Equilibrium of stress | tH L. W When in use, the compliant rubber layer induces a shear stress x-z, Oxz, at the bottom interface between the fiber-matrix layer and the compliant rubber layer (at z = 0), while the top of the fiber matrix layer is unloaded (at z = H) with oxz = 0. Given the stress equilibrium equations and assum no acceleration and no body forces, show that shear stress x-y. gxy, in the fiber-matrix laver can b

Structural Analysis
6th Edition
ISBN:9781337630931
Author:KASSIMALI, Aslam.
Publisher:KASSIMALI, Aslam.
Chapter2: Loads On Structures
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Equilibrium of stress
| tH
-y
W
When in use, the compliant rubber layer induces a shear stress x-z, Oxz, at the bottom interface
between the fiber-matrix layer and the compliant rubber layer (at z = 0), while the top of the fiber-
matrix layer is unloaded (at z = H) with oxz = 0. Given the stress equilibrium equations and assuming
no acceleration and no body forces, show that shear stress x-y, oxy, in the fiber-matrix layer can be
calculated as
Оху
HYxz dx
Transcribed Image Text:Equilibrium of stress | tH -y W When in use, the compliant rubber layer induces a shear stress x-z, Oxz, at the bottom interface between the fiber-matrix layer and the compliant rubber layer (at z = 0), while the top of the fiber- matrix layer is unloaded (at z = H) with oxz = 0. Given the stress equilibrium equations and assuming no acceleration and no body forces, show that shear stress x-y, oxy, in the fiber-matrix layer can be calculated as Оху HYxz dx
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