PHYSICS CHAPTER 12 Matter is made up of many particles called atoms or molecules. Matter can exist in one of the following states i.e. solid, liquid and gas. Introduction CHAPTER 12: Mechanical properties of matter (2 Hours) 1 PHYSICS CHAPTER 12 Learning Outcome: 12.1 Stress and strain (1 hour) At the end of this chapter, students should be able to: Define stress and strain for a stretched wire. Sketch and explain the graph of stress-strain. Distinguish between elastic and plastic deformation. Sketch and distinguish F-e graph for elastic and ductile materials. 2 PHYSICS CHAPTER 12 12.1 Stress and Strain 12.1.1 Elasticity of solids is defined as the property of a material that enables them to return to their original dimensions (shape and size) after an applied force (stress) has been removed. Deformation occurs when external forces act to stretch, compress or shear a solid. An object or a material which returns to its original length or size after being distorted suffers elastic deformation, i.e. it behaves within the elastic limit. Plastic deformation occurs when a material is deformed beyond its elastic limit. The behaviour of materials under deformation can be described by the following mechanical properties : Strength – ability of a material to withstand a force without breaking. 3 PHYSICS CHAPTER 12 Stiffness – resistance of a material to changes in shape and size. Elasticity Ductility – tendency of a material to change its size and shape considerably before breaking. Brittleness – tendency of a material to break without deforming. Table 12.1 shows the examples of elastic and inelastic materials. Elastic material Inelastic material Sponge Paper Spring Metal Rubber Plasticine Table 12.1 4 PHYSICS 12.1.2 CHAPTER 12 Stress, and strain, Consider a rod that initially has uniform cross-sectional area, A and length l0.Stretch the rod by applying the forces of equal magnitude F but opposite directions at the both ends and the rod will extent by amount e as shown in Figure 12.8. l0 A F F Figure 12.8 Simulation 12.1 e Stress is defined as the ratio of the perpendicular force, F to the cross-sectional area, A. OR F stress, A Where F : the force act perpendicu lar to the cross section 5 A : cross - sectional area PHYSICS CHAPTER 12 This type of stress is called tensile stress. Stress is a scalar quantity. The unit for stress is kg m1 s2 or N m2 or pascal (Pa). Strain ( ) is defined as the ratio of extension (elongation), e to original length, l0 . Where OR Strain, e l0 l l0 e : extension (elongation) l0 l : final length l0 : original (initial) length This type of strain is called tensile strain. Strain is a scalar quantity and dimensionless (no unit). 6 PHYSICS CHAPTER 12 12.1.3 Force-extension and stress-strain graphs Graphs for metal (ductile material) Plastic deformation Force, F Elastic deformation B Extension, e D E E D Plastic deformation C A A T OT Extension, e O Figure 12.8a C B Elastic deformation Force, F Figure 12.8b 7 PHYSICS CHAPTER 12 Stress , Elastic deformation B Plastic deformation D E C A OT Description Figure 12.8c Strain, A : proportionality limit B : elastic limit C : yield point D : point of maximum force (stress) 8 E : fracture (breaking) point PHYSICS CHAPTER 12 Explanation for Figures 12.8a, 12.8b and 12.8c OA - The force (stress) increases linearly with the extension (strain) until point A. Point A is the proportionality limit. - The straight line graph (OA) obeys Hooke’s law which states “Below the proportionality limit, the restoring force, Fs is directly proportional to the extension, e.” Fs ke where k : force (Hooke) constant B The negative sign indicates that the restoring force is the opposite direction to increasing extension. - This is the elastic limit of the material. - Beyond this point, the material is permanently stretched and will never regain its original shape and length. If the force (stress) is removed, the material has a permanent extension of OT. - The area between the two parallel line (AO and CT) represents the work done to produce the permanent extension OT. - OB region is known as elastic deformation. 9 PHYSICS C CHAPTER 12 - The yield point marked a change in the internal structure of the material. - The plane (layer) of the atoms slide across each other resulting in a sudden increase in extension and the material thins uniformly. oThis is because of the molecular structure is distorted. oThe plane (layer) of the atoms slide across each other resulting in a sudden increase in elongation and the material thins uniformly. oYielding is usually accompanied by ‘thinning’ of the material. before yield point at yield point Thickness of wire decreased 10 PHYSICS CDE D E CHAPTER 12 - This region is known as plastic deformation. - When the force (stress) increases, the extension (strain) increases rapidly. - The force (stress) on the material is maximum and is known as the breaking force (stress). This is sometimes called the Ultimate Tensile Strength (UTS). - This is the point where the material breaks or fractures. Ductile materials Brittle materials - undergo plastic deformation before breaking. - such as steel, copper, aluminium. - do not show plastic behaviour (deformation). - such as glass. 11 PHYSICS CHAPTER 12 Figure 12.9 shows the stress-strain graphs for various materials. Stress , Steel Glass Copper Aluminium O Strain, ε Figure 12.9 12 PHYSICS CHAPTER 12 Graph for rubber (elastic material) Stress , X 1 increasing stress W decreasing stress Y O Figure 12.10 ε1 ε 2 Strain, ε 13 PHYSICS CHAPTER 12 Explanation for Figure 12.10 Rubber undergoes elastic deformation. It is able to regain its original shape and length when the stress is removed but does not obey Hooke’s law. The strain produced when decreasing the stress (XY) is greater than the strain produced when increasing the stress (WX) as shown in Figure 12.10. The shaded area is called the hysteresis loop and it represents the energy loss per unit volume. This energy lost in the form of heat dissipation. 14 PHYSICS CHAPTER 12 Learning Outcome: 12.2 Young modulus (1 hour) At the end of this chapter, students should be able to: Define and use Young’s modulus formulae. Explain relationship between Young’s modulus and Hooke’s law. Derive and use strain energy, 1 U Fe 2 Deduce strain energy from the Fe graph and the stressstrain graph. 15 PHYSICS CHAPTER 12 12.2 Young’s Modulus is defined as the ratio of the tensile stress to the tensile strain if the proportionality limit has not been exceeded. OR Tensile stress Y Tensile strain Y F A e l 0 Y F l0 Ae It is a scalar quantity. The unit of Young modulus is kg m1 s2 or N m2 or Pa. 16 PHYSICS CHAPTER 12 Young’s modulus does not depend to the length of the wire but it depend to the material made the wire. Young’s modulus does not change if the length of the wire is increase or decrease. Table 12.2 shows the value of Young modulus for various material. Material Y (GPa) Aluminium 69 Copper 110 Steel 200 Nylon 3.7 Glass 70 Table 12.2 17 PHYSICS CHAPTER 12 Relationship between force constant, k and Young modulus, Y for a wire From the statement of Hooke’s law and definition of Young modulus, thus and F ke YAe F l0 YAe ke l0 k YA l0 18 PHYSICS CHAPTER 12 12.2.5 Strain energy When a wire is stretched by a load (force), work is done on the wire and strain (elastic potential) energy is stored within. Consider the force-extension graph of this wire until the proportionality limit ( Hooke’s law) as shown in Figure 12.11. Force Proportionality limit F Strain energy 0 Figure 12.11 e extension 19 PHYSICS CHAPTER 12 The total work done, W in stretching a wire from 0 to e is given e by W Fde Shaded Area 0 W strain energy 1 Fe 2 From the definitions of tensile stress and tensile strain, thus F stress F (stress ) A A e e (strain )l0 strain l0 strain energy strain energy volume 1 2 1 (stress )(strain ) Al0 Volume (stress )(strain ) 2 20 PHYSICS CHAPTER 12 This strain energy per unit volume is the area under the stress-strain graph until the proportionality limit (straight line graph) as shown in Figure 12.12. Stress Proportionality limit Strain energy per unit volume 0 Strain Figure 12.12 21 PHYSICS CHAPTER 12 Example 12.3 : A thin steel wire initially 1.5 m long and of diameter 0.50 mm is suspended from a rigid support. A mass of 3 kg is attached to the lower end of the wire. Calculate a. the extension of the wire, b. the energy stored in the wire. (Young’s modulus for steel = 2.0 1011 N m2) 3 Solution : m 3 kg; l0 1.5 m; d 0.5 10 m Y 2.0 10 N m 11 2 22 PHYSICS CHAPTER 12 Solution : m 3 kg; l0 1.5 m; d 0.5 10 Y 2.0 10 N m 11 2 3 m 23 PHYSICS CHAPTER 12 Example 12.4 : A copper wire LM is fused at one end, M to an iron wire MN as shown in figure below. L M N F The copper wire has length 0.90 m and cross-section area 0.90 106 m2. The iron has length 1.40 m and cross-section area 1.30 106 m2. The compound wire is stretched and the total length increases by 0.01 m. Determine a. the ratio of the extension of copper wire to the extension of iron wire, b. the extension of each wire, c. the applied force to the compound wire. (Given Y iron = 2.10 1011 Pa ,Y copper = 1.30 1011 Pa ) 24 PHYSICS CHAPTER 12 Solution :l0C 0.90 m; AC 0.90 10 6 m 2 ; l0I 1.40 m; AI 1.30 10 6 m ; e total 0.01 m; 2 YC 1.30 10 Pa; YI 2.10 10 Pa; 11 11 PHYSICS Solution : CHAPTER 12 PHYSICS CHAPTER 12 Exercise 12.1 : 1. A support cable on a bridge has an area of cross-section of 0.0085 m2 and a length of 35 m. It is made of high tensile steel whose Young’s modulus is 2.8 1011 Pa. The tension in the cable is 720 kN. Calculate a. the extension of the cable. b. the strain energy stored in the cable. ANS. : 0.0106 m; 3.81 kJ 2. A wire of length 0.50 m is fixed horizontally between two supports separated by 0.50 m. When a mass of 8.0 kg hangs from the middle of the wire, the mid-point sags by 1.00 cm. The diameter of the wire is 2.8 mm. Calculate the Young’s modulus of the wire. (Given g = 9.81 m s2) ANS. : 1.99 1011 Pa 27 PHYSICS CHAPTER 12 THE END… Next Chapter… CHAPTER 13 : Heat 28