) and C. C. Hua (華繼中) Department of Chemical Engineering, National Chung Cheng University Introduction Historical Sketch de Gennes (1971) Doi and Edwards (1986) The tube (or reptation) model and its derivatives have proven very successful, especially in describing the linear viscoelasticity of entangled polymer liquids Linear relaxation A Story about Nonlinear Viscoelasticity Reptation time Rouse time R 2.4 s d 545 s Chain Retraction (nonlinear relaxation) Chain Retraction (nonlinear relaxation) Orientation Relaxation (linear relaxation) d / R 3Zeq PS/DEP solution (Mw=5.5x106 g/mol; PI=1.01; Zeq=77) Application of the Rouse chain in two distinct cases Rouse chain Dilute solution Concentrated solution Only terminal chain retraction is captured for the case of concentrated systems Objectives of the current investigation: The Rouse Model Prediction on Short-time Chain Retraction Nonlinear Stress Relaxation Data in Single-step Strain Flows For time scales < R The impact of polymer entanglement ? Formulation of Stress Relaxation in Single-Step Strain Flows Nonlinear stress relaxation modulus: G(t , ) yx 15 (0) 2 GN (t ) Qyx ( ) (t ) 4 yx (t ) : tube survival probability (t ) : dimensionless chain stretching GN(0) : shear stress : strain : plateau modulus Q yx ( ) : D-E universal function The Rouse model (w/o IA assumption) 2 (t ) 1 1 N exp(tp 2 / R ) 2 (t 0 ) 1 N p1 where N Z eq and (t 0 ) E u N Z eq eq : No. of Rouse modes : No. of entanglements per chain at equilibrium Experimentally Determined Model Parameters PS/TCP solution 105 104 G G' and G" (Pa) 103 G 102 101 G' G" 100 e= 1.3 x 10-3 s; Zeq = 19 10-1 10-3 10-2 10-1 100 101 102 (rad/s) Number of entanglements per chain at equilibrium, Z eq Zeq Mw 1 M e,melt 2 The Rouse time, R ( Z eq e ) φ: volume fraction of polymer Theory/Data Comparisons PS/DEP solution 0.3 102 0.4 103 G(t,) (Pa) G(t,) (Pa) 103 PS/DEP solution 9 101 9 102 101 Exp. (Zeq=42) 100 Exp. (Zeq=118) Rouse model 10-1 Rouse model 100 100 101 t (s) Parameters: Zeq 42; R 0.35 s 102 10-1 100 101 102 103 t (s) Parameters: Zeq 118; R 2.10 s Self-consistently Renormalized Rouse Modes (a) t = 0 (at equilibrium) Stretching (b) t = 0+ A different number of entanglements per chain N is a dynamic variable A Renormalized Rouse model: Retraction (c) t < 2 (t ) 1 1 N 2 exp( t p / R ) 2 (t 0 ) 1 N p1 where N Z (t ) (t ) (t 0 ) Zeq PS/DEP solution 0.3 102 0.4 103 G(t,) (Pa) G(t,) (Pa) 103 PS/DEP solution 9 101 9 102 101 100 10-1 Exp. (Zeq=42) Exp. (Zeq=118) Rouse model Renormalized Rouse model Rouse model Renormalized Rouse model 100 101 t (s) Parameters: Zeq 42; R 0.35 s 100 102 10-1 100 101 102 103 t (s) Parameters: Zeq 118; R 2.1 s Theory/Data Comparisons for Various Polymer Species PS/TCP solution PαMS/PCB solution 103 104 0.5 0.3 102 G(t,) (Pa) G(t,) (Pa) 103 10 102 Exp. (Zeq=19) Rouse model Renormalized Rouse model 101 7 101 Exp. (Zeq=45) Rouse model Renormalized Rouse model 100 100 10-1 100 10-1 101 100 101 102 t (s) t (s) 1,4-PB/FO solution PMMA/PCB solution 103 0.3 G(t,) (Pa) G(t,) (Pa) 0.5 105 3.33 Exp. (Zeq=26) 104 5 102 Exp. (Zeq=17) Rouse model Renormalized Rouse model 101 Rouse model Renormalized Rouse model 10-1 100 t (s) 101 0.1 1 10 t (s) 100 Conclusions The instantaneous entanglement property has a significant impact on short-time chain retraction of entangled polymer solutions. Self-consistent mode renormalization leads to better agreement with experimental data. Remaining discrepancies might result from (a) Inaccuracy of short-time relaxation data and/or (b) Tube pressure associated with a deformed polymer network Acknowledgements National Science Council (93-2116-E-194-001) Excellency Project of the Ministry of Education of ROC (91-E-FA04-2-4A)
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