4.7 STRESS CONCENTRATIONS

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4.7 STRESS CONCENTRATIONS Force equilibrium requires magnitude of resultant force developed by the stress distribution to be equal to P. In other words, P = ∫A σ dA This integral represents graphically the volume under each of the stress-distribution diagrams shown.

4.7 STRESS CONCENTRATIONS In engineering practice, actual stress distribution not needed, only maximum stress at these sections must be known. Member is designed to resist this stress when axial load P is applied. K is defined as a ratio of the maximum stress to the average stress acting at the smallest cross section: K = σmax σavg Equation 4-7

4.7 STRESS CONCENTRATIONS K is independent of the bar’s geometry and the type of discontinuity, only on the bar’s geometry and the type of discontinuity. As size r of the discontinuity is decreased, stress concentration is increased. It is important to use stress-concentration factors in design when using brittle materials, but not necessary for ductile materials Stress concentrations also cause failure structural members or mechanical elements subjected to fatigue loadings

Steel bar shown below has allowable stress, EXAMPLE 4.13 Steel bar shown below has allowable stress, σallow = 115 MPa. Determine largest axial force P that the bar can carry.

EXAMPLE 4.13 (SOLN) Because there is a shoulder fillet, stress-concentrating factor determined using the graph below

Calculating the necessary geometric parameters yields EXAMPLE 4.13 (SOLN) Calculating the necessary geometric parameters yields r n = 10 mm 20 mm = 0.50 w h 40 mm 20 mm = 2 = Thus, from the graph, K = 1.4 Average normal stress at smallest x-section, P (20 mm)(10 mm) σavg = = 0.005P N/mm2

Applying Eqn 4-7 with σallow = σmax yields EXAMPLE 4.13 (SOLN) Applying Eqn 4-7 with σallow = σmax yields σallow = K σmax 115 N/mm2 = 1.4(0.005P) P = 16.43(103) N = 16.43 kN