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Such filaments can have aspect ratios of length to radius ranging from a few tens to several thousands.
Furthermore, existing individual bulging factor only applies to a different range of ratios of crack length to radius of shell.
In addition influence of length to radius ratio and radius to thickness ratio on the frequency behaviour of such shells have been attempted.
The effect of thickness distribution on natural frequencies was determined for two boundary conditions; viz., simply supported-simply supported and clamped-clamped with different length to radius ratios.
Parametric studies are carried out using the finite element method for different core to facing thickness ratios, length to radius ratios and boundary conditions.
Results are presented for cylindrical shells with different core to facing thickness and length to radius ratios and three boundary conditions: clamped-clamped, simply supported and clamped-free.
Similar(40)
A three-dimensional shell theory is presented which is applicable to doubly curved thick open shells which are arbitrarily deep (have a large side-length to radius of curvature ratio) in one principal direction but are shallow in the other direction.
The variation of length-to-radius ratio only causes the movements of instability regions.
Finally, the effects of number of layers, length-to-radius ratio and boundary conditions on the optimum results are investigated.
Once the stele-to-root base-radius ratio and the stele-to-cortex permeability ratio are given, the optimum root length-to-radius ratio can be found.
With the increase of the length-to-radius ratio of tube, the radiation heating efficiency decreases, but the radiation energy incident on the object surface is more collimated.
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