SHEARING DEFORMATION: S - Shearing forces cause deformation. An element subjected to shear does YN O N R AM O not change in length but undergoes a change in shape E - The change in angle at the corner of an original rectangular element is πΏ πΏ G πΎ= R R called the shear strain and is expressed as; N - The ratio of the shear stress π and the shear strain πΎ is called the E modulus of elasticity for shear or modulus of rigidity and is denoted as, πΊ; S π πΎ O πΊ= R AM - The relationship between the shearing deformation and the applied shearing force is; = ππΏ πΊ N πΏπ = ππΏ π΄π πΊ YN O where: π = π βππππππ πππππ R E π΄π = π βππππππ ππππ R Poisson's Ratio: G When a bar is subjected to tensile loading, there is an increase in N length of the bar in the direction of the applied load, but there is E also, a change in lateral dimension perpendicular to the load. The ratio Of the sideways deformation (or strain) to the longitudinal deformation (or strain) is called Poisson’s Ratio and is denoted by, π£ . For most E N G R R E YN O N R AM O S steel, it lies in the range of 0.25 to 0.30, and 0.20 for concrete. ππ₯ = ππ§ − ππ₯ S π£=− ππ¦ O where: R AM ππ₯ = π π‘ππππ ππ π‘βπ π₯ − ππππππ‘πππ ππ§ = π π‘ππππ ππ π‘βπ π§ − ππππππ‘πππ N ππ¦ = π π‘ππππ ππ π‘βπ π¦ − ππππππ‘πππ YN O * The negative sign indicates a decrease in transverse dimension, and ππ₯ is positive R E BIAXIAL DEFORMATION: R If an element is subjected simultaneously by tensile stresses, ππ₯ and N G ππ¦ , in the x and y directions, the strain in the x-direction is E the strain y-direction is ππ¦ πΈ ππ₯ and πΈ . Simultaneously, the stress in the x-direction will produce a lateral contraction on the y-direction of the amount −π£ππ¦ or − π£ππ¦ πΈ . The resulting strain in the x-direction πΈ − πΈ π π£ π₯ πΈ , ππ¦ = O , ππ₯ = ππ₯ +π£ππ¦ πΈ 1−π£ 2 ππ¦ +π£ππ₯ πΈ 1−π£ 2 N ππ¦ = π£ ππ¦ R AM ππ₯ = ππ₯ − πΈ ππ¦ S will be; YN O TRIAXIAL DEFORMATION: If an element is subjected simultaneously by three mutually ππ§ = R ππ¦ − π£ ππ₯ + ππ§ R ππ₯ − π£ ππ¦ + ππ§ N ππ¦ = 1 πΈ 1 πΈ 1 πΈ E ππ₯ = ππ¦ , ππ§ respectively, G strains ππ₯ , E perpendicular normal stresses ππ₯ , ππ§ − π£ ππ₯ + ππ¦ ππ¦ , ππ§ , which are accompanied by Note: S * Tensile stress and elongation are taken as positive. Compressive R AM O stress and contraction are taken as negative. Relationships between E, G and π; N πΊ= πΈ 2 1+π£ YN O Bulk Modulus of Elasticity or Modulus of Volume Expansion, π; - Is a measure of a resistance of a material to change in volume without R = π βπΰ΅ π R π= πΈ 3 1−2π£ E a change in shape or form; N π = π£πππ’ππ G where: E βπ = πβππππ ππ π£πππ’ππ βπΤ π = π£πππ’πππ‘πππ π π‘ππππ = π π = 3 1−2π£ πΈ O S βπ π R AM Illustrative Problem: A rectangular steel block is 3′′ long in the x-direction, 2′′ long in the y-direction, and 4′′ long in the z-direction. The block is subjected to a N triaxial loading of three uniformly distributed forces as follows; YN O 48 ππππ tension in x-direction, 60 ππππ compression in the y-direction, and 54 ππππ tension in the z-direction. If π£ = 0.30 and πΈ = 29π₯106 psi, determine E The single uniformly distributed load in the x-direction that would R produce the same deformation in the y-direction as the original loading R πΊππ£ππ: πΉπ₯ = 48 ππππ π π¦ = 2′′ πΉπ¦ = 60 ππππ πΆ N E z = 4′′ G π₯ = 3′′ πΉπ§ = 54 ππππ π R G N E E R YN O N R AM O S R G N E E R YN O N R AM O S R G N E E R YN O N R AM O S R G N E E R YN O N R AM O S Illustrative Problem: S A 150 mm long bronze tube closed at its ends is 80 mm in diameter and R AM O has a wall thickness of 3 mm. It fits without clearance in an 80 mm hole in a rigid block. The tube is then subjected to an internal pressure of 4.0 πππ. Assuming π£ = 1 3 and πΈ = 83 πΊππ, determine the tangential stress in N the tube. π πππ’ππππ: YN O πΊππ£ππ: π = 4.0 πππ ππ₯ E π· = 80 ππ πΏ = 150 ππ R G πΈ = 83 πΊππ N 1 3 E π£= R π‘ = 3 ππ R G N E E R YN O N R AM O S R G N E E R YN O N R AM O S Illustrative Problem: S The 50 mm rubber rod is placed in a hole with a rigid lubricated walls. R AM O There is no clearance between the rod and the sides of the hole. Determine the change in the length of the rod when the 8 ππ load is N applied. Use πΈ = 40 πππ and π£ = 0.45 for rubber. YN O πΊππ£ππ: π = 8 ππ E π· = 50 ππ R πΏ = 300 ππ G N π πππ’ππππ: βπΏ E π£ = 0.45 R πΈ = 40 πππ Illustrative Problem: O 5 8 − ππ diameter rod and it R AM experimental plastic. The test specimen is a S A standard tension test is used to determine the properties of an is subjected to 800 ππ tensile force. If an elongation of πΏπΏ =0.45 ππ and a decrease in diameter of πΏπ· = 0.025 ππ are observed in a 5-in gage length, N determine; YN O a) the modulus of elasticity of the material b) the Poisson’s ratio of the material E N G R R E c) the modulus of rigidity of the material R G N E E R YN O N R AM O S Problem Set No. 01: O S A 2-m length of an aluminum pipe 240-mm outer diameter and 10-mm wall If πΈ = 73 πΊππ and π£ = 0.33, determine; b) the change in its outer diameter E N G R R E YN O c) the change in its wall thickness N a) the change in the length of the pipe R AM thickness is used as a short column and carries a centric load of 640 ππ. Problem Set No. 02: O S A 20-mm square has been scribed on the side of a large steel pressure R AM vessel. After pressurization, the biaxial stress condition of the is as shown. Using πΈ=200 πΊππ and π£=0.30, determine the percent change E N G R R E YN O N in the slope of diagonal DB due to the pressurization of the vessel. Problem Set No. 03: O S The rectangular block of material of length πΏ and cross-sectional area R AM π΄ fits snugly between two rigid, lubricated walls. Derive the the expression for the change in length of the block due to the axial E N G R R E YN O N load π. Problem Set No. 04: S Two 1.75-in thick rubber pads are bonded to three steel plates to form O the shear mount as shown in the figure. Determine the displacement of R AM the middle plate when the 1200-lb load is applied. Consider the E N G R R E YN O N the deformation of the rubber only. Use πΈ = 500 ππ π and π£ = 0.48 for rubber.