We adopt Langevin dynamics to explore the stress-structure relationship of telechelic reversible associating polymer gel during startup shear flow, with shear strengths varying fromW(i)= 12.6 toW(i)= 12640. At weak shear flowW(i)= 12.6, the shear stress proportionally increases with shear strain at short times, followed by a strain hardening behavior and then passes through a maximum (sigma(max),gamma(max)) and finally decreases until it reaches the steady state. During the evolution of stress, the gel network is only slightly broken and essentially maintains its framework, and the strain hardening behavior originates from the excessive stretching of chains. On the other hand, the stress-strain curve at intermediate shear flowW(i)= 505.6 shows two differences from that atW(i)= 12.6, namely, the absence of strain hardening and a dramatic increase of stress at large strains, which is caused by the rupture of gel network at small strains and the network recovery at large strains, respectively. Finally, at very strong shear flowW(i)= 6319.7, the gel network is immediately broken by shear flow and the stress-strain curve exhibits similar behaviors to those of classical polymeric liquids.
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Petrobras SA, Rua Republ Chile 330, BR-20031170 Rio De Janeiro, RJ, BrazilPetrobras SA, Rua Republ Chile 330, BR-20031170 Rio De Janeiro, RJ, Brazil
Moises, G. V. L.
Alencar, L. S.
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Petrobras SA, Rua Republ Chile 330, BR-20031170 Rio De Janeiro, RJ, BrazilPetrobras SA, Rua Republ Chile 330, BR-20031170 Rio De Janeiro, RJ, Brazil
Alencar, L. S.
Naccache, M. F.
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Pontificia Univ Catolica Rio de Janeiro, Dept Mech Engn, Rua Marques Sao Vicente 225, BR-22453900 Rio De Janeiro, RJ, BrazilPetrobras SA, Rua Republ Chile 330, BR-20031170 Rio De Janeiro, RJ, Brazil
Naccache, M. F.
Frigaard, I. A.
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Univ British Columbia, Dept Math, 1984 Math Rd, Vancouver, BC V6T 1Z2, Canada
Univ British Columbia, Dept Mech Engn, 1984 Math Rd, Vancouver, BC V6T 1Z2, CanadaPetrobras SA, Rua Republ Chile 330, BR-20031170 Rio De Janeiro, RJ, Brazil