# MECHANICAL PRINCIPLES HNC/D PRELIMINARY LEVEL TUTORIAL 1 BASIC STUDIES OF STRESS AND STRAIN

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1 MECHANICAL PRINCIPLES HNC/D PRELIMINARY LEVEL TUTORIAL 1 BASIC STUDIES O STRESS AND STRAIN This tutorial is essential for anyone studying the group of tutorials on beams. Essential pre-requisite knowledge for Edexcel HNC Mechanical Principles UNIT 4 outcome. Essential pre-requisite knowledge for the Engineering Council Diploma exam D09 Mechanics of Solids. Essential pre-requisite knowledge for the Engineering Council Certificate Exam C105 Mechanical and Structural engineering. Covers part of the syllabus for the Engineering Council Certificate Exam C103 Engineering Science. You should judge your progress by completing the self assessment exercises. These may be sent for marking at a cost (see home page). On completion of this tutorial you should be able to do the following. Define direct stress and strain. Define shear stress and strain. Define the modulus of elasticity and rigidity. Solve basic problems involving stress, strain and modulus. It is assumed that the student is already familiar with the concepts of ORCE. D.J.DUNN 1

2 1. DIRECT STRESS When a force is applied to an elastic body, the body deforms. The way in which the body deforms depends upon the type of force applied to it. A compression force makes the body shorter. igure 1 A tensile force makes the body longer. igure Tensile and compressive forces are called DIRECT ORCES. Stress is the force per unit area upon which it acts. Stress = = orce/area N/m or Pascals. The symbol is called SIGMA NOTE ON UNITS The fundamental unit of stress is 1 N/m and this is called a Pascal. This is a small quantity in most fields of engineering so we use the multiples kpa, MPa and GPa. Areas may be calculated in mm and units of stress in N/mm are quite acceptable. Since 1 N/mm converts to N/m then it follows that the N/mm is the same as a MPa D.J.DUNN

3 . DIRECT STRAIN In each case, a force produces a deformation x. In engineering we usually change this force into stress and the deformation into strain and we define these as follows. Strain is the deformation per unit of the original length Strain = = x/l The symbol is called EPSILON Strain has no units since it is a ratio of length to length. Most engineering materials do not stretch very much before they become damaged so strain values are very small figures. It is quite normal to change small numbers in to the exponent for of Engineers use the abbreviation (micro strain) to denote this multiple. or example a strain of could be written as 68 x 10-6 but engineers would write 68. Note that when conducting a British Standard tensile test the symbols for original area are S o and for Length is L o. WORKED EXAMPLE No.1 A metal wire is.5 mm diameter and m long. A force of 1 N is applied to it and it stretches 0.3 mm. Assume the material is elastic. Determine the following. i. The stress in the wire. ii. The strain in the wire. πd A 4 σ A π x mm.44 N/mm Answer (i) is hence.44 MPa x 0.3 mm or 150 L 000 D.J.DUNN 3

4 SEL ASSESSMENT EXERCISE No.1 1. A steel bar is 10 mm diameter and m long. It is stretched with a force of 0 kn and extends by 0. mm. Calculate the stress and strain. (Answers 54.6 MPa and 100 ). A rod is 0.5 m long and 5 mm diameter. It is stretched 0.06 mm by a force of 3 kn. Calculate the stress and strain. (Answers 15.8 MPa and 10) 3. MODULUS O ELASTICITY E Elastic materials always spring back into shape when released. They also obey HOOKE'S LAW. This is the law of a spring which states that deformation is directly proportional to the force. /x = stiffness = k N/m igure 3 The stiffness is different for different materials and different sizes of the material. We may eliminate the size by using stress and strain instead of force and deformation as follows. If and x refer to direct stress and strain then = A x = L hence x σa εl L and Ax The stiffness is now in terms of stress and strain only and this constant is called the MODULUS of ELASTICITY and it has a symbol E. L E Ax A graph of stress against strain will be a straight line with a gradient of E. The units of E are the same as the units of stress. D.J.DUNN 4

5 4. ULTIMATE TENSILE STRESS If a material is stretched until it breaks, the tensile stress has reached the absolute limit and this stress level is called the ultimate tensile stress. Values for different materials may be found in various sources such as the web site Matweb. WORKED EXAMPLE No. A steel tensile test specimen has a cross sectional area of 100 mm and a gauge length of 50 mm, the gradient of the elastic section is 410 x 10 3 N/mm. Determine the modulus of elasticity. The gradient gives the ratio /A = and this may be used to find E. σ L 3 50 E x 410 x 10 x N/mm or MPaor 05 GPa ε x A 100 WORKED EXAMPLE No.3 A Steel column is 3 m long and 0.4 m diameter. It carries a load of 50 MN. Given that the modulus of elasticity is 00 GPa, calculate the compressive stress and strain and determine how much the column is compressed. πd π x 0.4 A 0.16 m x10 6 σ x10 Pa A σ σ x10 E so ε ε E 00 x10 x ε so x ε L x 3000 mm 5.97 mm L D.J.DUNN 5

6 SEL ASSESSMENT EXERCISE No. 1. A bar is 500 mm long and is stretched to 505 mm with a force of 50 kn. The bar is 10 mm diameter. Calculate the stress and strain. The material has remained within the elastic limit. Determine the modulus of elasticity. (Answers MPa, 0.01 and GPa.. A steel bar is stressed to 80 MPa. The modulus of elasticity is 05 GPa. The bar is 80 mm diameter and 40 mm long. Determine the following. i. The strain. ( ) ii. The force. (1.407 MN) 3. A circular metal column is to support a load of 500 Tonne and it must not compress more than 0.1 mm. The modulus of elasticity is 10 GPa. the column is m long. Calculate the cross sectional area and the diameter. (0.467 m and m) Note 1 Tonne is 1000 kg. D.J.DUNN 6

7 5. SHEAR STRESS Shear force is a force applied sideways on to the material (transversely loaded). This occurs typically: when a pair of shears cuts a material when a material is punched igure 4 igure 5 when a beam has a transverse load. when a pin carries a load. igure 6 igure 7 Shear stress is the force per unit area carrying the load. This means the cross sectional area of the material being cut, the beam and pin respectively. Shear stress = /A The symbol is called Tau D.J.DUNN 7

8 The sign convention for shear force and stress is based on how it shears the materials and this is shown below. igure 8 In order to understand the basic theory of shearing, consider a block of material being deformed sideways as shown. 6. SHEAR STRAIN igure 9 The force causes the material to deform as shown. The shear strain is defined as the ratio of the distance deformed to the height x/l. The end face rotates through an angle. Since this is a very small angle, it is accurate to say the distance x is the length of an arc of radius L and angle so that = x/l It follows that is the shear strain. The symbol is called Gamma. D.J.DUNN 8

9 7. MODULUS O RIGIDITY G If we were to conduct an experiment and measure x for various values of, we would find that if the material is elastic, it behave like a spring and so long as we do not damage the material by using too big a force, the graph of and x is a straight line as shown. The gradient of the graph is constant so /x = constant and this is the spring stiffness of the block in N/m. If we divide by the area A and x by the height L, the relationship is still a constant and we get A x L L Ax constant igure 10 x L τ But /A = and x/l = so constant A L Ax γ This constant will have a special value for each elastic material and is called the Modulus of Rigidity with symbol G. 8. ULTIMATE SHEAR STRESS τ γ If a material is sheared beyond a certain limit it becomes permanently distorted and does not spring all the way back to its original shape. The elastic limit has been exceeded. If the material is stressed to the limit so that it parts into two(e.g. a guillotine or punch), the ultimate limit has been reached. The ultimate shear stress is u and this value is used to calculate the force needed by shears and punches. G WORKED EXAMPLE No.4 Calculate the force needed to guillotine a sheet of metal 5 mm thick and 0.8 m wide given that the ultimate shear stress is 50 MPa. The area to be cut is a rectangle 800 mm x 5 mm A 800 x mm A so The ultimate shear stressis 50 N/mm x A 50 x N or 00 kn D.J.DUNN 9

10 WORKED EXAMPLE No.5 Calculate the force needed to punch a hole 30 mm diameter in a sheet of metal 3 mm thick given that the ultimate shear stress is 60 MPa. The area to be cut is the circumference x thickness πd x t A π x 30 x mm A so The ultimate shear stressis 60 N/mm x A 60 x N or kn WORKED EXAMPLE No.6 Calculate the force needed to shear a pin 8 mm diameter given that the ultimate shear stress is 60 MPa. The area to be sheared is the circular area A x 8 A 4 so A 50.6mm πd 4 The ultimate shear stressis 60 N/mm x A 60 x N or kn D.J.DUNN 10

11 SEL ASSESSMENT EXERCISE No.3 1. A guillotine must shear a sheet of metal 0.6 m wide and 3 mm thick. The ultimate shear stress is 45 MPa. Calculate the force required. (Answer 81 kn). A punch must cut a hole 30 mm diameter in a sheet of steel mm thick. The ultimate shear stress is 55 MPa. Calculate the force required. (Answer10.37 kn) 3. Two strips of metal are pinned together as shown with a rod 10 mm diameter. The ultimate shear stress for the rod is 60 MPa. Determine the maximum force required to break the pin. (Answer 4.71 kn) igure 11 D.J.DUNN 11

12 9. DOUBLE SHEAR Consider a pin joint with a support on both ends as shown. This is called a CLEVIS and CLEVIS PIN. If the pin shears it will do so as shown. By balance of forces, the force in the two supports is / each. The area sheared is twice the cross section of the pin so it takes twice as much force to break the pin as for a case of single shear. Double shear arrangements doubles the maximum force allowed in the pin. igure 1 WORKED EXAMPLE No.7 A pin is used to attach a clevis to a rope. The force in the rope will be a maximum of 60 kn. The maximum shear stress allowed in the pin is 40 MPa. Calculate the diameter of a suitable pin. The pin is in double shear so the shear sress is A τ x 40x10 d A 750 mm 4 d 4 x 750 π mm 750 x 10 6 m A D.J.DUNN 1

13 SEL ASSESSMENT EXERCISE No.4 1. A clevis pin joint as shown above uses a pin 8 mm diameter. The shear stress in the pin must not exceed 40 MPa. Determine the maximum force that can be exerted. (Answer 4.0 kn). igure 13 A rope coupling device shown uses a pin 5 mm diameter to link the two parts. If the shear stress in the pin must not exceed 50 MPa, determine the maximum force allowed in the ropes. (Answer 1.96 kn) INAL NOTE Shear stress and modulus of rigidity are important in the studies of twisting of shafts and this is covered in anther tutorial. D.J.DUNN 13

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