Uniaxial and biaxial stretching of silicone putty

D.R. Oliver
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Abstract

Two novel experimental methods are used. Vertical uniaxial stretching is obtained by attaching a perspex rod to the lower end of a silicone putty cylinder; the rod then descends into water of constant depth. The stress and rate of extension change little during each test, but the rate of extension may be varied from 0.005 to 0.10 s−1 by modifying the experimental conditions. Biaxial stretching is acchieved by placing a disc of silicone putty across the top of an open glass cylinder which is lightly pressurized. The sample expands as a spherical cap, the height of the centre above the cylinder being timed. The stress in the cap passes through a shallow minimum as it expands (at constant pressure) and the slowly varying rate of biaxial extension may be readily determined. This lies in the range 0.003–0.06 s−1. For low rates of uniaxial or biaxial extension, it is possible to plot the extension against time and to show how the extensional viscosity varies with the strain rate (or principal extension ratio). For high rates of extension, a ‘single point’ determination of the extensional viscosity may be made, with the stress and strain rate averaged at the mid-point of the sample's extension. The temperature is 26.5 ± 1.5 °C. The following is shown under the experimental conditions:

(a) the extensional viscosity (uniaxial or biaxial) is in the range 1.0 × 105 to 3.0 × 105 Pa s;

(b) for extensional strain rates between 0.01 and 0.04 s−1, the uniaxial and biaxial extensional viscosities are of comparable value;

(c) both forms of the extensional viscosity tend to decrease with increased extensional strain rate, the biaxial extensional viscosity falling more rapidly and being higher than the uniaxial viscosity at low strain rates and lower at high strain rates;

(d) there are no signs of rupture in uniaxial extension (principal extension ratios up to 1.8 and extensional strain rate up to 0.1 s−1);

(e) in biaxial extension, the sample tends to rupture more easily as the strain rate is increased. (The sample fails at the principal extension ratio of 2.0 at an extensional strain rate of 0.02 s−1 and fails at a principal extension ratio of 1.3 at an extensional strain rate of 0.07 s−1.)

硅酮腻子单轴、双轴拉伸
采用了两种新颖的实验方法。垂直单轴拉伸通过将有机玻璃棒连接到有机硅腻子筒的下端来获得;然后杆子沉入一定深度的水中。在每次试验中,应力和拉伸速率变化不大,但通过改变试验条件,拉伸速率可在0.005 ~ 0.10 s−1之间变化。双轴拉伸是通过在一个打开的玻璃圆柱体的顶部放置一块硅树脂腻子来实现的,这个玻璃圆柱体是轻微加压的。样品膨胀成一个球形帽,测量圆柱体上方中心的高度。当盖子膨胀时(在恒压下),其应力会经过一个浅层的最小值,并且可以很容易地确定双轴延伸的缓慢变化速率。取值范围为0.003-0.06 s−1。对于低速率的单轴或双轴延伸,可以绘制随时间的延伸,并显示拉伸粘度如何随应变率(或主延伸比)变化。对于高拉伸速率,可以进行拉伸粘度的“单点”测定,在试样拉伸的中点取应力和应变速率的平均值。温度为26.5±1.5℃。(a)拉伸粘度(单轴和双轴)在1.0 × 105 ~ 3.0 × 105 Pa s之间;(b)拉伸应变率在0.01 ~ 0.04 s−1之间,单轴和双轴拉伸粘度值相当;(c)两种形式的拉伸粘度都随拉伸应变率的增加而降低。双轴拉伸黏度在低应变率下下降较快,高于单轴黏度,在高应变率下下降较慢;(d)单轴拉伸时无破裂迹象(主延伸比高达1.8,拉伸应变率高达0.1 s−1);(e)双轴拉伸时,随应变率的增加,试样更容易破裂。(试样在拉伸应变率为0.02 s−1时,主延伸比为2.0时失效;在拉伸应变率为0.07 s−1时,主延伸比为1.3时失效。)
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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