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JJ310 STRENGTH OF MATERIAL Chapter 5(a) Beam Deflection

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JJ310 STRENGTH OF MATERIAL
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CHAPTER 5 (a) BEAM DEFLECTION 1
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  • CHAPTER 5 (a)

    BEAM DEFLECTION

    *

  • Learning Outcomes:At the end of this lecture, student should be able to;

    Understand beam deflectionExplain double integration methodState the boundary condition for simply supported beamDetermine the slope and deflection in every loaded situation as below:Simply support, with concentrated load at center of the beam.Simply support, with uniform distributed load.

    *

  • Beam Deflection Beam deflection is defined as the distance from the neutral plane origin to the position of neutral plane when the load is applied.

    ymaxF = Load y = DeflectionNeutral axis originNeutral axis after load applied*

  • General Formula M = EI d2y Moment Equation dx2

    Where;M = Moment (Nm) I = Second moment of area @ moment inertia (m4)E = Young Modulus (Pa)

    * EI also known as flexural rigidity

    *

  • Double Integration Method

    EI d2y = M (Moment Equation) dx2 If the beam has uniform cross-section and M can be expressedmathematically as x function, therefore;

    EI dy = Mdx + A (Slope Equation) dx

    EIy = Mdx + Ax + B (Deflection Equation)

    Notes: dy/dx = Slope (no unit) y = Deflection (m or mm)

    *

  • Case 1: Simply supported beam, with concentrated load at center (boundary conditions included)

    Consider this simply supported beam AB, with length L and carry the concentrated load at center. Take A as the reference point and by balancing the moment and force we get;

    RA = RB = F/2

    On the x-x section (distance x is based on point A), it is known that the moment at this section is;M xx = Fx / 2ABx = Ldy/dx = maxy = 0x = 0dy/dx = maxy = 0 x = L/2dy/dx = 0y = max

    xx*

  • General Formula

    a) EI d2y = M (Moment Eq.) dx2

    b) EI dy = Mdx + A (Slope Eq.) dx

    c) EIy = Mdx + Ax + B (Deflection Eq.)

    Solution

    Substitute M = Fx / 2 into eq. (a)

    EI d2y = Fx / 2 dx2

    Integrate once we get;

    EI dy = Fx2 + A dx 4

    Integrate once again we get;

    EIy = Fx3 + Ax + B 12

    *

  • Boundary Conditionsa) To find the variables A and BEI dy = Fx2 + A .. (Slope Eq.) dx 4

    When; x = L/2 , dy/dx = 0

    Thus;EI (0) = F(L/2)2 + A 4 A = - FL2 16*

  • EIy = Fx3 + Ax + B (Deflection Eq.) 12

    Substitute A = - FL2 16

    EIy = Fx3 FL2x + B 12 16

    When; x = 0, y = 0

    Thus;EI (0) = F(0)3 FL2(0) + B 12 16 B = 0

    *

  • Therefore, the COMPLETE slope and deflection equations are;

    i) EI dy = Fx2 - FL2 . (Slope Eq.) dx 4 16

    ii) EIy = Fx3 FL2x ..... (Deflection Eq.) 12 16

    *

  • b) To find the Maximum slope and deflection

    i)Maximum Slope

    EI dy = Fx2 - FL2 dx 4 16

    When; x = 0,x = L

    EI dy = F(0)2 - FL2 dx 4 16

    dy = - FL2dx16EI

    -ve sign indicates that the deflections is below the undeformed neutral axis *

  • ii) Maximum deflection

    EIy = Fx3 FL2x 12 16

    When;x = L/2

    EIy = F(L/2)3 FL2 (L/2) 12 16

    EIy = - FL3 48

    y = - FL3 48EI

    -ve sign indicates that the deflections is below the undeformed neutral axis *

  • Case 2: Simply supported beam, with uniformly distributed load (boundary conditions included)

    Consider this simply supported beam AB, with length L and carry the uniformly distributed load along the beam. Take A as the reference point and by balancing the moment and force we get;

    RA = RB = FL/2

    On the x-x section (distance x is based on point A), it is known that the moment at this section is;M xx = wLx / 2 Wx2/2ABx = Ldy/dx = maxy = 0x = 0dy/dx = maxy = 0 x = L/2dy/dx = 0y = max

    xx*

  • General Formula

    a) EI d2y = M (Moment Eq.) dx2

    b) EI dy = Mdx + A (Slope Eq.) dx

    c) EIy = Mdx + Ax + B (Deflection Eq.)

    Solution

    Substitute M = wLx wx2 into eq. (a)2 2

    EI d2y = wLx wx2 dx2 2 2

    Integrate once we get;

    EI dy = wLx2 - wx3 + A dx 4 6

    Integrate once again we get;

    EIy = wLx3 wx4 + Ax + B 12 24

    *

  • Boundary Conditionsa) To find the variables A and BEI dy = wLx2 - wx3 + A .. (Slope Eq.) dx 4 6

    When; x = L/2 , dy/dx = 0

    Thus;EI (0) = wL(L/2)2 w(L/2)3 + A 4 6 A = - wL3 24*

  • EIy = wLx3 wx4 + Ax + B (Deflection Eq.) 12 24

    Substitute A = - wL3 24

    EIy = wLx3 wx4 wL3x + B 12 24 24

    When; x = 0, y = 0

    Thus;EI (0) = wL(0)3 w(0)4 wL3(0) + B 12 24 24 B = 0

    *

  • Therefore, the COMPLETE slope and deflection equations are;

    i) EI dy = wLx2 - wx3 wL3 . (Slope Eq.) dx 4 6 24

    ii) EIy = wLx3 wx4 wL3x ..... (Deflection Eq.) 12 24 24

    *

  • b) To find the Maximum slope and deflection

    i)Maximum Slope

    EI dy = wLx2 - wx3 - wL3 dx 4 6 24

    When x = 0,EI dy = wL(0)2 - w(0)3 wL3 dx 4 6 24

    dy = - wL3 dx 24EI

    When x = LEI dy = wL(L)2 - w(L)3 wL3 dx 4 6 24

    dy = + wL3 dx 24EI

    +ve sign indicates that the deflections is above the undeformed neutral axis *

  • ii) Maximum deflection

    EIy = wLx3 wx4 wL3x 12 24 24

    When;x = L/2

    EIy = wL(L/2)3 w(L/2)4 - wL3(L/2) 12 24 24

    EIy = - 5wL4 384

    y = - 5wL4 384EI

    -ve sign indicates that the deflections is below the undeformed neutral axis *

  • Exercise1. A simply supported beam is 4m long and has a load of 200KN at the middle. The flexural stiffness is 300MPa. Calculate the slope at the ends and the deflection at the middle. (Answer: 6.67 x 10-4 , 0.89 mm)

    2. A simply supported beam is 8m long with a load of 500KN at the middle. The deflection at the middle is 2 mm downwards. Calculate the slope at the ends. (Answer : 750 x 10-6)

    3. A simply supported beam is 4m long with a UDL of 4KN/m. The dimension of the beam is 300mm x 100mm. Calculate the maximum slope and deflection. Given E = 200 GPa. (Answer: 2.13 x 10-3 , 2.7 x 10-3m)

    4. A simply supported beam is 5m long with UDL of 200 N/m. The flexural stiffness is 100MPa. Calculate the slope at the ends and the deflection at middle. (Answer: 1.04 x 10-5, 1.63 x 10-5 m*


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