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Dr. Chris Wilson Mechanical Engineering Tennessee Tech, Cookeville, TN

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Presentation on theme: "Dr. Chris Wilson Mechanical Engineering Tennessee Tech, Cookeville, TN"— Presentation transcript:

1 Dr. Chris Wilson Mechanical Engineering Tennessee Tech, Cookeville, TN
Visualizing Plane Stress and Plane Strain Dr. Chris Wilson Mechanical Engineering Tennessee Tech, Cookeville, TN

2 Outline 3-D Nature of Stress Plane Stress Plane Strain
Comparison of Plane Stress and Plane Strain Rules of Thumb Common Questions April 3, 2001

3 Stress in General Stress (and Strain) is a 3-D Quantity Defined at a Point in a Deformed Body Some Special Cases Triaxial Stress 2-D or Plane Stress (and Strain) Pure Shear Uniaxial Stress April 3, 2001

4 3-D Nature of Stress Craig, Mechanics of Materials, Wiley, 1996
April 3, 2001

5 3-D Stress-Strain Equations
E = Modulus of Elasticity (Young’s Modulus) n = Poisson’s Ratio April 3, 2001

6 3-D Stress-Strain Equations
Multiplied out... G = Shear Modulus April 3, 2001

7 What is Plane Stress? Thin plate
Uniform load distributed over thickness sz, txz, tyz zero on both faces Thin so sz, txz, tyz are zero throughout Ugural & Fenster, Advanced Strength and Applied Elasticity, 3rd Ed., Prentice Hall, 1995 April 3, 2001

8 Another Plane Stress Sketch
Bickford, Mechanics of Solids, Irwin, 1993 April 3, 2001

9 Plane Stress Example Gere, Mechanics of Materials, 5th Ed., Brooks/Cole, 2001 April 3, 2001

10 Plane Stress Equations
Note that the choice zeroing out the z-stresses is arbitrary (could zero out the x-stresses or the y-stresses). April 3, 2001

11 What is Plane Strain? Long prismatic member held between fixed, smooth rigid planes Lateral loading in x-y plane (e.g., cylinder under pressure) All cross sections experience identical deformation ez, gxz, gyz zero throughout Ugural & Fenster, Advanced Strength and Applied Elasticity, 3rd Ed., Prentice Hall, 1995 April 3, 2001

12 Using Poisson’s Effect to Help
Popov, Mechanics of Materials, 2nd Ed., Prentice-Hall, 1976 April 3, 2001

13 Plane Strain Equations
Note that the choice zeroing out the z-strains is arbitrary (could zero out the x-strains or the y-strains). April 3, 2001

14 Plane Stress & Strain Compared
Gere, Mechanics of Materials, 5th Ed., Brooks/Cole, 2001 April 3, 2001

15 Using Finite Element Models
Avoid FEM Jargon FEM Concerns Avoid Element Outlines Avoid Symmetry Models Avoid Free Meshing High Gradients at Fixed Ends Surface Effects in 3-D Models Mesh Convergence April 3, 2001

16 Plane Stress Model April 3, 2001

17 Plane Strain Model April 3, 2001

18 More Plane Strain Model
April 3, 2001

19 Mild Notch: 3-D Model Focus on sxx April 3, 2001

20 Mild Notch: 2-D Models Focus on sxx Plane Strain Plane Stress
April 3, 2001

21 Mild Notch: 3-D Model Focus on szz April 3, 2001

22 Mild Notch: Plane Strain vs. 3-D
3-D Sliced Twice Focus on szz April 3, 2001

23 Sharp Notch in Thin Section
3-D Solution April 3, 2001

24 Rules of Thumb D W L >> W & D Plane Stress If W  D
Plane Strain If W  5D (2D for Notch) 3-D If D < W < 5D (2D for Notch) April 3, 2001

25 Some Common Questions Mohr’s Circle or Mohr’s Circles?
Is ezz  0 for Strain Gages? What about sxx  txz  txz  0? szz  0  ezz  0? ezz  0  szz  0? Stress/Strain at Point or Whole Field? April 3, 2001


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