首页> 外文会议>Meeting of the Rubber Division, American Chemical Society Apr 29-May 1, 2002 Savannah, Georgia >RHEOLOGY OF PVC PLASTISOL ― VII EXPLORATION ON NON-LINEARITY OF VISCOELASTIC BEHAVIOR
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RHEOLOGY OF PVC PLASTISOL ― VII EXPLORATION ON NON-LINEARITY OF VISCOELASTIC BEHAVIOR

机译:PVC溶胶的流变学-粘弹性行为非线性研究

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Non-linearity (strain-amplitude dependence) of viscoelastic behavior was examined with a plastisol made with a commercial PVC resin dispersed in DOP at 50 volume percent. The measurements were made in shear at room temperature in the frequency range of 10 ~(-1) ― 10~2 rad/s. The strain amplitude was from 0.02 to about 10. At a fixed amplitude, the complex viscosity, | η~*|, decreased with the increase of frequency (pseudo-plastic), reaching a viscosity minimum and then, increased (dilatancy). At a fixed frequency, the viscosity decreased with the increase of amplitude, reaching a minimum and then, increased, in some cases, going over a maximum. At a fixed amplitude, the storage modulus, G', increased monotonically with the increase of frequency. However, at a fixed frequency, the modulus decreased, reaching a minimum and then, increased, in some cases, going over a maximum. In general, the steady state viscosity, η, was higher than |η~* I, when compared at numerically equal value of frequency and shear rate. The shear-rate dependence of η exhibited both pseudo-plastic flow and dilatancy. The first normal stress difference, N_1, - was almost zero in the pseudo-plastic region, but about - 80 Pa in the dilatant region. The negative value implies that another normal stress difference, N _2, is present. Viscosities measured with a spindle rheometer were somewhat higher than those measured with a concentric-cylinder rheometer. The difference is attributable to the shear-induced migration in the former rheometer and the formation of the immobilized layer in the latter rheometer.
机译:用由以50体积%分散在DOP中的市售PVC树脂制成的增塑溶胶检查粘弹性行为的非线性(应变-振幅依赖性)。在室温下以10〜(-1)〜10〜2 rad / s的频率范围内的剪切力进行测量。应变幅度为0.02至约10。 η〜* |随着频率的增加而降低(伪塑性),达到最小粘度,然后增加(膨胀率)。在固定频率下,粘度随振幅的增加而降低,达到最小值,然后在某些情况下超过最大值。在固定振幅下,储能模量G'随着频率的增加而单调增加。但是,在固定频率下,模量下降,达到最小值,然后在某些情况下上升到最大值。通常,当在频率和剪切速率的数值相等的数值下进行比较时,稳态粘度η高于|η〜*I。 η的剪切速率依赖性既表现出假塑性流动,又表现出剪胀性。在假塑性区,第一法向应力差N_1-几乎为零,而在膨胀区,第一法向应力差N_1-几乎为-80 Pa。负值表示存在另一个法向应力差N _2。用主轴流变仪测得的粘度略高于用同心圆筒流变仪测得的粘度。差异归因于前流变仪中的剪切诱导迁移和后流变仪中固定层的形成。

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