首页> 外文期刊>Journal of Rheology >EFFECTS OF MOLECULAR WEIGHT DISTRIBUTION ON DYNAMIC VISCOELASTICITY AND BIAXIAL EXTENSIONAL FLOW BEHAVIOR OF POLYSTYRENE MELTS
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EFFECTS OF MOLECULAR WEIGHT DISTRIBUTION ON DYNAMIC VISCOELASTICITY AND BIAXIAL EXTENSIONAL FLOW BEHAVIOR OF POLYSTYRENE MELTS

机译:分子量分布对聚苯乙烯熔体动态粘弹性和双轴扩展流动行为的影响

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Dynamic viscoelasticity and biaxial extensional flow behavior of polystyrene melts with various molecular weight distributions have been studied in wide ranges of temperature and strain rate epsilon(B). Two patterns of time dependence of the biaxial stress growth coefficient eta(B)(+) are Observed with increasing reduced strain rate epsilon(B) tau(0), where tau(0) is a characteristic relaxation time. At short times, eta(B)(+) coincides with the linear viscoelastic curve; then it shows strain hardening after that, or strain softening followed by a quasisteady state. These behaviors are observed for polydisperse polystyrenes at much higher epsilon(B) tau(0) than those for monodisperse polystyrenes. The quasisteady-state viscosity eta(B,qs) decreases with the strain rate. Addition of a very high molecular weight component causes considerable effects on tau(0) and on the strain rate dependences of shear eta* and biaxial eta(B,qs) viscosities as well as on the stress growth coefficient eta(B)(+), where eta* is the absolute value of the complex viscosity. The relaxation time 70 increases very much, and the strain rate dependences of eta* and eta(B,qs) become much weaker. The upturn tendency of eta(B)(+) becomes prominent when B compared at the same reduced strain rate epsilon(B) tau(0). On the other hand, when compared at the same value of the reduced viscosity eta(B,qs)/6 eta(0), a similar degree of strain softening in eta(B)(+) is observed for all polydisperse samples, where eta(0) is the zero shear viscosity. (C) 1995 Society of Rheology. [References: 11]
机译:研究了在各种温度和应变速率ε(B)的宽范围内,各种分子量分布的聚苯乙烯熔体的动态粘弹性和双轴拉伸流动行为。随着减小的应变率ε(t)增加,tau(0)观察到双轴应力增长系数eta(B)(+)的两种时间依赖性模式,其中tau(0)是特征弛豫时间。在短时间内,eta(B)(+)与线性粘弹性曲线重合。然后显示应变硬化,或应变软化,然后达到准稳态。对于多分散聚苯乙烯,在ε(B)tau(0)更高的情况下观察到了这些行为。准稳态粘度eta(B,qs)随应变速率降低。添加非常高的分子量组分对tau(0)以及剪切 eta * 和双轴eta(B,qs)粘度的应变率依赖性以及应力增长系数eta(B)( +),其中 eta * 是复数粘度的绝对值。弛豫时间70大大增加,并且 eta * 和eta(B,qs)的应变率依赖性变得更弱。当B在相同的应变率ε(t)(0)下降低时,eta(B)(+)的上升趋势变得明显。另一方面,当以相同的比浓粘度eta(B,qs)/ 6 eta(0)进行比较时,对于所有多分散样品,在eta(B)(+)中观察到相似的应变软化程度,其中eta(0)是零剪切粘度。 (C)1995,流变学学会。 [参考:11]

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