ENG2000 Chapter 7 Beams. ENG2000: R.I. Hornsey Beam: 1

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1 ENG2000 Chapter 7 Beams ENG2000: R.I. Hornsey Beam: 1

2 Overview In this chapter, we consider the stresses and moments present in loaded beams shear stress and bending moment diagrams We will also look at what happens when a beam is deformed in terms of the axial stress in the deformed beam and the flexural rigidity of a beam The chapter will finish by considering the failure of a column due to an axial compressive force buckling ENG2000: R.I. Hornsey Beam: 2

3 Beams with concentrated loads A beam is defined as a slender structural member For trusses we assumed that what happened in the members was unimportant to the system although the nature of the members clearly affects the strength of a truss here we look at what happens when beams are loaded We will look at the internal forces axial and shear and moments in the loaded beam Three types of beam are statically determinate ENG2000: R.I. Hornsey Beam: 3

4 simply supported beam cantilever beam combination beam ENG2000: R.I. Hornsey Beam: 4

5 Cantilever Free body diagram of the cantilever ENG2000: R.I. Hornsey Beam: 5

6 If we cut the beam at an arbitrary point, we can determine the system of forces and moments required to maintain equilibrium This system must include axial, shear and moment ENG2000: R.I. Hornsey Beam: 6

7 Sign conventions ENG2000: R.I. Hornsey Beam: 7

8 Shear force & bending moment diagrams In order to determine whether the beam can support the loads required, we need to determine the distribution of stress in the beam i.e. P, V, and M as a function of x Let s take the following example: we first cut the beam at an arbitrary location between the left end and the force and then the other side of the force ENG2000: R.I. Hornsey Beam: 8

9 For 0 < x < 2L/3 P = 0 V = F/3 M = Fx/3 For 2L/3 < x < L P = 0 V = - 2F/3 M = (2F/3)(L - x) ENG2000: R.I. Hornsey Beam: 9

10 Diagrams ENG2000: R.I. Hornsey Beam: 10

11 General equations For a generalised distributed load of w(x) N/m: dp dx = 0 (no axial force) dv dx = w (shear increases with x) dm dx = V (moment = shear x distance) ENG2000: R.I. Hornsey Beam: 11

12 A simple beam, such as this firewood, snaps when a moment is applied to each end Similarly, structural members can deform or fail due to bending moments This will allow us to calculate the distribution of axial stress Stresses in beams ENG2000: R.I. Hornsey Beam: 12

13 Geometry of deformation We will consider the deformation of an ideal, isotropic prismatic beam the cross section is symmetric about y-axis All parts of the beam that were originally aligned with the longitudinal axis bend into circular arcs plane sections of the beam remain plane and perpendicular to the beam s curved axis Note: we will take these directions for M 0 to be positive. However, they are in the opposite direction to our convention (Beam 7), and we must remember to account for this at the end. ENG2000: R.I. Hornsey Beam: 13

14 Neutral axis ENG2000: R.I. Hornsey Beam: 14

15 Concrete While we are mostly assuming beams made of steel or other metals, many means are made of concrete and concrete does not support a tensile stress For concrete beams, we assume that only the material on the compressive side of the neutral axis actually carries a load ENG2000: R.I. Hornsey Beam: 15

16 One solution to this is pre-stressed concrete where metal bars set within the concrete are pre-stressed to provide an initial compression to the concrete beam so it can withstand some tension, until the pre-stress is overcome The yellow guidelines highlight the camber (upward curvature) of a pre-stressed double T. The pre-stressing strands can be seen protruding from the bottom of the beam, with the larger strands at the bottom edge. The tension is these strands produces the camber, the beam is straight when cast. ENG2000: R.I. Hornsey Beam: 16

17 Expression for stress If we take a small element of width dx, and deform the beam ρ is the radius of the neutral axis at y = 0 (neutral axis), dx remains unchanged dx is width at y Hence we can write a strain ε x = (dx - dx)/dx = (dx /dx) - 1 Also dx = ρdθ and dx = (ρ - y)dθ ENG2000: R.I. Hornsey Beam: 17

18 Hence d x dx =1 y x = y leading to Which tells us that the extension parallel to the beam axis is linearly related to the distance form the neutral axis and the sign indicates compression for positive y, i.e. below the neutral axis We can now calculated the stress assuming no additional loads just the moment x = Ey ENG2000: R.I. Hornsey Beam: 18

19 Hence we can sketch of the stress normal to the axis of the beam ENG2000: R.I. Hornsey Beam: 19

20 Location of neutral axis The previous analysis used, but did not relate to the applied moment and we don t know where the neutral axis is located either Imagine that we cut the beam at some point Since the moment M 0 does not exert a net force the sum total of the stress at the cut section must also be zero ENG2000: R.I. Hornsey Beam: 20

21 Expressed mathematically da = 0 A x where A is the area of the beam s cross section Substituting in for x, yda = 0 Recall that the centre of mass is given by y com = ( y dm)/m A For a geometric shape, the equivalent point is the centroid, given by yda yda y = A A = A da Hence the neutral axis (at y = 0) passes through the beam s centroid ENG2000: R.I. Hornsey Beam: 21 A

22 Relating stress to applied moment For the free body diagram of the chopped beam, the sum of moments must also be zero for equilibrium For an elemental area of the cross section, the moment about the z-axis is y x da Hence the total moment for the segment is y da M 0 = 0 A x ENG2000: R.I. Hornsey Beam: 22

23 Using x = Ey we find that: 1 = M 0 EI where I = A y 2 da I is a very important figure of merit for a beam s shape, known as the moment of inertia Hence x = M 0 y I ENG2000: R.I. Hornsey Beam: 23

24 Conventional directions We have to revert to our convention for the positive direction of moments see Beam 7 and Beam 13 by letting M = -M 0 Hence, our equations are as follows Radius of curvature 1 M = EI positive ρ means the positive y-axis is on the concave side of the neutral axis EI is known as the flexural rigidity of the beam Extensional strain Normal stress x = y = My EI x = My I ENG2000: R.I. Hornsey Beam: 24

25 Interpretation of moment of inertia What does the moment of inertia and flexural rigidity, EI mean? Essentially, this says that the beam is stiffer if the material in the beam is located further away from the centroid (neutral axis) so any area, da, is more effective at stiffening the beam depending on the square of the distance hence, if you want to make a strong beam with little material, make sure that the material is as far as possible from the centroid hence, I beams I = A y 2 da ENG2000: R.I. Hornsey Beam: 25

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28 Parallel axis theorem If we know I for a particular axis, we can calculate the value for a different parallel axis in a straightforward way I x = I x + d y 2 A I y = I y + d x 2 A where I x,y are the moments about one set of axes and d x,y are the distances to the new set of axes y d x y d y A x x ENG2000: R.I. Hornsey Beam: 28

29 Summary so far So we can now calculate stresses and moments within a beam, and we know how the beam shape effects the stress Calculation of the deformed shape of the beam is possible, but beyond the scope of this course essentially, the ways in which the ends of the beam are ixed determines the deformed shape by providing boundary conditions to the differential equations relating deformation to load see chapter 9 of Riley However, we did say earlier that buckling of long slender beams is also important which is why we need trusses in the first place ENG2000: R.I. Hornsey Beam: 29

30 Buckling of columns Imagine a hacksaw blade s y = 520Mpa cross section is 12mm x 0.5mm so the blade should withstand a compression of 3120N 300kg However it is easy to cause the blade to fail ENG2000: R.I. Hornsey Beam: 30

31 Euler buckling Buckling is a geometric instability that causes a structural column to fail well before its ultimate load Let us assume a column has already deformed due to an axial load and we will determine the force we need to maintain equilibrium Cutting the beam at an arbitrary point gives us ENG2000: R.I. Hornsey Beam: 31

32 Here M = Pv where v is the beam s deflection It turns out that d 2 v dv 2 = M EI so d 2 v dv v = 0 where 2 = P EI ENG2000: R.I. Hornsey Beam: 32

33 The general solution to such a differential equation is where B and C are determined by the boundary conditions At x = 0, v = 0 so C = 0 v = Bsin x + C cos x Also v = 0 at x = L so Bsin λl = 0, or sin λl = 0, if the beam is deformed (v 0) The condition is now satisfied if where n is an integer = n L ENG2000: R.I. Hornsey Beam: 33

34 Hence P = n2 L 2 This represents a number of sinusoidal deformations with different wavelengths buckling modes 2 EI v = Bsin n x L We are looking for the minimum force to cause deformation, i.e. n = 1 P = 2 EI L 2 ENG2000: R.I. Hornsey Beam: 34

35 Note that the deformation is dependent on B but we consider the buckling load to be the force to cause an arbitrarily small deformation This is known as the Euler buckling load after Leonhard Euler s 1744 formulation We can increase the load required to cause buckling by restricting deflection at the appropriate places along the beam which is essentially what a truss does For the hacksaw blade I = bh 3 /12 (a rectangular section) = 1.25 x m 4 E = 200 GPa & L = 300mm hence P = 2.74N 300 grammes ENG2000: R.I. Hornsey Beam: 35

36 e.g. Cortlandt Street station in New York destroyed on 11 September ENG2000: R.I. Hornsey Beam: 36

37 Summary This completes our brief look at structural mechanics and statics Based on our knowledge of materials science, we pursued a course that explained mechanical properties of materials through to structures We will now return to materials science to explore other macroscopic properties arise from atomic bonding e.g. electronic, thermal, optical, magnetic ENG2000: R.I. Hornsey Beam: 37