lecture 13

18
Applications to Deformations in Structures AE PL AE L P U ; 2 2 A P L ernal Work done by forces on structure = internal Strain Ener Consider the truss shown at the right: External Work =½F where = deflection at B. All 7 members have same AE (axial

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Applications to Deformations in Structures

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  • Applications to Deformations in StructuresAPLdExternal Work done by forces on structure = internal Strain EnergyConsider the truss shown at the right: External Work =FD where D = deflection at B.All 7 members have same AE (axial stiffness)

  • This assumes that the system is linear-elastic, and therefore the deflection D is a linear function of F.D, Deflection at BLoad, FThe total strain energy stored in the system is the sum of the individual strain energies in each of the truss members numbered i=1 to 7.

  • DBEquating External Work to Internal Strain Energy:Since, in this case, EA is constant for all members,

  • Try it!A lightweight aluminum truss, E=70000 MPa, has a height, Lo=1m, and is made of tubular stock with a cross sectional area of 250 mm2. Determine the deflection at B when the load, F=20kN.OK!..

    Lets use an Energy method!

  • Solution:Solve the truss using statics to determine the forces in each member:Note: It doesnt matter if the axial load is compressive or tensile, both add to the total strain energy since the P term is squared.

    Forces

    Length of Members

    Pi2Li

    P1=-F

    L1=L0

    F2 L0

    P2=

    L2=

    2

    L0

    P3=-F

    L3=L0

    F2 L0

    P4=-2F

    L4=L0

    4F2 L0

    P5=

    L5=

    2

    L0

    P6=F

    L6=L0

    F2 L0

    P7=0

    L7=L0

    0

    Sum

    (7+4(2) F2 L0

    _1097407079.unknown

    _1097515264.unknown

    _1097515386.unknown

    _1097515444.unknown

    _1097515361.unknown

    _1097407100.unknown

    _1097407047.unknown

  • OK, already find the deflection.What is the maximum stress in the truss?P4 =-2F=40kN (compression)S=P/A = 40000/250 = 160 MPa assumptions about linear elasticity are OK, if Sy>160MPa

  • Beam Elements:yxydxdAzyF(x)A beam that is symmetrical in x-section about the z-axis, is subjected to bending. Consider a infinitesimal volume element of length dx and area dA as shown. This element is subjected to a normal stress: sx=My/IThe Strain Energy Density on this element is:

    For linear elastic material

  • Substituting, and multiplying by the Volume of the elementHence, the Strain Energy for a slice of the beam, of width dx, isyxdx

    _1097407435.unknown

    _1097407608.unknown

    _1097407347.unknown

  • Assumptions.There is no axial force on the element (case of pure bending)The shear stress & strain on the element is relatively small, and hence the contribution of shear strain energy is negligible.These assumptions are generally valid for long slender beams.

  • Strain Energy in Entire BeamIFLdConsider the cantilever beam as shownxy

    M=F(x-L)

    _1097407676.unknown

    _1097407765.unknown

  • Deflection ILdxyFExternal Work,Strain EnergyLinear-elastic,F dClassical Solution

    =

    _1097407826.unknown

    _1097522656.unknown

    _1097522689.unknown

    _1097522704.unknown

    _1097407857.unknown

    _1097407765.unknown

  • Try it!yxPL/2L/2Shear ForcePL/4P/2-P/2MomentDetermine Elastic Strain Energy due to bending for simply supported 3-point bending member of constant X-section.For 0 xL/2: M=Px/2Note by symmetry we can find the total strain energy by doubling the strain energy of the LHS.

  • yL/2L/2PDBDetermine DB.

  • DB can be determined by an energy method:.

    Find the Deflection for the x-section shown: L=2m, P=20 kN; h=50mm, b=20mm, SAE1045 Steel, E=200,000 MPa, Sy=400MPab=20 mmh=50mmzyIzz=bh3/12< Sy , OK

  • Elastic Strain Energy due to Transverse Shear Stressyx d = gxya txygxy

  • Shear Strain EnergyxydxdAzyF(x)f is called a form factor:Circle f=1.11Rectangle f=1.2Tube f=2.00I section f=A/Aweb

  • Try it.yxPL/2L/2Shear ForcePL/4P/2-P/2MomentDetermine Elastic Strain Energy due to shear strain for simply supported 3-point bending member of constant X-section.For 0 xL/2: T=P/2Note by symmetry we can find the total strain energy by doubling the strain energy of the LHS.

  • bmmh=2czyIzz=bh3/12A=bhfor rectangle x-sectionFor most metals G0.4E we find that:And for slender beam, L/h=10which may be neglected