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Mechanics of Elastic Materials. Why study mechanics? Useful for the analysis and design of load-bearing structures, such as: buildings bridges space shuttles.

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Presentation on theme: "Mechanics of Elastic Materials. Why study mechanics? Useful for the analysis and design of load-bearing structures, such as: buildings bridges space shuttles."— Presentation transcript:

1 Mechanics of Elastic Materials

2 Why study mechanics? Useful for the analysis and design of load-bearing structures, such as: buildings bridges space shuttles prosthetics biological implants Also used to characterize materials

3 Forces Force- A push or a pull Units- Newtons (metric) or Pounds (standard) Tensile Force- The applied force is pulling on both sides of the material Compression Force- Force is being pushed on both sides of the material

4 LOADS Dead Loads Live Loads Wind Loads Snow Loads

5 EQUILIBRIUM LOADS FORCES MOMENTS TORSION Summation of Forces Σ F=0 y Horizontal Direction Σ F h =0 y Vertical Direction Σ F v =0

6 AXIAL LOADS Compression pushing or shortening Tension pulling or elongating

7 Bridge Experiment Build a people bridge to experiment with the forces: compression, tension and torsion Have pairs of students face each other with palms touching and feet flat and about 0.5 m (1.5 ft) apart. Have students slowly move their feet back while keeping their palms touching until the bridge feels balanced and they cannot back up any further without falling over.

8 Bridge Experiment Where on the bridge do students feel forces of compression and tension ? Have one person move two steps to the left. What happens to the balance of the bridge? How does torsion affect the stability of the bridge? What forces might cause the support structure of a real bridge to rotate?

9 Stress The force per unit area, or intensity of the forces distributed over a given section. (units = Pascals [Pa] or pounds per square inch [psi]) σ = F/A F- ForceA- area Stress is how engineers normalize the force that is applied to a material to account for differences in geometry. Useful for predicting failure conditions for materials.

10 Strain Deformation per unit length (units: none [unitless]) ε =  /L L- original length  - change in length Strain is how engineers normalize the deformation that a material experiences to account for differences in geometry. Useful for determining how much a material can deform before failure.

11 Modulus of Elasticity A representation of the stiffness of a material that behaves elastically (units: Pascals [Pa] or pounds per square inch [psi]) E = σ / ε Modulus of elasticity is how engineers characterize material behavior. Useful for knowing how materials behave, material selection for device design, and calculating the stress in a material since it is easier to measure deformation than it is to determine the exact force on a material.

12 Solid Mechanics In-Class Examples

13 Example 1 This rod is exposed to a tensile force of 20 N. What is the stress in the rod? 20 N 0.5 m σ =F/A F = 20 N (given) A = 0.5 m * 0.5 m = 0.25 m 2 σ = 20 N / 0.25 m 2 σ = 80 Pa 3 m

14 Example 2 The rod below is exposed to a tensile force of 20 N and elongates by 0.03 m. Calculate the strain. ε =  /L  = 0.03 m (given) L = 3 m ε = 0.03 m / 3 m ε = 0.01 20 N 0.5 m 3 m

15 Example 3 The rod below is exposed to a tensile force of 20 N and elongates by 0.03 m. Calculate the modulus of elasticity. E = σ / ε σ = 80 Pa (from first example) ε = 0.01 (from second example) E = 80 Pa / 0.01 E = 8000 Pa or 8 kPa 20 N 0.5 m 3 m

16 Next: Complete the Solid Mechanics Worksheet

17 2 - 17 Deformations Under Axial Loading From Hooke’s Law: From the definition of strain: Equating and solving for the deformation,

18 Elastic Behavior stress strain elastic range plastic range yield stress ultimate tensile strength fracture stress F F tensile load direction neck steel tensile specimen

19 Understanding the Stress-Strain Curve elastic range – The linear portion of the stress-strain curve. When the force is released, the material returns to its original dimensions. plastic range – The region of permanent deformation. stress strain elastic range plastic range yield stress ultimate tensile strength fracture stress

20 Understanding the Stress-Strain Curve yield stress – The minimum stress that causes permanent deformation. ultimate tensile strength – The maximum stress that the material can withstand. Also defines the beginning of necking. stress strain elastic range plastic range yield stress ultimate tensile strength fracture stress

21 The Stress-Strain Curve necking – A localized decrease in cross sectional area that causes a decrease in stress with an increase in strain. fracture stress – Stress in which the material fails. stress strain elastic range plastic range yield stress ultimate tensile strength fracture stress F F tensile load direction neck steel tensile specimen

22 Image Sources Line diagrams: 2011 © Brandi N. Briggs, ITL Program, College of Engineering, University of Colorado Boulder tomruen, wikimedia.org http://sv.wikipedia.org/wiki/Fil:I-35W_bridge_collapse_TLR1.jpghttp://sv.wikipedia.org/wiki/Fil:I-35W_bridge_collapse_TLR1.jpg Glenn Research Center, NASA http://www.nasa.gov/centers/glenn/moonandmars/med_topic_atomic_oxygen.html http://www.nasa.gov/centers/glenn/moonandmars/med_topic_atomic_oxygen.html NOAA http://www.photolib.noaa.gov/htmls/corp2239.htmhttp://www.photolib.noaa.gov/htmls/corp2239.htm


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