Stress state of compound polygonal plate

Abstract

The constructions made of bars and plates with holes, openings and bulges of various forms are widely used in modern industry. By loading these structural elements with different efforts, there appears concentration (accumulation) of stress whose values sometimes exceeds the admissible one. The durability of the given element is defined according to the quantity of these stresses. Since the failure of details and construction itself begins from the place where the stress concentration has the greatest value. Therefore the exact determination of stress distribution in details (bars, plates, beams) is of great scientific and practical interest and is one of the important problems of the solid fracture. Compound details (when the nucleus of different material is soldered to the hole) are often used to decrease the stress concentration. In the present paper, we study a stress–strain state of polygonal plate weakened by a central elliptic hole with two linear cracks info which a rigid nucleus (elliptic cylinder with two linear bulges) of different material was put in (soldered) without preload. The problem is solved by a complex variable functions theory stated in papers [Theory of Elasticity, Higher School, Moscow, 1976, p. 276; Plane Problem of Elasticity Theory of Plates with Holes, Cuts and Inclusions, Publishing House Highest School, Kiev, 1975, p. 228; Bidimensional Problem of Elasticity Theory, Stroyizdat, Moscow, 1991, p. 352; Science, Moscow (1996) 708; MSB AH USSR OTH 9 (1948) 1371]. Kolosov–Mushkelishvili complex potential ϕ( z) and ψ( z) satisfying the definite boundary conditions are sought in the form of sums of functional series. After making several strict mathematical transformations, the problem is reduced to the solution of a system of linear algebraic equations with respect to the coefficients of expansions of functions ϕ( z) and ψ( z). Determining the values of ϕ( z) and ψ( z), we can find the stress components σ r , σ θ and τ rθ at any point of cross-section of the plate and nucleus on the basis of the known formulae. The obtained solution is illustrated by numerical example. Changing the parameters A 1, m 1, e, A 2, and m 2 we can get the various contour plates. For example, if we assume m 1=0, A 1= r, then the internal contour of L 1 becomes the circle of radius r with two rectilinear cracks (for the nucleus––a rectilinear bulges). Further, if we assume a small semi-axis of the ellipse b 1 to be equal to zero ( b 1=0), then a linear crack becomes the internal contour of L 1 (and the nucleus becomes the linear rigid inclusion made of other material). For m 2=0; A 2= R, the external contour L 2 turns into the circle of radius R. The obtained method of solution may be applied and in other similar problems of elasticity theory; tension of compound polygonal plate, torsion and bending of compound prismatic beams, etc.