lecture 13
DESCRIPTION
Applications to Deformations in StructuresTRANSCRIPT
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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)
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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.
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DBEquating External Work to Internal Strain Energy:Since, in this case, EA is constant for all members,
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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!
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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
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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
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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
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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
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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.
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Strain Energy in Entire BeamIFLdConsider the cantilever beam as shownxy
M=F(x-L)
_1097407676.unknown
_1097407765.unknown
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Deflection ILdxyFExternal Work,Strain EnergyLinear-elastic,F dClassical Solution
=
_1097407826.unknown
_1097522656.unknown
_1097522689.unknown
_1097522704.unknown
_1097407857.unknown
_1097407765.unknown
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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.
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yL/2L/2PDBDetermine DB.
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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
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Elastic Strain Energy due to Transverse Shear Stressyx d = gxya txygxy
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Shear Strain EnergyxydxdAzyF(x)f is called a form factor:Circle f=1.11Rectangle f=1.2Tube f=2.00I section f=A/Aweb
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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.
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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