On the Shear Stress in Bonded Joints

1968 ◽  
Vol 35 (1) ◽  
pp. 177-178 ◽  
Author(s):  
L. J. Segerlind
Keyword(s):  
2014 ◽  
Vol 14 (3) ◽  
pp. 75-94
Author(s):  
Piotr Rapp

Abstract The subject of this paper is formulation of shear stress equations for plane twodimensional adhesive layers present in adhesively bonded joints. The adherends are assumed to have the same thickness and be made of an isotropic material. The shape of the adherends in the joint plane is arbitrary. The adhesive joint can be subjected to a shear stress arbitrarily distributed on the adherends surfaces as well as normal and shear stresses arbitrarily distributed along the adherends edges. A set of two partial differential equations of the second order with shear stresses in the adhesive as unknowns has been formulated. For a particular case of rectangular joints a set of 12 base functions has been derived; their appropriate linear combinations uniquely define shear stresses in the adhesive for a joint loaded arbitrarily by a set of axial forces, bending moments and shear forces.


1992 ◽  
Vol 114 (1) ◽  
pp. 1-7 ◽  
Author(s):  
S. E. Yamada

To gain a better understanding of the stress state in surface mount joints and their design considerations, an analysis method of bonded joints is developed and consequently three parameters that govern the stress distribution are identified. The solutions are obtained in terms of trigonometric and hyperbolic functions, and then applied to a simplified surface mount device. Contrary to general belief that the surface mount joints are mainly subjected to shear, it is shown that a peel stress also exists in a joint. Especially in a short joint used to connect stiff members as in direct mounting of chips and chip carriers, the magnitude of the peel stress is far greater than the shear stress.


1973 ◽  
Vol 95 (4) ◽  
pp. 919-924 ◽  
Author(s):  
J. B. Sainsbury-Carter

In bonded lap joints it is well known that the shear stress within the adhesive peaks at points of discontinuity of the adherends. In order to control these stress concentrations to a satisfactory level, in linear elastic adhesives, tapered adherends are necessary. This paper presents the development of linear analytical procedure for the analysis and design of flat bonded joints with tapered homogeneous isotropic adherends. The geometry of this taper is calculated to minimize the shear stress concentrations in the adhesive. Reducing the shear stress peaks in the adhesive by tapering the adherends from the nominal thickness often creates a secondary tensile stress concentration in the adherends. Satisfactory shear stress concentrations in the adhesive and tensile or shear stress concentrations in the adherends can be achieved simultaneously by careful geometric design of the adherends.


2020 ◽  
Vol 134 (17) ◽  
pp. 2399-2418
Author(s):  
Yoshito Yamashiro ◽  
Hiromi Yanagisawa

Abstract Blood vessels are constantly exposed to mechanical stimuli such as shear stress due to flow and pulsatile stretch. The extracellular matrix maintains the structural integrity of the vessel wall and coordinates with a dynamic mechanical environment to provide cues to initiate intracellular signaling pathway(s), thereby changing cellular behaviors and functions. However, the precise role of matrix–cell interactions involved in mechanotransduction during vascular homeostasis and disease development remains to be fully determined. In this review, we introduce hemodynamics forces in blood vessels and the initial sensors of mechanical stimuli, including cell–cell junctional molecules, G-protein-coupled receptors (GPCRs), multiple ion channels, and a variety of small GTPases. We then highlight the molecular mechanotransduction events in the vessel wall triggered by laminar shear stress (LSS) and disturbed shear stress (DSS) on vascular endothelial cells (ECs), and cyclic stretch in ECs and vascular smooth muscle cells (SMCs)—both of which activate several key transcription factors. Finally, we provide a recent overview of matrix–cell interactions and mechanotransduction centered on fibronectin in ECs and thrombospondin-1 in SMCs. The results of this review suggest that abnormal mechanical cues or altered responses to mechanical stimuli in EC and SMCs serve as the molecular basis of vascular diseases such as atherosclerosis, hypertension and aortic aneurysms. Collecting evidence and advancing knowledge on the mechanotransduction in the vessel wall can lead to a new direction of therapeutic interventions for vascular diseases.


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