Is there a relation between the relaxation time measured in CaBER experiments and the first normal stress coefficient?

2010 ◽  
Vol 165 (19-20) ◽  
pp. 1265-1274 ◽  
Author(s):  
A. Zell ◽  
S. Gier ◽  
S. Rafaï ◽  
C. Wagner
Nature ◽  
1948 ◽  
Vol 161 (4093) ◽  
pp. 567-568 ◽  
Author(s):  
R. S. RIVLIN

2006 ◽  
Vol 79 (2) ◽  
pp. 267-280 ◽  
Author(s):  
C. M. Roland ◽  
C. G. Robertson

Abstract We have investigated the recovery of the overshoot in the transient viscosity, the first normal stress coefficient, and the dynamic modulus for entangled polybutadiene solutions subjected to nonlinear shear flow. The molecular-weight dependences of the various time scales (linear viscoelastic relaxation time, entanglement recovery time, and timescale for decay of stress following cessation of shearing) are all consistent with the usual 3.4 power law. Nevertheless, the time for recovery of the stress overshoot and plateau value of the dynamic modulus were substantially longer (by as much as two orders of magnitude) than the linear viscoelastic relaxation time calculated from the Newtonian viscosity and the equilibrium recoverable compliance. These results indicate that complete entanglement recovery requires cooperative chain motions over a length scale exceeding that associated with linear relaxation. This persistence of a disentangled state means that a state of low viscosity and reduced elasticity is retained for an extended time, suggesting that shear modification can be used to facilitate the processing of polymers.


2003 ◽  
Vol 47 (4) ◽  
pp. 1041-1050 ◽  
Author(s):  
Maria Eugenia Muñoz ◽  
Anton Santamarı́a ◽  
Julio Guzmán ◽  
Evaristo Riande

Normal stress effects arising in the torsional motion of a cylindrical mass of poly iso butylene solution are measured. The precautions which must be taken in making the measurements and the corrections which must be applied to them in order that the results may be compared with theory are discussed in some detail. The distribution of normal stresses over the plane ends of the cylindrical mass and the dependence of this on the experimental conditions is shown to be consistent with the phenomenological theory advanced by Rivlin (1948 a ). From the normal stress measurements, the normal stress coefficient, defined in this theory, is evaluated and the manner in which it depends on velocity gradient is found. Finally, the dependence of the normal stress coefficient on solution concentration and temperature is investigated.


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