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Snap-through-type nonlinear creep-buckling of a shallow sinusoidal shell

机译:浅正弦壳的卡扣型非线性蠕变屈曲

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This paper is concerned with creep and creep-buckling of the snap-through-type of a shallow, thin-walled, sinusoidalshell subjected to transverse (vertical) pressure. The material is governed by Odqvist's law of nonlinear viscoelasticity. Theshell wall is modelled as a sandwich type to which any actual wall may be reduced and which has been described in detail byHoff and others. The basic equations are formulated, and for a simply supported shell, approximate, analytic solutions areobtained describing the evolution in time of the deflection, i.e., the downward displacement of the initial rise. Instability isassumed to occur when the time rate of this deflection grows beyond all bounds. The time lapse after which instability occursis called the 'critical time' (lifetime) of the shell. It is of finite value for any loading, however small, as long as compressivestresses are created within the shell. If the shell exhibits nonlinear creep only, without elasticity as deformation mechanism,instability occurs when the shell traverses the horizontal plane. The effect of elasticity on the instability process results in aconsiderable reduction of the critical time. Here, instability occurs before the shell has reached the horizontal plane, as asnap-through phenomenon, as soon as the time rate of the deflection grows beyond all bounds.
机译:本文涉及的是承受横向(垂直)压力的浅薄壁正弦形壳的卡扣式蠕变和蠕变屈曲。该材料受非线性粘弹性的奥德奎斯特定律控制。壳壁被建模为夹心类型,任何实际的壁都可以减小为夹心类型,并且已经由霍夫等人进行了详细描述。公式化了基本方程,并且对于简单支撑的壳体,获得了近似的解析解,描述了挠度随时间的变化,即初始上升的向下位移。假定当这种偏转的时间率超出所有范围时,就会发生不稳定性。发生不稳定之后所经过的时间称为外壳的“临界时间”(生命周期)。只要在壳内产生压应力,它对于任何载荷都具有有限的价值,无论多么小。如果壳体仅表现出非线性蠕变,而没有弹性作为变形机制,则当壳体横穿水平面时会发生不稳定性。弹性对不稳定性过程的影响导致临界时间的显着减少。在此,一旦挠曲的时间速率超过所有范围,就会在壳到达水平面之前出现不稳现象,这是突跳现象。

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