Baixe Projeto de Engenharia Mecânica e outras Notas de estudo em PDF para Engenharia Mecânica, somente na Docsity! 3-D STRESS IN MECHANICAL DESIGN August 2000 Copyright 2000 C. E. Knight PURPOSE OF THE TUTORIAL This tutorial is designed to introduce and place strong emphasis on the role of 3-D stress in the process of mechanical design. Students in engineering are normally introduced to stress in its simplest one- component form defined by load divided by area of cross section.. This is a valid definition of a pure 1-D state of stress, but in many cases it seems to establish a baseline safe position for which many students don’t want to venture forth. Carrying this attitude through the mechanical design process is a recipe for failure. Everything in the mechanical design realm has solid 3-D characteristics. The same is true for the state of stress in the solid. In many simple cases the effective state of stress can be reduced to 2-D or 1-D, but only after careful consideration. In the early stages of mechanical design, the locations of most likely stress failure and the corresponding stress components acting at those locations must be identified. Once all the stress components at a given location are determined, they may then be combined to find principal stresses, maximum shear stress or other measures that are useful for predicting design success or failure. It is very important to remember that stress components for one location in a machine part should never be combined with stress components for a different location in the same part. One of the interesting developments in visualizing the combining of 2-D stress components was the creation of Mohr’s circle. This graphical representation of the 2-D stress transformation equations provides a quick, accurate and visual protrayal of the 2-D state of stress. It finds the principal stresses and a maximum shear stress (although this maximum shear stress may be quite misleading in 3-D stress). Review of Two-Dimensional Mohr’s Circle - Graphical Approach The beginning of a Mohr’s circle representation must be a stress element sketch of the 2-D state of stress as shown in the figure. This shows all potential non-zero 2-D stress components. The graphical Mohr’s circle uses coordinate pairs of these data to make a plot. They are (σx, τxy) and (σy, τyx). These two points establish the circle diameter. By convention normal stresses, σ are positive in tension and negative in compression, however, the shear stresses, τ, in the Mohr’s circle constructions are taken as positive if they make a cw moment about the stress element. In the stress element above, τxy is ccw (-) while τyx is cw(+). This convention is useful for determining the proper orientation of principal stresses and other components relative to the x,y coordinates. As an example, assume that σx is positive and τxy is positive (cw) with σy equal zero. First sketch the normal stress axis along the horizontal and the shear stress axis along the vertical. Then plot the first coordinate pair (σx, τxy) at point A. Then plot the second pair (0, τyx ) at point B. These two points form the diameter of the circle with its center at point C. Simple geometric triangles can then determine the circle radius and all principal stress and peak shear stress values. Example 3 As a final example, use the stress conditions σx = 90 (T), τxy = 40 ccw, σy = 30 (T), and σz = - 25 (C). First sketch the normal stress and shear stress axes and then plot the coordinate pair ( σx , τxy) at A. Plot the next coordinate pair ( σy, τyx ) at B. Connect points A and B to form the diameter of the 2-D Mohr’s circle with center at C. Draw the circle and determine two of the principal stresses. The center C is located at a stress value of 60. The triangle C, σx, and τxy form a 30, 40, 50 triangle, so the circle radius is 50. The two principal stresses from the 2-D circle are 110 (T) and 10(T). Since there are no non-zero z component shear stresses, σz is the third principal stress with a value of –25 (C). The maximum shear stress is at the peak of the largest circle and is equal to half the difference between σ1 and σ3.
